m s&e&B i JOB? ffitfE W& w& BULLETIN OF THE GEOLOGICAL SOCIET\ 7 OF AMERICA VOL. 4 JOSEPH STANLEY-BROWN, Editor LfBRART NEW YORK ^CiC/^x BOTANICAL ROCHESTER Published by the Society lso:; col MIL FOR 1893 Sir J. William Dawson, President T. C. Chamberlin, \ Vice-Presidents .1. .1. Stevenson, ) II. L. Fairchild, >'<<•/■< /''/•// I. ('. White, Treasurer Class of 1895 E. A. Smith, C. D. Walcott, Class of 1894 Henry S. Williams, X. II. WlNCHELL, Class of 1893 George M. Dawson, John C. Branner, • Members-at-la PRINT] JUDD >V DETWEILER, WASHINGTON, I1 ' NGRAVERS Moss Engraving Co., Puck Building, New York (ii) c:> CONTENTS Page Proceedings of the Fourth Summer Meeting, held at Rochester, August 15 and L6, L892 ; 1 1. L. Fairchild, Secretary 1 Session of Monday, August L5 1 Election of Fellows 1 Studies of the Connecticut Valley Glacier ; by C. 11. Hitchcock..-.. :; Session of Tuesday Morning, August 16 , 8 The Oneonta Sandstone and its Relations to the Portage, Chemung and Catskill Groups (discussion) ; by James Hall 8 Session of Tuesday Afternoon, August 16 9 Conditions of Accumulation of Drumlins (discussion); by Warren UlMIAM \) Ancient Waterways (abstract) ; by A. S. Tiffany 10 Register of the Rochester Meeting 12 Finite homogeneous Strain, Flow and Rupture of Rocks ; by G. F. Becker... 13 The Thickness of the Devonian and Silurian Rucks of central New York ; by C S. Prosser ill A new Tseniopteroid Fern and its Allies ; by David "White 119* Some Elements of land Sculpture ; by L. E. Hicks 133 Some dynamic and metasomatic Phenomena in a metamorphic Conglomerate in the < rreen Mountains; by C. L. Whittle 147 Phases in the Metamorphism of the Schists of southern Berkshire; by W. II. Hobbs U>7 Continental Prohlems; Animal Address by the President, G. K. Gilbert 171) Comparison of Pleistocene and present Ice-sheets ; by Warren Upham 191 Cretaceous and early Tertiary of northern California and Oregon; by J. S. DlLLER 207) On the Geology of natural Gas and Petroleum in southwestern Ontario; by H. P. H. Brumell 225 Notes on the Occurrence of Petroleum in Gaspe, Quebec ; by IT. P. II. Brumell. 241 The Faunas of the Shasta and Chico Formations ; by T. W. Stanton 245 Two Neocene Rivers of California; by Waldemar Lindgren 257 Some Maryland Granites and their ( >rigin ; by C. R. Keyes 299 Epidote as a primary Component of eruptive Rocks ; by C. R. Keyes 305 Relations of the Laurentian and Huronian Rocks north of Lake Huron; by A. E. Barlow 313 The Archean Rocks west of Lake Superior ; by W. 11. ( '. Smith 333 The Laurentian of the Ottawa District ; by R. W. Ells 349 Height of the Bay of Fundy Coast in Hie Glacial Period relative to Sea-level, as evidenced by marine Fossils in the Bowlder-clay at Saint John, New Brunswick ; by Robert Chalmers 361 Proceedings of the Fifth Annual Meeting, held at Ottawa, Canada, December 28, 29 and 30, 1892 ; H. L. Fairchild, S< m tary 371 Session of Wednesday, December 28 372 Report of the Council 372 *-*» (iii) °* IV BULL. GEOL. SOC. AM., VOL. 4. Page Reporl of the Treasurer 376 Election of Officers for 1893 378 Election of Fellows 378 Memorial of Thomas Sterry Hunt (with bibliography) ; by Raphael Pi mpelly 379 Memorial of John Strong Newberry (with bibliography) ; by J. F. Kemp 393 Memorial of James Henry Chapin (with bibliography); by \V. M. Davis 406 < in the < reology of natural Gas and Petroleum in southwestern On- tario (discussion by I. C. White and II. M. Ami); by II. P. II. Brumeli 408 Note on fossil Sponges from the Quebec Group (Lower Cambro- Silurian) at Little Metis, Canada (abstract); by J. Wm. Dawson. 409 Evening Sessii >n of Wednesday, December 28 411 A fossil Earthquake (abstract) ; by W J McGee 41 1 Session of Thursday, December 29 415 Third Annual Report of the Committee on Photographs 415 Notes on the glacial Geology of western Labrador and northern Quebec ; by A. P. Low 419 The supposed post-glacial Outlet of the Great Lakes through Lake Nipissing and the Mattawa River; by G. Frederick Wright. . . . 4'S.j Notes on the Geology of Middleton Island, Alaska; by George M. 1 >aws< >x 427 Session of Friday, December 30 4-'!2 Evening Session of Friday, December 30 4IJ4 The Huronian Volcanics south of Lake Superior (abstract) ; by C. R. Van Hise 435 On two Overthrusts in eastern New York ; by N. H. Darton 436 Register of the Ottawa Meeting, 1892 440 List of Officers and Fellows of the Geological Society of America 441 Index to Volume 4 4ol ILLUSTRATIONS. Front is] >iec< — Portrait of John Strong Newberry 1 Plate 1— White: New Tseniopteroid Fern (7 figures) . . .' -. . . 119 2 — Whittle: Secondary Enlargement of clastic Tourmaline (2 figures). 156 3 — Hobbs: Sections of garnetiferous porphyritic Schisl (2 figures) 178 4— Diller: Map of northwestern California ami southwestern Oregon 205 5— Lindgren : Recent and Neocene drainage Systems of the Yuba and American Rivers, Sierra Nevada, California 257 0 ( rradesof the Neocene Yuba and American Rivers, Sierra Nevada. California L'li:; 7 tions showing Neocene drainage Systems 265 * : ions showing Neocene drainage Systems 266 9 ( rrade Profiles of Neocene and present Rivers 296 10— Keyes: Gneiss Enclusion in Granite— Woodstock. Maryland 299 ILLUSTRATIONS. V Page Becker : Figure 1— Scission 24 " " 2 — Range of circular Sections 32 " " 3 — Stresses in finite Shear 36 " " 4— Systems of Forces 41 " " 5— Plastic Solid under Pressure 47 " " 6— Strained Cubes 56 " " 7— Widest possible Spacing of Fissures 57 " " 8 — Spacing <>f Fissures 58 " " 9— Effect of Potation on Fissures 59 " " 10— Results of Rupture by Pressure at 30° to fixed Plane 63 '< " 1 1— Results of Rupture by Pressure at 60° to fixed Plane 63 " " 12— Contraction of Mass cooling from one Side 69 " " 13— Primary tension Cracks 70 " " 14— Secondary tension Cracks 70 " " 15 — Cooling of Columns 71 " " 16— Paul uve's Experiment on Crushing 74 " " 17— Steps in Slate 76 " " IS— Origin of Cleavage in Wire 80 " " 19— Development of Cleavage by Extrusion '. 81 " " 20— Development of Cleavage by direct Pressure 82 " " 21— Effects of Compressibility 85 " " 22— Deflection of Cleavage by Grit 86 Hicks : ' ' 1— Weather Curve '35 " " 2— Water Curve of Erosion 136 " " 3— Combined weather Curve and water Curve 137 " " 4— Unstable artificial Curve 138 << " 5— Normal relief Form in an advanced Stage of Base-level- mg 1,j0 . << " 6— Typical Profile of the drainage Slopes of Mountains 138 « " 7 — Cross-profile of bad land Divide • • • 139 " " 8— Illustrating the Coexistence of steep Slopes with broad weather Curves in an early Stage of Base-leveling 140 " " 9— Miniature Butte in the Bad Lands 142 " 10— Cross-section of a constructive River 143 <: " 11— Cross-section of a river Valley having no Flood-plain . .. 145 " 12— Cross-section of a broad Valley of the Plains having no Flood-plain 145 Whittle: " 1— Thin Section of Ottrelite-schist 151 2— Thin Section of Ottrelite 152 '< " 3 — Thin Section of water-worn Tourmaline Pebble 157 " " 4— Thin Section of microcline Pebble 100 " " 5— Thin Section of microcline Pebble |(>3 Hobbs: " 1— Examples of Deformation and modified Growths of Min- eral in Schists 170 " " 2— Secondary Enlargement of Plagioclase '72 " " 3— Garnets with secondary Enlargements 174 " « 4— Portion of a Crown of Staurolite and Magnetite encir- cling a garnet Individual L75 vi BULL. GEOL. SOC. A.M.. VOL. 4. Page Gilbert: Figure I — < Jeneralized Profile, showing relative An -as of tin- Earth's Surface al differenl Heights and Depths 180 " " 2— The continental Plateau as related to the Western and Eastern Hemispheres 181 " " :j — The continental Plateau, developed on a plane Surface . . L85 4 — Oceanic Area complementary to the continental Plateau, developed on a plane Surface 185 5— Area of continental Plateau, developed with reference to a great ( !ircle 1 V|'. Keves: " 1 — Microscopic Crystal of Epidote in Ellicott City (Mary- land) < rranite 309 2— Epidote in Ellicott City Granite 309 " " 3— Epidote in Woodstock (Maryland) Granite 309 " 4— Epidote in Woodstock Granite 309 Darton: " 1 — Cross-section of Ridge on south Side of Rondout Creek, at Rosendale, Ulster County, New York, looking North. 4:;7 " " 2 — Cross-section of Overthrust west of South Bethlehem, Albany County, New Y< >rk 438 " " 3— Overthrust on Sprayt Creek. Section on north Bank, looking North 439 (10 plates, .").") figures.) PUBLICATIONS OF THE GEOLOGICAL SOCIETY OF AMERICA. Regular Publications. The Society issues a single serial publication entitled Bulletin of the Geolog- ical Society of America. This serial is made up of proceedings and memoirs, the former embracing the records of meetings, with abstracts and short papers, lists of Fellows, etc., and the latter embracing the larger papers accepted for publication. The matter is issued as soon as possible after acceptance, in covered brochures, which are at once distributed to Fellows and exchanges. The brochures are arranged for binding in annual volumes, which arc elaborately indexed. The Bulletin is sold to Fellows and the public either in full volumes or in sepa- rate brochures. The volume prices are, to Fellows, a variable amount depending on the cost of publication ; and to libraries and the public, the fixed amounts given below. The brochure [trices for volumes 1 and 2 are given on pages ix-xi of vol- ume 2; the prices for the brochures of volume 3 are givon on pages viii-ix of that volume. Volume 1, covering the work of the Society from the organization, in 1888, to the end of L889, comprises 593 | xii pages, L3 plates and 51 cuts. Price to Fellows, $4.50; to libraries, $5.00; to the public, $10.00. Volume 2, covering the workt)fthe Society for 1890, comprises 002 -p xiv pages, 2.'] plates and O.'i cuts. Price to Fel lows, $4.50; to libraries, $5.00 ; to the public, $10.00. Volume 3, covering the work of the Society for 1891, comprises 541 -f- xii pages, 17 plates and 72 figures. Price to Fellows, $4.00; to libraries, $5.00; to the public, $10.00. Volume 4, covering the work of the Society for 1802, is now complete, and com- prises 458 + xi pages, 10 plates and 55 figures. Price to Fellows, $3.50; to libra- ries, $5.00; to the public, $10.00. The volume is made up of 10 brochures, as follows : Brochure. Pages. Plates. Figures. P,iICB T0 Price to Proceedings of the Fourth Summer Meeting, held at Rochester, August 15 and It!, 1892. H. L. Fairchild, Secretary 1-12 Finite homogeneous Strain, Flow and Rupture of Rocks. G.F.Becker... 13-90 1-22 The Thickness of the Devonian and Silurian Rocks of central New York. C. S. Prosser 91-118 A new Taeniopteroid Fern and its Al- lies. David White 119-132 0-1 Some Elements of land Sculpture. L. E. Hicks 133-146 1-12 (vii) ELLOWS. THE 1'1'lil.lc: $0.10 $0.20 .70 1.40 .30 .60 .25 .50 .15 .30 Vlll BULL. GEOL. SOC. AM.. VOL. 4. Brochure. Pages. Plates. Figures. Peicb to Price to Fellows, the Public. o • > 1-4 .20 .35 1-5 .10 .20 .10 .20 4 .20 .35 15 .30 10 .20 50 1.00 Some dynamic and metasomatic I'he- oomena in a metamorphic Conglom- erate in the Green Mountains. C. L. Whittle 147-166 2 1-5 .25 .50 Phases iu the Metamorphism of the Schists of southern Berkshire. W. 11. Hobbs 167-178 Continental Problems. G. K.Gilbert. 179-190 Comparison of Pleistocene and presenl [ce-sheets. W. Upham 191-204 Cretaceous and early Tertiary of north- ern California and Oregon. J. S. Dilleb 205-224 On the Geology of natural Gas and Petroleum in southwestern Ontario; Notes <>n the ( >ccurrence of Petroleum in Gasp6, Quebec. II. P. H. Brc- m ell 225-244 The Faunas of the Shasta and Chico Formations. T. W. Stanton 245-256 Two Neocene Rivers of California. W. Lindgren 257-298 5-9 Some Maryland Granites and their Origin; Epidote as a primary Com- ponent of eruptive Rocks. C. R. Keyes 299-312 10 1-4 .20 .:!•"> Relations of the Laurentian and Huro- nian Rocks north of Lake Huron. A. E. l',\i:i.o\v 313-332 15 .30 The Archean Rocks west of Lake Supe- ri« »r. W. II. C. Sm eth 333-348 15 .25 The Laurentian of the Ottawa District. R. W. Ells 349-360 10 .20 Height of the Bay of Fundy Coast in the Glacial Period relative to Sea- level, as evidenced by marine Fossils in the Bowlder-clay at Saint John, New Brunswick. Robert Chalmers . 361-370 .10 .15 Proceedings of the Fifth Annual Meet- ing, held at Ottawa, Canada, Decem- ber 28, 29 ami 30, 1892 (with frontis- f 371-45S \ ._„ - , .. piece). H. L. Fairchild, Secretary. \ i-xi j 6 ' [rregulab Publications. In the interests of exacl bibliography, the Society takes cognizance of all publi- cations issued either wholly or in pari under its auspices. Each author of a memoir receives 30 copies without cost, and is authorized to order any additional number at a slighl advance on cost of paper and presswork; and these separate brochures are identical with those of the editions issued and distributed by the Society. Contributors to the Proceedings also are authorized to order any number of separate copies of their papers at a slight advance on cost of paper and press- work; hut such separates are bibliographically distinct from the brochures issued by the Society. PUBLICATIONS. IX The following separates of parts of volume 4 have been issued: Editions uniform with the Brochures of the Bulletin. 430 eopies. January 3, 1893. ' February 21, c tt OQ ->, ' ' ' 25 Pages 13- 90, 430 (i 91-118, 180 c< 119-132, plate i; 130 it 133-146, 30 a 147-166, plate '7 . — J 55 i i 167-178, 1 1 230 it 179-190, 430 (t 191-204, 30 i t 205-224, plate 4, ISO a 225-244, 130 a 245-251 i, so u 257-2'. is, plates 5-9 ; 130 < i 299-312, plate 10; 130 a 313-332, 30 i i no '2 oiu OKjO—'J-tO, 30 a 349-360, 30 3(31-370, 30 a 27, a 27, March -'4, April 14, May 20, June 8, t c 19, July 31, August 4, a 4, t i 7, if 7, Pa Special Editions* es 379-393, f 30 copies. September 393-406, frontispiece; 30 406-408, 409-410, 411-414, 415-418, 410-421, 423-427, 427-131, 435-136, 436-430, 441-450, vii-viii, 30 a 30 a 30 u 100 t i 100 a 30 a 200 11 150 a 30 it 100 u LOO tt 50 tt It it 23 23 23 23 23 23 23 23 < )ctober 18 Without covers. *Bearing the imprint ["From Bull. Geol. Soc. A.M., Vol. I. 1892."] ■(•Fractional pages are sometimes included. II— Bull. Geol. Soc. Am., Vol. I, 1892. CORRECTIONS AND INSERTIONS. All contributors to volume -1 have been invited to send in corrections and inser- tions to be made in their contributions, and the volume lias been scanned with sonic care by the Editor. The following are such corrections and insertions as are deemed worthy of attention : it a Page 20, in formula for tan X ; for11 a — " reada-\-. 21, first line of foot-note ; " " unchanged length " " unchanged direction, 21, foot-note, 2d equation ; " "y/x — " " yjx=. 27, third formula; " "a = " " — a=. 29, formulas (8) ; " "cos{v — /*) " " , letter the triangle in the upper right-hand corner, a b c 37, formula for T, reverse si^ns of G and Q. .'!7, line 13 from top; for "page 34" read page 31. 59, last formula ; " "4" "2. 80, foot-note; " "p. 74" "p. 54. The above are simply misprints, and the correct expressions were em- ployed by Dr Becker in the deductions and computations. L85, erase the misplaced "s" to the left of figure 4. 22:;, line 20 from top; for " Wasacht" read Wasatch. 304, " 8 " " " "magnatic" " magnetic. " 306, " 2 " bottom; " "no. 85" " no. 65. " 314, " 14 " top; " "Wahnapital" " Wahnapitae. " 318, lines 15 and 17 from top; " " " 331, line 5 from top; " " Walter MeOuat" " Walter McQuat. " 333-348; " " Contchiching " " Coutchiching. " 340, line 13 from top ; " " Vermiline " " Vermilion. " 341, lines 14 &20from bottom ; " "RatRoat" " Rat Root. " 342, line 1 from bottom ; " "no. 9" " no. 1. " 340-348; " "AticOban" " AticOkan. :!C>L', line 2(1 from top; after (" true meridian ") omit and. 363, " *i " " omit "obviously." ;;(;:;, " s " " after " Carboniferous " insert systems. 363, " '.) " " omit "systems." 364, " s " bottom ; after " courses " omit of them. 365, " 14 " top; for " Belanus" read Balanus. 366, " 4 " bottom; enclose" Yoldxa arctica of Sars " in parentJiesis. 369, " (> " top; for " has been formed " read has also been formed. 400, " 22 " bottom; " "B.G.Harrington" " B.J.Harrington. 40'.), " 13 " " " " these" " them. 109, " 7 " " " "Sasiothrix" " Lasiothrix. 41(1, " 7 " top; " " hair" " base. no. " pi " •• after " closely " insert or loosely. (i CORRECTIONS AND [NSERTIONS. XI Page 410, line 16 from top ; after " Palawsaccus" insert * " 410, " 16 " " for u Palawsaccus" read Palseosaccus. Also at the bottom of the page insert the following foot-note, to which the star should refer : * It has since been described and figured by Dr G. J. Hinde, under the name Palaseoaceus dawsoni, in the London Geological Magazine, February, 1893, p. 56. " 410, line 24 from top; for " cusiformis" runt ensiformis. " 410, " 23 " " " "Astiopollition" " Astropolithon. Additions to Newberry Bibliography. Page 400, between lines 12 and 13 from top; insert Remarks on copper Ores in the Triassic Sandstones of the United States: Proc. New York Lye. Nat. Hist. , vol. ii?, 1874, pp. 16, 17. " 401, " " 13 and 14 " bottom; " Remarks on the Genesis of the Newark Sandstones contiguous to the Pali- sades, New Jersey: Proc. New Yuri: Lye. Nat. Hist., vol. i, 1870-1871, pp. 131, 133, 134, 137. " 402, " " 18 and 10 " " " Remarks on Serpentine of Staten Island : Trans. New York Aa id. Sci., vol. i, 1881, pp. 420-422. " 402, " " 7 and 8 " " " Remarks on the intrusive Character of the Trap of Bergen Hill, New Jersey : Trims. New York Acad. Sci., vol. ii, 1y ( !. II. Hitchcock 3 Session of Tuesday Morning, August 1(1 N The Oneonta Sandstone and its Relations to the Portage, Chemung and ( 'atskill Groups (Discussion) ; by .lames Hall 8 Session of Tuesday Afternoon, August Hi 0 Conditions of Accumulation of I (rumlins (Discussion) ; by Warren TJpham. 0 Ancient Waterways (Abstract) ; by A. S. Tiffany K) Register of the Rochester Meeting 12 Session of Monday, August 15 The Society met at 2.30 o'clock p m, in the geological lecture-room, Sibley Hall, University of Rochester; the President in the chair, and about twenty-five members present. The President, Mr G. K. Gilbert, opened the meeting with appropriate introductorv remarks. ELECTION OF FELLOWS The Secretary announced as the result of the balloting for the election of Fellows that the following persons were elected Fellows of the Society : Alfred E. Barlow, B A, M A, Geological Survey, Ottawa, Out, Field Geologist ; now engaged in strati graphical geology and working on the Arehean rocks north of lake Huron. Henry Phareth Hawdon Brumell, Geological Survey, Ottawa, Out. Assistant, Division Mineral Statistics and Mines; now engaged in mining geology and geology of natural gas and oil. I— Bull. Geol. Soc Am, Vol. 4, 1892. (I) A PROCEEDINGS OF ROCHESTER MEETING. Mabius Robisox Campbell, U. S. Geological Survey, Washington, D. C. Geologist ; now engaged in stratigraphy and structure of the Paleozoic rocks of the Appa- lachian province. A.ntonio del Castillo, School of Engineers, City of Mexico. Engineer of Mines and Director of National School of Engineers. Director of the Geological Commission for the preparation of the Geological Map of the Republic of Mexico. Harold W. Fairbanks, B S, San Diego, Cal. Geologist on staff of State Mining Bureau; now engaged in general Held geology. Leox S. Gkiswold, A B (Harvard, 1889), 238 Boston St, Dorchester. Mass. Geolo- gist : engaged in field work on Triassic area of Connecticut. Albert P. Low, B of Sc, Ottawa, (Jut. Field Geologist Geological Survey Depart- ment ; now engaged in the study of the Archean. Vernon Feee.max Marsters, A B, Bloomington, Ind. Associate Professor of Geology in Indiana State University ; now engaged in the study of general geology and petrography. Albert C. Peale, M D, Washington, D. C. Geologist United States Geological Survey ; engaged in structural geology and stratigraphy of northeastern Rocky Mountain region. William B. Scott, M A, Ph D (Heidelberg), Princeton, X. J. Professor, College of New Jersey ; now engaged in study of vertebrate paleontology. Charles Henry Smyth, Junior, A B, Ph B, Ph D, Clinton, X. Y. Professor of Geology in Hamilton College ; now engaged in the study of the geology of the western Adirondack region. Joseph Staxley-Browx, Washington, D. C. Assistant Geologist United States Geological Survey ; now engaged in the study of petrography and structural geolog3' in northwestern United States. Charles Livy Whittle, West Medford, Mass. Assistant Geologist United States Geological Survey; now engaged in field work in the Archean rocks of south- ern Vermont. The President announced that the Council had determined that other sessions of this meeting should be held on Tuesday, August 16, at 10 . o'clock a m and at 2 o'clock p m. No further business being offered, the President declared the scientific work of the meeting in order, and announced^ the first paper on the printed program, which, in the absence of the author, was read by W J McGee : NOTES ON THE PHOSPHATE FIELDS OF EASTERN MARION AND ALACHUA COUNTIES, FLORIDA BY LAWRENCE C. JOHNSON The paper was discussed by Charles H. Hitchcock. E. \\ . Claypole, R. A. V. Penrose, Junior, 1. C. White and W -I McGee. C. H. HITCHCOCK THE CONNECTICUT VALLEY GLACIER. 3 The second paper presented was — ON THE DENTITION OF TITANICHTHYS AND ITS ALLIES BY E. W. CLAYPOLE it On behalf of the Committee on Photographs Mr C. W. Hayes an- nounced that the photographs recently acquired were displayed in the adjoining hall of the University Geological Museum. The following paper was then read : STUDIES OF THE CONNECTICUT VALLEY GLACIER BY C. II. HITCHCOCK Reference may be made firs! to the literature of the subject by Professor E. Hitch- cock, who believed the Lee marks in general were produced by icebergs, and recog- nized true glacial phenomena in the AVestfield and Deerfield river valleys tributary to the Connecticut. This was in 1853. Ten years later Professor J. D. Dana com- mented upon these and related farts, and presented the view that the markings were not produced by Local glaciers, but were made by the general ice sheet, the variation in direction having been due to pressure. Professor Louis Agassiz, in 1872, recognized local glaciers entirely subsequent to and independent of the main ice sheet in a part of the White mountains. The present author has also recorded similar views in various papers and reports. . A more thorough examination of the main Connecticut valley in the vicinity of Hanover, New Hampshire, has recently been made in order to afford a better under- standing of the facts. Over a territory thirty miles long and from ten to fifteen miles wide nearly every 1 dge has been scrutinized, and the directions of stria? re- corded. The record includes two bundled observations within this area. The attempt was made to have this record exhaustive, and to include the markings on both sides of the valley movement. The general conclusion is that two move- ments are indicated: first, in the direction S. 30° E., principally on the highland borders; secondly, in the direction S. 10° W., existing only in the depressed area. More specific conclusions are the following: 1. In addition to the Connecticut valley movement in the direction indicated by the topography, there were numerous branches to it, corresponding to the smaller tributaries. The phenomena observed authorizing this generalization are striation and the transport of bowlders. The test cases are where the movement has been in direct opposition to the general southeasterly current. Thus, on adjacent ledges two miles north of Hanover, there are striae pointing X. 60° W.„and others S. 20° W., the first being tributary to the second, and less deeply scored. Next, there are a dozen excellent examples of the westerly transportation of large blocks of a peculiar protogene-gneiss. These occur in Lebanon, Hanover and Oxford, and in a few cases there are stria? to correspond, trending southwesterly. This particular rock occurs only on tin- eastern side of the valley, and it is not possible, therefore, to say that its fragments were transported by ice in the course S. .">0° E. 2. Near the upper limit of the valley striations there are several examples of the S. 30° E. course, which are isolated and situated in the midst of the S. 10° W. 4 PROCEEDINGS OF ROCHESTER MEETING. markings. So far as observed, the first occupy depressions in the ledge, or else are located on tlic lee side of the valley scorings. Our inference is that the S. 30° E. markings were mice quite abundant and have been mostly obliterated by the later local glacier. These examples are not confined to the eastern border of the valley- but have been found elsewhere in the lower regions. :;. While it cannot be regarded as a universal fact, many observations show that Hat bowlders imbedded near the surface of the till have been striated by the valley movement as well as by the older action. Hummocks of till can be referred to either of the movements by observing these directions. It would appear that the older till had been deposited before the local glacier had an existence. Agassiz has described this same condition of things in the Bethlehem glacier. The most obvious effect of the later movement has been the removal of the rough blocks from the surface of the older till, and hence smoothed hummocks indicate a later and local movement. 4. Bowlders have been carried by ths southeasterly movement entirely across the valley and lodged upon the farther side. As our studies have been mainly confined to the depressed region, many cases of this kind have not been observed. The best illustration of it is the presence of numerous bowlders of the mount Ascutney granite in Claremont and Newport, New Hampshire. This mountain lies in the midst of the S. 10° W. striation, but blocks have been carried from it toward the southeast, evidently before the glacier commenced to move down the valley. Others have been carried southerly, as if caught by the later current. 5. As a rule, the line is sharply defined between the two directions of striation. 6. The valley movement reached the altitude of 900 feet above the sea in Clare- mont, 1,000 to 1,800 feet in Hanover on the eastern border. 1,900 feet on the western border in Norwich, Vermont, and perhaps 2,500 feet on mount Ascutney. This mountain is a cone, somewhat west of the median line of the valley. 7. The noted esker described by Warren Upham between Windsor, Vermont, and Lyme, New Hampshire, occupies the area in question, and the stones found in it correspond to ledges on the west and north, but not to those on the eastern side of the valley. Pebbles of porphyry from the White mountains can always be found among them by a diligent search. These could not have been brought by the general ice movement of S. o0° E. The distance of transportation is often as much as sixty miles. The evidence of the presence of a Local glacier down the Ammonoosuc river, a principal tributary of the Connecticut, is more pronounced thananything that can be adduced for the area now being discussed. It must have been the upper part of the same local "lacier. The papers by the earlier authors were based upon the notion that a single ice sheet mdy is required to account for all the glacial phenomena, and that the ( !on- necticut Valley glacier came into being in the decline of the aires after the ice had ceased to be supplied from Canada. The facts, so far as known in New England, do not nec issitate the existence of more than one ice age, but it is conceivable that the system of glaciers radiating from the Green and White mountains may repre- sent a second Lee sheet. In this connection the attention of glacialists is called to the interesting southwesterly striation found upon certain highlands in southern Vermont and western Massachusetts, as described in < reology of Vermont, volume 1, page 7o. These evidently represenl a phase of glaciation different from the on,, described in this paper. C. H. HITCHCOCK THE CONNECTICUT VALLEY GLACIER. 0 A free discussion followed the reading of this paper. Professor W. H. Mies, speaking of his observations in the Alps, said — About the Matterkorn and the Weisshorn I have observed thin glaciers with a movement different in direction from the thicker glaciers which formerly existed in the same places. I believe that under some conditions the upper surface of a wlacier mieht have a different direction of movement from the lower surface, and have seen glaciers moving over till, kanies. etc. In one instance I had the fortune to observe under favorable conditions a -lacier passing over a surface sparsely strewn with bowlders, and at one point found that a bowlder was being slowly pushed forward by the ice, but at the same time the body of the glacier moved much more rapidly than the bowlder, so that its bottom was marked by a long- groove extending some yards down stream from the bowlder. Professor I. C. White observed — Contrary to my former belief, I now know of no mountains in northern Penn- sylvania which were not buried in the Pleistocene ice sheet. Mr McGee remarked — The paper and the discussion suggest a feature ofice movement not alwaysappre- ciated. which is well exemplified in northeastern Iowa about the margin of the driftless area. There were in this region two ice invasions of approximately hut not exactly equal extent : in the first the ice advanced farther in the north and not so far in the south as in the later invasion, so that the drift borderingthe driftless area represents the lower till or older sheet in the north, the upper till or later sheet in the south. >s~ow both in the north, about the headwaters of < >neota river, and in the south, about the lower reaches and tributaries of the Maquoketa, there is a remarkable relation between the elements of the topography and also between the distribution of the drift and the surface configuration — a relation best displayed in southeastern Jackson county and northeastern Clinton county. Here the characteristic curves of the glacial topography pass gradually into the more strongly accented lines of the water-cut topography by which the driftless area is distinguished, and it is significant that the transition from ice-molding to water- carving is not only horizontrl hut vertical — that first the bottoms, later the mid- sides, and finally the rims of the valleys lose the glaciated curves and assume the water-cut angles ; and this is especially true of the transverse valleys. Moreover in some cases the transverse valleys are partly lined with an ice laid deposit differ- ing from the prevailing drift of the region in that it is made up almost wholly of local debris, sometimes apparently removed lint a few feet or rods from the parent ledges; while even the furthermost traces of the drift are made up predominantly of far-traveled crystalline rocks, and occupy faintly glaciated summits some miles beyond the limit of ice-molding in the valleys. In brief, Loth the distribution of the drift and the topographic configuration indicate that the thin margin of the ice bordering the driftless area first pushed into and filled certain transverse valleys. and then rode over the imprisoned ice as on a bridge, the surface of slip being transferred from the bottom of the valley to the plane of its rim. In valleys oblique G PROCEEDINGS OF ROCHESTER MEETING. to the ice-flow the slip appears to have been divided between the valley-bottom and the plane connecting its walls. Mr Warren Upham said — Instead of attributing the courses of glaciation in the Connecticut valley to a local glacier, as suggested by Professor Hitchcock, my observations of the glacial drift in thai valley and over the adjoining country lead me to think that the striae bearing toward the south and west of south are due to local deflection of currents of the ice sheet during the time of its departure, rather than either to any glacier later- existing there or to longer continuance of a remnant of the ice sheet there than on the higher land at each Hide. The Connecticut valley esker (called a kame in Geology of New Hampshire, volume iii) was traced by Professor Hitchcock and myself along the axis of this part of the Connecticut valley for a distance of about twenty-five miles, from Lyme. New Hampshire, to Windsor, Vermont. It is believed to have been deposited in the ice-walled channel of a superglacial stream near its debouchure from the ice sheet to the land from which the ice had retreated. The size and extent of this esker and its material, which is obliquely bedded gravel and sand without bowlders, show that it was formed by a large superglacial river draining a considerable area of the melting ice sheet. When the ice had become thinned by ablation, its surface here descended from each side toward the glacial river by which the esker was being formed, and there was probably also some indentation orembayment of the receding glacial boundary at the river's mouth in the valley. At this time the currents of the ice sheet which had passed southeast- ward even in the bottom of the valley, as known by the oldest sets of strife there noted by Professor Hitchcock, became deflected, as I think, toward the south and west of south, taking the course of the valley, in obedience to the law that the currents of the outer part of the ice must everywhere turn perpendicularly' toward its edge. Professor Niles added — The Alpine glaciers suggest a relation between ice and topography quite different from that assumed by Mr Upham. During past ages glaciation was much more extensive in the Alps than at present ; yet as the ice retreated, it did not withdraw from the valleys but disappeared from the divides and shrank into the valleys ; and to-day, as probably at every stage since the Alpine ice reached its greatest ex- tension, the margin of the ice is not indented by notches coinciding with the val- leys, but is marked by streams of flowing ice pushing far below the general snow level. Mr McGee added— While analogies drawn from Alpine glaciers are of great use in researches con- cerning ancient glaciers of this country, it should be borne in mind that ice-work is not necessarily similar in regions of high relief like1 the Alps, and in regions of low relief like the plains of | he Mississippi valley and perhaps also the plateaus of New England. In regions of high relief the terrestrial surface is rugose and the general flow of the ice is obstructed by the inequalities. Accordingly, while the C. H. HITCHCOCK THE CONNECTICUT VALLEY GLACIER. 7 glacier may, if of continental type and of sufficient thickness, assume a fairly uni- form general slope and a moderately definite direction of general movement, trie prevailing movement, particularly in the lower portions of the sheet, may be purely local and determined by the local slopes. This predominance of local over general movement is magnificently illustrated along the lower reaches of Frazer river in British Columbia, where the lesser mountains, up to three or four thousand feet in altitude, are converted into huge tors; but while the prevailing trend of the great flutings in which the direction of flow is recorded is toward the coast, the trend is by no means uniform, and many flutings indicate prevailing movement down the slopes, such as might be expected in a slowly settling neve. Now in such regions as British Columbia and the Swiss Alps, this local downward impulse must so far preponderate as to keep the valleys filled, howsoever rapidly ablation may progress, leaving the divides to be first laid bare. On the other hand, there is good reason for believing that in the plains of the upper Mississippi valley the ice pushed forward under a general impulse which so far preponderated over the local impulse down the gentle slopes that when ablation commenced, superglacial streams were formed and gradually cut through the ice and into the subterrain, so that the entire surface became diversified by a drainage corresponding in many respects to that of to-day — in short, in northeastern Iowa at least, this superglacial drainage was superimposed upon the land surface and remains to-day a record of the sur- face configuration of the continental glacier. These types of glacial action must be carefully distinguished; but there is perhaps a question as to which type was represented by the ice-work of New England. Profess* >r ( Jlaypole drew illustrations from Alpine glaciers. He thought the Connecticut valley glacier more comparable to Alpine valley glaciers, and particularly to the lower part of the Mer de glace. Mr Gilbert regarded the possibility of upper ice moving over inferior ice as demonstrated. He had observed phenomena which nothing else could explain. In the " finger lakes " of New York each valley has been shaped by undercurrents in the ice, while the region lias been planed differently. Professor Hitchcock regarded the Connecticut valley glacier as a local glacier from the White mountains toward the close of the glacial episode. Professor John C. Branner read the next paper : THE OZARKS AND THE GEOLOGICAL HISTORY OF THE MISSOURI PALEOZOIC BY G. C. BROADHEAD Remarks were made by J. J. Stevenson and H. S. Williams. The Society then adjourned until the following day. 8 proceedings of rochester meeting. Session of Tuesday Morning, August 16 The Society assembled at 10.15 o'clock a m, President Gilbert in the chair. The first paper read was — PHASES IN THE METAMORPHISM OF THE SCHISTS OF SOUTHERN BERKSHIRE BY WILLIAM II. HOBBS This paper is published elsewhere in this volume. The next paper was then presented by the author, and was illustrated with maps and drawings: THE ONEONTA SANDSTONE AND ITS RELATIONS TO THE PORTAGE, CHEMUNG AND CATSKILL GROUPS BY .1 i.MES HALL During a long discussion, Professor H. S. Williams spoke as follows : It is difficult to map such formations, the physical conditions of deposition being related to the faunas in a very complicated manner. The physical conditions change the character of the deposits, while the fauna may persist; a series of dis- similar rocks being together one faunal formation. In determining the extent of formations paleontology outranks lithology. In reply to a question by Professor J. J. Stevenson, Dr Hall said — The Chemung wedge is lithologically distinct as well as in its fossils. Professor Stevenson compared Dr Hall's section of strata with his own New York section and with Professor I. C. White's observations in Penn- sylvania. Professor White stated that a similar formation extends from New York to White Sulphur springs, in Virginia, and even into Ken- tucky. He -would call it all Chemung. Professor E. W. Glaypole spoke in compliment of the paper, which contained observations made before many Fellows of the Society were born. He said that in Ohio shales re- place the sandstones of New York and Pennsylvania. During Devonian time physical conditions greatly changed in a few hundred miles from east to west; in western Pennsylvania changes occurred within an extent of only twenty-five miles. The President spoke of the classification of formations and the principles of nomenclature, and remarked that nature is more transitionary than our nomenclature can adequately present. In closing the discussion Dr Hall spoke of the Long persistence of faunas, through important changes of receding and readvancing sea- t WARREN UFIIAM — ACCUMULATION OF DRUMLINS. 0 shores, local deepening of the ocean, etc. For colors on maps he pre- ferred designating the lithology. This paper is printed in full elsewhere in this volume. The concluding paper of the morning session was read in the absence of the author by Mr R. S. Woodward : FINITE HOMOGENEOUS STRAIN, PLOW AND RUPTURE OF ROCKS BY G. F. BECKER This paper is printed in full in the succeeding pages of this volume. Session of Tuesday Afternoon, August 16 The Society was called to order by President Gilbert at 2.10 o'clock. A paper was read by the author under the following title : CONDITIONS OF ACCUMULATION OF DRUMLINS BY WARREN UPHAM A short abstract of this paper is given in The American Geologist for October, 1892, volume xii, page 218, and it is published in full, with additions, in the same journal for December, 1892. Professor R. D. Salisbury remarked — It seems to me that the use of the term " englacial drift " is objectionable. I re- gard the foliation of drumlins as due to great pressure. The arrangement of drumlins is not parallel to the terminal moraine ; they are sometimes at right angles to it. Drumlins seem to me to he a normal feature of the drift and ought to be common ; their absence is more singular than their occurrence. Some are found at right angles to the direction of ice movement, but they were always formed near the ice margin, and were englacial and subglacial. Mr F. J. H. Merrill remarked— I have found Cretaceous rocks in the Long island drift hills, which seem to me to have a bearing on the question and to indicate the subglacial origin of the drift. Mr W J McGee said— I agree with Professor Salisbury in regarding drumlins as normal phenomena. Their formation is illustrated in homely fashion by the frequent accumulation of masses of debris beneath any heavy body dragged on the ground; they well ex- II -Bull. Gkol. Soc. Am., Vol. 4. 1892. 10 PROCEEDINGS OF ROCHESTER MEETING. emplify the physical law that " starting friction " is greater than " moving friction." They should be looked for, not in the area of active glacial degradation, but about the critical line at which deposition began, i e, the point of oscillation between degradation and deposition. Mr Upham remarked — I musi continue to regard the isolation and strange distribution of drumlins as a very singular, important and unexplained feature. The next paper was — THE EXTRA-MORAINIC DRIFT OF THE SUSQUEHANNA VALLEY BY G. FREDERICK WRIGHT Professor R. D. Salisbury and Mr W J McGee remarked upon the matter of the paper, challenging the observations and inferences of the author. The next paper was as follows : A NEW T.ENIOPTERID FERX AXD ITS ALLIES BY DAVID WHITE Remarks wrere made by Professor E. W. Clay pole and by the author. The paper in full is printed in later pages of this volume. The twro following papers w ere read consecutively by the author : THE OVERTURN OF THE LOWER SILURIAN STRATA IN RENSSELAER COUNTY. N. Y BY A. S. TIFFANY ANCIENT WATERWAYS. BY A. S. TIFFANY [Abstract] The writer gave a brief account of an ancient waterfall in a paper read before the American Association for the Advancement of Science at Ann Arbor, and published in pamphlet form in 1885. This waterfall eroded the hard, horizontally disposed Corniferous limestone of what is now Rock island (Illinois) to a depth of 70 feel and a width of 900 feet. The cavity was afterward filled with Coal Measure shales. The boring of artesian wells in [llinois and Iowa has since developed a number <<\' excavations of still greater depth filled with drift. \t Dixon, Illinois, at an altitude of ris feel above sea-level, a well drilled by Mr Wilson ran through L50 feel of bowlder clay, though the < lalena and Trenton lime- stones of the vicinity rise in cliffs many feet above the top of the well see Geol. 111., volume v. pages H'S-130). A. S. TIFFANY ANCIENT WATERWAYS. 11 At Victor, Iowa county, Iowa (elevation, 806 feet), an artesian boring went through 348 feet of drift, while at Homestead, 22 miles eastward (elevation, 86(3 feet), the Kinderhook lias but a light covering of drift. Again, at Wilton, Musca- tine county, Iowa (elevation, 672 feet), about 50 miles east of Homestead, an artesian well went through drift, including a large bowlder, to a depth of 300 feet ; while at Limekiln, six miles northwestward, the Niagara limestone is in place at a higher elevation, and at Moscow, only four miles west of Wilton (elevation, 652 feet}, the Hamilton shales form the river bluffs. Phenomena analogous to those of Eock island occur in Missouri, as shown by the Report on Coal, published by AVinslow in 1801. This preliminary report gives a map of the coal mines and coal pockets in rocks of different ages in twenty counties. They are horizontally disposed basin-shaped cavities, with diameters of 800 to 1,000 feet, from j;0 to 80 feet deep, filled with strata of coal and shale, bituminous and cannel coal frequently occurring in the same pocket. These pockets range from the margin of the Coal Measures in place to 120 miles distant from them. Swallow located 23 of these pockets in Cooper county, four of them lying within five miles above Booneville. Since Swallow's report was published, many more of these pockets have been explored and the coal worked out. They extend to near Boone- ville, and lie in close proximity to the beds from which Messrs Blair and Sampson and the writer made large collections of Keokuk crinoids, the Keokuk rocks rising in the sloping cliff more than 50 feet above the coal. The coal beds vary in thick- ness from 20 to 30 feet, while the accompanying shales are very thin. According to Swallow, these abnormal deposits are found in ravines and cavities of denuda- tion in rocks of all ages, from the Archimedes limestone down to the Calciferous. The well-known bed in Calloway county is said to be over 80 feet thick. These excavations in rocks of different ages show the enormous erosion which took place in the Mississippi valley anterior to the coal period, and the basin shape of some of them suggests that they were produced by ancient waterfalls. Remarks were made by E. W. Claypole and Samuel Calvin. The three following papers were read by title : SOME DYNAMIC AND METASOMATIC PHENOMENA IN A METAMOEPHIC CON- GLOMERATE IN THE GKEEN MOUNTAINS BY CHARLES L. WHITTLE PRELIMINARY NOTES ON THE GLACIATED AREA OF NORTHEASTERN KANSAS BY ROBERT HAY THE THICKNESS OF THE DEVONIAN AND SILURIAN ROCKS OP CENTRAL NEW YORK BY CHARLES S. PROSSER The President made a few appropriate remarks and declared the meet- ing adjourned. 12 PROCEEDINGS OF ROCHESTER MEETING. Register of the Rochester Meeting, 1892 The following Fellows were in attendance at the meeting Henry M. Ami. John C. Branner. Samuel Calvin. Edward W. Claypole. Aaron H. Cole. Herman L. Fairchild. P. Max Foshay. Homer T. Fuller. G. K. Gilbert. James Hall. C. Willard Hayes. Robert T. Hill. Charles H. Hitchcock. William H. Hobbs. H. C. Hovey. Joseph P. Iddings. Joseph Le Conte. Thomas H. McBride. W J McGee. F. J. H. Merrill. William H. Niles. R. A. F. Penrose, Junior. R. D. Salisbury. John J. Stevenson. A. S. Tiffany. Warren Upham. David White. I. C. White. R. P. Whitfield. H. S. Williams. Robert S. Woodward. G. Frederick Wright. BULLETIN OF THE GEOLOGICAL SOCIETY OF AMERICA Vol. 4, pp. 13-90 January 3, 1893 FINITE HOMOGENEOUS STRAIN, FLOW AND RUPTURE OF ROCKS. BY GEORGE F. BECKER. (Presented before the Society August 16, 1892.) CONTEXTS. Page. Phenomena and Plan of Discussion 14 Evidences of Movement 14 Scope of the Inquiry 15 Finite rotational Strain K> Limitations of the Problem 16 Displacements 17 General Conditions 17 Strain Ellipse IS Rotation 19 Lines of constant Direction 20 Simple Strains 21 Pure Rotation 21 Dilation 21 Shear 22 Compound Strains . . Z I How treated 23 Pure Deformation 23 Shearing Motion or Scission 2-1 Two Shears in the same Plane 25 Plane undilational Strain 26 St rain due to Pressure 29 Elongation 30 Planes of maximum tangential Strain 30 Position of undistorted Planes 30 Planes of maximum Strain '■'< 1 Angular Range of undistorted Planes .".1 Case of tri-dimensional Strain :;:; Numerical Example of Strain 34 Finite Stress 35 Relation of Stress and Strain 35 Stresses in a Shear 36 Simple Pressure 37 III-Bull. Geol. Soc. Am., \'..i,. -i, 1892. (13) 14 G. F. BECKER FINITE STRAIN IN ROCKS. Page. Meaning of Hooke's Law 38 St less System 40 Lines of unaltered Direction 4:! Properties of Matter 44 Viscosity 44 Flow 4o Relation of plastic Solids to Fluids 46 Rupture 48 ( ideological Applications 4i» Cases to be considered 49 Effect s i if direct Pressure 50 Rigid Disk in resisting Medium .">:; Inclined Pressure arid yielding Medium 55 Inclined Pressure and unyielding Resistance . 56 Partial Theoiy of the Spacing of Fissures 57 Examples of inclined Pressure 61 Distortion on Planes of maximum Strain f>4 Various Results of Strain 65 Theory of slaty Cleavage 66 Influence of Shock 66 Secondary Action on ruptured Pocks 68 Effect of tensile Stresses 68 Review of Theories of slaty ( Jleavage 71 Why needful 71 Origin of Jointing 72 Jointing and Cleavage 75 Phenomena of slaty Cleavage 7"> Theories of slaty Cleavage 77 ( tbjections to Plypothesis of Heterogeneity 79 Analysis of Experiments 80 P>ehavior of included Grit Beds and Fossils • . 83 Conclusions as to Slate 86 Summary 87 Phenomena and Plan of Discussion. Eoidences of Movement. All observers are aware that few. rock masses are continuous for any considerable distance. It is seldom that more than a few yards of a rock exposure can be examined without revealing- joints, fissures or slickensides. Still more frequently rock masses show slaty or schistose cleavage* impressed upon them by dynamical causes. In a very great proportion of such cases a little attention also discloses ♦ Schist and the adjectives derived from it are used in literature in somewhat variable senses. As I use it, schist denotes eleavable rocks which an- allied to slates, but in which tin- cleavage surfaces arc not all sensibly parallel to on< another as they air in true slate. By no means are schists all crystalline of metamorphic. FAULTS, JOINTS AND CLEAVAGE. 15 the fact that the partings are locally arranged on a definite system. In slaty cleavage the cleavage planes are substantially parallel and very close together ; in flags of the slaty class the intervals between cleavage pianos are greater ; in schists the partings range through small angles, and in these last rocks there are frequently two sets of partings, each cleavage making a small angle with others of the same set, but a large angle with those of the other set. Where the rock is divided by cracks these are often parallel and spaced with a considerable approach to uniformity. Sometimes they occur at a fraction of an inch from one another, while in other instances they are rods apart. In still other cases there are two systems of such cracks crossing one another at right angles, or at angles which approach to right angles. Not infrequently such a double system of fissures is accompanied by a second of like character, at right angles to it, dividing the rock into polyhedral fragments of greater or less size. Slaty cleavage is at present regarded by most geologists as due to a pressure acting in a direction perpendicular to the planes of cleavage, and this opinion is supposed to be well supported by experiments. Indications are not wanting, however, that many observers are ill satisfied with this explanation. Less attention has been paid to jointing, concern- ing which there is no consensus of opinion. By some it is considered as due to tensile stresses, while others insist on its intimate association with cleavage. Jointing is also often treated as distinct from faulting and as being unaccompanied by any relative movement of the joint walls. No systematic attempt appears to have been made to elucidate these various structures, which are generally recognized, however, as at least sharing a dynamic origin. Even the experiments on cleavage seem to me not to have been studied with as much care as they deserve. Scope of the Inquiry. — Orogeny can never be satisfactorily discussed until the dynamic significance of cleavages and cracks is clear. A neces- sary step toward this end consists in the elucidation of those areas, great or small, throughout which the phenomena are uniform; for, however complex the conditions may be in any body of rock, they may be con- sidered as uniform over a sufficiently small fraction of the whole mass. Even this seemingly modest step cannot be completed in the present state of science. In the mechanics of artificial structures and machinery it is sufficient to discuss very small deformations, for such only are ad- missible. In geology this is wholly insufficient, the strains frequently being of enormous amount ; so great indeed that laboratory experiments hardly aid one to conceive that they are possible. Yet there is no doubt among geologists that pebbles, even of quartzite, in conglomerates are not infrequently elongated by pressure to double their original length without rupture. Thus in geological mechanics it is absolutely essential IV— Bum,. Geol. Son. Am., Vol. 4 18!)2. 16 G.F.BECKER — FINITE STRAIN IN ROCKS. to consider finite strains as well as infinitesimal ones.* Now, to discuss such strains completely it would he needful to know the relation between finite strains and the forces which produce them. This relation is not yet known. One might infer that until it were ascertained discussion would he useless. I hope to show, however, that many relations of finite strain can he elucidated without the assumption of any law connecting stress and strain, and that these relations are of great assistance in the study of orogeny. The general principles governing finite distortion have, of course, heen indicated by natural philosophers; hut little attention has heen given to their development, because the theory of finite strain is needless for computation of machinery, while this subject will not offer much purely mathematical interest until the stress-strain law is known experimentally. In particular, but little attention has been paid (so far as I am aware) to the planes of maximum strain, which turn out to be those in which geologists have a special interest. f In the following pages the attempt will lie made to develop all the manifestations of uniform or homogeneous finite strain in rock masses regarded as isotropic, exhibiting viscosity and capable of flow, which can be elucidated without assuming a law connecting stress and strain. For this purpose finite strain must first be discussed by itself; then it must he considered just how far the relations of stresses are capable of coor- dination with those of strain. The influence of viscosity and solid flow must next be shown. Readers willing to assume that these subjects have been logically treated will probably skip them and proceed to the geological applications which follow. Finally, the results will be com- pared with actually observed phenomena and with the experiments which several investigators have made on slaty structure. FlNITli ROTATIONAL STRAIN. LIMITATIONS OF THE PROBLEM. The mechanical effects short of rupture which force can produce in any mass are translation, rotation, dilation and deformation. The effects of mere translation may be considered separately from the other effects of force, or, in other words, one may consider these other effects relatively to some chosen point of the body itself. * I have previously endeavored t" show that some fissure systems are satisfactorily explained on the hypothesis of small strains : Bull. Geol. Soc. Am., vol. 2, 1891, p. 49. f < tn finite strain consult Thomson and Tait, Nat. Phil., 1879, sec. L81 ; and Ibbetson, Math. Theory of Elasticity, 1887, p. 09. 1 am much indebted t" l> Iff is the length of any- one of the axes, A, B and G are the three roots of the cubic — (n-AUv-B)(ji-0) = 1 f.» | 9 — (1 + flr) | [f2--f !/ (1 + « + 1 + /)2 + (a -" ^)2 + (l + «Xl+/)-«*} = 0. .(4) The volume assumed after distortion by the unit cube may be called /,3 = A BC=(1 + g) •[ (1 + «)(!+/)- a& } . (5) A3, and — Rotation. — The limitations of this discussion imply that the plane of A G can only revolve about G, so that the position of this plane is de- termined when the position of A is known. The angle which A makes with o x is, say, v, and this angle can immediately be inferred from (1) by a well-known formula which gives — a2 — &' + (l +/)'--( l+«)' Since the plane i? 0 is at right angles to that of A G, its position follows. To find the position which the same material lines A and B occupied in the unstrained mass, it is convenient to remember that they must have been at right angles to one another before strain as well as after it ; for mere rotation changes no angles, and irrotational strain is by definition a deformation in which the ellipsoidal axes maintain their direction. Hence, if// was the angle which the fiber A made with o x before distor- tion, its equation was y\x == tan //, and by the displacement formulas y' a + (1 + /) tan ft tan v = — = -rz — : — s — ,—j—, x (1 + e) -f- b tan ft The angle which the other axis made before strain was ,»■ + 90°, so that tan (fi + 90°) = — cot ft, while after strain it becomes v -f- 90°. Hence — tan 0 + 90°) = ?~(l+flZ* = ~ «* '■ v J ( 1 -\- e) — b cot fl 20 G. F. BECKER FINITE STRAIN IN ROCKS. From these two equations v can at once be eliminated, since tan v cot v = 1. Writing out this equation and reducing, one rinds— ton2,«- 2— ^1 + e) + a(1+'> - P~a!, + (1+/)*— (1 + e)1 The equations for v and p. can be combined to simpler forms. It will be found on trial that the values already deduced lead to — tan 0 + A0 = (i + , )_(i+/) 5 tan (v - /,) = (1 + ^(1 + f)- (6) The angle v — ;>. is the angle of rotation, so that the condition of no rotation is evidently a = b. When the strain is infinitesimal, a — b is infinitesimal, while 1 + e + 1 + ,f approaches 2. Hence v — fi is zero for vanishing strain. If the common limiting value of v and ,u is va, tan (y + ,a) = tan 2 v0, or — a 4- b tan 2 v_ = (1 + 0 -(!+/)■ Of course this same value is obtained by letting a, b, e and / approach zero in the formulas for tan 2 // and tan 2 v. Thus v — v0 = vo — //. It is evident that as rotation proceeds new fibers of matter constantly suc- ceed one another in the position of axis, the whole series of fibers in the unstrained mass forming a wedge, v0 — ,a or — — — • Lines of constant Direction. — Lines parallel to o z retain their direction relatively to the x y plane throughout strain. If the mass were inflexible and subjected to rotation, only these lines would maintain their direc- tion ; but when there is strain two other lines may retain their original direction, the two coinciding in the limiting case which separates that of three such lines from that of one. If /. is the angle which any line in the x y plane makes with o x before strain and / the angle which it makes after strain, then — tanx=y-J=ar(1+{)tanx- x 1 -f- e + b tan /. If X = /. this gives — which represents two real lines, unless the quantity under the radical ROTATIONAL STRAINS. 21 is negative. The two coincide when this quantity is zero, or when 4 ab -f (e — f)3 = 0. The value of tan /- then reduces to ± y —alb, showing that a and b must have opposite signs. This particular case occurs in the strain often known as shearing motion, as, for example, when a rivet is shorn by tension of the plates which it connects. It will be discussed later. The condition of no rotation can be derived from tan /.. The equation represents two lines, and if v.x and ■/.,, are the two angles, tan x1 tan y-.2 = — a I b. If there is no rotation, the axial lines are lines of unchanged direction and tan xt tan *.,= — 1, or a = 6.* SIMPLE STRAINS. Pare Rotation. — If the mass undergoes rotation without strain, each of the axes is equal to unity, and h has the same value. Then by (3), e ==f and a + b = 0, and by (5), (1 -f e)'2 = 1 — a2. Hence tan (v — p.) = al\/ 1 — ft'2, or sin (y ■-- ,"■) = a. This result can also be derived imme- diately from the displacement formulas. Dilation. — When the only strain is dilation, A--B = C —h, whether or not the displacements cause rotation. • Then by (3) e =/and a + b == 0. By (2) also (1 + ''■)"' + a2 — (1 +(/)2- The rotation is then given by — a a J 1 + « -,/ h* — a2 When there is no rotation, so that the displacements cause pure dilation, ft = b = 0 and e =f= g = h — 1. In dealing with dilations it is usually convenient to consider h, the ratio of dilation, as greater than unity, excepting when its value is unknown. The volume of a compressed mass is then l//t3, which does not vanish unless the ratio of dilation is infinite. ♦The length of the lines of unchanged length exhibits a somewhat remarkable relation. Let k be the length of such a line. Then— xl = y- = k, x y and by the displacement formulas— ?/ _ k — (1 +e) _ a x b k-(l+f) This gives— 2£ = l + e + l +/± tfiao + (e—f)*. If A.'j and k« are the two values of k, then — fcj fc2=(l +/) (1 + e) — ab, which by (2) is the product of the semi-axes or A B. Thus the product of these lines remains in- variable, whether or not they coincide with the axes. 22 G. F. BECKER FINITE STRAIN IN ROCKS. In any case whatever one may express the axes A and C under the forms A = A«, C = hp where « and p may be perfectly independent. Then, since ABC - h3, B =- hjap. The values >*, \jap and p are the values which A, B and C would have were there no dilation, and upon the properties of « and p depend those of pure deformation, accompanied by rotation: Shear. — A shear is the simplest possihle deformation. It may be de- nned as an irrotational strain, unattended by dilation, in which one axis of the strain ellipsoid retains its original length. The unit sphere is thus converted into an ellipsoid, the axes of which are «, 1, l/«; and a is called the ratio of shear. It is taken as greater than unity, excepting when it is dealt with as an unknown quantity. In dealing with shears it is convenient to employ the following ab- breviations : * 2 S = « — u~l ) 2 t = a -j- a-1. These forms imply that *2 — s2 = 1. The displacement formulas for a shear, the contractile axis of which makes an angle fl with ox are — %' = x (t — s cos 2 #) — ys sin 2 # ; i/ = y (a -f- s cos 2 #) — xs sin 2 # ; z* —z. To verify this statement consider that a = b, so that there is no rotation ; (j = 0 and (1 + c) (1 +/) — a0 =1) so that there is no dilation; tan Q, -j- //) = tan 2 v = tan 2 #, showing that the axes of the strain ellipsoid make angles »9 and >(> 4- 90° with o x; finally b (1 +/) + a (1 + e) is nega- tive, so that the minor axis of the strain ellipsoid makes an acute positive angle with o x as required. When # = 90° these equations reduce to — x' = xa; y' = yja; z' = z, and when & = 45°, a case of importance, x' = xff — ys ; y1 = ya — as ; 2' = 2. The quantity 2 s is called the amount of the shear. There are various aspects of this quantity. One way of looking at it is as the sum of two distortions. The elongation of the major axis is «— 1 and the contrac- — • ■ *Let a = cot "co; then it is easy to see that o- = l/sin 2 td and s = cot 2 to. Here, as will be show n later, 2 "to is the acute angle between the circular sections of the strain ellipsoid. The convenience of s and a- depends upon this fact, and the significance of the formulas is increased by bearing it in mind. The quantities s and a may lie regarded as hyperbolic sine and hyperbolic cusint "fan area \J< = In a ; and then !mi° — ■ 2 "to is the corresponding transcendental angle. This view of the functions, however, is not needful for the purposes of this discussion. MEASURE AND PROPERTIES OP SHEAR. 23 tion of the minor axis is 1 — 1 / «. The sum of the two is a — a-1 = 2 s. While 2s measures shear and is not unfitly called the amount of shear, s might e |ually well have been regarded as the measure of shear ; indeed, this would have been more convenient, because it would have accorded with the received nomenclature of stresses. Many of the properties of shear can be inferred in the simplest manner from its definition. Since it involves neither change of volume nor of the area of the strain ellipse, it can consist only in re-arrangement of matter, each fiber perpendicular to the plane of shear, retaining its original thickness, length and direction, though shifted to a new position. Since the major axis of the shear ellipse exceeds unity and the minor axis falls short of unity, there must be four intermediate radii of unit length, and the symmetry of the conditions shows that these four radii form two diameters. Thus there are two diameters winch have the same length after strain as before strain. These diameters are the traces on the x y plane of planes passing through >> :. ami these planes undergo no dis- tortion through strain. In them the circular sections of the strain ellipsoid evidently lie. All planes parallel to these are also, by the properties of homogeneous strain, planes of no distortion. Any two planes of no distortion must stand at the same perpendicular distance apart after strain as before, for were it otherwise the volume of the ellip- soid would lie changed. Thus a shear can consist only in the sliding of planes of no distortion upon one another and in changes of the angles between the two systems of undistorted planes. The behavior during the straining process of the planes of no distor- tion is of great geological importance ; but as this behavior depends to son^e extent upon rotation, it appears appropriate to. defer its discussion until some of the simpler compound strains have been explained. COMPOUND STRAINS. How treated. — For the immediate purposes of this paper it is needful to examine compound strains of several varieties. It seems desirable also to examine the simpler combinations in somewhat more detail than is absolutely essential to the results which will be deduced from them in the subsequent sections in order to give assurance that the geological deductions are not vitiated by the omission of important properties of strain. It is to be hoped also that the treatment here submitted may facilitate the solution of geological problems not touched upon in the present investigation. Pure Deformation. — Any pure deformation is resoluble into two shears at right angles to one another, one axis being common to the two ele- V— Bum.. Geol. Soc. Am., Vol. 4, 18112. 24 G. F. BECKER FINITE STRAIN IN ROCKS. mentary strains. This will be demonstrated by a proof that any relation whatever between the axes A, B and C of the ellipsoid whose volume is proportional to h3 can be brought about by two such shears. Let A = ha, B = hy, and let C = hp, where A and B are entirely arbitrary. Then since ABC = h3 = BJr, with o ./-, the displace- ments are given by— x' = x (I +s sin 2 <(>) — ys (1 + cos 2) ; y' = y (1 — s sin 2 ) + x s (1 — cos 2 <£). The product, a b = — s" sin'- 2 0, is an essentially negative quantity. Hence the signs of a and b arc necessarily different. Compare tin' discussion of formula (7). -(■Thomson and Tait, Nat. Phil., see. 17"). 26 G. F. BECKER FINITE STRAIN IN ROCKS. shear coincides with oy, displacing / to .<•" and //' to ,'/". the ratio being <>Y. then the displacement formulas :;: are — n -j ji V V7 ''s X = x a. = xax-i the strain reduces to two shears or, in other words, the scission vanishes. If a = 0 and (1 + e) / (1 4- /) = «32 the strain is an axial shear combined with a scission.* *A second Resolution.— The above method of resolution is the most convenient for computation, but it fails to disclose a relation of much geological significance. It is a fact that any plane undila- tional strain is resoluble either into two shears at an angle # or into a shear and a scission at an angle The significant difference between these two combinations is that the two shears cause a relatively small rotation which is an infinitesimal of the second order when the strain is infinitesi- mal, while the shear and scission produce a large rotation which is of the same order as the strain when this is infinitesimal. The criterion discriminating the two classes of strains is exceedingly simple. When a and b have the same sign the strain is invariably equivalent to two shears. When a and 6 have opposite signs the strain is invariably equivalent to a shear and a scission. As in the case of the other resolution, it is easiest to discriminate changes of notation from equations of condition synthetically. Let a and b have the same sign. Then to show that the strain is compounded of two shears one may proceed as follows : Adopt the notation — ,(!+/) +«(! + «). Sin2& = -Yba. a^ 2 j/ ab s2 a Each of these expressions is possible whenever a and b have the same signs, and then only. In addition, the condition of piano undilational strain is (1 + e) (1 +/) — ab = 1. Here, then, is a number of equations just sufficient to determine a, 6, e and/. Remembering that 1 + e and 1 +/ are necessarily positive, they give — a-**"*; b=-ass2sin2&; 1 + e = a8 (); 1 +/= 1~sl8iw2 with ox if the given values of a and b arc satisfied by choosing the upper sign in these expressions. In tin' opposite case the direction of the scission makes an angle 0 with o y. RESOLUTION OF STRAINS FROM DISPLACEMENTS. 29 The foregoing synthesis shows how a plane undilatio'nal strain maybe resolved when the displacements are given. Cases also arise in which it is desirable to find the displacements a, 6, e and / from a known shear and values of v and //.. If the ratio of the shear is «, the values of «r and s can he derived from it, and these two values, together with the values of v -f ;>■ and •> — ,"■ constitute four equations from which a, b, e and / can be deduced. They give — a = s sin (y + //) + n sin (y — //) ; 1 -p e = cos Q> — /j.) + s cos (* 4- ;i) • b = s sin (v + //.) — (7 sin (y — /1) ; 1 +/= cos (y — //.) — s cos (v -j- //.). (S) These values, substituted in the formulas of preceding paragraphs, show to what simplest strain system a given rotation and shear are referable. Strain due /<> Pressure. — For the sake of keeping the discussion of strains together, it may be assumed here by anticipation that a pressure produces a cubical compression of ratio h * and two ecpial shears of ratio a at right angles to one another. For brevity, let — 2 t = a — or1 ; 2 r = a + aT\ Then the displacement formulas for a strain due to a pressure in the direction -V are — x' = j (r — t cos 2 <*/) — ■'! t sin 2 # ;y' = \(T + t cos 2 >'/) — j t sin 2 = * ^T - *>• *- Here h is taken greater than unity, and is the reciprocal of the value which in a given case would satisfy (5). 30 G. P. BECKER — FINITE STRAIN IN ROCKS. Here the rotation is of the same order as the strain and is not negligible when the strain is small. If the strain produced by vertical pressure is combined with a shear at 45°, the value of z will be unchanged. If v., and •*, are the values of a and s for this added shear, and if/" and //'" are the final displacements for this case — x ==TT-5%' y -'-an- h >* = *'> ian (r-~fi = = ^m In this case, when the strain is infinitesimal, the rotation is an infini- tesimal of the second order. Elongation. — Simple elongation (unattended by changes in the area of the section perpendicular to the direction of elongation) is sometimes regarded as a simple strain. It may as well or better be considered as compounded of two shears and a dilation. In discussing dilation it was pointed out that the three axes of the strain ellipsoid may be written A = ha, B = Ji jap, C= hp. When the strain is simple elongation in the direction of JB, ha = 1, hp = 1 and B = h3jAC=h3. Thus elongation consists of two shears each of ratio h and a cubical dilation h. In the case of contraction or negative elongation a value \ is to he substituted for // and A: = 1 jh. Tims contraction is compounded of cubical compression ljk and two shears. If A is the same in the two cases, the same shears are involved in each strain but differently com- bined. In elongation the tensile axes of the shears coincide, while in contraction the contractile axes coincide. The same two shears which without dilation would stretch a mass to an infinite length, when differently combined would reduce it to an in- finitesimal thickness without cubical compression. PLANES OF MAXIMUM TAGENTIAL STRAIN. Position of wndistorted Planes. — Attention has already been called to the fact that in a simple shear the circular sections of the strain ellipsoid are undistorted planes parallel to which relative motion takes place, and further inquiry into them is essentia] to a full elucidation of this strain. In the other plane undilational strains there are similar plane-, though their behavior is modified in essential respects. In tri-dimensional strain the corresponding planes are no longer undistorted, 1 >ut nevertheless influence the character of the deformation. It seems most logical to begin with a discussion of the case of simple shear and afterwards to modify the results for complex strains. MAXIMUM STRAIN. 31 The circular sections of the shear ellipsoid for which the ratio is a make an angle with the major axis whose cotangent is a* If this angle is called m, the amount of shear is — 2 s = a — «-' = cot w — - tan us = 2 cot 2 us = 2 tan 1 90° — 2 us). Here s, or half the so-called amount of shear, appears as measured by the divergence from 90° of the angle 2 us between the circular sections of the shear ellipsoid. A right angle is the value which 2 m assumes when the strain is infinitesimal. The original position of the particles constituting the planes of no dis- tortion, relatively to the fibers which coincide with the axes of the ellipse, bears a simple relation to en. Suppose the shear to be axial and that the sphere .>','' + V\ + zi = ^' is converted into the ellipsoid x2/a2 -f y2\ = "'///•'7 then the original position of the material plane forming the circular section of the shear ellipsoid was dl tan us = „.= fan (90° — US). Thus these material planes made before shear the same angle with the minor axis of the ellipsoid which they make after strain with the major axis. Planes of maximum Strain. — It is instructive to regard the planes of no distortion from another point of view. Consider any two very thin plane layers in the unstrained mass which include between them the axis o z, and let the angle which they make with, ox be ).. Thus in the undistorted mass the angles bounding the wedge through which the cir- cular sections will sweep are v0 ± 45° and <>. ± (90° — ro). On the side of the minor axis toward which rotation takes place this range is therefore — v0 4- 45° - | n + 90° - ro 1 = ro - 45° + i^A and on the opposite side of the minor axis the range is — | ,, _ (90° - en) } - (v0 — 45°) = ro - 45° - VJZ^. The difference of range is thus the angle of rotation, and is actual when- ever the strain is a rotational one. In a simple shear, then, there is no difference in range, and the range on each side is en — 45°. In the case of scission or shearing motion it is easy to see that 2 (w — 45°) = v — //., so that the range is zero on the side from which rotation takes place, and one and the same set of fibers are exposed to maximum tangential strain throughout the process of strain, while the other circular section sweeps through the maximum possible angle. In any case of plane strain the difference in range is at once assigned by the angle of rotation, so that for two shears in the same plane at an angle of 45° the difference is measured by tan (v — //) = ss1\o. (l)] tan 2 en = {A _ By - 4 ^ _jy + (ft + by2 (■>) Case of Strain in three Dimensions. — It has been pointed out already that the relative motions of the particles in the xy plane due to a shear a are unaffected by an axial shear p in the B (.'plane. The sole effect of the second shear, so far as the x // plane is concerned, is to change the length of all lines parallel to the common axis of the shears uniformly in 34 G. P. BECKER — FINITE* STRAIN IX ROCKS. the ratio 3. Hence if before the imposition of the ft shear a Line made an angle w with A, this shear will alter the angle w to, say, a», and— tan a. Equations (6) also show that v + (x = 38° 40' and v — /x == — 6° T. If the displacements constituted a pure rotation, sin (y — <>■) would equal a. As tins is not the ease, there is strain. Formula (5) gives h = 0.962, so that the strain is a compres- sive one. If deformation were confined to the xy plane, 1 H- g would equal h. Hence there are two shears. To find them it is most con- venient to determine the axes of the ellipsoid from (3), which gives A = 1.275. B = 0.635, C= 1.1. Then also a = I / h = 1.325, j= C h = 1.143. Equation (1) shows that the major axis makes a positive acute angle with ox. The rotation, dilation and the ratios of the two shears are now known. To resolve the rotation and the a shear into component, plane, undila- tional strains, let %, bv e1 and^ be the displacements which would pro- duce only the a shear and the rotation. Then formula (8) leads to these values — ■ „, =0.0695 : 6, = 0.2872 ; 1 + e, = 1.2572 : 1 -\-f1 = 0.8113, which give for the elementary plane strains — a2 = 0.9168 ; o... = 1.2524 ; s, = 0.0708. The a shear with the rotation is therefore equivalent to a shear with its contractile axis coinciding with oy of ratio 1.2-324, together with a shear the tensile axis of which makes a positive angle of 4-3° with ox, its ratio NUMERICAL EXAMPLE. 35 being l/«2 = 1.0908 ; and lastly, a scission for which sl = 0.0708. Since <-)/2 = 19° 20', and at this same time the positions of the lines of maximum strain were at v ± 45° ; i. e., at 04° 20' or — 25° 40'. The original position of the fiber winch eventually constitutes the final major axis was at an angle <>. or 20° 20]' to ox. The original position of the fibers which at the end of the strain undergo maximum strain was at /.« ± (90° — 03) ; i. c, 75° 18 V and — 30° 37 ¥. The angles in the unstrained mass bounding the fibers which subsequently undergo maximum strain on the side from wdiich rotation takes place are thus, <>■ 4- 90° — w and v0 + 45°, and these differ by 10° ^Y. On the other side the limiting angles are ^0 — 45° and /i — (90° — m), which differ by only 4° 57*'. Thus the fibers on the positive side of the major axis pass through the condition of maximum strain more than twice as rapidly as do those on the negative side of the major axis. If the resistance wdiich the mass offers to deformation varies with the rapidity of deformation (as is the case with real substances), this difference wrill somewhat affect the results. Had a and b different signs, this difference would be far greater. The angle m for this example is by formula (10) 33° 25', so that the ,3 shear changes the direction of the lines of maximum strain by some o\ degrees, though without tending to produce any further relative motion upon them. Figure 2 is drawn for the displacements au bx, <\ and /n and illustrates the range of planes of maximum strain for this example. Finite Stress. relations of steess and strain. In the foregoing discussion the geometrical properties of homogeneous strain due to given displacements as exhibited on any principal plane of a strain ellipsoid have been developed, and I am aware of no important property of such strain which has been omitted. If the relations of dis- placement to stress (or force per unit area) could be as fully developed, we should have a substantial basis for a theory of finite distortion, since however heterogeneous a strain may be, any infinitesimal portion of the mass is homogeneously strained. 36 G. F. BECKER FINITE STRAIN IN ROCKS. The relations between finite stress and displacement lack satisfactory experimental basis and cannot therefore be fully developed, but it is desirable to show just where knowledge cuds and ignorance begins. Stresses in n Shear. — From the discussion of the properties of shear, it follows that the imdistorted planes are necessarily subjected to purely tangential stresses ; for they are neither elongated nor drawn apart during strain, while normal forces acting upon them would produce such effects. The stress phenomena in a shear can be examined as a case of equi- librium, and such an examination reveals the somewhat important fact that the planes of maximum tangential stress do not coincide with the planes of maximum tangential strain.* It also teaches how the two component forces involved in a finite shear are related, and thus, in spite of ignorance of the direct relations between stress and strain, the inquiry is by no means fruitless. J r -Q i i i i i JP i i -* : i i i a i a. \ i i Figure 3.— Stresses infinite Shear. Let the rectangle o b represent one-quarter of a strained cube and let — ■ Q and Pbe the stresses (or forces per unit area) holding it in this state of strain. Then it is easy to find the stress on any plane cutting the x y plane at right angles along the line a e. Let the normal to the plane make an angle # with o x. Then — ab = ac sin >'J ; be = ac cos >>. If i^and G are the component stresses on ac parallel to ox and o y, these components must hold the stresses on a h and a c in equilibrium. Now, the total force on a c in the direction of o x is — Fa c and the whole force on b c is Pb c. Q and G are similarly related, so that — — Fac = Pbc = Pac cos , ■ or — — F=Pcos <'/; G = — Qsin &. *In at least some treatises on elasticity and geological mechanics it seems to have been assumed that these planes do coincide. FORCES IN A SHEAR. 37 The position of the plane remaining" constant, it is permissible to com- bine J57 and G like simple forces to a. tangential component, T, acting in the direction of a c, and a normal component. iV, acting- perpendicularly across ac. Evidently, if P and Q are considered as in general positive quantities — T= — Fs!n 9 — G cos 9 = (P-f- Q) sin 9 cos ■>. N= —Fcos 9 — G sin 9 = P cos' 9 -| Q sin' 9, and T will be a maximum with reference to 9 when — cos2 9 = sm2 -V or 9 = ± 45°. Although the tangential stress is greatest for this angle, one has no right to infer that the maximum tangential strain is at 45°, because there is a normal stress on the plane at this angle amounting to (P-f Q) '-■ On the contrary, it was shown above (page 34) that the maximum tan- gential strain in a shear occurs for planes which make an angle with ox the tangent of which is 1 H. or the normal to which is given by tan 9 = a. The conditions of this plane are also such that there can be no normal stress acting upon it, and hence N= 0, so that one of the stresses must have a negative value and — ■ tan? 9 = Q This relation enables one to determine the forces which produce a finite shear. The area on which the stress Q acts is a, and the force acting on the distorted cube in this direction is minus Q a. The area on which P acts is 1/a, and the lateral force is therefore P/« ; hut by the last equation — Qa = Pja, so that a finite shear, as well as an infinitesimal one. results from the action of two equal forces acting at right angles to one another in opposite senses.* Simple Pressure. — -Knowing the composition of a shear enables one to pass synthetically to the case of simple pressure or traction. If two equal shears at right angles to one another are combined, the contractile axes coinciding, each mu3t produce the same effect as the other if the mass is isotropic. Each must also produce the same effect as if it acted alone. This statement does not imply a relation between stress and strain, for the shear in the xy plane leaves the mass unstrained in the y : plane. Hence two equal shears, each of ratio «, reduce the unit cube * I have met with no demonstration of this relation between finite shearing stress and strain, bul I am not prepared to state that none has been published. 38 G. F. BECKER FINITE STRAIN IN ROOKS. to a thickness l/«2 any of the sides of the mass having a length a. The upper surface has an area «2 and the side an area, 1/a. The tensile stress on sides of the mass is /' in each direction, so that the two tensile forces are each Pja. When only one shear acted on the mass the contractile stress was Q, but the second shear increased each' unit area to «, so that the contractile stress of the first shear was thereby reduced to Q J a. The stress due to the second shear is of precisely the same amount, so that the total contractile stress becomes 2 Q/aonan area «2. Thus the total force acting on this surface is 2 Qa} which, as has heen shown, is equal to 2 Pja in absolute value. Let the mass thus strained he subjected to an hydrostatic pressure equal to PI a. Then the tensile forces would be balanced and the pressure on the upper, surface would become 3 Q a. Thus, two equal shears combined with an hydrostatic pressure equal to either component of either shear, applied to the unit cube, reduce to a simple pressure acting on one surface of the cube. Had the shears been so combined that their tensile axes coincided, a dilational stress equal to either component of either shear would have been needful to reduce the system to a simple traction. Conversely, it is evident that a finite traction or pressure is resoluble into a dilational stress (positive or negative) and two shearing stresses, just one-third of the force being employed in each of the three component stresses. It is well known that precisely this resolution takes place for infinitesimal tractions, but the analysis of such tractions is usually stated as if the conclusions were true only for the limiting case of infinitesimal forces. These results seem to exhaust what can be known of the relations of finite stress and strain without a further knowledge of the actual value of a in terms of Q. No two different pressures or different shears or dila- tions can be compared without a law relating to stress and strain. Meaning of Hooke's Law. — It was to fill this gap that the famous law of Hooke was proposed. This is Ut tensio sic vis, which is now translated, Strain is proportional to stress. The brevity of Hooke's law has often been admired. The fact is that it is too brief folly to express the mean- ing really attached to it. It does not appear in this form of the law whether the stress (or pressure per unit area) is to be reckoned for the solid in an unstrained state or after the mass bus reached a condition of equilibrium under the action of the external forces tending to deform it. But since the purpose of the mathematical theory of elasticity is to find equations expressing equilibrium of elastic masses, it is clear that this equilibrium must be supposed established before one can reason on the system of stresses which will maintain it, As a matter of fact, the lunda- hooke's law. 39 mental equations are always derived in this way. and the stress is taken primarily as the force per unit area of the mass in a state of equilibrium. Tims, a less ambiguous statement of this law would be: Stress in an elastic mass which has reached a condition of equilibrium is proportional to the strain which the mass has undergone. It is a curious fact that this is not the law which Hooke intended to express. Hooke's words arc " JJt tensio sic vis: That is, the Power of any Spring is in the same proportion with the tension thereof: That is, if one power stretch or bend it one space, two will bend it two, and three will bend it three, and so forward."* Thus Hooke's law as he meant it is clearly load is proportional to strain, and he had no idea of confining his law to infinitesimal deformations. When the stresses and strains are infinitesimal it is easy to show that the two assertions, stress is proportional to strain and loadis proportional to .-train, are really equivalent : but for finite deformations they lead to very different results. Let a unit cube he extended to a length 1 + e by a load L, and let the reduced area of the cross-section he J. Then the tension per unit area or the stress P is given by — L = AP, and if stress is proportional to strain, p= Me, or L = AMe, where M is the constant, called Young's modulus and sometimes (though* improperly) the modulus of elasticity. As was shown above, exactly one-third of the load is-employed in producing dilation, however great L may he. Hence if/.' is the modulus of compressibility, the volume of the distorted cube is 1 /. '■'> !:. The volume is also the area of the dis- torted mass multiplied by its length, or J. (1 + e). Thus — , 1 + LIB /■ Substituting this value in the last equation gives an equation between Load and strain, viz : L — Me + Le 3 k ~ M = 0, ■ > fc ♦ Quoted by P. G. Tait, " Properties of Matter," 1890, p. 204, from Hooke's lectures " de Potentia Restitutiva." VII— Bum,. Gkol. Soc. Am., Vot. 4, 1892. 40 G.F.BECKER — FINITE STRAIN IN" ROCKS. which is ;ui hyperbola in L and e asymptotic to ■ , and L ::/.•--. 1/" :\I,-M Thus the fundamental assumption really made in the theory of elas- ticity is thai the load-strain curve is an hyperbola instead of the straight line which Hooke supposed to represenl the relation. The difference, however, as already remarked, is without consequence, so Long as de- ductions from it are confined to very minute deformations/- Stress System. — Any force acting on one face of a cube may be resolved into a normal component and two tangential components acting in the directions of the edges of the face. Hence the most general system of forces of constant direction acting on a cube is resoluble into six normal components and twelve tangential ones. If the center of inertia of the cube is at rest, the normal forces on opposite faces must be equal, and *Naturt of tin' Proof of Hooke's Liw. — Hooke's law holds good, or, in other words, there ia a linear relation involving a finite parameter betwe ra sm ill str - - and strains, provided — train curve fulfills two conditions, viz.. that the curve is continuous both in form and value, and that the tangent of the angle which it makes with the axes at the origin is finite. Ii seems to me that some discussion and even some confusion would have been avoided if -elasticians had taken this u lometrieal view of the functions rather than a purely alg bi deal one. Thus Green simply assumed that the stress-strain function was developable, and that the development contained i term in which only the first power of the variable appeared, while < lebsch seems to have lool upon this algebraical relation as a mathematical n ssity. This it certainly is not, for there are many continuous functions the development of which contains no term in the first power of the variable. These all represent curves which coincide with one of the axes at the origin : e. g . the hyperbola referred to the vertex as origin.— Mr J. W. [bbetson, in his excellent Mathematical Theorj of Elasticity, makes an attempt to demonstrate Hooke's law by pure reason, independently 8f experiment, tie expressly assumes, however, that the eurvi is i luous, and he states, without any atl imp! al pi th I i i ite of • n i ition of any traction component with any strain rdinal -can never change sign or vanish. '1'his last is equivalent to asserting that the curve cannot coincide with either axis at the origin. These two assumptions tog ther cover the whole ground of Hools i's law, and really leave nothing to be | I 5aint-Venant, in his edition of Clebsch, p. 10, attempted to show thai if the internal stresses of an elastic mass depend in any it in i mas manner on the mutual distances of the molecules, Hooke's law follows. He points out thai continuity involves a linear relation between the differentials of a function and th differentials of any variable. He then sho on the assumption mad - corresponding small and strains are corresponding differentials, and deduces the conclusion stated above. This arg«menl does nol sa al all, for though one maj undoubtedly wri =Adx, when- A is con i 'iii md tl on is therefore linear, yet A may have and often do !S have the valu iro or infinity. Saint-A maul made no attempt in the passage referred to to show that I must !"■ finite in the case of elastic strains, and seems to have overlooked the necessity for such a proof, [n the ime work, ] elastician forcibly remarks : "Generally and philosophically no purely mathematical consid I the mer in which thi ictingonthe elements of a bodj an I th ■ ■< mges which they produce depend upon one another." Experiment alon md o ily somewhat refined experiment, betr 13 - the I i i thai even the h ir lesl substance? yield somew hat to the smallest pressures, and that the stress-strain curve is con t inn in form as well as value from positive to negative strains. One set of experiments is needful how th i • I itl ud of a steel bar which is clamped at the i listorts it, and other set is re [tiired to shew that the distortion is of the 9am • absolute amo tnl whether the tly settles on the upper or the lower end id' the i, GENERAL STRESS SYSTEM. 41 the twelve tangential forces must consist of six couples, each tending to produce rotation. In this paper consideration is confined to those cases in which there is a tendency to rotation only about the line o t, and this limitation elimi- nates four of the couples. Thus the case to be considered here consists of three pairs of normal forces and two unequal couples tending to pro- duce rotation in opposite directions. This force system is shown in the following diagram : & -" ■ p *- 1 R ^ 1 "l <: — c 1 1 J -c' -*. ' ->c, -*T Figure i. — System of Forces. It has already been shown that any normal force, whether finite or infinitesimal, is resoluble into a dilation and two shears, exactly one- third of the force producing dilation, and the remainder producing two equal shears at right angles to one another. Analyzing each of the nor- mal forces P, Q, R separately, it will appear that the action of all of them may be tabulated as two shearing stresses and a dilation— thus : Axes of .'■ >i : Dilation Shear . . Shear . . Sum . . . ':!/'+ Q+ R) KQ + R-2P) 0 '; IP+Q + R) }(Q+ R — 2P) I (Q+ P — 2R) i(P+ Q+ R) 0 HQ + -P-2 R) Q i; Turning now to the coiiples <\ and C2, and supposing Qx > C!,, their combination is equivalent to two equal and opposite couples, each equal 42 G.P.BECKER — FINITE STRAIN IN ROCKSi to (.[. and a single unbalanced couple, C\ — < ',. The combination of two equal and opposed couples is easily shown to be equivalent to a shear, the axes of which bisecl the angles made by the component forces.* Here, therefore, the balanced couples arc equal to a shear at 45° to Por Q. There now remains a single unbalanced couple tending \i n<- 1< l<- and both of these may become imaginary. f Thomson and Tait speak of these lines as unaltered indirect! luring the change of straii they may have meant by rather than during. Nat. Phil., section 181. 44 G. P. BECKER — FINITE STRAIN IX ROCKS. belo re strain will keep this direction during strain only when the mass acts as if it rested on or against an inflexible support. 1 f this support is parallel to o x, either tan x = 0 or : tan y. =llZJ = tan (90° -f 2 x0). Properties of Matter. Viscosity. — The ideal elastic substance is one which requires a perfectly difinite stress to hold it permanently in any given state of strain at a given temperature. This stress is wholly independent of previous states of strain or rates of straining. Heal substances fulfill this definition only under certain conditions, and careful experiments always show that the more rapidly deformation is produced, the greater is the resistance to be overcome. Thus a spring, suddenly stretched by a given weight, yields rapidly to a certain extent and may seem to become stationary ; but careful observation shows that is continues to yield slowly to the traction for a time, though it ultimately comes to rest. If the material were ideally elastic, it would immediately assume this ultimate state of strain- and the fact that the attainment of equilibrium is gradual proves that the original resistance is a function of the rate of deformation. Fluids show similar phenomena. Viscosity is that property in virtue of which matter presents to stress a resistance into which the rate of deformation enters as a factor. Viscosity and shear are inseparable, and mere dilation is unattended by viscous phenomena* The coefficient of viscosity of a substance is ceteris paribus, the shearing stress required to produce the unit shear in the unit time. The degree of viscosity is considered as increasing with this coeffi- cient, so that sealing wax and tar are more viscous than water, and steel is more viscous than lead or copper. Substances which yield indefinitely though slowly to stresses, however small, are now known as viscous fluids. Those which in the course of time reach statical equilibrium under the action of deforming stress, such as tallow and steel, are called viscous solids. If stress is applied very slowly (or rather infinitely slowly) viscosity does not come into play. Thus, a viscous solid or fluid in permanent * Viscous resistance is often likened to friction. Each is a dissipative resistance to tangential motion, but there are marked differences between them. Friction exists only where there is normal pressure, and is therefore wholly absent on the planes of maximum tangential strain in a shear. Friction also has its maximum value when the surfaces between which it exists are at rest. Viscous resistance opposes relative motion of surfaces between which there is no normal pressure when the rate of motion is finite, bul vanishes when this rate is infinitesimal. Thus their is rather an analog} than a similarity between viscosity and friction. VISCOSITY. 45 statical equilibrium acts like an ideally clastic or ideally fluid mass. Under these conditions the resistance winch a solid offers to deformation is due entirely to its "rigidity," this term being defined in the theory of elasticity as the degree of resistance winch a solid in permanent equi- librium opposes to stresses tending to change its shape* Under this definition india-rubber and tallow possess rigidity as well as cast iron, but the modulus of rigidity of the metal is greater than that of the gum or the tat. In short, rigidity is an essential property of solids. A highly viscous fluid subjected to a stress of brief duration presents greal resistance to deformation. Thus, if the earth were substantially a mass of sufficiently ultra-viscous fluids, it would behave to the attrac- tions of the sun and moon sensibly like an infinitely rigid body, because of the rapid change in the direction of these attractions. There are valid grounds, however, tor the belief that the earth is really solid. The viscosity of rocks often controls the directions in which they yield to stress. When two equal stresses acting on the same rock-mass change their directions at different rates, that stress which rotates at the smaller rate will encounter the smaller resistance and will produce the greater effect, It has been shown in the earlier part of this paper that all rota- tional strains are accompanied by relative tangential motion on two sets of mathematical planes which rotate relatively to the mass at different rates. The difference of their effects due to viscosity will be discussed under the head of geological applications. Flow. — At least some solids in the so-called "stale of ease " (freedom from internal partial constraint) almost completely recover their original form after small strains when time is allowed to overcome the viscosity. It is apparently true of all bodies, however, that when strained beyond a certain limit short of rupture, they are permanently deformed. The process by which this deformation is effected is termed flow, and the limit at which a, substance initially in a state of ease begins to flow is called the limit of solidity. When the limit of solidity differs hut little from tin; ultimate strength, the substance is known as brittle. When the limit of solidity is a fixed quantity, so that any excess of stress pro- duces continuous flow, the mass is said to be plastic. When a continu- ously increasing stress is needful to produce continuous How, the sub- stance is said to be ductile, and in this case a " hardening " of the mass attends the flow, as. for example, in the manufacture of wire. Plastic flow thus differs from ductile flow. 1 am not aware of any phenomena which point decisively to. the existence of ductility and the attendant hardening among rock masses, but it cannot he amiss to call *The word rigidity, as used in the theory of elasticity, lias nearly the same aning as stiffness in common parlance. 1(> G. F. BECKER— FINITE STRAIN TX ROCKS. attention to this property, which possibly plays some pari in the interior of the earth if not near the surface. Plastic flow certainly plays an important part in geological mechanics- The motion of glaciers is known to be in part ascribable to it. and it is clearly evinced in the details of rock structure. At greal depths below the surface a partial gradual relict' of strain in any rock mass will bring to bearagrad.ua! increase of stress difference, which may be considered entirely indefinite in amount. Granting, then, that there is no infinitely brittle rock or no rock in which the ultimate strength tails short of the limit of solidity, flow must ensue at great depths whenever a sufficient relief of strain occurs. No geologist need- to be reminded of the instances pointing to such flow. They are innumerable and most various. If a mass capable of plastic flow is suddenly subjected to ;i definite load greater than it can hear without flowing, one-third of the load will immediately he employed in compression and the process of flow will produce no further modification of the volume. Flow is thus continuous shear. The shearing process must take place along certain lines, and these must he the lines which are first strained beyond the limit of solidity. In other word-, flow must take place along the lines of maximum tan- gential strain discussed in a former part of this paper. ami which by I 10) stand at an angle 90° — <» to the line of a simple, direct pressure. When the load is of fixed amount, the stress will gradually diminish as the mass flattens out; so that the last lines of How will make a smaller angle with the line of force than the earlier ones. A greater amount of flow would occur along the earliest lines affected. If the mass were of such a char- acter as to show evidences of the relative motion after equilibrium had been reached, a cross-section of it would reveal a structure at Least com- parable with schistosity. the flatter lines being more pronounced than the steeper ones. Relation of plastic Solids to Fluids. — Let S he the resistance which a plastic solid opposes to distorting stress at the elastic limit, and let u he the stress which would he required to produce the unit shear it' the mass were perfectly elastic (or, in other words, the modulus of rigidity); then if stress is proportional to strain. S/n is the shearing strain which the mass experiences at the elastic limit, and any greater -train would be accompanied by flow. If the mass continues to How as long as the stress is maintained above the fixed limit S/n, the substance is known as per- fectly plastic. If S is infinitesimal, the mass will yield to any shearing stress, however small. Such a mass, resting on a level surface, would spread out to a layer of infinitesimal thickness, much like a fluid. It does not follow. PLASTIC SOLIDS. 47 however, that because S is very small, n is also small. The rigidity of a mass seems quite independent of its elastic limit. Tims wrought iron and cast steel have nearly the same modulus of rigidity, though the elastic limit is very different for the two substances. A material, then, may have a very low elastic limit and yet oppose great resistance to de- formation within that limit. If the rigidity of a mass is great, the lines of maximum tangential strain under pressure will make angles of little more than 45° with the line of pressure. If such a mass is prevented from undergoing relative motion in these directions, a much greater force will he necessary to com- pel it to move in any other direction. Fancy a cube of matter of low elastic limit, but great rigidity, placed in a shallow tray just wide enough to receive it; and let a small, uniformly distributed pressure be applied to the upper surface of the cube. Then, above the edge of the tray, the mass would break down at angles of about 45°, but the lamina' standing Figure 5. — Plastic Solid under Pressure. at 4o° and supported by the tray could not move sensibly. The result would be that a pyramidal mass would remain in the tray, forming an angle of 45° with the line of pressure. This is substantially the way in which a body of solid, discrete parti- cles would act. A cube of such material released in a, tray would resolve itself into a pyramid, sloping at the angle of rest. It is also easy to show that the maximum value of this angle is 45°.* A mass of very tine powder composed of frictionless spheres would be perfectly plastic, inas- much as it would yield to any shearing stress, however slight, which were not resisted by external constraint. The elastic limit would also be zero. Its rigidity could be displayed only when flow were prevented by constraint in the direction in which flow tends to take place. It would then evince rigidity by its ability to retain a pyramidal shape. In short, a mas-; resembling shot of infinite fineness appears to represent the case of a perfectly plastic solid with infinitesimal elastic limit. *The angle of rest is, say, p, and tan p = S/ N, where N is the normal pressure, and R the fric tional resistance due to'this pressure. This resistance cannot exceed the pi — ure to which it is due, and B - A cannot exceed 1, tli<- tangent of 15 - VIII— Bui.t.. Geol. Soc. Am., Vol. -1, KS92. 48 G. F. BECKER FINITE STRAIN IN ROCKS. Consider now the case in which n is very small and S great. This case also bears some resemblance to a fluid. A cube of material with these qualities would yield to the slightest pressure, and the strain ellipsoids would be flattened to infinitely thin disks. The lines of maximum tan- gential strain would therefore be perpendicular to the line of pressure. To convert this solid into a liquid the elastic limit and the rigidity must both disappear; but this is not of itself sufficient. The flow of a liquid takes place perpendicularly to the direction of pressure; consequently, in the solid which approaches infinitely near to the liquid state, the strain ellipsoids must be infinitely flattened before flow begins. This relation is secured if S is infinitesimal and n is an infinitesimal of the second order. In the discussion of strains it was shown that the lines of maximum tangential strain, or the lines on which flow must take place, make an angle with o x, which has a certain value, m. It appears from the above that this angle has a value of 45° for an infinitely rigid solid, even if this solid is perfectly plastic and has no elastic limit, so that it is reduced to molecular powder. For fluids, on the other hand, this angle is zero, and the rigidity is an infinitesimal of the second order. Intermediate values of m answer to solids of moderate rigidity. Rupture. — In a homogeneous mass under pressure, rupture must take place on the lines of maximum tangential strain: for rupture is strain carried to such an intensity that cohesion is overcome. A mass in which flow has preceded rupture cannot be regarded as homogeneous, since in the direction in which flow occurs the strength of the mass may be and perhaps must be weakened. In the case of pressure this makes no dif- ference, the tendency to flow and to rupture being in the same direction. Tensile stresses produce ruptures by a different method. One can conceive of a mass breaking up by mere dilation or without any relative tangential motion, while purely compressive forces cannot be imagined as leading to rupture. In tensile strains shears cooperate with dilation. Thus, if a bar under tension is homogeneous, the tension will be relieve. 1 by the smallest possible fracture, which is in a direction perpendicular to the axis of the bar. If, however, the bar has undergone flow along the surfaces of maximum tangential strain and has thus been sensibly weakened in these directions, it may split diagonally to the axis or irregularly along some other path of least resistance. Thus, a rubber band when suddenly stretched almost always breaks as straight across as if cut with scissors, but a bar of mild steel gradually stretched to the breaking point often splits diagonally, while a wooden bar gives a most irregular surface of fracture. In rocks, tensile rupture and fracture by pressure can often be distin- RUPTURE. 49 guished. Granites, and even conglomerates, often break under pressure in extraordinarily smooth, continuous, plane surfaces. Under tension the rupture of granite would follow an irregular surface of least resist- ance, leaving projecting crystals on each side ; and in conglomerates few pebbles would be broken, nearly every one adhering either to one frag- ment or the other. Stratified rocks under tension would behave much like a wooden bar. Only unusually uniform rocks could give smooth surfaces of rupture under tension. Such surfaces do occur in the case of columnar eruptives, and these columns can be shown to be produced by tension in the cooling mass. Even when tension produces surfaces of rupture which are smooth, they are apt to be curved or broken. In a word, tension tears masses asunder; pressure cuts them to pieces. Geological Applications. Cases to be considered. — It is probable that pure dilation and pure irro- tational shear are strains of rare occurrence in rock masses. One of these requires two, the other three pairs of forces acting at right angles to one another with identical intensity. Simple pressure, on the other hand, is common, especially where disturbances are not in progress. During orogenic changes inclined pressures must be frequent. The most im- portant stress systems are therefore direct pressures and inclined press- ures. The last includes two cases, in one of which the mass suffering pressure rests upon or against an unyielding support, while in the other the mass rests upon or against materials which yield readily. In the former of these cases the stress system reduces to a simple pressure, com- pounded with a scissive stress ; in the latter to a pressure and a shearing stress. In dealing with each strain viscosity and a tendency to How or rupture must be considered, the aim being to relate actual phenomena to their immediate causes and to enable the geologist, in some measure at least, to judge of the local direction of the forces the effects of which he observes. When gravity acts noon a mass homogeneous strain is. strictly speak- ing, impossible, excepting within infinitesimal limits of space, each level surface being subjected to greater pressure than the next above it. On the other hand, the forces involved in the deformation and fracture of rocks are very great, except in some extreme instances, such as that of moist clay. For ordinary firm rocks the ultimate strength is such that a column of from one to several thousand feet in height would be needful to produce at its base a pressure sufficient to induce rupture. Conse- quently,in masses of such material from a few score of feet to n lew hun- dred feet in thickness, gravity plays but a small part compared with 50 G. F. BECKER — FINITE STRAIN IN ROCKS. rupturing stress ; and portions of the rock having dimensions of this order may often properly be regarded as homogeneously stressed. When large masses are similarly strained, gravity may determine in which of several directions, all equally stressed by external pressure, rupture will take place. Cases of such determination 1 have discussed in a formerpaper* Effects of direct Pressure. — A direct, uniformly distributee1 pressure of sufficient intensity, applied to an elastic brittle mass presenting great re- sistance to deformation, would induce fracture. The ruptures would take place along those lines subject to the greatest tangential strain, since these are the directions in which the material would first be strained beyond endurance. These lines would stand at 45° to the line of force if the mass presented infinite resistance to deformation. If this resist- ance is not infinite, they will stand at greater angles to the line of force. The angle which the normal to the direction of rupture makes .with the line of force is called w in the discussion of the strains (see p. 34). There will generally be more than one direction of rupture, and in masses the thickness of which in the direction of pressure is considerably smaller than the lateral extension, there will often be four systems of parallel fissures, two systems answering to each of the two equal shears arising from simple pressure. If, however, there is any inequality of re- sistance in the plane perpendicular to the line of pressure, whether this is due to the character of the mass under pressure or to inequalities in the support which this mass receives from its surroundings, the strain ellipsoid will have three unequal axes, and rupture will take place only in the plane of the greatest and the least of these axes. In this very common case the mass will be divided into columns, with angles de- pending upon the strain. "When the mass is large and the pressure is horizontal, gravity opposes the tendency of the vertical axis of the strain ellipsoid to elongate, and rupture will tend to take place by relative motion in horizontal planes, separating the rock into vertical columns. The constraint of surrounding masses may outweigh this tendency. Something can be said of the spacing of the fissures thus formed, but this subject can be most conveniently discussed under the head of in- clined pressure. If the pressure continues alter rupture has occurred, the Mocks or columns will grind against one another producing slickensideSj and sometimes further ruptures, of which the discussion will also be deferred. Many rocks under the action of direct pressures rapidly applied behave approximately as highly elastic brittle masses of greal rigidity, and in these cases the range of the planes of maximum strain is practically nil. Consequently, systems of fissures at sensibly right angles to one another ♦Bull. Geol. Soc. Am., vol. 2, 1891, p. 62. SIMPLE DIRECT PRESSURE. 51 are not infrequent, nor js it very unusual to find such a pair of systems of fissures accompanied by a second similar pair in a plane at right angles to the first. The residual blocks are then bounded by from four to eight planes. In the last case four of the planes are parallel to the other four * In many cases the rock does not rupture without previous deforma- tion of considerable amount. When this happens the lines of rupture make an angle of nTore than 45° with the line of force. The normal to the direction of rupture then makes an angle w with the line of force, and this angle decreases with the deformation. If the deformation were very great,as it would be with a mass of india-rubber, u> would approach zero. If the direct pressure were relieved by rupture and the rock were perfectly elastic, the residual fragments would recover their original shape, and their acute angles would then lie in the line offeree. Thus when rocks show fissures cutting one another at acute angles it is certain that finite deformation has taken place. If the mass has remained under tension, the line of force when direct bisects the obtuse angles. If the mass has been relieved of pressure and the rocks have acted as elastic masses, the line of force bisects the acute angles. It is usually possible from general conditions to judge which of two rectangular directions is the more probably that from which a rupturing force has acted. I have, however, never yet met an instance in which it seemed to me that the line of force bisected the acute angles" of fissure systems. Orogenic forces are commonly very persistent, and even if a mass behaved as substantially elastic up to the moment of rupture, it is improbable that the residual blocks would continue capable of regaining their original shape after the lapse of, say, even a few years. In many cases it is quite clear that deformation has become permanent. Thus I have examined very numerous pebbles in conglomerates, some of which had been much flattened by pressure and others also much fractured. The direction of flattening was then a certain indication of the direction of force, and this direction bisected the obtuse angles between the fissure systems intersecting the pebbles. In other cases the character of slicken- sides and accompanying faults shows that no reversal of motion has taken place, and that the residual masses must have lost the elasticity which they seem to have exhibited up to the moment of rupture. Observations on artificial structures seem to confirm this opinion. It lias been pointed out by Mr. Clarence; King aim1 others that slabs of marble supported at their ends or corners gradually sag toward the center. So, too, in old buildings, such as the Alhamhra, 1 have seen slabs of rock very much bent by c\m\ pressures acting for hundreds of * When a rock fragment is lioun.li> I by planes \\ ith more than lour differently directed normals, it must have undergone successive ruptures 52 G. F. BECKER FINITE STRAIN IN ROCKS. years. This does not imply that there is no true elastic limit, but only that it is lower than brief laboratory experiments would lead one to suppose. Were there no elastic limit, it seems to me that we should find, for example, quartz crystals in vugs among the more ancient rocks sensibly distorted by their own weight. Usually then the line of a simple, direct pressure which has produced two or four systems of fractures in large rock masses, or in the pebbles of conglomerates, will he found to bisect the obtuse angles between the fissures as the mass now stands. In any case, where it is suspected that the line of force bisects the acute angles between fissures, the slickensides should be minutely examined to ascertain whether they show reversal of motion, and all the attendant phenomena should be investigated. When a simple pressure on a rock mass increases very gradually, it will for some period exceed the elastic limit of the rock and fall short of the ultimate strength. Flow must then take place. The only feature of this flow which will reveal itself to observation will lie the relative move- ments of adjoining particles. Hence, although the path in space of each particle will lie hyperbolic,* the evidence of movement will indicate rela- tive transfer of adjoining particles in opposite directions along lines of maximum tangential strain. The energy of this relative movement will evidently increase with the excess of the pressure above the limit at which flow begins, sometimes called the limit of solidity. Thus, if one supposes the pressure suddenly to surpass the limit of solidity and then to be kept constant, the mechanical effects of the rela- tive motion (and the chemical effects attending the expenditure of energy) will be very pronounced on the lines on which flow begins. As the pro- cess continues and the stress diminishes with the increase of the area of the mass, the lines first affected will make an increasing angle with the line of force, while the new fibers of the material which are forced into the direction of maximum strain will be less and less affected. The result will at least resemble schistose structure and will be marked by the presence of lines of relative movement intersecting one another at very acute angles. In the case of direct uniform pressure there will be four such sets, each set at a large angle to all the others. If the load were to increase in the same proportion as the area of the loaded mass, so that the stress would be kept uniform, an indefinite amount of flow might be produced, provided that the rock is not hardened ♦During flow there, is no progressive change of volume. Hence, a point for which at the incep- tion of flow x = 1, y = 1, will be moved to a point x', i/, and .<■"- y' — 1. The curves of this form are sometimes called the lines of flow They would be more aptly called lines of absolute movement. They should carefully hi' discriminated from the lines of relative movement, which are straight. The hitler are the only ones of which the deformed mass can give direct evidence. 1 n i he case of simple shear the lines of absolute movement are simple hyperbolas asymptotic to the axes. ARRANGEMENT OF PEBBLES BY WATER. 53 like drawn wire. If the Aoav were very great (literally infinite) the lines along which relative movement took place at the inception of strain would become horizontal. The schistose partings would then in each set range through the %ngle «>. Relative motion, in a mass subjected to direct uniformly distributed pressure, can only take place perpendicularly to the line of pressure when the strain ellipsoids are infinitely thin discs or when the rigidity is zero. In other words, only liquids, viscous or otherwise, can act in this manner. The behavior of semi-fluid material, like wet clay, approximates closely to that of a viscous fluid. Rigid Disc in rcxixliiHj Medium. — The behavior of an elastic mass under simple pressure leads to an extremely simple method of proving a dynamical proposition of much importance to geologists. A simple pressure acting against a resistance converts any sphere of unstrained matter into an oblate ellipsoid of revolution, the minor axis of which is in the direction of the pressure. If the constant pressure were to exceed the constant resistance, the mass would move in the direction of the pressure and of the minor axis of the oblate ellipsoid. Now, it is a well- known fact that the whole or any portion of an elastic mass which is in equilibrium, whether at rest or in motion, may be supposed to become infinitely rigid without disturbing the equilibrium. This is an almost self-evident proposition, for a mass is in equilibrium only when there is no influence tending to change its form, and it therefore makes no differ- ence whether this form is capable of change or not. Hence in the present case the strain ellipsoid may be supposed replaced by a rigid mass. Consequently a rigid ellipsoid of revolution moving under the influence of a pressure against a resistance will be in equilibrium when it opposes its greatest surface to the resistance. Similarly an elastic sphere under tension becomes a prolate ellipsoid, and consequently a rigid prolate ellipsoid moving under the influence of tension against resistance will be in equilibrium when its longest axis coincides in direction with the tension. If a cube were circumscribed about either of these spheres, with four of its edges in the direction of the force, it would become a rectangular parallelopiped with sides parallel to the axes of the ellipsoid. Any plate or rod may be made up of a single layer or row of such flattened or elongated cubes. Hence any rigid disc or rod moving against a resist- ance under the influence of pressure will be in equilibrium when its smallest dimension is in the direction of pressure. If it moves under the influence of traction, its longest axis will fall into the line of traction. If a flattened pebble is dropped into a running stream, the water will exert a pressure upon the stone until its inertia is overcome, and during 54 G. F. BECKER — FINITE STRAIN IN ROCKS. this time the pebble will tend to swing across the current so as to present its greatest area to the pressure. As soon as the resistance duo to its inertia is overcome, the pebble will sink through the water as if the fluid were at rest till its edge touches the bottom, and it will then lip down stream till it meets support. In rapid steams irregularities in the bottom cause local upward currents, which project pebbles into the main current much as if they had been dropped into it. These pebbles sink to the bottom again where the movement of the water is more uniform. Many pebbles thus deposited will, with few exceptions, be inclined down stream and will rest against one another, like overlapping tiles. This relation explains the fact that both in modern streams and in the ancient river channels containing the auriferous gravels, many of which have been tilted since their deposition, the pebbles, as miners say. "shingle up stream," or, as zoologists would express it, "imbricate" toward the source. Elongated, rOd-like pebbles are usually found lying across the channel. The indication afforded by this behavior of pebbles seems entirely trustworthy so far as the local current is concerned. In applying it, however, it must be remembered that powerful streams arc often accompanied near shore or close to obstructions by local " hack currents," in which the pebbles would be arranged in a direction opposite to that of the main stream. If a flat pebble or a mica scale is allowed to subside in relatively quiet water, the fluid may be considered as exerting a pressure on the lower side against a resistance due to the action of gravity on the stone. The disc will then tend to assume a horizontal position. It is for this reason that allothigenetic mica scales in sandstones or other rocks usually follow the direction of the bedding. In massive sandstones this is an assistance in determining the true stratification. A very familiar illustration of the action of the strain ellipsoid moving against resistance is afforded by a bubble of gas rising through still water. The spherical bubble is compressed to an ellipsoid, which might be re- placed by a rigid mass of the same density, and it rises with its equator in an almost perfectly horizontal plane. On beaches pebbles are sometimes imbricated for a few feet in one or another direction and sometimes lie nearly flat. The constant reversal of the currents due to breaking and retreating waves prevents any exten- sive methodical arrangement, and this fact is of assistance in discriminat- ing marine gravels from river deposits. There are also instances of the almost self-evident fact that a rod-like mass moving under the influence of traction, like a vessel under tow, will move end on. In glassy rocks, such as many rhyolites and andesites? the mass often shows a handed structure, marked by the presence of EFFECTS OF INCLINED PRESSURE. 55 microlites, most of which are parallel to the banding. Those microlites are no doubt of greater density than the glass, but, on account of the viscosity of the melted glass and the enormous surface per unit volume which the microscopic prisms expose, they cannot be supposed to attain their actual arrangement as a result of gravity like the mica scales in sandstone. On the other hand, if one supposes an irregular orientation of the microlites in the glass, and that tangential motion has been set up between adjacent layers of the viscous mass, every microlite standing across the direction of relative motion would be swung into the line of relative motion by the opposite traction exerted on its two ends by the moving layers. It appears to me, therefore, that " rhyolitic structure " indicates "shearing motion " or, as I have called it, scission in the direc- tion of the banding * Inclined Pressure and yielding Medium. — An inclined pressure acting on a tabular mass of rock is equivalent to a direct pressure and a tangential force. This last, with the resistance necessary to keep the center of inertia of the rock at rest, forms a couple. If the rock is surrounded by masses of comparatively feeble resistance, it will then rotate until the couple is exactly balanced 1 >y the resistance to rotation. The rock is thus subjected to the action of a simple pressure and two balanced couples, constituting a simple shear, neither of the axes of which coincides with the line of pressure. As has been shown above, the strain produced by a pressure and a shearing stress is a rotational one, the amount of rotation, however, being small as compared with that involved in some other strains. One of the directions of maximum tangential strain will therefore sweep over a greater range of material particles than the other, or will affect a given set of particles for a shorter time. That set of planes of maximum strain which shifts its position more rapidly will encounter greater resistance from viscosity and will produce the smaller effect. If the mass is strained beyond the elastic limit, but not to the point of rupture, a schistose structure will result , but one set of schistose partings will be confined to a somewhat smaller angle than the other and the more pronounced partings will be associated with the smaller angle. If the pressure is intense enough to produce rupture, fracture will take place chiefly along the partings which have the smaller range. The axes of the strain ellipsoid will bisect the angles which the last schistose partings make with one another, and the minor axis of the * The above discussion is incomplete. A full treatment would ot cour ■ i ign a definil i value to the couple which resists the tilting of a disc moving in a fluid. The reader will find the subject more fully developed in Thomson and Tail, Nat. Phil., sections 320-325, with interesting instances. That discussion is decidedly difficult, while the main points in which geologists are inl iresl ■'! seem tu be adequately demonstrated by the exceedingly elementary method here presented. IX— Bull. Gkol. Soc. A.m., Vol. 4, 1892. 56 G. F. BECKER FINITE STRAIN IN ROCKS. strain ellipsoid, or the direction of maximum compression, will lie between the line of pressure and the compressive axis of the additional shear. When the rock is ruptured without sensible deformation the strain under discussion will not be rotational and will be indistinguishable from that which would result from a simple shear; for in the xy plane one of the shears arising from direct pressure cooperates with the shear resulting from the preliminary rotation, and their combined effect will be greater than that of the second shear in the y z plane arising from the direct pressure component. The character of the finite strain is best seen by an illustration such as that in the diagram, figure 6, A. X\ Ftguee G. — Strained Cubes. The dotted squares are strained to the rhombs, drawn with full lines. A results from two shears at 45° to one another, the ratio of each shear being 5/4. B results from a shear and a scission, the ratio of each of the two shears involved being also 5/4. The central crosses mark the direction of the ellipse axes. The angle R is the material angle through which one set of planes of maximum tangential strain sweeps, and r is the other corresponding angle. In A, R — r = v — ^ = 2° 45'. In B,R — r = 15° 21'. Inclined Pressure and unyielding Resistance. — When a tabular mass of rock subjected to inclined pressure rests against a mass which does not yield considerably, the free couple which results from the tangential component of the pressure and the resistance of the supporting mass can only be equilibrated by strain in the rock itself. The strain will then- fore include as one component a shearing motion or scission. This strain is rotational, the angle of rotation being far greater in this case than in that of a yielding support. The rotation is here of the same order as the strain. Consequently one set of planes of maximum tan- gential strain Avill sweep through the mass much more rapidly than the other, and the difference in their action will be very pronounced. The nature of the distortion is seen in figure 6, B. FISSURING BY INCLINED PRESSURE. 57 Partial Theory of the Spacing of Fissures. — When a slab of rock resting broadside against an inflexible support ruptures under the influence of a pressure inclined to the supporting plane, it is easy to see that the pressure can be relieved only by several cracks, which must divide the mass into sheets bounded by planes of maximum tangential strain. Such a division is extremely common on a large scale in granite and other relatively homogeneous masses ; on a small scale it is frequent in the pebbles of conglomerates which have been subjected to pressure. It is therefore very desirable to ascertain the conditions which determine the thickness of the sheets. A slab of rock must evidently rupture in such a manner as to relieve the pressure upon it, and this relief must be accompanied by a readjust- ment of the fragments. This consideration at once assigns a superior limit to the spacing of the cracks. Suppose, for example, that in a case illustrated by the following diagram cracks were to form only at a and c5 then, since a perpendicular from the upper end of a falls between a and c, a lr c Figure 7. — Widest possible Spacing of Fissures. the fragment a a c c cannot rotate without increasing its vertical dimen- sion, and the pressure cannot be in any way relieved by the ruptures. But if a third crack, b b, is so placed that its lower end is perpendicularly below the upper end of a, the fragment a a b b can be rotated so as to decrease the vertical dimension, and thus to relieve pressure. Hence the cracks must be at least so near to one another that the terminations of adjacent cracks are in vertical lines, and the higher the angle which the cracks make with the fixed plane, the nearer must they be to one another. This, however, is an extreme case; for an infinitesimal rota- tion of the vertical line a b about any point of it would not diminish the thickness of the mass. The actual distance between fissures must there- fore be less than that assigned by this limit. When the process of straining is so slow that the mass can fully adjust itself at each instant to the external forces (an important limitation) it seems impossible to avoid the conclusion that the actual spacing will be such as to depotentialize the greatest possible amount of energy for a given length of fissure. In other words, the cracks will be so disposed as 58 G. F. BECKER — FINITE STRAIN IN ROCKS. to "do the most good." If so, the spacing can he determined if one can succeed in expressing in exact terms the depotentialization of energy per unit length of crack. The lines of maximum tangential strain make angles with o x. Let w he the thickness of one of the sheets into which rupture may divide the slab of rock, and let # he the angle which the diagonal between the obtuse angles of the sheet makes with o x, as indicated in the follow- ing diagram, figure 8. Then, if the thickness of the slab at the moment of rupture is 2 /, a little consideration shows that — iv = 21 cos (y + <**") \ 1 — tan (y -\- to) cot # j- • It is evident that the total length of the cracks is inversely propor- tional to the thickness of one sheet or to w. Figure 8.— Spacing of Fissures. To determine the relief of pressure it is convenient to begin by con- sidering a mere change of strain. Suppose a slab to he in equilibrium under the action of a simple, direct pressure. Let the mass now undergo a small change in physical properties, such that it yields by a small additional amount to the pressure. Then the potential energy of the system is diminished in proportion to the amount of this secondary yielding, measured in the direction of the force. Only one fiber passing through the center of the mass, however, will move solely in the same direction in which the pressure acts, all other particles moving on hyper- bolic bines. If the pressure were inclined to the surface at an angle cr. the depoten- tialization of energy under similar circumstances would also be measured SPACING OF FISSURES. 50 by the movement of particles in the direction of the pressure, irrespective of the movements which they execute in other directions. The rupturing of the slab into sheets may be regarded as a change in its physical properties such as is contemplated above. f\f 1 c ^^*C~' -s** ""' — - — y^' \ ^^"^ ' ^s- s s ^s s ^^ *\-d-s ^^ r^ "" " ~Z^ "'? ^^ ' ' ^^ ' i ^^ / t^* J^*^ ^ ^*^ ^s^ ' _^"^ 1 ^r s ^^r , ^ ' " — *^ i a. b Figure 9. Cut a shows'the same mass as figure 8, the sheets now being rotated through a small angle S by the pressure acting in the direction . Cut 6 represents the corner c' of one sheet on an enlarged scale, together with the original position of this corner at c. The line c' r is the distance measured in the direction of the force through which the point c has moved in passing from c to c', so that c' r is proportional to the depotentialization of energy. The angle of rotation being small and arbitrary, say, . 4 I2 8 , . f 1 tan(y + ut)} < Cc r) = — — cos 0 4- «0 i 1 — — -, — - - cot >> sin

with o x, as on those planes discussed above. When two sets of fissures form at large angles to one another they must seemingly develop simultaneously; for. if a single set of sheets were to form first, and secondary fissures were to be produced by the grinding of the sheets against one another, it is easy to see that the secondary fissures would make but a small angle with the primary divisions, and there would be more evidence of movement on the first fissures than on the subsidiary cracks. These cracks would also not in general pass from one primary sheet to the next. When the two sets of joints form simultaneously, each set must form under similar conditions, and I can think of no reason to suppose that they do not form independently. Hence the theory already developed seems to apply also to the second set of fissures, the only change needful being the substitution of to — v for m -f- '■>. The results derivable from this theory of division certainly accord with some well known facts. Thus, if a tough mass is acted upon by a shear- ing tool, it is a matter of daily experience that the mass undergoes a single cut. For this case viscosity comes into play, and by the theory only one set of fissures will he developed, cr = 0, to -{- v — 0 and w I. which means that only one fissure will intersect the mass. Again, it' one attempts to cut a brittle substance like glass with a shearing engine, the mass, according to experience, shatters instead of simply dividing. By the theory as applied to this case the elastic deformation is extremely small, neither set of planes of maximum tangential strain has a sensible range, and to -J- v = 0, while to — v = 90°, nearly. Hence only a single fissure will tend to form in the direction to -f >. but the mass will be divided into scales of almost infinitesimal thickness in the direction to — v. In other words, the theory substantially accounts for the facts. EXAMPLES OF FISSTJEING. 61 In theory as in practice, only masses capable of considerable deformation under the system of external stresses can be divided by a single clean cut. This conclusion seems to throw some light upon a general feature of geological fractures. In the laboratory rocks are very brittle substances, and every geologist has experienced a feeling of surprise that in natural rock-exposures clean cuts in a single direction are so frequent. It now appears that cuts of this description can occur only when the stresses are such as to produce a considerable elastic or plastic deformation of the mass. There is, of course, abundant other evidence that such stress systems really accompany orogenic movements. Examples of inclined Pressure. — According to a famous theory developed by Navier and Poisson the ideal isotropic solid is characterized by the property that in a simple elongation of small amount the linear lateral contraction is just one-fourth of the increment of length. Though must elasticians refuse to acknowledge the theoretical basis of this conclusion (viz, that the action between two molecules is reducible to a single force acting between the centers of mass), there is no doubt that several sub- stances, and especially glass, behave sensibly as this theory demands. As some rocks are glasses, it is certainly legitimate to assume, for the purpose of illustrating the theory of rupture developed above, that the relation 1 / 4 holds true* Let a pressure Fact upon a slab of a rock fulfilling Poisson's ideal at an angle of 30° and let the mass rest against a rigid support. Then if U and Q are the horizontal and vertical components — U= — F cos 30° = —F\(^ ; Q=—F sin 30° = — C If also n is the modulus of rigidity, it is easy to show and is well known j that — * Possible Test of Poisson's Hypothesis.— One of tin1 obstacles attending the discussion of Pois.-.>n'-. solid and the question whether or not the coefficients of rigidity and compressibility for isotropic solids are independent consists in the fact that it is difficult to determine Young's modulus and the modulus of rigidity for tin- same liody with sufficient accuracy to justify theoretical conclu- sions. There seems to be a method of direct comparison which would test the question if the experimental difficulties should not prove too great. If M is Young's modulus, /= — F sin

= l/(2— 3 ef + bl — y 25 e + 1/ . 2v/(l + e)2(l-4e) ^2y = -(i-4i)*-(it°«r-y For the present displacements the formulas give — m = 28° 43'; > = — 22° 37'. For the spacing of the two possible sets of fissures, therefore— w = I cos (w ± y) = (1 - 4 e) cos (« ± v), which for this set of displacements gives 0.765 and 0.481. Supposing that both systems of fissures form, the following diagram (figure 10) shows their disposition at the moment of rupture* * Example for = 00°.— It may be of interest to some readers to give a second example of a similar strain. In the diagram, figure 11, the force is supposed to art at t>0° to the plane of support. If. also, 6 %, the following values result: e = 0.0866 ;/= — 0.3464 ; gr = e; xo = 36°35'; w=32°4'; v = — 16° 32'; ju. = — :J2° 34'; h = 0.9172; A = 1.230; 5 = 0.575; G = 1.087 ; D = orf = 0.869 : » 0.630 or 0.432. The range for one set of planes of maximum tangential strain is o° 21', and for the other set 16° 26'. EXAMPLES OF FISSURING. 03 It is apparent from the formulas that e and b fully determine w, v and w. It is also true that if the two values of w and the angles between the Figure 10. — Results of Rupture by Pressure at 30° to fixed Plane. It is assumed that/= — 4e and that 6= — 1. Thus c = 0.0577 =g and/ = — 0.2309 ; to = 31° 20' ; (o = 28° 42'; v = — 22° 37'; /«. = — 51° 19'; ft = 0.951; .4 = 1.562; £ = 0.521; C=1058: D — 0.92G; w = 0 7U5 or 0.481. The range for one set of planes of maximum tangential strain is o° 41' and for the other 28°. cracks (or 2 w) were known by observation, the displacements and the value of

-f- v with ox, whose major axis is C'and whose minor axis is D, corresponds to a circle in the original mass. The strain involves a compression in the direction of M -f- v and an elongation in the direction o z. * La'eral Constraint.— [fa mass were no! only supported on a rigid foundation but confined by rigid walls perpendicular to th,e fixed foundation and parallel to the horizontal component of the force, the strain is also easilj calculated on Poisson's hypothesis. Evidently g = 0, and it is easj w>see that /= — 3e. Of course, 6 retains the same value as if there were no lateral constraint. 1 am no! aware that any particularly interesting results arise in this case, which differs from plain undila- tional strain only in the fact that there is cubical compression. It applies t" Mr Sharpe's theory of slaty cleavage. EFFECTS OF STRAIN DISCRIMINATED. 65 Various Results of Strain. — In the foregoing pages a theory of slow rup- ture lias been presented, which will be supplemented a little later by considering the possible effect of vibration in those cases in which the rupture is sudden. Observation seems«to indicate that many rocks have been strained to the breaking point so gradually that the theory developed is applicable.* In applying the results reached to the elucidation of geological phe- nomena the physical character of the rock must be carefully considered. Some rocks when strained with moderate rapidity approach in behavior the ideal, elastic, brittle, non-viscous solid. h\ such cases an inclined pressure will produce two systems of cracks sjich as those illustrated in figures 10 and 11. If the mass is held in the strained state, so that the fragments have no opportunity to recoil, the direction of the force may then be inferred approximately by mere inspection. The plane in which it lies will be perpendicular to th'o systems of fissures. Its direction will intersect the obtuse angle made by the fissures, arid it will make a smaller angle with the short side of the parallelogram of cracks bounding a column of the rock than with the long side. The direction of the force (•.■in be calculated exactly from the lengths of the sides of the parallelo- gram and the angle between them, if Poisson's hypothesis is assumed. If the rock is viscous but not plastic (or if it is strained under such conditions as to bring the viscosity into play, but not to keep the rock for a considerable time in a state of strain exceeding the elastic limit and falling short of the ultimate strength), the effect of the viscosity on the long sides of the parallelogram will be far greater than on the short sides, because of the difference in range of the two planes of maximum tangen- tial strain. He.nce fissures will form only in the directions of the short sides of the parallelogram and the rock will be divided into sheets. If the conditions are such as to develop both the viscosity and the plasticity of the rock-mass, flow will tend to take place parallel to the short side of the parallelogram because of the inferior viscous resistance. If the plasticity is sufficiently great, the strain will not manifest itself as rupture in this direction, but merely as plastic deformation. If the plas- ticity is not sufficient to prevent all rupture, it will at Least diminish the amount of rupture needful to relieve the strain, and there will be mingled effects of deformation and rupture. These mingled effects might consist either in a wider spacing of this set of fissures or in the distribution of short cracks through the mass. Of these the latter seems the more Drobable. The area corresponding to ♦ Striking instances of the rupture of casi iron blocks are depicted in the frontispiece of Tod- hunter's History of Elasticity. In a general way they accord with the theory developed in the text; but the blocks employed were too slender to give the full syst :m of fissures demanded by the theory for slabs of moderate thickness and greai area. GG G. F. BECKER — FINITE STRAIN IN ROCKS. one parallelogram of the figures must receive a certain amount of relief, and if this is not entirely accomplished by flow it must be completed by rupture; but a rupture at each end of the parallelogram would relieve the strain without the help of flow. Thus it appears most logical to suppose that in such cases short " close joints " will be distributed through the plastically deformed mass, excessively minute variations in the resist- ance of the material determining their precise disposition. The set of planes corresponding to the long side of the parallelogram cannot behave in the same way as those already discussed. This set sweeps through the mass so rapidly that there is no time for flow of con- siderable amount to take place. Hence, if they receive expression at all, it must be as sharply cut fissures or as u master joints." Theory of Slaty Cleavage. — In considering what properties would he ex- hibited by a plastic, viscous rock which had been rigidly supported and subjected to a pressure inclined at a moderate angle to the plane of sup- port, it is difficult to see how the mass would differ from true slate. The relative tangential motion along the set of planes which eventually makes an angle « d- ^ with the plane of support would inevitably manifest itself as a cleavage, alternating in some cases with close jointing. In the direc- tion of 02, or perpendicular to the plane of the figures 10 and 11, this cleavage would be invariable. In the direction a> -\- v the cleavage would be confined to a very small angle, less than one degree in the examples given above. Thus the mass would cleave very sharply along lines parallel to o z, less sharply along w 4- v- Expansion would take place parallel to o z, while contraction would take place in the direction w -j- v. This contraction might be accompanied by a puckering of the cleavage surfaces, because the cleavage planes formed at the inception of strain would be still further contracted as strain progressed. The amount of relative distortion in the directions o z and e reduced to the simple cleavage of slate. X In my opinion he was on the right path to a sufficient expla- nation, but he certainty did not achieve it. Professor John Tyndall's famous experiments on slaty cleavage in wax in a direction perpendicular to the pressure were published in 1856.§ He dissented from Sorby's theoiy, regarding his wax as homogeneous, and finding that the intermixture of scales rather interfered with than promoted cleavage. Dr Sorby replied to Tyndall, citing experiments of his own on clay mixed with mica scales and pointing out that wax con- tains prismatic crystals ; so that, in his opinion, the wax must be consid- ered as composed of elongated elements capable of re-arrangement by pressure, according to his theory. || Mr Daubree found that clay without mica scales when extruded through a small opening assumes a schistose structure, the lamination being close in proportion as the material is more finely divided.^] He also obtained evidence of schistose structure in flint glass, softened by heat and forced through an opening. In this case at least there could be no question that the resultant structure was independent of hetero- geneous particles. Dr Sorby made an addition to his theory of slaty cleavage in 1880. In his original theory it was assumed that the mica before compression was distributed through the mass without any order. As a matter of fact, the mica scales in shale are, for the most part, parallel to the bedding. *Ed. New Phil. Mas;., vol. 55, 185:;, p. 1::;. fSee formula (9), p. 33. tComptes Rendus, vol. 40, 1855, p. 978. gPhil. Mag., vol. 12, 1856, p. 37. || Phil. Mag., vol. 12, 185G, p. 127. |G6ol. Exp., 1879, p. 413. THEORIES OF SLATE. 79 In certain cases, however, he observed that the bedding was almost obliterated by the disturbances due to the pressure. The supplementary hypothesis is that the preliminary effect of pressure is to give the mica an irregular distribution, the final effect being to rearrange the mica scales in the planes of cleavage.* Objections to the Hypothesis of Heterogeneity — In my opinion, there are the gravest objections to the hypothesis that slaty cleavage is due to the lack of homogeneity of a rock mass which has been subjected to the action of force. Neither Tyndall nor Daubree found that the presence of scales promoted schistosity, but just the reverse. The wax employed by Tyndall may have consisted largely of prismatic bodies ; but before pressing his wax he softened it, making these bodies, as well as their groundmass, very plastic. He also kneaded the mass, so that the com- ponent particles must have welded. Even if every one of the prisms had assumed a horizontal position, there is no reason to suppose that the cohesion between them and the groundmass of the wax was feebler than that between the different portions of any one prism, or that any schis- tosity, at all approaching slaty cleavage, would have resulted. Similar remarks apply to Daubree's experiments on clay. Dr Sorby's supplementary hypothesis is suggestive in the same con- nection. All geologists will grant that disturbances are sometimes such as nearly or quite to obliterate the bedding of shales, but none will assert that this is a condition of slaty cleavage. We all know that the bedding is often most distinctly preserved in masses of roofing slate, and that the lamination is not infrequently fairly regular. In such cases it seems to me impossible to contend that the mica scales originally concordant with the bedding have been stirred up in such a manner as to be distributed at all angles through the mass. Again, there are many somewhat indu- rated shales not affected by slaty cleavage in which there are countless mica scales, nearly all of them concordant with the bedding. If the dis- tribution of mica scales constituted the fissility called slaty cleavage, such beds should split like slate in the planes of bedding. Such beds are sometimes fissile to a certain extent, but cases in which this fissility could be mistaken for slaty cleavage are very rare, if, indeed, any are known. When rocks split along their lamination at all like slate, geolo- gists expect to find, and usually do find, that the rock possesses true slaty cleavage coinciding locally in direction with the planes of bedding, but superinduced upon and independent of bedding; Similar objections apply to Mr Sharpe's theory of the flattening of the rock components. It affords no explanation of Professor Tyndall's ex- periments, and were it correct some tine-grained sandstones, at any rate, *Q. Joui-. Gcol. Soc, vol. xxxvi, 1880, p. 7;i. XII— Bull. Geol. Soc. Am., Vol. 4, 1892. 80 G. F. BECKEB — FINITE STRAIN IN HOCKS. would cleave along the bedding exactly like slate which docs not accord with observation* It appears to me, therefore, that no theory of slaty cleavage will be satisfactory which does not apply to the case of homogeneous matter. Analysis of Experiments. — Slaty cleavage has been produced artificially in several different ways. Plastic substances compressed between rigid masses exhibit such cleavage; so too do plastic masses extruded through small openings ; poor qualities of iron or brass when drawn to wire often show thin splinters, indicating the presence of cleavage; metals, pastry and clay rolled out into sheets show similar fissility, and. as Professor E. Reyer has pointed out, the bruise produced on soft rocks by a slanting blow with a pick exhibits a like structure. r These cases seem very different, but they must have common features, unless, indeed, slaty cleavage is due to essentially diverse causes. Most of the mechanical operations indicated are very complicated, hut their common features may be reduced to simple terms by considering a very small cubical portion of the mass before distortion and inquiring how it is affected by strain. Figure 18. — Origin of Cleavage in Wire. If one end of a wire is filed to a flat surface perpendicular to its axis. and the wire is then drawn through two or three successive holes of a draw-plate so that the flat end is the last to come through, it will he found that this end has become concave. If one considers a small cube in the undistorted wire, not on the axis, it is clear that this cube will be converted into an oblique parallelopiped, as is illustrated in the foregoing diagram, showing the wire in section. The concentric layers of the wire move upon one another much like the joints of a telescope. The little cube is elongated in the direction of the axis, its height is diminished, and its right angles in the plane of the axis are converted into acute or obtuse ones. It is clear that the sphere which might he inscribed in the small cube has been distorted to an ellipsoid, the major axis of winch becomes more and more nearly hori- zontal as the strain increases. The strain is thus a rotational one. and. according to the theory of strain set forth in this paper, a cleavage should be developed nearly in the direction of the axis. *See p. 74. f Theoretische Geologie, 1888, p. ."iTT. ARTIFICIAL SLATY CLEAVAGE. 81 If a bar were substituted for a wire, and slots for the circular openings of the draw-plate, the strain would be exactly equivalent to that pro- duced by an inclined pressure acting on a rigidly supported cube. It cannot be doubted that in such a case the end of the bar would also become concave, and that evidences of schistosity would appear. When a plastic mass is extruded through a small opening, whether circular or rectangular, the action is very similar to that involved in drawing wire, excepting that the external force is a pressure instead of a tension. The friction on the moulding surface delays the motion of the external layers relatively to the internal layers, and so-called "fluxion structure results. In the following diagram it is plain that a cube of the plastic mass at a would become an oblique parallelopipedon at 6* Fiouke 10. — Development of Cleavage by Extrusion. When an oblique blow is struck with a pick the bruise will manifestly show a distortion of a very small cube similar to those already considered. The case of a direct pressure, such as was employed by Professor Tyn- dall, seems at first sight very different from the foregoing. To convince myself as to the mechanics of the matter I repeated his experiments, with the following results : f A cake of wax can be compressed to less than half its thickness between glass plates well greased with a heavy oil without bulging of the edges, as shown in figure 20, a, b. If such cakes are cooled to — 15° C. they show no slaty cleavage, but exhibit a tendency to split at an angle of some 60°, more or less, to the line of pressure. If the plates are not greased, hut only wet with water, as in Tyndall's experiments, there is ;i strong tendency to bulge along the *M Daubr6e, in his Geologie Experimentale, r. mm. ids striking experiments on this mode of de- formation. f White wax is I irtter than yellow for the purpose of this experiment. To get comparable masses least cylindrical cakes at as low a temperature as practicable. These wen led off and then kept iu water at about 40° C. for an hour or more. I', -low this temperature the wax is boo hrittle to mould with ease or rapidity. The compressed cakes were cooled in ice and salt. Cakes chilled without preliminary distortion show no cl savag • under the hammer or chisel, and Crack \ ery like fine-grained basalt. 82 G. F. BECKER FINITE STRAIN IN ROCKS. edges, so that the cake assumes the form of an ordinary American cheese. Cakes compressed to one-quarter of their thickness were very greatly distorted in this sense, as shown in figure 20, c. When cooled and struck sharply on the edge with a hammer, they showed slaty cleavage. The character of the distortion of a small included cube follows from the dis- tortion of the mass, and, as appears from the following diagram, it is a distortion similar to that which takes place when a cube is subjected to inclined pressure, as illustrated in figure 6, B, page 5V). The reason for the bulging edges is at once seen to be the frictional resistance between the glass plates and the escaping wax. This resist- ance, combined with the vertical pressure, gives resultant forces, marked r r in the figure, which are not vertical but lie on conical surfaces about the central vertical axis. When this friction is obviated by the use of a lubricant, so that a nearly uniform distribution of pressure is obtained, there is no tendency to relative horizontal motion among the layers, and in a dozen or more trials with lubricators I failed to find any trace of horizontal cleavage. A tendency to cleave is sensible in these cases, but it coincides with the planes of maximum tangential strain as nearly as the imperfection of the surfaces enabled me to judge. Figure 20. — Developmt ni of Cleavage by direct Pressure. Thus it appears to me that Professor Tyndall's brilliant experiment has been misinterpreted. He produced slaty cleavage not by a pressure uniformly distributed and vertical to the cleavage planes, hut by a sys- tem of forces inclined to the cleavage planes. The effect of rolling metal, clay, or pastry is similar to that of direct pressure combined with lateral friction. A cake of plastic material is reduced to a sheet with bulging edges like figure 20, c, and an infinitesi- mal cubical portion of the mass is distorted as in the other cases. I am aware of no other ways in which slaty cleavage has been pro- duced artificially. In all of those discussed the distortion attending development of the cleavage is substantially the same. The elementary cube is deformed as it would be by a force inclined to one face of the cube when the opposite face rests upon an inflexible support. In some cases there is lateral constraint ; in others there is none. The splinters on rolled metal and pastry seem to show that the cleavage developed is not quite parallel to the surface of the mass. tyndall's experiment. S3 It might seem as if the varying directions of pressure detected in Tyn- dall's experiment were geologically unimportant. Granting that the vertical, uniform pressure at first applied to the wax is conically resolved, does it not follow that in orogenic movements also a similar resolution occurs ; so that, after all, slaty cleavage is due to a pressure originally uniformly distributed and perpendicular to the cleavage? This query must receive a negative reply. The reason why the pressure in the experiment is resolved into a conical system of forces is that the hodies between which the wax is squeezed do not themselves yield sensibly. Thus horizontal relative motion attended by friction is brought about. Were these bodies as soft as the wax, they too would extend, laterally and the pressure would remain uniformly distributed. It would also produce no slaty cleavage. In orogenic movements there is seldom any diversity between the resistance of adjoining rock masses approaching the difference between plates of glass and warm wax. Among rocks, therefore, a direct pressure will, as a rule, be distributed with an approach to uniformity, and there will be little or no relative motion between adjoining rock masses in directions perpendicular to the pressure. Hence, also, important masses of slate will not be produced in this way. Perhaps no combination is entirely wanting in mechanical geology. In artificial cuttings, clay beds underlying harder materials have been known to be squeezed out laterally, and these masses must have been affected like the wax in Tyndall's experiment ; but this case scarcely forms an important exception. In most cases of the geological occurrence of slate there is little direct evidence of the mode of formation, and it is for this reason that the ex- periments are of so much value. Sometimes, however, the method of formation of natural slate is clear. I refer especially to the slaty selvedges which are not infrequently seen bounding small faults in granite and which have been mentioned under the head of secondary action on ruptured rock. No geologist can doubt that these selvedges are produced by the inclined pressure attending faulting, and it is manifest that the distortion of an elementary cube would be exactly that which so con- stantly accompanies the artificial production of slaty cleavage. Thus, in some cases at least, natural slate is produced by the same means which are employed in producing artificial slate. Behavior of included Grit Beds and Fossils. — The theory that slate is produced by a uniformly distributed pressure perpendicular to the planes of cleavage, such as it has been usual to suppose existed in Tyndall's experiment, implies that the strain ellipsoid is an oblate figure of revolu- 84 G. F. BECKER — FINITE STRAIN IN ROCKS. tion. In such a slate a fossil which lay in the cleavage plane would simply be flattened. From the observed fact that fossils are frequently, though not always, relatively elongated to a sensible degree in one direc- tion in the cleavage plane, Mr Sharpe inferred lateral confinement as well as vertical pressure. On the theory of inclined pressure, a fossil would always be elongated in the direction of the grain of the slate and contracted across the grain in the cleavage plane, excepting when the pressure made no angle with the fixed plane. A still greater elongation, however, would take place in the direction of the major ellipsoid axis, called A in this paper, which is at right angles to the grain and makes a large angle with the cleavage plane. That such distortions do exist I have convinced myself by the examination of specimens, but I have not had an opportunity of examin- ing any large collection of fossils from slates with reference to this point. The relations of beds of hard grit occurring in slate bear a close rela- tion to those of fossils. If such a bed were bounded by surfaces parallel to the plane x y (or A B), the bed would behave either to a vertical or to an inclined pressure as an independent mass. On the currently accepted theory it would develop a horizontal cleavage. On the theory of inclined pressure it would develop a cleavage in a direction between that of the pressure and that of the fixed plane; and this would nearly coincide with the cleavage of the surrounding softer mass, because the direction of cleavage lies near that of constant direction and changes but little during strain. The smaller the angle which the force makes with the fixed support, the smaller would the divergence in the two cleavages be. " Steps " are produced when a grit bed cuts the cleavage across the grain, the plane of the cleavage in the slate and the surface of the grit bed making an acute angle. The grit is a harder material than the slate, and the cleavage developed in the grit makes a larger angle with the bedding than it does in the slate. To account for steps according to the theory of inclined pressure one may consider the elementary stresses separately. It has been shown that the shear in the plane B C does not tend to produce relative motion on the cleavages. One may therefore suppose the stress, minus this shear, to be applied to the rock first, and this shear to come into action later. Figure 22, a represents a cube in the y z plane, with a layer of harder material passing diagonally through it. If a shear and a shearing motion or scission in the x y plane are impressed upon this mass, both portions must yield simultaneously, because if the force were insufficient to strain the harder layer, this would protect the surrounding mass from the action of the force. Hence these strains would produce in both masses a cleav- age, the traces of which on the y z plane would be parallel to o z, and STEPS IN SLATE. 85 the appearance of the mass would be that shown in figure 22, b, where the fine horizontal lines represent mere cleavage, not partings. Now let the final shear at right angles to the x y plane be applied. It will elon- gate the mass in the direction o z and contract it in the direction o y. But since the more rigid layer yields to this stress less freely than that in which it is imbedded, the grit bed will rotate more nearly as if it were a- rigid mass, and will assume such a position as is shown in figure 22, c In short, the hard layer will be deflected in just the same way that an imbedded scale of mica parallel to it would be deflected. Thus the cleavage in the hard layer will not be parallel to that in the adjoining mass and will form a larger angle to the bed planes. It thus seems sufficient to suppose the grit bed to have a greater coef- ficient of rigidity to account for the phenomena of steps.* *Dr Sorby's theory of this phenomenon, as stated by Mr Harker, is as follows: "Since the grit yields less than the slate to the compressive force, the total voluminal compression is greater for the slate than for the grit. Hut near the junction of the two rocks the change of dimensions in the direction parallel to the bedding must be the same for both. Consequently, in the direction per- pendicular to the bedding, the slate undergoes a less expansion (or greater compression) than the grit; and the cleavage planes, which are in each rock perpendicular to the direction of greatest compression, will therefore be less inclined to the bedding in the slate than they are in the grit.'- This is a very ingenious explanation, but I have not been able to convince myself that it is sound. It depends primarily upon the hypothesis that a large cubical condensation is involved in the production of slate. This certainly docs not seem to be the case when slaty cleavage is produced in moist clay or wax, for such substances are probably compressible only to a very minute extent. It also implies that there is a very great difference between the cubical compressibility of the grit and the shale. I know of no good reason to suppose that such a difference exists. The difference in hardness does not imply such a relation, for cast iron, though so much harder than gold, is nearly three times as compressible ; but even if it be granted that the relations of compressibility are those demanded, it is not clear that any means is provided of changing the direction of the force in the manner required by Sorby's theory of cleavage. One may suppose a cubical portion of a rock mass to undergo the pressure needful to develop slaty cleavage without change of volume, and that cubical contraction takes place subsequently. If the mass contains a stratum of smaller compressibility than the remainder, the cleavage on the theory now under consideration would be perpendicular to the direction of the force throughout the mass before cubical contraction occurred. In this stage the mass would have the appearance of figure 22, b. The effect of the shrinkage would then be to deflect the slaty laminae close to the contact in curves with points of inflection at the contact, but to leave the direction of the cleavage at a little distance from the contact unchanged. The appearance after cubical contraction would would then resemble that illustrated in the following diagram : Figure 21. — Effects of Compressibility. But this does not represent the phenomenon to be accounted for; so thai although the hypothesis of varying cubical compression would explain a change of direction in the surfaces of cleavage al the contact with a gritty bed, it does not, so far as I can see, account for steps. 86 G. F. BECKER — FINITE STRAIN IN ROCKS. Conclusion as to Sidle. — The fact that slaty structure occurs not only in argillaceous rocks hut, though less frequently, in limestone, grit beds, granite and basic eruptives, while it has been artificially produced in wax, clay, metals, dough and glass, throws much doubt on the hypothesis that slaty cleavage is due to re-arrangement under pressure of embedded flakes and grains of matter. This doubt seems confirmed by the fact that although the component grains of many undisturbed shales and sandstones are so arranged that their largest sections lie parallel to the planes of bedding, such rocks do not show any cleavage closely resem- bling that of slate. Hence a satisfactory explanation must apply to homogeneous matter. Examination of the experimental methods of producing slaty structure shows that in all cases the distortion of a small portion of the mass is rotational, and is such as would be produced upon a cube resting on a rigid support and affected by an inclined force, with or without the co- operation of lateral forces in the plane of support. =Z=^ Figure 22. — Deflection of Cleavage by Grit. The theory of finite strain in viscous plastic masses shows that rota- tional strains of this description should be accompanied by the develop- ment of a cleavage. The grain of a mass thus distorted should have an absolutely constant direction parallel to the plane of support and per- pendicular to the line of force. Elongation should, in general, take place in the direction of the grain, and contraction at right angles to the grain on the cleavage plane. When, however, the force makes no angle with the plane of support there should be no distortion in the plane of cleav- age. There should also in all cases be a second direction of elongation perpendicular to the grain and at a considerable angle to the cleavage plane. This theory explains at least most of the characteristics of slate, in- cluding that of steps. The second elongation just mentioned certainly exists in some case-*, but I have not data enough to assert its universality. The practical difficulties of fully determining the position of the strain ellipsoid from a fossil are such that the omission of other observers to NEW THEORY OF SLATE. 87 note the existence of this elongation dors not seem to me fatal to the theory. Many observers have obtained satisfactory evidence of elonga- tion in the direction of the grain of the slate, while few, if any, of them appear to have sought for another direction of elongation not in the plane of cleavage. The theory here advanced has the advantage of being based on some of the best-established facts of natural philosophy and of connecting- cleavage in the most intimate and definite manner with schistosity, joint- ing, faulting, and systems of fissures. It also exhibits the cleavage of slate and the master joints, which usually intersect the cleavage planes at very large angles, as two features of a single strain. Neither Hooke's law nor any other exterpolated generalization has been employed in reaching conclusions as to the origin of slaty struc- ture. Poisson's hypothetical solid was assumed only in an example in order that the formulas might receive a numerical and geometrical illustration. Summary. The studies here presented are an outgrowth of field-work in the Sierra Nevada of California. That range is intersected by faults, joints, schis- tose and slaty cleavages to such an extent that, on a scale of one mile to the inch, their average separation would be for the most part micro- scopic. In many areas thes< ■ < ly i tamic manifestations are very systematic. Such of them as can be considered as concomitants of infinitesimal strain have been treated in a former paper. In a great proportion of cases, however, the strains have been finite. Only such areas are here considered as may be regarded as uniformly affected by finite strains. In the first portion of the paper finite strain is considered from a purely kinematical standpoint. The subject is treated rather fully be-* cause, for the purpose in hand, it is needful to take an extended view of the possibilities. The most important topic is that of the planes of maximum tangential strain and the manner in which they range rela- tively to the material of a solid which is undergoing strain. The relations of stress to strain are next sketched, the nature of a finite shear is elucidated, and Hooke.'s law is examined. Hooke's law is shown to differ from the statement that '-stress is proportional to strain" when the deformations are finite. Viscosity, flow, plasticity, ductility and rupture are defined, and the relation of plastic solids to fluids is explained. XIII— Bull. Gkol. Soc. Am., Vol. i, 1892. 88 G. P. BECKER — FINITE STRAIN IN HOCKS. The conclusions reached are then applied to cases such as may arise in geology. Large masses of rocks, it is assumed, may be considered as homogeneous. Were it necessary to take into consideration the minute texture of rocks, any general conclusions as to their behavior under orogenic stress would be impracticable. Simple irrotational .pressure is first taken up. It is shown that such a pressure will produce two sets of fissures crossing one another at angles approaching 90° if the rock is brittle. If it is plastic, two sets of schistose cleavages will replace the fissures. The line of force bisects the obtuse angles of the cracks or cleavages. Use is made of the theory of this case to prove in a very simple manner why mica scales and flat sand grains tend to arrange themselves parallel to the bedding of sedimentary rocks, and why flat pebbles in water-channels " shingle up stream." A mass resting on a yielding foundation and subjected to an inclined force is briefly discussed. This case closely approaches that of the simple irrotational pressure. It seems to account for unsymmetrical schistosity. The most interesting case is that of a mass resting upon a rigid founda- tion and affected by a force inclined to the foundation at any angle. It really includes the case of the simple irrotational pressure. If the mass is brittle and is strained so gradually as not to bring viscosity into play, the material will rupture in columns, the axes of which are parallel to the fixed plane of support and at right angles to the force. If the strain' is so rapidly produced as to excite viscosit}^, only one set of fissures will form, and these will be intermediate in direction between the line of force and the projection of the force on the fixed plane. If the rock is plastic (or if it is kept strained between the elastic limit and the breaking point sufficiently long to undergo considerable deformation) the fissures inter- secting the angle between the line of force and the fixed plane will be replaced to a greater or less extent by cleavage planes; and if the force • does not approach the vertical to the fixed plane, these cleavage planes will preserve a nearly constant direction and have a slaty character. In this case the second set of planes of motion, if they receive expression at all. will cut sharply across the cleavage planes as master joints. This seems to be the only way in which slate-like structure can result from the action of force on homogeneous matter. The spacing of fissures formed, by inclined pressures is discussed on the hypothesis that they are so disposed as to lead to the greatest depo- tentialization of energy. This leads to an exceedingly simple formula for the thickness of a column in a direction perpendicular to either pair of bounding planes. The formation of a single system of parallel fissures SUMMARY. 89 and the existence of undistributed faults are shown to arise in particular cases of the formula. This formula is applicable only when the rupture is not brought about by a very rapid strain. When the strain is impul- sive it is shown that the interference of vibrations attending rupture may cause further parallel ruptures. The suggestion is made that thick slates and flags may possibly be due to plastic deformation attended by vibrations. As jointing has been referred to tensile stress, rupture through tension is discussed. It is shown that curved or broken lines, and not plane partings, must result; and the columnar structure of lavas receives a seemingly sufficient explanation. The last portion of the paper is occupied by a review of the theories and observations on jointing and slaty cleavage. It is maintained that joints are always attended by macroscopic or microscopic faults, and that they are closely allied to slaty cleavage. The ascription of slaty struc- ture to the presence of deflected mica scales and flattened particles is pronounced unsatisfactory. Glass, wax and other substances in which slaty cleavage has been artificially produced can hardly owe their cleavage to such a distribution of flat particles, while sedimentary rocks in which the fiat particles are mostly parallel to the bedding do not show slaty cleavage. Analysis of certain well-known experiments and of some made for this paper shows that artificial slaty cleavage is always attended by rota- tional strains, such as those to which slaty cleavage is ascribed above. The theory of this paper (that slate is due to pressures inclined at small angles to the cleavage plane and standing at right angles to the grain of the slate) is shown to account for grain, " side " and " end," for elongation of fossils in the direction of the grain, contraction in the cleavage plane at right angles to the grain, and for master joints which intersect the cleavage plane along the grain and make a large angle with this plane. The most important result of the investigation is that jointing, schis- tosity and slaty cleavage all imply relative movement, and are thus as truly orogenic as faults of notable throw. They may all be regarded ns orogenically equivalent to distributed faults. The great number of joints and planes of slaty cleavage compensates for the minute movement on each, and the sum of their effects is probably at least as important as that of the less numerous faults of sensible throw. In the light of this conclusion it appears that if one could reproduce the orogenic history of the Sierra in a moderate interval of time on a model made to a scale of one mile to the inch, it would seem to yield 90 G. F. BECKER — FINITE STRAIN IX ROCKS. to external and bodily forces much like a mass of lard of the same dimensions* * I desire to express my thanks to Professor R. S. Woodward, of the i oast and Geodetic Survey, for his kindness in reading this paper in manuscript and for giving me the benefit of his advice. This is not. the first time I have had the advantage of Professor Woodward's profound knowledge of physics and keen scientific judgment. Washington, D. C, July 1, ISO.'. BULLETIN OF THE GEOLOGICAL SOCIETY OF AMERICA Vol. 4, pp. 91-118 February 21, 1893 THE THICKNESS OF THE DEVONIAN AND SILURIAN ROCKS OF CENTRAL NEW YORK BY CHARLES S. PROSSKR (Presented before the Society August 16, 1892) CONTENTS Page Introduction ill Records of the Wells 92 Binghamton Well and Section 92 Norwich Well and Section 94 Morrisville Well and Section 95 Chittenango Well and Sect ion 97 Utica (Globe Woolen Mills) Well and Section 100 Campbell Well and Section 101 Syracuse (State) Well and Section 101 Greenpoint (Gale) Well and Section 103 Tully Well Number 2, 1) Group and Section 104 Fulton Well and Section 105 Sandy Creek Well Number 4 and Section 100 Watertown Well and Section 107 General geologic Section of central New York 108 Composite Section 108 Review of I >ata used 108 Generalized geologic Secti< >n 110 Review of Authorities 110 Comparative Sections of eastern, central and western New York 118 Introduction. The discovery in commercial quantities of natural gas and oil in the Trenton limestones of Ohio and Indiana led to the drilling of numerous test-wells in other states that were underlain by this formation. The attention of prospectors was early directed to New York state as a promis- ing field, and in the spring of 1887 a test-well was drilled in central New XIV— Bull. Gkol. Soc. Am., Vol. 4, 1892. l'" ' 92 C. S. PROSSER DEVONIAN AND SILURIAN ROCKS. York, near Morrisville, Madison county. At that time the writer, who was an instructor in the geological department of Cornell university, recognized the value of the data that might be obtained from these well records in giving the thickness and dip of the various terranes composing the series of New York rocks. During the remainder of 1887 and the years of 1888-'89, when test-wells were being drilled at numerous localities in New York, various wells were visited personally and arrangements made with the owners and drillers for securing reliable and complete sets of samples. As a result of these efforts, a large amount of data con- cerning the thickness of the New York geologic formations has been obtained, and two papers describing the sections along the meridians of Cayuga lake and the Genesee river have been published* In the present paper it is intended to describe another of these general sections crossing the state in a north-and-south line. The section selected is the one containing the record of wells drilled at Binghamton, Nor- wich, Morrisville, Utica, Chittenango, Tully, Syracuse, Fulton, Sandy Creek and Watertown, and as it is approximately along a line somewhat east of the 76th meridian, with one-half of its length following the Che- nango river valley, it may very appropriately be' designated the section of Central New York. Records of the Wells. Binghamton Well and Section. — The southernmost well of this series, which is first to be considered, is one drilled at Binghamton, Broome county, New York. This well is located on the farm of ex-Sheriff Brown, one-half mile south of the Susquehanna river and about ten rods from the southeastern corner of the city limits. It was reported by Mr G. M. Kepler as on the hillside about 70 feet above the city proper, which would make its elevation about 940 feet above tide.f The oeolooic horizon of the mouth of the well is in the Chemung sta^e, but not at its summit, which is considerably higher. Vanuxem stated that " the Catskill group covers the highest grounds on the south side of the Susquehanna [river]. "J Personal examination in this region shows that Vanuxem was inclined to make the base of the Catskill too low, and that Chemung fossils occur in what he called Lower Catskill. The general order of the faunas and formations of the Chenango valley *The Thickness of the Devonian anil Silurian Rocks of Western Central New York. Am. Geol., vo'. vi, October, 1890, pp. 199-2] 1 . The Thickness of the Devonian and Silurian Kocks of Western New York, approximately along the line of the Genesee river. Proc. Rochester Acad. Science, vol ii, May, 1892, pp. 49-104. tThe altitude of the X. Y., L. E. and W. R. II. station at Binghamton i- state, I by Gannett to be 80S feet (Bull. U. S. Geol. Surv., no. 76, p. 52). IGeol. New York, part iii, 1S4:>, p. 29G. BINGHAMTON WELL AND SECTION. 93 section from the Hamilton stage up into the Upper Catskill has been well described by Professor H. S. Williams* The Binghamton well was drilled during the fall of 1887 and the winter of 1888 by Mr G. M. Kepler, superintendent of the East Pennsylvania Oil and Gas company, to whom the writer is indebted for a series of specimens illustrating its geologic section, as well as to the driller. Mr C. W. Henderson, for valuable information in reference to this well. SECTION OF WELL AT BINGHAMTON, NEW YORK. Approximate altitude, OJfi feet. Depth. Thickness.^ Kind of rock. Formation. Feet. Feet. 5d 100 Bluish gray argillaceous shale Chemung and Portage.; 150 100 < Srayer and more arenaceous 250 100 Bluish argillaceous shale " 35 it >< 50 200 Bluish finely arenaceous shale 550 150 < rrayish and blue arenaceous and argilla- ceous shales 700 50 Grayish finely arenaceous chips, with fragments of f< >ssils and calcite crystals . " 750 50 i trayish arenaceous shale " " 800 50 Arenaceous and somewhat calcareous; some of the chips have a brownish-red tint *Proc. Am. Assoc. Adv. Sci., vol. xxxiv, 1886, Chart of "Meridional Sections of the Upper De- vonian Deposits of New York, Pennsylvania and Ohio,': section no. ix. fFrom this well samples of the drillings were saved from each additional fifty feet of depth ; consequently it does not follow that each lithologic zone has the exact thickness assigned to it in this column. Jin this well-record it is impossible to draw a dividing line between the Chemung and Portage stages; therefore the rocks composing them are classed together under the heading of Chemung and Portage. The Portage stage might be divided into Upper Portage, Oneonta sandstone and Lower Portage. The above division of the Portage would agree in a general way with that of Dr H. S. Williams as shown on section ix (Chenango) of Ids " Meridional sections of the Upper Devon- ian of New York, Pennsylvania and Ohio" (Proe. Am. Assoc Adv. Sci , vol xxxiv). In discussing the " classification of the geologic deposits " the Professor wrote : " The Catskill deposits [Oneonta sandstone] of Chenango and Otsego counties are intrinsically not distinguishable from the upper stage of the Catskill, but appear at a lower position stratigraphieally in the interval occupied by the ' Ithaca group ' of the Cayuga section and by the middle part of the Portage group of the Ge„esee section" (ibid., p. 234). Also, "the interval occupied in the Genesee section by the typical Portage fauna is . . . in the Chenango and Unadilla section . . . filled by a preliminary: stage of the Catskill [Oneonta sandstone]" (ibid , p. 233). Professor Hall in 1885 said : -The Oneonta sandstone in Otsego and Chenango counties is suc- ceeded directly by strata bearing fossils of Chemung age," arid his correlation of the Upper De- vonian was as follow s : ■■ Catskill group. Chemung group. ^ _x„ ( Portage croup. Oneonta i Hamilton (upper). Hamilton group " (Geol. Surv. N. Y., Palaeontology, vol. v, pt. i, Lamellibranchiata, ii, p. 518). u u 04 C. S. PROSSER — DEVONIAN AND SILURIAN ROCKS. Depth. Thickness. Kind of rock. Formation. Feet. Fed. 850 50 Blue arenaceous shale Chemung and Portage. 900 LOO Arenaceous chips, which arc mainly of a brownish-red color, a few gray ones. . . 1,000 200 Dark gray arenaceous shale. (Thesample from 1,150 feet is similar to the upper part of the Norwich well) " 1,200 :;•">(> Bluish argillaceous shale " " 1,550 400 Mainly gray to bluish arenaceous shale; si mie dark gray argillaceous shale 1,950 50 Fine chips of brownish-gray finely arena- ceous material ; slight effervescence . . . 2,000 50 Light gray finely arenaceous sandstone (?) 2,050 200 Bluish argillaceous shale with some arena- ceous chips ; streak white, non-calcare- ous Place of Genesee ? 2,250 50 Very fine dark blue chips, which imme- diately effervesce strongly in cold HC1 and are evidently from a strongly cal- careous stratum ; possibly the Tully limestone Tully ? 2,300 50 Blackish argillaceous shale, somewhat calcareous; streak brown, like Hamil- ton Hamilton ? 2,350 50 Gray argillaceous shale; streak white, strongly calcareous Hamilton. 2,4:00 150 Gray argillaceous slightly arenaceous shale ; streak white 2.550 50 (.ravish arenaceous sandstone and blue argillaceous shale, strongly calcareous; fragments of fossils, one Spirift ra f " 2,600 4DO Grayish and bluish argillaceous and arenaceous shales and sandstone (?). . . " 3,000 117 Gray arenaceous chips with fragments of fossils and calcite crystals 3,117 Dark gray arenaceous chips which are strongly calcareous. Bottom of well . . " Norwich Well and Section— The next well-record to be considered is that of one drilled near Norwich, Chenango county, about thirty-five miles northnortheast of Binghamton. The well was drilled by Mr A. W. McQueen in 1887-'88, who kindly favored me with its record and a set of samples. Natural gas was found at various horizons down to 1,200 feet, but in such small quantities that it would burn but a few hours before being exhausted. NORWICH WELL AND SECTION. 95 SECTION OF THE NORWICH WELL. Approximate altitude, 1,000 feet. Depth. Thickness. Kind of rock. Formation. Feet. Feet. • 50 25 Dark gray or bluish-gray arenaceous shale; non-calcareous < >neonta of Conrad. 75 50 Mostly argillaceous shale, but part of the chips are from a fossiliferous layer which contains Spirifera mesacostaMs, Hall (?) .... Portage. 125 50 Bluish gray arenaceous chips " 175 75 Chips, very fine, and of a dull gray color, non-calcareous ; " Sherburne sandstone ". " 250 200 Dark gray and greenish gray argillaceous and arenaceous shales ; " fresh water and gas at 384 feet " 450 170 Bluish argillaceous shale, non-calcareous; probably Hamilton Hamilton (?). 020 65 Gray shale, quite calcareous and rather arena- ceous, with mica ; must be Hamilton .... Hamilton. 685 190 Lithology same as above, slightly calcareous, " gas pocket " of driller " 875 585 Dark gray arenaceous shale, slightly calcare- ous ; fossils at 1,020 feet ': 1,460 190 Bluish argillaceous shale, quite calcareous, fossils ; Clionetes scitula, Hall (?) ■ " 1,650 400 Dark gray argillaceous and arenaceous shales " 2,050 185 Very dark blue to blackish shale ; streak- white, non-calcareous " 2,235 99 Very dark almost black argillaceous shale with brownish white streak, non-calcare- ous ; Marcellus shale or black band in the Hamilton Marcellus (?). 2.:;:!4 Black argillaceous shale, non-calcareous, brown streak ; true Marcellus. Bottom of well Marcellus. This well begins in the Lower Portage, Oneonta group of Conrad or the Paracyclas Virata stage of the Hamilton fauna, as named by Dr H. S. Williams,* and terminates in the Marcellus. The Hamilton is shown to have a probable thickness of from 1.615 to 1,785 feet, which is the most important fact furnished by the record of this well. Morrisville Well and Section. — In- the spring and summer of 1887 the first test-well was drilled in central Xew York at Eagle ville, about- one mile south of Morrisville, Madison county, and twenty-live miles slightly *See Prosser in Proc. Am. Assoc. Adv. Sci., vol. xxxvi, 1887, p. 210. 9G <'. S. PROSSER — DEVONIAN AND SILURIAN ROCKS. west of north of Norwich. This well begins in the lower half of the Hamilton stage at an altitude of probably more than 1,200 feet, and was drilled to a depth of 1,889 feet, terminating near the bottom of the Onondaga Salt group. SECTION OF THE MORRIS VILLE WELL.* Approximate altitude, 1,200 (?) feet. Depth. Thickness. Kind of rock. Formation. Feet. Feet. 340 31+ Pure argillaceous black shale with brownish-black streak Marcellus shale. 371 93 Dark and light gray limestone, which effervesces very strongly in cold II CI. Upper Helderherg (Cor- niferous) limestones. Place of Oriskany (?). 404 180 Dark gray limestone, mixed with some quartz grains, which are prob- ably from the Oriskany sandstone above. The dark gray strongly calca- reous limestone continues clown to 028 feet, where a very light gray calca- reous sample was obtained. At 578 feet a pocket of gas was struck which burned for a short time Lower Helderberg. 050 125 fA dark gray limestone, which effer- vesces more slowly in cold IIC1 than the samples above, and leaves a large residue of argillaceous material ; gas in small amount at 755 feet Onondaga Salt group {'!). 775 185 Mainly dark gray limestone, but alter- nating with light gray to drab lime- stone ; effervescence usually moder- ately strong in cold HC1, leaving large residue; frequently grains of selenite . Onondaga Salt Group. 900 58 Greenish-gray shale, which has a slight effervescence in cold HO " 1,018 5 Chocolate-colored shale; slight efferves- cence in warm HC1 1,023 87 Greenish shale; slight effervescence in warm HO 1,110 09 Dark gray to blackish marlite, which effervesces quite readily in cold li( '1 . " *Thiswell was described l>y Prosser in Proc. Am. Assoc. Adv. Sci.,vol. xxxvi. 1887, pp. 208, 200. ■f-The sample from 619 feet is a dark limestone, [earing a considerable argillaceous residue, with some grains of selenite (?), and hears a strong resemblance i" the upper part of the ' >nondaga Sail group. However, the light colored, strongly calcareous sample from 628 feet makes it appear probable that it is better to consider the Onondaga Salt group as beginning at about C50 feet. 1,300 100 1,400 60 1,460 105 1,565 225 1,790 25 (1 « MOKRISVILLE WELL AND SECTION. 97 Depth. Thickness. Kind of rock. Formation. Feet. Feet. 1,179 36 Bluish-gray marlite, which is quite cal- careous Onondaga Salt group. 1,215 -44 Dark gray to drab impure limestone or marlite ; effervesces strongly in cold HC1 1,259 41 Dark gray to drab marlites mixed with crystals of salt. The driller reported 10 to 12 feet of rock-salt at 1,259 feet ; also chocolate and green shales Chocolate' and green variegated marls, with a little bluish shale . . . " Mostly chocolate shale, with an occa- sional green and blue chip " Mostly green and bluish marls, with an occasional red chip Clear red shale, with an occasional green chip Blue argillaceous shale, slightly calcare- ous ; small amount of salt from evap- oration about the cork of the vial. " " 1,815 5 Drab gray limestone or marlite ; effer- % vesces readily in cold 1IC1, but leaves a large residue ; salt as in sample above Dark blue argillaceous shale and mar- lite Dark blue limestone, which has a strong effervescence in cold HC1 " " The last sample, from 1,889 feet, is partly limestone, but contains more blue argillaceous shale. Bottom of the well in the Onondaga Salt group*. . . " " Chittenango Well and Section. — A well which has furnished an important section for the purposes of this paper was drilled during' the first half of 1890, at Chittenango, Madison county. Mr F. W. Lamphere, of that vil- lage, carefully preserved a complete set of samples from this well, with an accurate record of their depths, which eventually reached me for ex- amination. Chittenango is seventeen miles northwest of Morris ville, *In the preliminary record of this well it was reported that possibly the Niagara was reached at 1,805 feet and the Clinton at 1,87-1 feet (Prof. Am. Assoc. Adv. Sci , vol. xxxvi, pp. 20S-209). A com- parison of the samples from this well with those of the Chittenango and other wells convinces me that the Morrisville well did not reach the Clinton stage, but probably ceased near tin" bottom of the Onondaga Salt group. The driller at l.sso feet reported the Clinton iron ore ami stated that "slight impressions of lenticular grains, about the size of a pin-head, oval and apparently of a con- cretionary nature, were seen." It is probable that some, other substance must have been considered iron ore, as the samples from 1,879 feet and 1,884 feet do not indicate its presence. 1,820 54 1,874 15 1,889 98 C. S. PROSSER DEVONIAN AND SILURIAN ROCKS. and the well is located in the western part of the village, on the bank of the Chittenango creek. The Chittenango station of the New York Central and Hudson River railroad is 417 feet ahove tide, and, baro- metrically, the mouth of the well is about 27 feet higher, making the altitude approximately 444 feet above tide. Natural gas in small quan- tities was obtained at several horizons. A little gas was struck at a depth of 950 feet in the Medina. The largest amount occurred in the Trenton limestone at a depth of 2,651 feet, hut gas was reached at 2,690, 2,875, 2,884 and 2,904 feet. At fi rs1 , aft< r 1 >ei ng closed for thirty minutes, there was a sufficient volume of gas to produce a pressure of 25 pounds to the square inch, hut by the middle of August, 1890, it had decreased to 12 pounds. SECTION OF THE OHITTENANGO WELL* Approximate altitude, IfJ^jeel above tide. Depth. Thickness. Kind of rock. Formation. Feet. Feet. 182 24 Bluish and grayish chips mixed with reddish dirt Drift (?). 20G 179 Bluish marlite, which effervesces quite strongly in cold HC1 " 385 5 Mostly chocolate-red marlite with some greenish and a few gypsum chips. . . . Onondaga Salt group. .'590 10 Bluish marlite with some red and green shale " " 400 34 Clear reddish-chocolate shale with just a few green chips " " 434 11 Mottled chocolate and green shales. .. . 445 16 Green shale with a few reddish chips. . " " 461 54 Dark gray and bluish-gray limestone, which effervesces rather slowly at first in cold HC1, hut hecomes strong on standing. The samples leave a considerable residue. Occasionally some red and green chips ; at 500 feet grains of salt 515 52 Bluish-gray and bluish-black limestone with some pinkish chips ; strong effer- vescence in cold HC1 Niagara (?). 567 •"-'! Green argillaceous shale, generally non- calcareous ( Jlinton. 600 44 Bluish-gray shale, which is slightly cal- careous and arenaceous " *The record of this well is based upon a set of specimens purchased by the United States Geo- logical Survey and now deposited in the United States National Museum. f'HITTENANGO WELL AND SECTION. 99 Depth. Thickness. Kind of rock. Formation. Feet. Feet. 644 11 Dark gray and rather pinkish chips, which effervesce strongly in cold HC1 and contain hematite ii-on ore ; some greenish, argillaceous, non-calcareous shale Clinton " iron-ore bed." 655 225 Green argillaceous shale, non-calcare- ous ; brachiopod shells at 800 feet. . . Clinton. 880 10 Greenish to greenish-gray chips, not so argillaceous and scarcely calcareous ; a few reddish chips like iron ore .... " 890 12 Greenish quartzitic chips mixed with green argillaceous shale ; a good many white, vitreous, angular chips that are apparently quartz grains Medina. 902 4 Mainly chocolate-red chips of sand- stone (?) mixed with white quartz grains " Gray band " (?) of Me- dina. 906 48 Greenish argillaceous shale and sand- stone mixed with white vitreous grains of quartz Medina. 954 456 Mainly brownish-red quartzose sand- stone, with some greenish-gray sand- stone and argillaceous green shale ... " 1,410 107 Greenish-gray quartzose sandstone,with some bluish shale Oswego sandstone. 1,517 640 Mainly blue argillaceous shale, with some bluish-gray arenaceous shale or sandstone Lorraine or II u <1 s o n shale. 2,157 233 Blackish argillaceous shale ; streak slightly brownish Utica shale. 2,390 60 Blackish argillaceous shale, with brown streak, but mainly gray calcareous chips ; at about the top of the Trenton limestone " " 2,450 50 Clear sample of dark blue limestone ; strong effervescence in cold HC1 ; undoubted Trenton Trenton limestone. 2,500 390 Dark gray and light gray limestone, with some dark blue limestone, steongly calcareous ; fossils, brachio- pods (Orthis ?), at 2,600 feet ; brachio- pods at 2,710 feet Trenton. 2,890 88 Moderately dark gray limestone ; fair effervescence in cold HC1, but con- taining a large amount of non-calcare- ous material (argillaceous?) " XV— Rurx. Geoi,. Soc. Am., Vol. 4 1892. 100 C. S. PEOSSER DEVONIAN AND SILURIAN ROCKS. Depth. Thickness. Kind of rock. Formation. Feet, Feet. 2,978 4s._l Lightish gray, with some dark gray magnesian limestone; effervescence very slight in cold HC1, hut becomes strong on heating Trenton. 3,0262 Bottom of well. The well begins in the colored marls of the Onondaga Salt group, and reaches the Clinton at a depth of 567 feet. The thickness of the dif- ferent stages in this well is as follows: Clinton, 323 feet; Oneida con- glomerate, 12 feet; Medina sandstone, 508 feet; Oswego sandstone, 107 feet ; Lorraine shales and sandstones of the Hudson series, 640 feet ; Utica shale, 233 feet, and penetrates the Trenton limestone to a depth of 636* feet. Utica {Globe Woolen Mills) Well and Section. — A well was drilled by the Globe woolen mills to the depth of 1,720 feet in the city of Utica, near the level of the Erie canal, and the samples were kindly placed at my disposal for study by Mr Charles D. Walcott, of the United States Geo- logical Survey. This well is about thirty-one miles east of Chittenango and twenty-five northeast of Morrisville. SECTION OF THE GLOBE WOOLEN MILLS WELL AT UTICA, NEW YORK. Approximate altitude, J+28 feet. Depth. Thickness. Kind of rock. Formation. Feet. Feet, 370 200 Clear, black argillaceous shale with brownish streak, slightly calcareous Utica shale. 570 330 Dark blue limestone ; strong effervescence in cold HC1 ; fragments of fossils at 650, 810 and 850 feet ; fragments of brachiopods at 730, 750, 790 and 830 feet Trenton limestone. 900 180 Drab to bluish-gray massive limestone, which effervesces strongly in cold HC1, and light gray, glistening limestone, which does not effervesce strongly in cold HC1 " " 1 ,080 180 Light gray powder, which is strongly calcare- ous ; very marked effervescence in cold IIC1 Calciferous (?). 1,260 140 Slightly brownish-gray sample, composed largely of white vitreous quartz grains with some mica grains ; non-calcareous Calciferous. 1,40!) 320 Mainly light gray samples, composed chiefly of white or vitreous quartz grains; some are of slightly brownish color, and part of the samples are quite badly iron-stained. . Potsdam (?). 1,720 Bottom of well. CAMPBELL AND SYRACUSE WELLS AND SECTIONS. 101 Campbell Well and Section. — Very interesting for comparison with this well is the record of the Campbell well, three miles west of Utica, which was drilled to a depth of 2,250 feet. This well was described by Mr Charles D. Walcott in August, 1887,* and through his courtesy the writer has had the pleasure of studying the set of samples saved from it. The record of this well as reported by Mr Walcott may be briefly summarized as follows : SECTION OF THE CAMPBELL WELL NEAR UTICA, NEW YORK. Formation. Lorraine shale of the Hudson group.. Utica shale. Trenton limestone. ( rap of 180 feet between the Trenton and Calciferous, 100 feet of which probably belongs»to the Calciferous, which would make the top of the Calciferous at about 1,230 feet. Calciferous and arenaceous strata, 260 feet ; Calciferous in all about 360 feet in thickness. Potsdam. 100 -f- Pre-Cambrian and Archean. The careful study of the Campbell well record and specimens has fur- nished much assistance in interpreting the record of the Utica well. The top of the Trenton limestone is reached at a depth of 570 feet in the Utica well and at 800 feet in the Campbell well, a difference of 230 feet. Supposing the formations to have about the same thickness, then the top of the Calciferous might be expected at a depth of about 1,000 feet, and the light gray, strongly calcareous rock, which is considered as rep- resenting the Calciferous, occurred at 1,080 feet. In the same manner the top of the. Potsdam would be reached at about 1,360 feet, while the sample which is regarded as probably coming from near the top of the Potsdam was reached at a depth of 1,400 feet, and the bottom of the well, at a depth of 1,720 feet, is still in this formation, the Archean not having been reached. The line of separation between the Trenton limestone and the Cal- ciferous is somewhat difficult to determine, and it is especially so between the Calciferous and Potsdam. The point at 1,400 feet, indicated as the beginning of the Potsdam, can only be taken as probably near the line of separation between these two formations. Syracuse (State) Well and Section. — In 1884 the "state well" was drilled at the southern end of Onondaga lake, near Syracuse, about fifteen miles *Proe. Am. Assoc. Adv. Sci., vol. xxxvi, pp. 211, 212. I>swego sandstone. 58o 695 Mainly blue argillaceous shale, with some arenaceous shale and a little quartzose sandstone; arenaceous chips containing fragments of fossils at 875 feet Lorraine shale of the Hudson group. 1,280 120 Black shale with brownish streak Utica shale. 1,400 335 Mainly bluish-gray limestone, which effer- vesces strongly in cold HC1 ; some dark blue and light gray limestone ; fragments of fossils at 1,638, 1,665 and 1,735 feet. . . Trenton limestone. 1.735 * Last sample " This well was first described by Mr Charles A. Ashburner in 1888, who reported that the well had been drilled to the depth of 1,727 feet, and gave the following section : " Medina sandstone 400 feet, Hudson River shale 880 " Utica shale and slate 120 " Trenton limestone 327 " Total 1,727 " "At 1,727 feet, 327 below the top of the Trenton limestone, gas was struck in such force as to throw sand from the well to the top of the derrick, a height of 74 feel 10 inches. The gas caught on tire and the derrick was burned down." f In April, 1890, Mr ( 'hades D. Walcott published the same record, with the additional 323 feet to which the well had been drilled, making its total depth 2,050 feet, X Sandy Creek Well Number 4 and Section. — Several wells have been drilled near Sandy Creek and Lacuna, Oswego county. New York, for natural gas, which was obtained in moderate quantities. Mr Gilbert X. Hard- ing, of Lacona, saved and forwarded to me a set of samples from well No. 4 of the Sandy Creek Oil and Gas Company, limited. Lacona is * This is the depth from which the hist sample came in the set furnished me for study. Mr Walcott reported that the well was drilled :;i."> feet deeper, reaching a depth of 2,050 feet, and that it passed through 650 feel of Trenton limestone (Bull. Geol. Soc. Am., vol. i. p. 349). fTrans. Am. I n-t. Min. Eng., vol. xvi. p. 958. | Bull. Geol. Soc. Am., vol. i, p. 349. SANDY CREEK; WELL AND SECTION. 107 forty miles north-northwest of Chittenango or twenty-eight miles north- east of Fulton. SECTION OF WELL NUMBER 4, AT SANDY CREEK, NEW YORK. Depth. Thickness. Kind of rod:. Formation. Feet. Feet. 50 350 Mainly blue argillaceous shale, but with some bluish to dark gray, fine-grained sandstone, which contains fine grains of mica; segments of crinoid stems at 200 feet Lorraine shale of tbe Hudson group. 400 145 Blackish argillaceous shale with moder- ately brownish streak Utica shale. 545 600 Dark blue, dark and light gray limestone chips, most of which effervesce very strongly in cold HC1 ; fragments of fos- sils at 600 and 700 feet; fragments of brachiopods at 675, 750, 880, 900, 950 and 1,050 feet, and numerous fragments of well preserved brachiopods at 765, 800, 830 and 850 feet ; gas at 675, 765 and 790 feet. Samples from 545, 830, 880 and 1,030 feet were blown out by gas Trenton limestone. 1,145 Bottom of well in the Trenton limestone. Walertoton Well and Section. — At Watertown, Jefferson county, 24 miles north-northeast of Lacona, a well was drilled to the depth of 530 feet by the Black River Gas and Fuel Company. A little gas was found at the depth of 253 feet, according to the driller. Mr Albrant, to whom the writer is indebted for the samples from this well. SECTION OF WELL AT WATERTOWN. NEW YORK. Depth. Thickness. Kind of rock. Formation. Feet. Feet. 92 8 Light greenish, very compact, fine-grained lime- stone, which effervesces strongly in cold IIC1... Trenton. 100 26 Light gray limestone, strongly calcareous 126 135 Mainly light green limestone, which does not effer- vesce strongly in cold HC1 at first, but increases on standing 261 14 Very light gray fine-grained limestone ; effervesces strongly in cold HC1 275 255 Many pinkish white chips, which are usually non- calcareous; also dark green and dark gray, the gray being somewhat calcareous; near the bot- tom are some vitreous white quartz grains ( lalciferous ? 530 Bottom of well KVI-Buli-. Geoi,. Soc. Am., Vor.. I, 1892. 108 C. S. PEOSSER — DEVONIAN AND SILl'JUAN ROCKS. General geologic Section of central New York. Well. Depth. Thirl: in SS Feet. Feet. inghamton. 0 2,250 CD I _- iz Composite Section. — From the preceding well-sections a general section has been compiled, giving the approximate thickness of the different formations, together with the total thickness from the Chemung, as ex- posed at Binghamton, New York, down to the Archean. Formation. Mouth of the Binghamton well in the Chemung. From 900 to 1,000 feet brownish-red arenaceous chips, prob- ably the horizon of the "Oneonta sandstone." At 1,850 feet, about the mouth of the Norwich well and lower, the " Sherburne sandstone." Place of the Genesee shale and the Tully lime- stone. Hamilton. Marcellus shale. Upper Helderberg (Corniferous .limestone). Place of Oriskany sandstone. Lower Helderberg. Onondaga Salt group. Niagara. Clinton. Medina. Oswego sandstone.- Lorraine shale of the Hudson group. Utica shale. Trenton. Calciferous. Potsdam. Pre-Cambrian and Archean. 2,250 1,785 4,035 100 (?) Morrisville . . 4,135 93 4,228 -.-.(?) 1S6 (?) 4,414 1,239 -f 5,653 + 52 (?) Chittenango. 5,705 323 6,028 520 6,548 107 6,655 640 7,295 233 7.528 637 + Utica 8,165 4- 320 (?) 8,485 410 (?) 81,895 .... Review of Data used. — It will he interesting to compare the thickness of these formations with that obtained for them in wells more remote from the meridian of this section. The combined thickness of the Chemung and Portage groups was shown by the Bird Creek well, eight miles southwest of Elmira, to be con- siderably more than 2,700 feet for that region,* while in the Ithaca well the Hamilton is 1,142 feet thick : the Marcellus shale, 82 feet; the Upper Helderberg (Corniferous limestone). 78 feet: Oriskany sandstone, 13 feet; Lower Helderberg. approximately llo feet, and the bottom of the well is in the Onondaga Salt group after passing through 1,285 feet of limestone, shale and salt belonging in that group. The Seneca Falls * Prosser : Am. I teol., vol. \ i. p. '-!"i REVIEW OF DATA USED. 100 well began in the upper part of this formation and passed through 950 feet before reaching the Niagara limestone* As near as can be determined, the Niagara limestone has a thickness of 52 feet in the Chittenango well, while in the State well near Syracuse it is 332 feet thick ; in the Gale well, 320 feet, and in the Clyde well, 335 feet.f However, it is often very difficult to decide on the dividing line between the lower gray marls aim limestones of the Onondaga Salt group and the beginning of the Niagara limestone; hence there is some doubt as to the accuracy of the thickness of this formation. The Clinton group has a thickness of 323 feet in the Chittenango well ; in the State well 98 feet, and the Gale well of 149 feet. There is appar- ently too. great a difference in the thickness of this formation as given in the State and Gale wells when their proximity is considered, but the samples as labeled seem to furnish the above result. The Clinton is approximately 83 feet in thickness in the Clyde well, and in the Seneca Falls well the Niagara and Clinton groups have a thickness of 400 feet.'! The Medina is 508 feet thick in the Chittenango well and 807 feet in the State well. The Gale well penetrated the Medina 583 feet ; in the Clyde well it is 942 feet thick, and in the Wolcott well 690 feet. 1 1 The Oswego sandstone is 107 feet thick in the Chittenango well ; 185 feet in the Fulton, and in the Wolcott 210 feet. The Clyde well stopped after passing through 92 feet § of it and the State well penetrated it to a depth of 150 feet. The Lorraine shale of the Hudson group isG40 feet in thickness in the ( '1 littenango well and 695 feet in the Fulton well. The Sandy Creek well began in the Lorraine, passing through 400 feet before reaching the Utica shale. In the Wolcott well there is 820 feet of shales and sandstone which may be referred to the Lorraine and the Utica shale.^[ The Utica shale which forms the surface rock at Utica was shown by the Globe Woolen Mills well to have a thickness of at least 570 feet in that city. Mr Walcott reported its total thickness to be 710 feet in the Campbell well, three miles west of Utica.** This shale is 233 feet thick in the Chittenango well ; 120 feet in the Fulton, and 145 feet at Sandy creek. The Trenton limestone in the Utica well has apparently a thick- ness of 510 feet, but on account of the great difficulty in deciding upon what shall be considered the top of the Calciferous this statement must be accepted as partly an estimate. Mr Walcott in a similar manner con- cluded that the Trenton had a thickness of about 430 feet in the Camp- bell well.ff The Chittenango well penetrated this formation to a depth of 637 feet, and in the same way the Sandy Creek well passed through * II. id., pp. 202-203. r [bid., p. 204. t Ibid-, l'l>- 203, 204. || Ibid.', p. 204. g Ibid., p. 204. fl Ibid., p. 204, **Proc. Am. Assoc. Adv. Soi., vol. xxxvi, p. 212, tt Ibid., p. 212. 110 C. S. PltOSSER — DEVONIAN AX!) SILURIAN ROCKS. 690 feet of Trenton; the Fulton well, 650 feet, and the Wolcott well, 750 feet* A Generalized geologic Section along the Meridian of the Chenango river from the Top of the Chemung down to the Archean. In order to show the variations in the ahove section as compared with our previous knowledge of the thickness of these terranes, a general geologic section ranging through the same series of formations has been compiled from books and geological articles. In this compilation the maximum thickness of the terranes, as near the line of section as possi- ble, has been taken. The notes following the section give the authorities and references. Depth. Thickness. Authority. Formation. Feet. Feet. 0 2,000 A Chemung and Portage. 2,000 20 B Genesee. 2,020 25 C Tully. 2,045 1,100 D Hamilton. 3,145 100 E Marcellus. 3,245 70 F Upper Helderberg (Corniferous). 3,315 20 G Oriskany. 3,335 120 H Lower Helderberg. 3,455 700 I Onondaga Salt group. 4,155 50 (?) J Niagara. 4,205 200 K Clinton. 4,405 400 L Medina. 4,805 100 M Oswego sandstone or Oneida conglomerate 4,905 600 N Lorraine shale of the Hudson. 5,505 180 O Utica. 5,685 330 P Trenton. 6,015 350 Q Caleiferous. 6,365 410 (?) II Potsdam. 6,775 Archean. Review of Authorities. Authority and reference for the thickness of the terranes, as given in the preceding section. A. — Dr H. S. Williams estimated the thickness of the rocks from the base of the true Catskill down to the horizon of the Genesee shale or the top of the Hamilton, for the Chenango valley, as approximately '2.000 feet (Proc. Am. Assoc. Adv. Sci., vol, xxxiv, 1886, Chart on the " Merid- ional Sections of the Upper Devonian Deposits of New York, Pennsyl- ' Am. Geo)., vol. vi, p. 204. REVIEW OP AUTHORITIES. Ill vania and Ohio," section no. ix). On a section crossing the Catskill range from Schenevus to Glasco, prepared by Professor James Hall, it was shown that the " Portage and Chemung have a thickness of more than 2,000 feet" for that region (ibid., vol. xxiv, B, 1876, p. 82). B. — Prosser noted: "Black argillaceous shales 20 feet in thickness near Smyrna [in the Chenango valley, in the northern part of Chenango county "] (ibid., vol. xxxvi, 1887, p. 210). C. — Prosser reported : " Limestone layers, separated by calcareous shales, with a total thickness of 25 feet . . . near Upperville, in Smyrna township." At least part of this series belongs to the Tully limestone (ibid., p. 210;. Emmons said: "In Albany and Schoharie counties it [Tully limestone] is unknown. . . . The thickness . . . is from 12 to 15 feet " (Agriculture of N. Y., vol. i, 1846, p. 186). D. — Professor Hall wrote : " The thickness of this group [Hamilton] on the eastern limit of the district [fourth geological district, Cayuga lake region] cannot be less than 1,000 feet" (Geol. N. Y., pt. iv, 1843, p. 194). Vanuxem said: "The group is of great thickness; in no part probably less than 300, and swelling to 700 feet" (Geol. N. Y., pt. iii, 1842, p. 151). Professor Dana stated that " the greatest thickness — about 1,200 feet — is found east of the center of the state" (Manual Geology, 3d ed., p. 266) ; but it is also stated that " the Hamilton strata are 1,000 feet thick in central New York" (ibid., p. 267). While Professor Hall said, " The thickness of this group [Hamilton] along the Schoharie creek is much greater than has been supposed, amounting probably to 3,500 feet " (Proc. Albany Institute, vol. 1, 1871, p. 133). 1,100 feet seems to be a fair average for this section, based upon Hall's estimate for Cayuga lake and Dana's for eastern central New York. Emmons stated: "By estimating the fossiliferous and non-fossiliferous parts by themselves and summing up the result, we obtain from 1,000 to 1,200 feet thickness. In Albany and Schoharie counties the thickness appears to be much greater than in the western counties " (Agri. of N. Y., p. 185). E. — Vanuxem wrote : " Near Marcellus and in other parts of Onondaga where best observed they show no fossils for one or two hundred or more feet where thickest" (Geol. N. Y., pt. iii, p. 147); also, "A boring of 100 feet for coal was made in the Marcellus shales by Mr Sage near the road from Chittenango to Cazenovia" [Madison county] (ibid., p. 149); and Dana states that " The Marcellus shale rarely exceeds in thickness 50 feet" (Manual Geol., 3d. ed., p. 267). Emmons stated: " It is probably less than 100 feet at Schoharie and Manlius " (Agri. of N. Y., p. 183). F. — Vanuxem said: "The Corniferous limestone is at its maximum thickness in the village of Cherry Valley [Otsego county], where it is probably from 60 to 80 feet thick" (Geol. N. Y., pt. iii, p. 141) ; while 112 C. S. PROSSER — DEVONIAN AND SILURIAN ROCKS. he stated that the thickness of the Onondaga limestone " rarely exceeds 10 or 14 feet " (ibid., p. 132), and at Vannep's, near Perryville, Madison county, ho gave the thickness as " about 10 feet" (ibid.., p. 135). Dana wrote : " In New York the thickness of the limestone seldom exceeds 20 feet for the Onondaga and 50 feet for the Corniferous " (Manual Geol., p. 250'. Emmons reported 100 feet of Onondaga and Corniferous lime- stone at Cherry Valley, in Otsego county (Agri. X. Y., table on p. 178; also see statement on p. 175). From the above statements it appears to be a fair estimate to call the ( !orniferous limestone of our section 60 feet thick and the Onondaga limestone 10 feet. G. — Yanuxem said : "'At Oriskany Falls [southwestern corner of Oneida county], to the north of the village the sandstone is exposed for some distance, forming a ledge or mass about 20 feet thick " (Geol. X. Y.. pt. iii. p. 125) ; while " the greatest thickness in the district is on the old Seneca road between Elbridge and Skaneateles [in the western part of Onondaga county], appearing to be about 30 feet thick" (ibid., p. 283, and see p. 126). Emmons reported: "At Oriskany Falls, 20 feet; at Perryville and below Cazenovia, only a few inches " (Agri. X. Y., p. 170). H. — Professor S. G. Williams stated: " The exposure of lower Helder- herg rocks at Oriskany Falls, 18 miles south of Utica, is interesting, partly because it is so laid open by deep and extensive quarries as to give nearly a complete section of about 120 feet of rocks, 115 feet of which can be definitely measured from the Oriskany sandstone, here 10 feet thick, down to the bank of the abandoned Chenango canal " (Am. Jour. Sci., 3d ser., vol. xxxi, p. 142). Emmons reported 121 2 feet at Cherry Valley, Otsego county (Agri. X. Y., table on p. 178). I. — Yanuxem. in 1840, reported " a thickness in Onondaga county of about 7reat thickness in Onondaga county, " being more than 500 feet thick at Salina, which the deep boring of 1839 made known" (Yanuxem. 5th Ann. Pep. Third Geol. Dist. X. Y.. 1841. p. 147). This was also re- stated in the final report (see Geol. X. Y.. pt. iii. pp. 278, 279). Professor Hall reported that on a line from Seneca or Ontario to Oswego county it is "more than 1,000 feet in thickness" (27th Ann. Rep. X. Y. Stale Mus. Nat. Hist,. 1875, p. 128, and Proc. Am. Assoc. Adv. Sci.. vol. xxii, 1874, B, p. 332); while Dana says: "They [the Onondaga Salt group beds] are 700 to 1,000 feet thick in Onondaga and Cayuga counties and only a few feet on the Hudson " (Manual Geol., p. 233). Emmons re- REVIEW OF AUTHORITIES. 113 ported 700 feet of red shale in Madison county and 100 feet of green shale at Cherry Valley (A-gri. N. Y., table on p. 178). J. — Vanuxem stated : " It [the Niagara] thins out to the east, leaving not a trace to be seen east of a line passing south through the village of Mohawk, in Herkimer county" (Geol. X. Y.. pt. hi, p. 90); while Pro- fessor Hall wrote : " Starting from the typical localit}^ of the Niagara group, where, of the shale and limestone, we have a thickness of some- thing more than 200 feet, and tracing the outcrop in an easterly direc- tion, we find a very gradual but pretty constant thinning ofthebeds of the formation, so that at a point 100 miles east of the Niagara river it has a thickness of scarcely 100 feet. Farther eastward, in Oneida county, the formation is still thinner " (27th Ann. Rep. N. Y. State Mus. Nat. Hist., 187"). p. 123 ; also Proe. Am. Assoc. Adv. Sci., 1874, vol. xxii, B, p. 327). Vanux- em, in 1840, stated that " the greatest thickness of this group [the Protean, divided later into Niagara and Clinton] must be over 200 feet" (4th Ann. Rep. Third Geol. Dist. N. Y., p. 375). Emmons stated : " On Swift creek, in Oneida county, it is a dark concretionary mass, about four or five feet thick, accompanied with a dark-colored slate" (Agri. N. Y., p. 151"). K. — Vanuxem was able to measure part of this group on Swift creek, a tributary of Sauquoit creek, in the southwestern part of Oneida county, where beds to the thickness of 94 feet are exp< >sed, but he states distinctly that this is not the entire thickness of the group (Geol. N. Y., pt. iii. pp. 84, 85) ; while Dana states : " In Oneida. Herkimer and Montgomery counties the rock is 100 to 200 feet thick. . . . Near Canajoharie, which is not far from its eastern limit, the formation has a thickness of 50 feet " (Manual Geol., p. 220). Emmons stated : " It is 1 »etween 5t > and 60 feet in Warren, in Herkimer county " (Agri. N. Y., p. 150). L.— The Medina in the State well, near Syracuse, has a thickness of about 807 feet (see Englehardt, Ann. Rept. Supt. Onondaga Salt Springs for 1884, pp. 1(3, 17) ; Avhile Professor Hall wrote : u This rock [Medina] thins out entirely in an easterly direction in Oneida county, showing from that point westerly as far as Lake Ontario a gradual increase in thickness " (Geol. N. Y., pt, iv, 1843, p. 43). Since the line of the present section is about half way between Syracuse and the eastern side of Oneida county, it would seem from the above statements that 400 feet would be about the thickness of the Medina for this section. M. — On the northern branch of Salmon river, which is very nearly in line with the present section, Vanuxem stated : " Not less than about 100 feet of the rock [Oswego sandstone] is there exhibited" (Geol. N. Y.. pt. iii, p. 70). Emmons stated: " The whole thickness of the sandstone and limestone is not over 100 feet " (Geol. N. Y., pt. ii, p. 126). Professor Emmons also reported the Oneida conglomerate at Utica as "a mass 20 or 30 feet thick overlying and resting immediately upon the thin-bedded 114 C. S. PROSSER — DEVONIAN AND SILURIAN ROCKS. Lorraine shales " (Agri. N. Y., pp. 125, 120). Vanuxem reported the Oneida conglomerate in Herkimer to he "from 15 to 25 feet thick ; " while in a gulley southeast of Utica "it appears to present its maximum thickness of ahout 35 feet" (Geol. N. Y., pt. iii, p. 76). Dana stated the thickness of the Oneida conglomerate to be " 100 to 120 feet in Oneida county, New York " (Manual Geol., p. 218), and, further, "the Oneida conglomerate is the surface rock in Oneida and Oswego counties, New- York. It is here 20 to 120 feet thick, but thins out to the eastward in Herkimer county " (ibid., p. 220). He evidently used the terms Oneida conglomerate and Oswego sandstone as synonymous, and gave the thick- ness of the Oswego sandstone for that of the Oneida conglomerate. N. — Above the Utica shale, on the south branch of Sandy creek, Jef- ferson county, New York, a locality not far west of the line of this section, Mr YValcott measured 600 feet of shales and sandstones belonging to the Lorraine stage iBull. Geol. Soc. Am., vol. 1, April, 1890, pp. 348, 349). On the " diagram " for the Lorraine section Mr Walcott gave 180 feet as Utica, then 100 feet of shale and calcareous sandstone, with 720 feet of the Lorraine above (ibid., p. 350). Furthermore, Mr Walcott has stated : "The data obtained in the study of the strata of the Hudson terrane enables me to state that that terrane has a thickness of over 6,000 feet in the valley of the Hudson" (Ninth Ann. Rep. U. S. Geol. Surv., pp. 116, 117). Vanuxem wrote: "In Schoharie county the Hudson group is undisturbed and unaltered, and its maximum thickness is not less than 700 feet" (Geol. N. Y., pt. iii, p. 61). Mather concluded: " In the val- leys of Norman's kill, the Mohawk river and the Schoharie kill, they [Hudson] are beautifully exposed to view. . . . No actual meas- urements of these strata have been made, but it is estimated that they have a thickness of from 500 to 800 feet " (Geol. N. Y., pt. i, 1843, p. 369). Ashburner described the Knowersville well, in Guilderland township, Albany county, seventeen miles from Albany, which began 595 feet below the top of the Hudson and reached the Trenton at a depth of 2,880 feet. Consequently the Hudson group and Utica shale, if the latter be repre- sented in this well, have a combined thickness of 3,475 feet (Trans. Am. Inst. Min. Eng., vol. xvi, pp. 951, 952). Professor Hall gave it as from 800 to 1,000 feet thick in central and northwestern New York (Gd >1 . Surv. N. Y., Paleontology, vol. iii, pt. i, text, p. 20, foot note). Professor Em- mons reported the entire thickness of the Lorraine shales at the northern termination of the Helderberg range as "not less than 700 feet" (Agri. N. Y., p. 125). O. — Mr Walcott measured ISO feet of "dark bituminous shale in bands, alternating with a smoother lead-colored shale," along the south branch of Sandy creek, Jefferson county, New York, which was "characterized by the fauna of the Utica shale*' (Bull. Geol. Soc. Am., vol. i. p. 318). REVIEW OF AUTHORITIES. 115 Emmons stated : " The Utica slate, in the gorges of Lorraine and Rod- man [in the southern part of Jefferson county], is about 75 feet thick; it is, at least, less than 100 feet" (Geol. N. Y., pt. ii, p. 118) ; and also he said : " I am satisfied that its thickness never exceeds 75 feet " (ibid., p. 400). Vanuxem considered its thickness and reported it as " often show- ing a thickness whose maximum is about 250 feet" (Geol. N. Y., pt. iii, p. ^>G). Dana said : " The Utica shale is 15 to 35 feet thick at Glenn's Falls, in New York, 250 feet in Montgomery county, 300 feet in Lewis county " (Manual Geol., p. 196). Finally, Mr Walcott stated : "At the typical locality in the vicinity of Utica the formation has a thickness of over 600 feet" (Trans. Albany Inst., vol. x. 187'.), p. 1). This statement was repeated in 1888 when the Campbell well was described, in the record of which 710 feet was referred to the Utica shale (Proc. Am. Assoc. Adv. Sci., vol. xxxvi, p. 212). Walcott stated in 1890 that " at Utica the Utica shale is 710 feet in thickness " (Bull. Geol. Soc. Am., vol. i, p. 347). P. — Mr Walcott reported that in the Campbell well, west of Utica, there was probably 330 feet of Trenton limestone, and in the vicinity surface outcrops 290 feet in thickness (Proc. Am. Assoc. Adv. Sci., vol. xxxvi. p. 212). Vanuxem stated that the Trenton limestone at Copenhagen, Lewis county, "must be 300 feet thick, showing a great increase in its progress from the Mohawk river, where in no place is it 30 feet in thick- ness " (Fourth Ann. Rept. Third Geol. List. N. Y., pp. 364, 365); also, '• on the Mohawk its thickness rarely exceeds 30 feet, but it increases through Oneida and Lewis, being 300 feet in the north part of the latter county" (ibid., p. 371). In his final report this statement is repeated as follows : " The greatest thickness of the Trenton limestone is in Lewis county, toward the northern end, where it cannot be less than 300 feet. It diminishes in thickness going east and south, rarely exceed- ing 30 feet in any part of the Mohawk valley. It is not so thick at the east as at the west end " (Geol. N. Y., pt. iii, p. 49 ; also, see similar statement on p. 268). Emmons said : " The greatest thickness which I have been able to give to the Trenton limestone is 400 feet. At Chazy, where it is made up of alternating beds of limestone and shale, this, according to the best estimate I can make, is the thickness of this rock. The gray variety is, however, wholly wanting at this locality ; if that is to be considered as a distinct mass, the whole thickness may be greater than I have given it ; but at Watertown, where both varieties exist, the thickness cannot much exceed the above estimate. At Glen's Falls it is much less "(Geol. N. Y., pt. ii, p. 116); also, "the thickness of the Trenton limestone at Watertown, including the whole mass, which extends south, and which is embraced in the section, is about 300 feet" (ibid., p. 388). The Black River limestone " is about 10 feet thick XVII— Bull. Gkol. Soc. Am., Vol 4, WX2. 116 C. S. PROSSER DEVONIAN AND SILURIAN ROCKS. ! & i a oj 02 c g S.2 £5 .JO o o o o O 1C CO r-l i— CO 03 o m a © CD S - o s o "S CO «, 00 -C-; Q 05 O o CD o 02 , — i 72 03 1) <"5 CD 02 cc -^ ■43 .S 02 r* + O d C-f iO o CO o l^ T— I CO o o o cf o CI a. o o o o 1^ o CI s £ o ^ ,9 12 O o g i^ o 02 cd 02 i— i 02 s3 cd > a CD O 7. g i— ^ CHART OF GEOLOGIC SECTION. 117 51) 8 .3 o 55 -a 'o G c3 O H5 O r3 O o HO co~ o o CO © CM CO © CO CO iC CM CM ^h CM CO lO o o 3 co r^ © © CO CO CM >— I CM O CC ■* o o o CM O lO 2 ° o o CM rr o © © o © © 00 CO i— i co i—i oo © © lO i— I co ■* »o CO \ G *o o Tc o o 03 G o 3 03 03 o cc 03 to © CO © © © -H o CO w <— ■ o 03 la 03 ." CO p .03 ISi (3 — 03 O ^5 O P EH co - < o c= a) c .2 CD — 39 >> < ■= © O -^ — % '- a ~ o e co p cc - > CD CO 5 o a) >> CD 3 & a IE CD co 00 ~ 4J OS o /- = -3 3 -~ J5 = o U3 41 co — s g « M .8 — 03 CO (D 13 08 — Q ° CD CD - — OS P. -— — § 2 a ■•5 = -2 o 3 * •S > = CO CD — H CS 1% 2 Jd- S<2 118 C. S. PROSSER DEVONIAN AND SILURIAN ROCKS. at Fort Plain " (Vanuxem : Geol. N. Y., pt. iii, p. 40). The Birdseye limestone " is about 30 feet [thick], but, like other limestones in this group, it thins out remarkably toward the south " (Emmons : Geol. N. Y., pt. ii. p. 110; also, see p. 385). Q. — Mr Walcott reported surface outcrops of Calciferous 350 feet in thickness for comparison with the Campbell well west of Utica, in which it possibly lias a thickness of 360 feet (Proc. Am. Assoc. Adv. Sci., vol. xxxvi, p. 212). Emmons wrote : " The entire thickness of the Calciferous sandrock is between 250 and 300 feet " (Geol. N. Y., pt. ii, p. 106). R. — Mr Walcott reported Potsdam (?) sandstone 410 feet in thickness in the Campbell well west of Utica (Proc. Am. Assoc. Adv. Sci., vol. xxxvi, p. 212). Emmons stated that on the northern or Canadian slope it " is about 300 feet thick " (Geol. N. Y., pt. ii, p. 103). Mr T. B. Brooks reported in St. Lawrence county Potsdam and pre-Potsdam at the maxi- mum 700 feet thick, part of which must be before the typical Potsdam (Am. Jour. Sci., 3d ser., vol. iv, p. 22). Vanuxem in 1839 stated that the thickness of the whole series, from the gneiss at Little Falls to the top of the Corniferous, " taking the measure of each rock and group where its thickness is greatest, exceeds 2,000 feet" (Third Ann. Rept. Third Geol. Dist, N. Y., pp. 276). The estimated thickness of this same series as compiled from various author- ities is 3,530 feet, while the actual- thickness as obtained from the well sections is 4.760 feet. In addition, Vanuxem stated : " There [then] re- mains from 12 to 1,500 feet before completing the whole of the series of the third district; all which are anterior in origin to the coal " (ibid., p. 276). This would make a total thickness of only 3,500 feet for the entire series, while our compiled section gives 6,775 feet from the top of the Chemung to the Archean, and the actual thickness of the rocks from the Chemung, at Binghamton, which is something like 1,500 feet below the top of Vanuxem's series* to the Archean is approximately 8,895 feet. Comparative Sections of eastern, central and western New York. For the purpose of comparison it has been thought advisable to prepare a chart (page 116) giving the thickness of the different geological for- mations for four sections, crossing New York in a line from north to south. The author is responsible for the sections denominated *' western," "western-central" and "central New York," but the section for "eastern New York " was measured and prepared by Charles A. Ashburner. *Compare the Chenango section (ix) in Professor Williams' "Meridional Sections of the Upper Devonian Deposits of New York, Pennsylvania and Ohio" (Proc. Am. Assoc. Adv. Sci., vol. xxxiv). Topeka, Kansas, December, 1892. BULL. GEOL SOC. AM ; ..' . ,: • ■■•■■■ /HIIHIIWII |l|l lll||'«.lll|IM'»-llir»»|F»..- I ^g^'H' '.'■ ii" »>mi - , '."f* >"j*"p ;i' r-r ■'"•' '■■'■"'iH.Uul'.,-:"'.:-:. "ii'SitZlil'-ti'M 1 NEW T/E <^J -.-,- VOL. 4, 1602 PL. 1. rr"~" 4 4 C ";. :. "T*"" J :ro'd fern BULLETIN OF THE GEOLOGICAL SOCIETY OF AMERICA Vol. 4, pp. 119-132, pl. 1 February 23, 1893 A NEW TSENIOPTEROID FERN AND ITS ALLIES BY DAVID WHITE (Read before the Society August 16, 1892) ( !ONTENTS Paste Introduction 119 Diagnosis 119 Locality 120 Specific Resemblances. 120 Generic Reference 121 Suggested genetic Relations 123 Systematic Position and Relation of the megalopterid Group 125 Graphic Presentation of Relations 129 Conclusions 129 Introduction. — Among several collections of fossil plants from the Lower ( !oal Measures of the Carboniferous of Henry county, Missouri, have been found a number of specimens representing a remarkable and apparently new species which presents a striking combination of tseniopteroid and alethopteroid characters. Tins species is of peculiar interest from the fact that it exhibits divisions of a type well known in certain Paleozoic and Mesozoic tseniopteroid forms arranged and developed in the manner familiar in the genus Alethopteris, as will be seen in the accompanying figures and following description : Tseniopteris missouriensis, n. sp. Pl. I, figures 1-7. Diagnosis. — Fronds bipinnate(tripinnate?),the larger divisions linear- lanceolate, acute, composed of pinnatifid pinnules near the base, above which are simple pinnules; primary rachis broad, shining, marked by somewhat irregular lines, and consisting of a thickened central portion, broadly but shallowly canaliculate above, half-round below, and of thinner marginal laminae ; pinnules opposite, sub-opposite or alternate, XVIII— Buo,. Gkol. Soc. Am., Vol. 1, 1892. (U") 120 D. WHITE — A NEW T.ENTOPTEKOID FERN AND ITS ALLIES. slightly distant, at right angles or reflexed below, becoming more oblique above, ribbon-like, gradually tapering from the lower part, with borders straight or slightly undulate and nearly parallel, to a rather acute ti]>, long, sometimes reaching a length of 8 cm or more, and measuring 6 to 13 mm in width, the lower ones slightly narrowed toward the cordate, nearly symmetrical base with its narrowed attachment which overlaps the marginal lamina of the rachis, the higher ones becoming attached by the whole base, those near the top of the pinnae becoming shorter, more distinctly decurrent and confluent, the margins more rapidly converging ; limb of the pinnules rather thick, dull, broadly canaliculate along the midrib, somewhat convex near the borders, overlapping the marginal lamina? of the rachis. constricted to a rather narrow attachment in the lower and middle pinnules, spreading and uniting those near the apex of the pinna? where it forms a wing incised by acute and decurring angles at the confluence of the pinnules ; nervation tamiopteroicl, midrib strong, depressed, broad and striate beneath, broadly canaliculate above, origi- nating from the central portion of the rachis, passing along the middle of the lamina and tapering to the apex of the pinnule ; lateral nerves rather fine salient above, distinct beneath, originating at an oblique or some- times nearly a right angle from a slender cord-like bundle often distinctly in relief traversing the center of the canal, usually forking at or near the midrib, rarely simple, curving quickly if oblique, and passing fairly straight and generally parallel perpendicularly to the border, usually forking again at a varying distance in the lamina, and counting 24 to 28 per cm at the margin ; basal nervils of the upper decurrent pinnules springing from the rachis ; those of the uppermost alethopteroid pin- nules becoming rather more oblique in passing to the margin. Locality. — Represented by ten specimens from Hobbs1 bank, nine miles south of Clinton, Missouri, and one specimen from Deepwater, about eight miles southeast of Clinton. Specific Resemblances. — Among the known Paleozoic plants are several species described as Damseites, Alethopteris, Taeniopteris and Desmopteris which have many characters in common with Tivnioptcris misxoiiricnsis. Of the American forms, Danssites {Alethopteris) macrophylla, Newb. sp., Alethopteris maxima, Andr., the types ranged under Orthogoniopteris and Protoblechnum, and an unpublished species of Callipteridium described by Lesquereux deserve comparison. Newberry's Alethopteris macrophylla,1 the fully developed pinnules of which are somewhat similar to tbose of our specimens, is alethopteroid in arrangement, only the lowest, so far as I have observed, becoming contracted to the obliquely cordate base. Besides its more delicate habit, it further differs by the obliquity of the 1. Geol. suvv. Ohio, Pal. I. i>. 383, pi. xlviii, figs. ::, :■„,. SPECIFIC RESEMBLANCES. 121 narrowed bases of the distinct pinnules, the more slender upper, con- fluent pinnules and the closer nervation. There is perhaps no generic difference between the two plants. Alethopteris maxima, Andr.,1 as seen in a specimen from Rushville, Ohio, determined by Professor Lesquereux, is an alethopterid, though the difference between it and Protoblechninu may not be of generic rank. Still earlier in the geologic series a form perhaps somewhat similar existed in the Alethopteris ingens, Daws.,2 the pinnules of which, more than one inch in width and three inches or more in length, have the Bauxites nervation, or the J. discrepans, Daws.,3 both from the middle Devonian of St. Johns, New Brunswick, the long, ribbon- like, open pinnules of which are united, however, by a narrow decurrent wing. So far as the form and development of the pinnules, and to some extent the nervation, is concerned, a closer resemblance obtains in the cases o£ Pseudodanxupxix reticulata, Font.,4 from the Upper Trias at Clover Hill, Virginia, or the forms of Tseniopteris munsteri, Goepp. (Angiopteris, fide Schenk), from the Lias of Bornholm.5 Tin; upper pinnules of the Virginia species are united, as figured by Fontaine, while the lower ones are long, ribbon-like, and distinctly and nearly equally rounded at the base, as in our plant from Missouri. Perhaps its nearest affinity is, how- ever, with the Tie nioptcr is jejunata of Grand Fury,''' from the Upper Car- boniferous and Permian of France. In this species, of which the upper parts of the pinnae are, I believe, unknown, the pinnules are sometimes short-pedicelled, the lamina thin, and the nerves generally more oblique near the midrib and more regular, as figured, in passing to the margin than in our species.7 Inform the Missouri species is also close to certain species referred by Stur8 and Zeiller9 to Desmopteris, Stur, which has a somewhat different nervation, though it appears to be allied to the alethopteroid gr< >up. Generic Reference. — In the characters of the rachis with its thickened, sulcate, center and marginal laminae, in the origin of the nervils in the median canal of the pinnule, the ribbon-like lamina of which is rounded at the base where it overlaps the rachis, and, to a less extent, in the character of the nervation, the middle pinnules (figure 5) of our species are referable to Tseniopteris or to Danseites, according to one's interpreta- 1. Geol. Surv. Ohio, Pal. II, p. 421, pi. I, figs. ::, Za-b. 2. Foss. PL, Dev. Sil. Form., Can., pi. xviii, tig. 206, i>. 54. 3. Op. cit., p. 54, figs. 203-205. 4. Older Mcs. Fl., U. S. Geol. Surv. Monogr., vi, p. 59, pi. xxx, figs. 1-4. 5. Bartholin: Botanisk Tidsskr., vol. xviii, lift, i, Kjobenhavn, L892, p. ■£',, pi. ix, fig. 9. 0. Fl. Carb. Loire, p. 121 ; Zeiller, Fl. 1'oss. Commentry, pt. 1, p. 280; All., pi. xxii. figs. 7-!); Zeiller, Fl. foss. Autun, Epinac, p. 102, pi. xii, fig. 6. 7. The nervation seen in the figures of T. missouriemis is drawn with fidelity in detail from the originals. 8. Carbon. -Fl. Schatzlarer Sch., i. See D. belgiea, Stur. p, isi, pi. Hi, rigs. 7-9. 9. Fl. foss. Valenciennes, p. 21G, pi. xxxviii, figs. 3-5. See Ettingshausen: fl. Radnitz, p. 1", pi xvi, figs. 2-4. 122 D. WHITE — A NEW TTENIOPTEROID PEEN A.ND ITS ALLIES. tion or restriction of those genera, while it has much also in common with certain Triassic and Jurassic forms referred by various authors to Angiopteridium, Angiopter'is, Marattia and Danseopsis. One or two of the lowest pinnules found arc sublobate or crenulate on the lower side, as though in the procsss of subdivision, such as I take to be the case in the Danseites (Alethopteris") macrophylla figured by Newberry.1 On the other hand, the upper, sessile, confluent or decurrent pinnules (figure 2), though springing from the central portion of the rachis (a condition indi- cated in some species of Alethopteris), are equally distinctly alethopteroid, being comparable to those pinnules seen in the upper part of primary pinna; of various Alethopteridese, such as Alethopteris valida, Boul.,2 or in the A. gigantea and A. longifolia of Achepohl,3 both of which may be allied with the group of long-pinnuled Paleozoic Danseites. It is prob- ably generically inseparable from the Danseites (Alethopteris) macrophylla, Newb. sp. But under the name Danseites we have two quite different groups of plants. The genus Danmtes, as construed by Ettingshausen, Heer and Schimper,4 embracing those forms in which the pinnules, having the characters of Tssniopteris, are rounded at the base and attached by the midrib only, differs widely from the interpretation put upon Goeppert's ambiguous genus by Stur5 and Zeiller,6 who, on account of the obscure fruiting figured by Goeppert,7 have denned it to contain a number of pecopteroid forms with small pinnules and sori which, though not under- stood in certain respects, are strongly analogous to those of the living Dansea. The Dunn ilex ernersoni of Lesquereux,8 referred to Goeppert's genus by reason of the appearance of its obscure fruiting,9 represents, according to the figures, an alethopterid form related by habit and venation to Gallipteridium, while the D. macrophylla, Newb*. sp., was not placed by Lesquereux in Ta niopteris, to which it was considered referable in size and nervation, because it was pinnate, the unequally cordate base excluding it at the same time from Alethopteris. However, cordate or 1. Oeol. Surv. Ohio, Pal. I, p. 383, pi. xlviii, tigs. :i, 3a. 2. See Zeiller, Fl. foss. Valenciennes, p. 231, pi. xxxii, xxxiii, tig. l. 3. Niederrh.-Westphal. St. 'ink., p. 78, pi. xxiv, tig. 12 3 p. 134, pi. xli, figs. 1, 1'. I. [n Zittel, Traite, iiyp. 85: "Feuille simple (ou double?), pen nee. Folioles inserees seulemeul par la. nervure mediane, arroDdies :i la base, lineaires, devenant insensiblement pointues, poss6- ilant les caraeteres des 'J'" niopteris, ;i bord entier : nervure moyenne ;is»7, forte, nervures lateral.es se detaehant de alles-ci a angle droit, nombreuses, les unes simples, les autres bifurquees. Fructi- fications disposers en deux series le long de la nervure m6diane." 5. Carbon.-Fl. Schatzlarer Sch., p. 221, figs. -Y\a-c. 0. Fl. foss. Valenciennes, p. 41. 7. Systema, p. 380; Danceites asplenioides, p. 380, pi. xix, figs. -1, •">. 8. Coal Flora, p. L57, pi. xxviii, tigs. l-:s. 9. The Pecopteris asplenioides described by Fontaine anil 1. C. While (Permian Flora, p. 72, pi. xxv, fig. I), from the Permo-Carboniferous, is perhaps closely related generieally, by its fruiting, to D. ernersoni, Lesq. GENERIC REFERENCE. 123 neuropteroid bases are not very rare in-the lowest pinnules of Alethopteris and Callipteridium. In recent works interpreting the fossil according to the habit of recent ferns, a simple frond is not generally made an essen- tial character of the genus Tmniopteris. So far, I believe, no one has de- scribed the upper portion of the pinna of any of the pinnately divided speeies now retained in the latter genus, the remains consisting generally < f detached pinnules and fragments separated by reason of their decidu- ous tendency. My reference of the Missouri species to Ta niopteris is provisional. The fern is in its habit, and to some extent its nervation, evidently closely related to Alethopteris. As remarked above, it should perhaps be in- cluded in the same genus with Danasites (Aleth.) macrophylla (Newb.) Lesq. ; but from the character of the rachis, midrib, form of pinnules and the nervation, and from the observed development of the upper part of some of the tseniopteroid forms in the older Mesozoic and Carbonif- erous, I have been led to place it among the Taeniopterideae, and notwith- standing the high degree of its superficial identity with them arattiaceous forms comparable in their fructification to Danasa or Angiopteris, it seems better, in default of all knowledge of the fruiting of our species, to refer it to the genus Tmniopteris, the former resting-place of many of the Meso- zoic species, rather than to the equivocal genus Dana ilex. It is certainly ineligible to admission in the Dana ites of Goeppert and Stur. The name Danasites, in the sense in which it is employed by Heer and Schimper, should, if used at all, perhaps be applied to those species only of which either the fruiting is known or the generic identity with other contem- poraneous fruiting species is by other evidence satisfactorily proven, leaving their apparent representatives from the Paleozoic, the fruiting of which is not known, in the convenient and non-committal genus Taeniop- teris, without presupposing any direct genetic relation to any particular fruiting genus. Suggested genetic Relations. — The combination of alethopteroid and tseniopteroid characters in the plant from the Lower Coal Measures of Missouri more than strongly suggests a genetic relationship between the pinnate tseniopterids (including the Paleozoic Danseites of the type A macrophylla), and in probable sequence the Mesozoic tseniopteroid marat- tiaceas, on the one hand, and the Lower Carboniferous alethopteroid genera on the other; or, considering together with the alethopterids their close natural allies, the neuropterids, we may suppose the relationship to extend, as I shall try briefly to indicate, back to the megalopterid stock, in which they may have had their origin. The genus Megalopteris, described from the Middle Devonian of Saint Johns, New Brunswick, by Sir William Dawson as a subgenus of 124 I). WHITE — A NEW TjENIOPTEROID FERN AND ITS ALLIES. Neuropteris,1 becomes, in the Lower Carboniferous, alethopterokl in its mode of development and configuration, while its nervation is that of Alethopteris or Odontopteris. The pinnules are further distinguished by their thick midrib, which is canaliculate above, semi-cylindrical beneath, nan-owing in passing up, but distinct to the apex of the lamina. Les- quereux, who frequently pointed out its ancestry to, or at least its com- mon descent with, the neuropterids, adds2 that " except for the characters of the nervation [open, curving, close, dichotomous] this genus is not separable from Danseopsis, I leer. Saporta and Marion :i include the genus Megalopteris with Cannophyllites, Brgt., in the Cannophyllitess, which they regard as being near the Dolerophylhas among their " Progymnosperms," a- view in which Count Solms-Laubach and Schenk do not concur. Between the more alethopteroid forms of Megalopteris, such as M. hartii* M. ovata,5 M. minima,6 M. abbreviata1 and the alethopteroid genera found in the Lower Carboniferous of Ohio and West Virginia, the resemblance is so close as at once to force a comparison. Among the forms from below the Maxville limestone in Ohio, the generic delimitations of which are perhaps more artificial than is com- mon even among Paleozoic ferns, the Alethopteris maxima, And.,8 is found to have a close tamiopteroid nervation in pinnules which are decurrent and confluent in the upper part of the pinna, but scarcely confluent in the lower part, where their mode of clecurrence, in a semi-auricle, is nearly that given as a chief characteristic of Orthogoniopteris, regarded by An- drews, its author, as comparable to Angiopteridium and Neriopteris, with many of the characters of Dansea.9 Alethopteris holdeni of Andrews10 is described by Lesquereux " as agreeing in most respects with Orthogoniop- teris, but is removed by him to form a new genus, Protoblechnwm, its nerves being rather more curved than in Orthogoniopteris, while it is excluded from Alethopteris by its supposed simply pinnate fronds. It would, per- haps, be not incorrect to designate these " Waverly " forms, occurring in the same deposit with the above-mentioned species of Megalopteris, as Alethopteroid megalopterids. Neriopteris, from the conglomerate series of northern Ohio, with its sessile or short-petioled pinnules and oblique nervation, in fineness and regularity rivaling that of Macrotaeniopteris, has. 1. Foss. PI. Dev. Upp. Sil. Can., p. 51, p!. xvii, tigs. 191-194. 2. Coal Flora, I, p. 148. See Ann. Rep't Geol. Surv. Pa., L886, pt. 1, p. 47.".. 3. Evol. re,g. veg., Phanerog., p. 77. 4. Andrew s, < Jeol. Surv. < >hio.. Pal. II, p. 416, pi. xlvi, figs. 1, la. 5. Ibid., p. 417, pi. xlvii. figs. 1, '-', 2a. 6. Ibid., p. 4lii, pi. xlviii, figs. l-:s. 7. Lesquereux, Coal Flora, p. 151, pi. xxiv, fig. :;. 8. [bid., p. 421, pi. 1, figs. 3. ■;n-h. 9. [bid., |>. tl.s. pi. 1, figs. 1, la. 10. Ibid., p. 420, 1)1. li, figs. 1. 2, 2a, 11. Coal Flora, v.,i. I. p. L88, SUGGESTED GENETIC RELATIONS. 125 i according to Newberry, an equal degree of affinity to Alethopteris and • Teeniopteris, and is separated from Teeniopteris only on account of its once or twice pinnate frond and the oblique nerves. It is interesting to note, in connection with this circumstance, the case of the Alethopteris macro- phylla described from the same horizon by Newberry, who says that but for the rectangular nervation lie should be inclined to include it in Neriopteris, while Lesquereux, on the other hand, refrained from referring it to Teeniopteris- only because it was pinnate, placing it in Daneeites in- stead. The backward rolling of the margin of Neriopteris may be only a more pronounced phase of what is common in species of Alethopteris, or it may be an indication of fructification. Newberry's description and figure of Neriopteris lanceolata 1 may with advantage be compared with those given by Lesquereux2 under the name Megalopterisf marginaia. Systematic Position and Relations of the megalopterid G roup. — A critical comparative study of the alethopteroid megalopterids will hardly fail to lead to the conclusion that in the early part of, perhaps before, the Sub- carboniferous, the Megalopteris stock attained a high differentiation, in which the Alethopteroid group produced in Neriopteris, Orthogoniopteris, Alethopteris, Protohlechnum and Danseites (Heer-Schimp.) certain forms embracing the essential characters of the pinnate Tseniopteridese. From this Lower Carboniferous group, doubtless including many undiscovered variations, may well have descended such forms as the Teeniopteris mis- souriensis in the Lower Coal Measures of the American continent, the T. jejunata, Grand Eury, and T. carnoti, Zeill., of the Upper Coal Measures of France, or the perhaps somewhat doubtful megalopteroid, T. truncata, Lesq.,3 from the Conglomerate series. As interpreted by superficial characters, the sequence of the Paleozoic tseniopteroid types into the Triassic forms, many of which have at some time rested in the genus Teeniopteris until the fruiting, either of them- selves or of contemporaneous obviously generically identical species, has been discovered, proving them to be true ancestors of living genera in the Marattiaceee, affords strong evidence at once both of the great an- tiquity of the group and its lineal descent from the Megalopteris stock. The figures of Goeppert's Teeniopteris munsteri, from the Rhetic of Bavaria, given by Schimper* on referring the species to the genus Ma- rattia, though apparently diagramatic in part, and those published by Bartholin5 deserve a comparison with Neriopteris and Dana ilex of the type macrophylla, Newb. sp., and the species becomes more interesting 1. Geol. Sunr. Ohio, Pal. I, p. 381, pi. xlv, figs. 1-3, 3a. 2. Coal Flora, I, p. 152, pi. xxiv, tig. 4. 3. Coal Flora, III, p. 743, pi. xciv, fig. 8. 4. In Zittel : Traite, II, p. 85, fig. R4; Traits pal. vfig., Atlas, pi. xxxviii, fig. I. 5. Botanisk TMsskr., vol. xviii, hft. 1, 1802, p. ■£',. pi. ix, tigs. G, 9. 120 I). WHITE — A NEW T-SJNIOPTEROID FERN AND ITS ALLIES. in view of the discovery in the Conglomerate series of Ohio of a form thoroughly Mesozoic in aspect that has been referred to the genus Danseites (Heer-Schimp.) by Lesquereux. From the study of many specimens of Tasniopteris munsteri, Goepp., fruiting from the Rhetic of Bavaria, Schenk was led1 to refer the species without hesitation to the genus Angiopteris, being unable to find any character warranting a ge- neric separation. Raciborski, on the other hand, is convinced that the fruiting of what he considers the same species in the Rhetic of Poland is that of the true Marattia. A nother tasniopteroid species which merits con- sideration is the Danasopsis marantacect ( Presl.) Hcer, from the Keuper, the fruiting of which is distinctly marattiaceous, and which was regarded by Schenk2 as very close to the living Dana a. The fine illustrations of this species given by Schimper3 may with great interest be compared with the Megalopteroid group from Ohio. The habit of Schimper's specimen, representing the upper portion of a pinna, seems such as to suggest that the lower pinnules may be distinct and not confluent, a suggestion em- phasized by the figures given by Schoenlein4 and Saporta.5 As tending to confirm this view, I may add that in Pseudodanasopsis, a genus of plants from the Upper Trias of Virginia, separated by Fontaine from Danasopsis chiefly on account of its anastomosing nerves, the lower and middle pinnules of the species P. reticulata, Font., represented by numerous specimens in the United States National Museum (No. 3488), are distinct, distant, equilaterally rounded at the base and in all re- spects distinctly tseniopteroid, except for the frequent anastomosis of the nervils, although the upper portions agree to a great extent with the habit and characters of Danasopsis marantacea. The establishment of the existence of the actual genera Angiopteris or Marattia in the Rhetic attributes to them a remarkable antiquity, un- equaled, so far as I know, among any other living fern genera; but indis- putable specimens of Dansea, with their fructification, were described by Zigno 6 from the Lias of Verona, proving for this genus a nearly equal antiquity. It follows that the epoch of indefinite length marking the genesis or lineal descent of these two marattiaceous genera must there- fore have terminated by the close of the Triassic. However, since none of the forms of the Danasopsis or tseniopteroid Danasites types have been found with distinct fruiting earlier than the Keuper, the direct lineage of the actual genera cannot be traced backward into the Paleozoic with any greater definiteness than a high degree of probability or likelihood. 1. Die loss. Pflanzeur., p. 30, (i.e. HB. 2. ( »p. cit.. p. 35. :;. Traits pal. v6g., Atlas, pi. xxxvii, figs. l-:t. I. A.bbild., pi. vii, lig. 2. 5. V6g. Jurasa., I, pi. Ixv, p. 154. (i. PI foss. oolit., \<<\. I, pi. xxv. pp. -.'os, 209. POSITION AND RELATION OF MEOxALOPTEROID GROUP. 127 In the absence of fruiting it may therefore justly seem inexpedient to many to refer pre-Keuper tseniopteroid species to genera like Angiop- teridium or Danseopsis, founded on or implying a known direct relation- ship to a certain marattiaceous genus. It is for this reason that, as stated above, I have preferred the use of Tssniopteris as a generic name devoid of all implication of an antecedent relation of a species to any particular genus. The probable relationship of the Carboniferous Tssniopteris to the Meso- zoic Marattiacess has been well expressed by Professor Zeiller,1 while that of the Mesozdic types of the genus has been ably discussed by Zigno,'2 Saporta3 and others, nearly all of whom ally them directly with the liv- ing genera. The occurrence of pinnate tseniopterids, such as Tssniopteris jejunata, Grand Eury, and T. carnoti, Zeill., in the Carboniferous and Per- mian of France; T. coriacea and T.fallax, Goepp., in the Permian of Bo- hemia; T. eckardi, Germ., in the Permian of Tyrol, and the Danseopsis Rajmahalehsis, Feist., in the Trias of India, the last two of which were regarded by Schimper4 as agreeing entirely with the Keuper Danseopsis, completes the continuity of the discovered pinnate tseniopteroid forms from the Subcarboniferous types to the Keuper, and may be considered as belonging to a not improbable genetic series passing from the alethop- teroicl megalopterids of the Lower Carboniferous — perhaps from the genus Megalopteris itself— to fruiting forms, in the late Trias, of the living genera Angiopteris, Marattia and Dansea. The relationship of the simple-leaved species of Tssniopteris to those with pinnate fronds is somewhat uncertain, though it does not seem im- probable that all came from the same stock, it is not impossible that the species of the type T. multinervis, Weiss., or T. smithsii, Lesq., as well as the genus Lesleya,5 may have come from the megalopterid type through an early variation. M. Zeiller. who has discovered forms referred by him to the latter genus in the Upper Carboniferous and Permian of France," associates it with Ta niopteris, and indeed the obliquity sometimes seen in the nerves of Tssniopteris,'1 as well as the distinctly tseniopteroid aspect of Lesleya, gives strong support to this view. The descent of the two 1. "Aucune des Teniopteridees du terrain houiller n'arencore ete rencontree 6 Petat fertile; raais quelques-unes d'entre elles presentent d'assez etroites affinites avec eertaines Teniopteridees sec- ondares reconnues anjourd'hui eomme tres voisines au morns des genres Angiopteris, Marattia, on Dancea, pour qn'on soitfonde a croire qu'elles doivent, elles aussi, appartenir aux Marattiaees." Fl. foss. bassin perm. Autun et Epinae, p. 160. 2. Fl. foss. oolit., vol. i. 3. Pal. franc., veg. Jurass., vol. i. 4. In Zittel: Traite, II, p. 86. 5. Lesquereux, Coal Flora, I, p. II::, Atlas, pi. xxv, figs. 1-::. 6. Fl. foss. bassin Autun Epinae, p. 166. See pi. xii, fig. 2; and Fl. foss. Commentry, pt. 1, p. 285, pi. xxiii, fig- 6. 7. See T. multinervis, op. cit., pi. xiii, fig. 1. XIX -Bull. Geol. Soc. Am, Vol 4. 1892 12S D. WHITE A NEW T.ENIOPTEROID FERN AND ITS ALLIES. forms may reasonably be considered as common, if not lineal, the Les- leya appearing to date back nearer, the type of Megalopteris dawsoni.1 On the other hand, the conspicuously unequally rounded bases seen in some species of Macrotseniopteris* suggest that the leaves may be only petioled divisions, comparable in arrangement to the pinnules of Neriopteris lan- ceolata, Newb., and be derived from pinnate forms. It may not be going too far to add that from some Permian or Triassic species of T&niopteris or Macrotseniopteris, essentially distinguished from the former only by the greater size and sometimes thinner texture, may well have originated the Oleandridium, thought by Schenk3 to be probably marattiaceous. As tending to confirm the hypothesis of the descent of the genera Angiopteris and Dansea from the Megalopteris stock may be noted the probable relationship of the neuropterids, whose origin, as Neuropteris, in or with Megalopteris is generally accepted by those who have studied specimens of the latter genus, to the Marattiacese. Although no satisfac- torily definite fruiting of any of the Neuropteridese has yet been discovered, the internal structure of the stems described by Renault4 as Myelopteris or Myeloxylon, and afterwards identified as Neuropteris, Odontoptosis and Alethopteris, is found to resemble that of the living Marattiacese. more than any other known type of fern structure. Thus, from the evidence afforded by their internal structure, which has led M. Renault5 to include Alethop- teris among the Neuropteridese,, the marattiaceous nature of Megalopteris has already received strong support. In this connection it is interesting to compare the illustrations of some of the more alethopteroid species of Neuropteris, suchas N. retorquata, Daws.,6 and N. selwynii, Daws.,7 from the Middle Devonian, N antecedens, Stur,8 and N dluhoschi, Stur9 (cf. N elrodi, Lesq.) from the Lower Car- boniferous, N biformis, Lesq.,10 N matheroni, Zeill.,11 and the figures given 1. It is quite possible that from the Leslei/a type may have been derived the Glossopte.ris group appearing in the Middle Carboniferous and Permo-Carboniferous of Australia. Lesquereux's diag- nosis differs, as he remarks, from Brongniart's description of the latter only by the nerves not anastomosing. In this connection it is interesting to consult Newberry's Tceniopteris ijlossopte- roides (Macomb Expedition, 1S76, p. 147, pi. vii, figs. 2, 2a) from the Trias of Sonora, New Mexico. The supposed fruit dots represented in his figure 5 appear quite similar to the dots seen between the nerves of Alethopteris maxima, Andr. 2. See M. magnifolia, (Rogers) Sehimp., Fontaine, Old. Mes. PI., Monogr. U. S. G. S., vi, p. 19, pi. ii, tig. 1, i>l. iii, iv, v. 3. Palseontogr., xxxi, 1881, p. bis. 4. Cours hot. foss., iii, p. 163.. 5. 6p. cit., p. 152. 6. Foss. PI. Dev., Upp. Sil. Can., p. 50, pi. xvii, fig. 200. 7. Ibid., fig. 198. 8. Culm-Flora, p. 53, pi. xv, figs. l-r>. 9. Op. cit., p. 289, pi. xxviii, fig. 9. 10. Coal Flora, p. 121, pi. xiii, fig. 7. 11. FI. foss. Commentry, pt. 1. pi. xxviii. fig. 7. GRAPHIC PRESENTATION OP RELATIONS. 129 by Von Roehl under N. plicata1 (= N. rectinervis, Kidst.)2 from the Coal Measures, and N. voltzii, Brgt.,3 and N. salicifolia, Fisch.,4 from the Per- mian, with the phases often seen in the basal portions of some species of Alethopteris, as, for example, .4. lonchitica, A. grandini, or Callipteridium sullivantii.5 On the basis of their fruitings, which are either exannulate or with only a rudimentary ring, as well as from the analogies of their structure, all modern authors agree in considering a large number of Paleozoic species with pecopteroid nervation as most nearly allied to the Marattiacese among living ferns.6 This conclusion is natural, in view of the known antiquity of certain living marattiaceous genera, as well as the probable long existence of the eusporangiate ferns in Paleozoic time before the leptosporangiate forms appeared. Graphic Presentation of Relations. — The following diagram represents in graphic form the general idea of development for a few genera; but it is not to be understood that the relations of individual genera are sup- posed to be in all cases as therein indicated, nor that the scheme is meant to imply a presumed proof or even the existence of evidence sufficient to form the basis of a proof. The lines should indicate in most cases a common rather than a lineal descent. It must be remembered that such a scheme is largely mere speculation. Many of the implied relations are improbable as well as incompatible. Some suggestions embodied in the chart constitute my only excuse for presenting it. Conclusions. — In the foregoing discussion of what may be regarded as a tentative hypothesis for the line of descent of several of the living- genera of Marattiacese from the Megalopteris stock, I have not presumed to attempt a proof or demonstration among a body of forms whose fruit- ing is essentially unknown; I have rather sought to bring together some of the evidence in favor of what I consider a good working theory. Ac- cording to this hypothesis, we may suppose that the pinnate Tasniop- teridese, or a portion of that group (without prejudice of any important 1. Foss. Fl. Steink., Westfalens, pi. xx, figs. 7, 8; pi. xiii, fig. 8. 2. Trans. Roy. Soc. Ediub., xxxv, 1888, p. 314, figs. '-'-4. 3. Hist., pi. lxvii. 4. Kutorga, Verb. Euss. Kais. Min. GeselL, St. Petersb., 1842, pi. i, fig. 2. 5. From the analogous characters of the nervation the genera Neuropteris, Odontopteris, Lesteya, Dictyopteris, Neriopteris, Megalopteris, and Tcenioptens were included in the Neuropterid group by Lesquereux in one of his last publications on the Carboniferous flow (Ann. Rep. Geol. Surv. Penna., 1886,pt.l,p.475). Renault (Cours. bot. foss., 3me annee) makes the Neuropteridece include Neuropteris, Odontopteris, Dictyopteris, Alethopteris, Lonehopteris, Callipteridium, and Callipteris. More recently Grand Eury (Geol. Pal. bassin houill. Gard., p. 286. construes the, tribe so as to contain AulacopU ris (Mydopteris), Alethopteris. Callipteridium. Neuropteris. Dictyopteris, Odontopteris, Tamiopleris, and a new pecopteroid genus, Parapeeopteris, intermediate in form between the neuropteroid Pecopteris species and those of Neuropteris, with fructification after the fashion of Damea. 6. See Renault, Cours. bot. foss., 3e annee; Stur. Carbon PL Schatzlav. Sch., ii; Zeiller, PL foss. Autun Epinac; Kidston, Trans. Geol. Soc. Glasgow, vol. ix, p. 1. 130 D. WHITE A NEW T/ENIOPTEROID FERN AND ITS ALLIES. 6C p5 o w w - H-9 i « i © ■A e SJ ci o"s ~ c gq «) a = *r ^ .S1^ SVS s 5> ^ to <& "C -- O O 03 o •iiAVOm[uu S'uijm. w ■ H 0 u O -^ O a ■s OS O 0 7-* M 0> £ & O 0 O h3 o > p s ft p G c CONCLUSIONS. 131 systematic distinction between the pinnate and simple forms), came from an early Megalopieris stock, probably through the alethopteroid forms. The earliest flora, so far as I know, in which any of these occur, that of the Middle Devonian at Saint Johns. New Brunswick,4 besides contain- ing the Megalopteris daivsoni, has also representatives of Neuropteris, most of which are alethopteroid, and of Alethopteris, including the A. grandis and A. discrepans already referred to. It is not improbable that the three of these genera originated in a common stock ; and since the Megalopteris group offers a comprehensive type from which the Neuropteris and Ale- thopteris, as wrell as the known Megalopteris species, might well have descended, that name may conveniently be employed in the hypothesis to designate the type existing previous to the Middle Devonian, from which the ncuropteroid, alethopteroid and tseniopteroid groups, includ- ing in the latter some species of living marattiaceous genera, descended. 1. See Dawson, Foss. PI. Dev., Upper Sil. Form. Can., Geol. Serv. Can., 1871. Explanation of Plate 1. Tseniopteris missowriensis, n. sp. Figure 1. — Fragment from upper middle portion of pinna. Pinnules nearly dis- tinct. Figure 2. — Portion near tip of pinna. Pinnules confluent. Figures 3 and 4. — Apex of pinna, showing true AklhopU m development. Figure 5. — Fragment from middle of pinna, showing taeniopteroid pinnules, dis- tinct, contracted at the base, attached to the central axis of the rachis. Figures 6 and 7. — Fragments of detached pinnules. The broad character of the median canal is not well indicated, nor the wide midrib, especially prominent on the back of the pinnule. The origin of the nervils in the median strand is well represented. (132) BULLETIN OF THE GEOLOGICAL SOCIETY OF AMERICA Vol. 4, pp. 133-H6 February 25, 1893 SOME ELEMENTS OF LAND SOULITI'IJK BY LEWIS EZRA HICKS {Offered to the Society for Publication August 15, 1892) CONTENTS Pago Introduction l;;:; Relief Forme subject to fixed Laws 133 Predominance of Curves, over Angles 134 SI ructural Angles 134 • Character of Hock governs Form 134 Incessant Activity of sculpturing Forces 134 Flatness characteristic of continental Blocks 134 Weather Curve and water Curves 135 Weather Curve 135 Convexity of weather Curve 135 Water Curves : horizontal and vertical 136 Concavity of water Curve 136 Combined weather Curve and water ( !urve 137 Reversed Curves 138 Gilbert's "Exception" explained 3 38 Water Curve of Deposi t ion 142 Alluvial Cone 142 Flood-plains 142 Cross-section of constructive River .... 14:; True Form of Cross-section 1 44 Cross-section of River having no Flood-plain 144 Anomalous Valleys of the great Plains L45 Summary 14<> Introduction. Relief Forms subject to fixed Laws. — Every element of form which gives character and expression ton landscape is determined by fixed Laws. It is true that the arrangement of lulls and vales does not conform to any simple geometric pattern. The sculpturing forces are complex, and the net result of their interaction is necessarily also complex and promis- XX— Bull. Geol. Soc. Am., Vol. I. 1892. (!.'!:>) 134 L. E. HICKS — SOME ELEMENTS OF LAND SCULPTURE. cuous; still the action of each single force is regular, exact and unvary- ing, and the complex results are harmonious. Predominance of Curves over Angles. — Most pleasing to the eye are those forms in a landscape which arc bounded by curved lines and surfaces. Most striking, picturesque, rugged and impressive are those which are hounded by planes and angles. The former arc far more common, and are produced by weathering and the washing of water. The latter de- pend upon the primitive structure of the rocks. Angular structural" forms are the rough blocks which nature furnishes. Wind and frost. sun and rain, rills and rivers, are the tools which carve out of these rough blocks the beautiful landscapes which adorn the earth and make it a fit abode for man. Structural Angles. Character of Rock governs Form. — The laws of structure are intricate. and structural forms are infinite in variety. The planes may face in any direction, the angles may be acute or obtuse. That depends wholly upon the forces of upheaval and the laws of fracture in the different rocks; granite, limestone, basalt, conglomerate, each imparts a definite and characteristic expression to the landscape, because each breaks in a way peculiar to itself. Incessant Activity of sculpturing Force*. — But with all this variety in de- tail there are certain broad, general features of structure which exert an important influence in the evolution of earth forms. The pent-up forces within the earth thrust up from time to time fresh blocks, to be disinte- grated by the weather and carved by running water. ' These sculpturing forces never rest, while the forces of upheaval are intermittent. This incessant and universal activity of the sculpturing forces is the reason why the pleasing forms hounded by curves are more common than rough structural angles. Flatness Characteristic of continental Blocks. — Though the internal forces are inconstant they are mighty. Mountains and continents are the burdens which they lift with ease. The lands are lifted and at the same time broken, faulted, bent and tilted this way and that. The resulting planes may slope north, south, east or west, and the pitch may be steep or gentle. Very steep structural planes are. however, of limited extent, while the great continental blocks must of necessity lie nearly flat, though the edges may lie precipitous. Broad, flat blocks are therefore the usual raw materials for the sculpturing forces, and the resulting weather and water curves are dominated by these massive and nearly level, primitive elements of structure. Massive breadth and relatively slight inclination of the general surface are the fundamental character- STRUCTURAL CURVES AND THEIR PRODUCTION. 135 istics of structure which prevail in the midst of the infinite variety of relief forms. Weather Curve and water Curves. Weather Carre. — The weathering of structural blocks reduces their salient angles, which are attacked from both of the adjacent faces at once. At the point x, figure 1, the disintegrating forces act with twice as great intensity as at b, since the attack conies from two directions. The effects are more than twice as great at x, because the products of decay are quickly removed, exposing fresh surfaces to the attack, while at b they remain to cover and protect the subjacent beds. Thus the structural block m n o p is rounded oil' by weathering. The new outline a b c is composite. The portion <1 b e is ;i weather curve, convex upward. If weathering alone, without the aid of flowing water, has been concerned in the sculpturing process, the talus slopes a d and e c will be structural planes, not curves. The structural angle e c p will he determined by the am j> c FtiiUHE 1. —Weather Curve. resting angle of the materials composing the talus, and that again will depend upon the size and form of the particles ; hut in humid regions the talus slopes will he quickly molded into water curves, as hereaiter described. The resulting form , figure 3. This is usually true of streams rising in extensive swamps and wet meadows. Even the mountain streams often flow sluggishly at first upon broad Hat summits, then pitch headlong over the escarpment. We have seen above that breadth and flatness are the domi- nant elements of structure. The precipitous edges of broad continental Figure 3.— Combined weather Curve (a b) and water Curve (b c). blocks being rounded off impose their own curves upon the rivers. Thus the convex portion (a 1>, figure 3) is not really a water curve, it is a temporary accommodation of a water gradient to the structural form upon which it flows. The true water curve (b c, figure 3) will moreover gradually encroach upon the upper convex curve a b, and, if the base- * leveling be continued long enough, it will establish itself as a smooth concave curve from c to a. Hence this exception, as in the case of cata- racts, is an incident only of river history, the only differences being that it is more common and less transient; but, as 1 said above, it almost deserves to take rank as a distinct and coordinate law on account of its universality. The convex portion of the curve (a />, figure 3) is not, however, a new kind of curve, but one that has already been defined, viz, the weather curve. The double reversed curve (a /> c, figure 3) is the combination of the weather curve and the water curve of erosion. It is Hogarth's line of beauty, the most universal of earth forms. Almost every hill slope in a rolling country presents an upper convex portion 138 L. E. HICKS — SOME ELEMENTS OF LAND SCULPTURE (weather carve) and a lower concave portion (water curve). Some land- scape engineers have caught nature's hint and give a terrace the form shown in figure 3, which' is at once more elegant and more solid and durable than a slope in which the convexity is carried uniformly down Figure 4. — Unstable artificial Curve. to the base, as in figure 4. The latter is unnatural and unstable, while the former is natural and stable. Reversed Carre*. — Tins combination of the weather curve with the ver- tical water curve of erosion when carried out upon both sides of a struc- tural block (as m a <> j>. figure 1), which is symmetrical and homogeneous, will give the pair of reversed curves shown in figure 5, instead of the Figure 5. — Normal relief Form in an advanced Stage 0/ Base-leveling. simple convex weather curve db e, figure 1. Figure 5 is the normal pattern of relief forms in a region of advanced land sculpture. The summit b a b is a simple, typical weather curve. The talus of figure 1, with its clear-cut structural angle, e c p, has been replaced by the vertical water curve b c (figure 5), which is concave upward. Gilbert's "Exception" explained. — This same combination of weather and water curves is the true explanation of the li exception " noted by Gilbert* who states : " There is one other peculiarity f of bad-land forms which is of great significance, hut which I shall nevertheless not undertake to explain. According to the law of Figi re 6. — Typical Profile of the drainage Slopes of Mountains. * Report oii the Geology of the Henry Mountains, pp. 122-123. t Figure 6, which is a reproduction of Gilbert's figure 54 (ibid., ]>. 116), shows an angle. Such would be tin- actual result of intersecting water curves bui for tin- effed of weathering, which rounds oil' the angle and replaces it by a curve convex upward. Gilbert's exception to law of divides. 139 divides, as stated in a previous paragraph, the profile of any slope in the bad-lands should be concave upward, and the slope should be steepest at the divide. The union or intersection of two slopes on a divide should produce an angle [figure 6]. But in point of fact the slopes do not unite in an angle. They unite in a curve, and the profile of a drainage slope, instead of being concave all the way to its summit, changes its curvature and becomes convex. . . . From a to m [figure 7] and from b to n the slopes are concave, but from m to n there is a convex curvature. Where the flanking slopes are as steep as represented in the diagram, the con- vexity on the crest of a ridge has a breadth of only two or three yards, but where the flanking slopes are gentle, its breadth is several times as great. [Compare figure 5 with figure 7.] It is never absent. Fku'kk 7. *— Cross-profile of bad-land' Divide. " Thus in the sculpture of the bad-lands there is revealed an exception to the law of divides, — an exception which cannot be referred to accidents of structure, and which is as persistent in its recurrence as are the features which conform to the law, — an exception which in some unexplained way is part of the law. Our analysis of the agencies and conditions of erosion, on the one hand, lias led to the conclusion that (where structure does not prevent) the declivities of a continuous drainage slope increase as the quantities of water flowing over them decrease, and that they are great in proportion as they are near divides. Our observation, on the other hand, shows that the declivities increase as the quantities of water diminish, up to a certain point where the quantity is very small, and then de- crease; and that declivities are great in proportion as they ai'e near divides, unless they are very near divides. Evidently some factor has been overlooked in the analysis, — a factor which in the main is less important than the flow of water, but which asserts its existence at those points where the flow of water is exceedingly small, and is there supreme." The missing factor is a simple and omnipresent one, namely, weather- ing. From a to m the water curve predominates, and its law of skyward concavity and increasing declivity is supreme. From m to h the weather curve predominates. As Gilbert remarks, "the flow of water is exceed- ingly small" there. It falls as rain and beats upon the crest, hut that is a kind of weathering. Besides supplying the missing factor which explains the puzzle and reconciles the results of scientific analysis with the facts as learned by * Figure 7 is a reproduction of Gilbert's figure 60, in his Report on the Geology of the Henry Mountains, p. 123. 140 L. E. HICKS — SOME ELEMENTS OF LAND SCULPTURE. observation, I will add two observations suggested by the above quota- tion. In the first place, the remark of Gilbert that "where the Hanking slopes are as steep as represented in the diagram, the convexity on the crest of the ridge has a breadth of only two or three yards, but where the flanking slopes are gentle, its breadth is several times as great,'' conveys a partial truth, and at the same time suggests a broader truth. Gilbert merely affirms a relation between the steepness of the decivities and the breadth of the convex portion of the crest; but both of these correlated elements of form depend upon the relative intensities of water sculpture and weathering, and these in turn depend upon the struc- ture and the stage of base-leveling in the given region. The general law of relative intensities may be stated as follows: If water sculpture predominates, the slopes will be steep and the divides narrow and high ; and, conversely, if weathering predominates, the slopes will be gentle and the divides broad and low; but this general law is profoundly modified by structure and time. The broad, flat blocks which, as we have seen ct Figure 8. — Illustrating the Co-i cistt nee of steep Slopes with broad weather Curves in an tarty Stage of Base-leveling. fi«() = weather curve ; b c = water curve. above, are the normal types of raw material to be moulded by land sculpture, yield broad weather curves in the early stages of base-leveling wholly on account of their primitive structure. This is an exception to the general law, inasmuch as water sculpture is usually energetic in these early stages, and yet the weather curves are 1 >r< >ad. 1 1 is als< » an exception to Gilbert's statement that the crest is narrow if the slopes are steep. Many cases occur in the earlier stages of base-leveling in winch broad, flat weather curves are conjoined with very steep water curves, as in figure 8. Many cases also occur in the same early stages of base-leveling in which the crest is narrow and the slopes steep, as affirmed by Gilbert and illus- trated by his figure G'>. For example, the same mesa represented in cross-section by figure 8 would present many subordinate ridges between its lateral ravines with steep slopes and narrow crests. It is evident, therefore, that in this early stage of base-leveling, structure is the domi- nant factor whether the crest is narrow or broad. The steep water curves are the direct result of structure, since it is only by upheaval EXPLANATION OF GILBERT'S EXCEPTION. 141 that such high gradients originate; and the broad crests are equally the direct effects of structure. The narrow crests exemplify the law of rela- tive intensities, as stated above. Water sculpture is more energetic than weathering upon the precipitous edges of structural blocks; hence the slopes are steep and the crests narrow. With the lapse of time the influence of structure gradually diminishes, and the stage which base-leveling has attained exerts the greater modi- fying influence upon the general law. In other words, time exerts a modifying influence in proportion to its quantity, measured from the beginning of the process of 1 rase-leveling. If this process has just begun, structure is supreme; but if it has reached its later stages the accumu- lated effects of time are supreme. Weathering and water sculpture both tend to become less energetic as the surface approaches base-level and the gradients flatten out, but the former retains a greater relative efficiency. The transportation and removal of the solid products of weathering does indeed steadily diminish, but solution — one form of weathering — and the transportation of its products goes on to the very last stages of land sculpture, after erosion has ceased. These last stages are therefore marked by water curves of slight declivity and weather curves of great breadth and flatness, both in fact closely approaching, but never quite reaching, an absolute base-level. The general law with its modifications ma}r be summed up thus : In early stages of base-leveling the predominance of water sculpture' gives steep slopes and narrow crests, except where the latter have a breadth which is imposed upon them by the structure, and in late stages of base- leveling the predominance of weathering gives water curves of gentle declivity and broad, low weather curves. The second observation suggested by the quotation from Gilbert is that the principles explained by him as applying to "bad-land forms " are equally applicable to all kinds and all stages of land sculpture. Bad lands constitute a certain striking phase of land sculpture, but they are nowise exceptional, so far as the general laws and processes of land sculpt ture are concerned. All of the factors are present and active. The resul- is unique, not because of the absence of any familiar factor nor because of the presence of any new factor, but solely because of the relative intensity of the factors. Structure and water sculpture strongly predomi- nate over weathering. Structural forces have supplied the canon clays and marls as raw material — a matrix soft, homogeneous and peculiarly susceptible to rapid erosion on account of these properties and its con- siderable elevation. Water sculpture, attacking it with an energy pro- portional to its height above base-level and its lack of cohesion, cuts deep gashes so rapidly that weathering has little opportunity to round off the XXI— Bull. Geol. Soc. Am., Vol, i, 1882. 142 L. E. HICKS — SOME ELEMENTS OF LAND SCULPTURE. sharp edges. Indeed, this important factor occasionally seems, for the time being, to be wholly wanting. Forms like figure 9 are not uncommon in the bad lands. The summit b b is protected with turf and the water curves b c extend to the very crest without a trace of a weather curve; but the elimination of this factor is transitory. Visit the same butte some years later and you will find, if water sculpture is still vigorous, that the two water curves have so nearly joined that the turf has dis- appeared and a short weather curve occupies the narrow crest, as in figure 7 (Gilbert's figure 60), or, if water sculpture has been dormant, the angles b b are replaced by weather curves. In a bad-land region all stages of the process may be observed, from the level-topped sharp-angled butte, often receiving the significant name " Box butte " or " Trunk butte," shown in figure 9, to low domes like figure 5, which are not bad-land forms at all. The same laws, the same processes are concerned in all these varied results,'and a philosophic view of the subject demands that Figure 9.— Miniature Butte in tlie Bad Lands. all phases and stages of land sculpture be grouped comprehensively instead of singling out a particular phase, though that maybe a striking one. Water Carve of Deposition. — The water curve of erosion, having its sky- ward face concave, is not the only vertical water curve. There is also the curve of deposition, which is convex upward. Where a mountain torrent debouches upon the plain, the debris carried or rolled along by it spreads out in a mass which is fan-shaped in ground plan and conical in elevation. Alluvial Cone. — Such a deposit is usually called an alluvial cone, but, in view of its radial extension from the mouth of the gorge, Hilgard calls it a debris fan. The cross-section presents a typical water curve of depo- sition, convex upward. Flood-plains. — The flood plains of rivers, so far as they are built up by sediment spreading laterally from the channel during floods* follow the * This is the usually accepted meaning of the term flood plain, namely, that it is the work of a constructive river which is silting up its valley, or certain portions of it, during inundations. Gil- bert uses the term in a very different sense. He says in Geology of the Henry Mountains, p. 132: "* * flood-plains are usually produced by lateral corrasion. There are instances, especially neai' the seacoast, of river plains which have originated by the silting up of valleys, ami have been afterward partially destroyed by the same rivers when some change of level permitted them to FLOOD-PLAINS. 14 I v same law. It is true the curvature is faint, so faint that in the field it may he imperceptible to the eye, and in diagrams most authors ignore it, and represent the cross-section of a flood-plain by a straight line; but the curve, though slight, is real. If compared with the debris fan of a mountain torrent it would be found to correspond to the outer margin, where it blends into the plain and the convexity is slight. Strictly speaking, a flood-plain extending many miles along a river cannot be likened to a single alluvial cone; it is a composite structure made up of a multitude of overlapping cones, each having its apex upstream at that point where the silt composing it left the channel. The overlaps obscure the convexity of individual cones, and the net result is a curve of large radius and low convexity. Cross-section of constructive River. — The typical cross-section of a river having a flood plain — a constructive river— so far from showing a straight line from the channel to the bluffs, presents a convex curve of deposition, besides a number of other distinct elements. If no terraces are present the section will be as in figure 10, each half of the valley presenting a Figure 10. — Cross-section of a constructive Rivt r. a b = Weather curve at crest of bluffs ; ic^= Water curve of erosion ; e d = Swamp ; de= Water curve of deposition. weather curve, two water curves of opposite character, and a swamp along the line of intersection of the water curves. The presence of ter- races adds much complexity. The swamp at c d is caused by a de- pressed surface and an impervious subsoil. Only the finest argillaceous sediments spread so far from the channel or from the bluffs, and these cut their channels deeper; and these instances, conspiring with the fact that the surfaces of flood plains are alluvial, and with the fact that many terraces in glacial regions are carved from uncon- solidated drift, have led some American geologists into the error of supposing that river terraces in general are records of sedimentation, when in fact they record the stages of progressive cor- rasion." The question about the true significance of terraces is aside from the present discussion, but the ordinary meaning of flood-plain is too well settled to disturb it by so radical a departure as that here proposed. Since Gilbert himself admits it to be descriptive of'a real phenomenon, we might conclude that there are two kinds, flood-plains of eorrasion and flood-plains of sedimentation, and that all we need is to distinguish these and use the term in each case with its proper adjunct; but a closer analysis reveals two difficulties. In the first place, since tin' products of eorrasion on one side of a stream are deposited as sediments on the other side, it turns out that the plain of cor. rasion, or planation, is also a plain of sedimentation. This difficulty tends to merge the two kinds into one ; but there is an opposite and more radical difficulty which rends them apart. The plain of planation is not properly a flood-plain at all. Lateral eorrasion is nut exclusively a flood phe- nomenon, though it is active in floods. The plain of planation differs so much from true flood de- posits that the term flood plain ought to he restricted to the latter, as is usually done, 144 L. E. HICKS — SOME ELEMENTS OF I. AND SCULPTURE. form a gumbo * which imparts the impervious quality to the subsoil, and at the same time their small bulk and relatively slow growth occasions a line of depression. Even when well drained, this part of the river bottom is apt to be cold and sour mitil redeemed by tillage and the admixture of silicious elements. True Form <;/' Cross-section. — The old definition of the upper course of a river postulates a V-shaped cross-section.. This is not strictly true, even of fresh ravines at the headwaters. The sides are water curves of erosion, and they conform to the general law that the slope varies inversely as the quantity of water flowing upon it. Since the bottom of a slope re- ceives the water from above as well as its own quota of the rainfall, its pitch must always be less steep than that above if it is a true water curve. One side of a ravine may be ;i talus with its sharp structural angle and uniform declivity, the corrasion at its base proceeding so rap- idly as to give no time for a water curve to form. Very rarely, when the bottom only of a ravine is undergoing erosion, a talus slope may exist on both sides, and the section will then be accurately V-shaped; but if the corrasion at the base of either wall lags or stops, the wash of that slope will speedily convert it into a concave water curve of erosion. The actual result is usually composite, including elements or remnants of a structural angle, modified by a water curve. At all events, it is a curve rather than an angle, and a V with curved sides quickly passes into a U. The middle course of a river is usually said to have a U-shaped valley, hut in fact this form belongs to all parts of a river, the onl}' difference being the breadth of the U. It is in the upper course alone that it has anything like normal proportions. In the middle, and especially in the lower course, it sprawls out and flattens down until all resemblance to the fifth vowel is lost. Moreover, the presence of terraces and water curves of deposition so complicates the cro Flood-plain. — The most important real distinction between the different parts of a river valley is the presence or absence of a flood-plain. If this is present the section will he as in figure 10; if it is absent, it will be as in figure 11. in which, as compared with figure 10, the middle portion, including the flood-plain with its convex curvature, has been cut out. There is a wide range of variation among different rivers in that por- tion of the valley which has a cross-section like figure 11. It may he very narrowly U-shaped, or it may open out to such breadth as to he- come anomalous. Under ordinary climatic and geologic conditions the *Gumbo is a peculiar, tenacious, fine-grained clay. The use .-mil meaning of this term in the western states is so well established, that it promises t" become a useful and expressive word. ' ANCXMALOIS STRUCTURAL FORMS. L45 narrow U-form would include the whole course of the river above the initial flood plain. Figure 11.— Cross-section of a river Valley having no Flood-plain. Each half of the valley has only two elements, the weather curve a b and the water curve b c. Anomalous Valleys of the great Plains. — But certain peculiar conditions sometimes intervene to prevent the development of a Hood plain where it normally belongs. Then we have the anomaly of a valley some miles in breadth without a flood-plain, which is so diametrically opposed to our ordinary conceptions of rivers that we are at once impelled to seek its explanation. It is upon the great plains at the eastern base of the Rocky mountains that we find the most striking examples of wide valleys without flood-plains. The lower part of the water curve (m n, figure 12) Figure 12. — Cross-section of a broad Valley of the Plains having no Flood-plain, a l> = weather curve ; b m n = water curve, of which the lower portion, m ??, is greatly extended. may be a mile or two in breadth. At the point m the valley wall begins to be well defined. The valley floor m m is also well defined, but quite remarkable for its wide departure from horizontality. The point m may be fifty feet above n. It is unmistakably a valley floor, but its steepness is astonishing and perplexing. Moreover, the anomaly does not stop with the unusual form of the cross-section. The quality of the land contra- dicts all expectations which would naturally be entertained respecting river bottoms. Instead of a uniform stretch of rich alluvium we find irregular alternations of loam, sand, gravel, gumbo and alkali patches. The best element, the loam, may indeed predominate, and hence the valley may support a prosperous agriculture; but the valley lands of the plains are generally inferior to the table lands, thus reversing the condi- tions which usually prevail. The plains are built up of incoherent masses of sand, gravel, (day Idb' L. E. HICKS — SOME ELEMENTS OE LAND SCULPTURE. and marl, in which the rainfall is absorbed and reaches the rivers by slow percolation, instead of flowing quickly and copiously On the sur- face; hence, if there are any floods at all. they are infrequent and irregular. Without regular floods there can he no distinct flood-plain, the silt deposited during the rare overflows being obscured and sub- ordinated to the heterogeneous wash from the hills. The patchy char- acter of the soil arises from local conditions affecting the wind drifts and washings from the bluffs, bringing down here gravel, yonder sand, and again the mingled silicious. calcareous and argillaceous elements consti- tuting loam. Alkaline carbonates and sulphates are developed in low, undrained spots, where water lies and evaporates. By the meanderings of the channel the valley floor is plowed up and redeposited, but this process tends to still greater differences rather than greater uniformity. The assorting action of the currents segregates the coarser and finer ele- ments and deposits each by it-self. The absence of floods intensities and perpetuates these diversities. No general 1 danket of rich silt is spread in annual layers to cover and blend into one the heterogeneous soils, nor do the copious waters spread over the alkali patches to dilute and wash out their bitterness. Thus arise these anomalous, wide valleys without flood-plains, in which the whole valley floor from the bluffs to the channel on either side slopes sharply inward, and the soils are patchy and wholly unlike ordinary bottom lands. Summary. This paper makes no pretensions to an exhaustive treatment of the elements of land sculpture. There are other forces at work, and the forces named operate in ways not herein discussed in detail; but in the broad, general view of the subject the face of nature is moulded chiefly by these forces : (1) Upheaval, which furnishes the structural blocks to be chiseled into pleasing forms ; (2) Weathering, which rounds off the asperities and covers the land with graceful, swelling curves; (3) Washing of water. which yields concave flowing lines upon slopes of erosion, and low con- vex curves of deposition. The combination of the weather curve with the water curve of erosion is here noted and explained for the first time. It constitutes the greatest charm of natural landscapes, and its effects are universal. BULLETIN OF THE GEOLOGICAL SOCIETY OF AMERICA VOL. 4, PP. 147-166, PL. 2 FEBRUARY 25, 1893 SOME DYNAMIC AND METASOMATIC PHENOMENA IN A METAMORPHIC CONGLOMERATE IN THE GREEN MOUNTAINS * BY CHARLES LIVY WHITTLE (Presented before the Society August 16, 189%) CONTENTS Page Metamorphic Conglomerate 148 Approximate Relation to known geologic Horizon 148 Ottrelite Schist 148 . Occurrence and Extent 148 Physical and microscopic Characters 140 Mineralogic Constituents 150 Parallel Grouping of ottrelite Prisms 151 Parallel Grouping of rutile Grains ■ 152 Alteration of Ottrelite into Chlorite 152 Relation of the two Minerals 152 Optical Characteristics 153 Groundmass of the Rock 153 Mineralogic Constituents 153 Feldspar 153 Sericite 153 Anatase. 153 Rutile 154 In General 154 Order of Crystallization 154 Metamorphism of the clastic Material in conglomerate Phase 155 Occurrence • • 155 Character of the Rock 155 Secondary Enlargement of clastic Tourmalines 156 Two Periods of Disturbance indicated 158 Alteration of clastic Feldspars 150 Clearing Action of growing Sericite 160 Alteration of clastic Microcline into Plagioelase 161 Chlorite Schist and Phyllite 164 Their Plications built into secondary Albites L64 Composition of the Groundmass 165 * Published by permission of the Director of the IT. 8. Geological Survey. XXII— Bull. Geol. Soc. Am., Vol. 4, 1892. (147) 148 C. L. WHITTLE METAM0EPH10 CONGLOMERATE. Metamorphic Conglomerate. Approximate Relation to known, geologic Horizon. — The geologic position of the limestone and quartzite of the Rutland valley has lately been de- termined definitely,'1' the limestone paleontologieally and the quartzite stratigraphically. Occurring next below the limestone, the quartzite is the northern continuation of the Clarksburg-mountain quartzite, in Massachusetts, in which Walcott has found the Olenellus fauna characteristic of the Lower Cambrian horizon. About one mile north of Rutland village, in Vermont, Dr Wolf and Dr Foerste were fortunate enough to find Lower Cambrian fossils in a silicious limestone that lies superjacent to the quartzite. Northeast of Rutland the quartzite is found associated with a sandy phyllitic schist that belongs to a series of metamorphosed elastics having a vitreous quartzite or conglomerate at its base. This whole series, barring the Lower Cambrian quartzite and limestone, has been subjected to the most intense dynamic action. The sequence of the dif- ferent members of the series is in many regions hopelessly obliterated and confused by the mountain-building forces that have produced new structural planes, a new mineralogic composition, and have additionally complicated the geologic order of succession by sharp folding, which is, as a rule, too much involved for decipherment. These phenomena are particularly noticeable in the conglomerate horizon and its many phases, and it is in this rock that I wish to describe some of the evidences and effects of metamorphism shown by the destruction of old clastic minerals and in the production of new ones. OTTRELITE SCHIST. Occurrence and Extent. — One of the most conspicuous phases of the con- glomerate is due to the development of ottrelite in great abundance, so that it is not uncommon to find fully 25 per cent of the rock made up of this mineral. The ottrelite is commonly most abundantly developed where the rock has now a well-marked schistose character that is either due to an original finer-grained deposit or is a result of the shearing and crushing action of dynamic forces. It is often found, however, occurring in the grouudmass of the coarsest conglomerate or along planes of shear- ing in a blue, hyaline quartzite. Still another phase is more nearly mas- sive, fully 40 per cent being ottrelite, the rock at first sight simulating in appearance some porphyritic hornblende dike. The rock is a very *"0n the Lower Cambrian Age "t the Stoekbridge Limestone" : Bull. Geol. Soe. Am., vol. •_. 1880 pp. 331-338. LOCALITY AND CHARACTERISTICS. 149 variable one, but, considered as a whole, it forms one of the most impor- tant stratigraphie horizons found in the more crystalline areas of the Green mountains. In lateral extension it has been traced, with unim- portant breaks, all the way across the Green-mountain anticlinal axis, as mapped by Hitchcock * from Mendon, Vermont, to North Sherburne, Vermont. In vertical extension it has considerable thickness, although accurate determination is very difficult, owing to the obliteration of planes of bedding in most instances and the complexity of the flexures; but it seems safe to assume a thickness of several hundred feet, at least in sev- eral localities that have been most carefully studied, viz : a spur extend- ing south from Mount Carmel, in the town of Chittenden, and the east and west crest forming the southern portion of the mountain, somewhat inappropriately named "Old Aunt Sal."f The latter mountain is situ- ated in the town of Mendon, the next town south of Chittenden. The phases studied thus far in the laboratory are from this latter locality and from the western part of the " Rabbit ledge," just south of Mendon " city." Physical and microscopic Characters. — In the hand specimen the ottrelite of the most massive occurrence of the ottrelite-1 tearing rock appears either as isolated areas, generally with rudely circular outlines, or as groups of them in a background of fine-grained pinkish-brown to dark-purple quartz, in places constituting nearly pure ottrelite. These areas possess approximately a common diameter of about three-sixteenths of an inch. In structure the}'' are made up of radiating imbricated plates generally arranged in essentially one plane for any single area ; but the positions of the different areas seem in the main to be accidental, although locally they may be arranged parallel, as shown by a tendency in the rocks to cleave into rude slabs, a tendency augmented by thin folia of serecite. A well marked spherocrystalline habit characterizes all the ottrelite areas. In some this radiated growth seems to be perfect. Microscopic- ally the radiated structure is much more evident. Composite and fan- shaped areas, penetrating one another irrregularly, coexist with isolated prisms and beautiful spherocrystalline aggregates, yielding imperfect crosses in polarized light. Only sections cut parallel to the bundles of plates (basal sections) show well the radiated structure ; all other sec- tions show this character less and less, depending upon the plane of the section, until it is transverse, when the mineral appears prismatic. The areas of spherocrystals are not infrequently bounded by overlapping six- sided plates, of which three are usually free; the others are intergrown and confounded in thy central position of the aggregate. * Figure 4, section vi, Hitchcock's Green mountain gneiss, G-eoI. of Vt., vol. 4. 1861. fThe name Blue Ridge is given this mountain on the Rutland topographic sheet completed in 1891, butl have decided to use here the most commonly adopted local name 150 C. L. WHITTLE — METAMOE.PHIC CONGLOMERATE. The extreme mobility of the ottrelite-bearing solution is indicated by the manner in which the ottrelite needles have insinuated themselves into included feldspar grains along no visible lines of fissuring. Mineralogic Constituents. — As in all described occurrences of this min- eral, an abundance of inclusions exists. It is noticeable that, while quartz and occasionally feldspar are included, sericitc. which is the principal micaceous constituent of the rock, is seldom enclosed by the growing ottrelite. but may be wholly or in ]>art the nucleus about which an ag- gregate formed. Such nuclei seem in some cases to have governed the growth of the ottrelite. There was a tendency as the mineral formed for the plates to orient themselves parallel to the sericite nucleus, so that when such a nucleus is surrounded by basal ottrelite it is apt to be basal also. Whether this is another example of parallel growth or is acci- dental I cannot state definitely. By far the most abundant interposi- tions are a multitude of extremeW minute black to brown dots and aggregates. With a number 7 objective these are resolved, in the main, into rutile, occurring in knee-shaped and heart-shaped twins, but gen- eralhr in rounded forms, in which twinning is not distinguishable. In other cases the highest objectives are incapable of individualizing the grains, as is mentioned by Renard* In some crystals the rutile is grouped in reticulated lines conforming rather rudely to the planes of the two principal cleavages, but as a rule it is grouped along irregular lines that traverse the ottrelite and the groundmass alike. It may have been arranged originally in structural lines, developed along planes of bed- ding, that afterward were built into the ottrelite with total disregard of any observed relationship, in the same manner that quartz and feldspar droplets were built into albites in another phase of this rock. Other inclusions are graphite (determined by deflagration) and little coffee- brown ilmenite plates (titaneisen glimmer). A powerful current from an electro-magnet applied to that portion of the powdered rock which ran through a 120-mcsh sieve attracted but a little of the particles, so that magnetite and probably ferrous oxide are absent. The usual test for titanium gave a positive reaction. As in biotite and chlorite, pleochroic zones about crystals of zircon are very common in the ottrelite, and their characteristic dependence of maximum pleochroism upon the maximum pleochroism of the enclosing mineral is observable. While zircon usually occupies the centers of these zones, other zones occur having no perceptible associated inclusion."f ♦Researches sur la Composition et la Structure des Phyllades Andennes. Phyllade i »ttrelit6fere do Montherme. Bulletin du Mus6e D'Hist. Nat. de Belgique, vol, 3, 1884-85. p. 252. 1 1 am disposed to refer the brown material making these z ss to minute rutile grains. < ittre- lite containing such zones was subjected to the temperature of a Hansen burner withoul destroy- ing them, so they are probably of a mineralogic nature. OTTRELITE PRISMS. 151 Although twinning with composition face parallel to 0 is not uncom- mon in the ottrelite, a large part of what seems to be twinning is seen to be clue to overlapping plates. As the stage is revolved the wavy extinc- tion caused by this may be observed, — the usual spherulitic structure. Parallel Grouping of ottrelite Prisms. — Examples of crystal growth set up in several places at the same time occur in the rock where each part is controlled by every other, resulting in an irregularly outlined prism com- ix »sed of many individuals separated by areas of the grounclmass and yet all oriented together (see figure 1 ). This phenomenon is unlike that Figure 1. — Thin Section of ottrelite Schist. X 25. Showing formation of ottrelite at many different points. Each small area is oriented with all the others, forming a large area showing a general prismatic outline. The prism has been developed transverse to the sehistosity of the rock. The background is largely gneissic quartz, with some secondary feldspar. (Drawing from mierqphotograph.) of andalusite, which occurs so frequently grown into large individuals, enwrapping all other minerals of the background, but is another exam- ple of independent parallel growth analogous to that of quartz in pegma- tite, although in no way determined by the crystallographic position of the minerals of the groundraass. Such growths are commonly developed nearly at right angles to the layers of quartz and feldspar that make up the sehistosity, and are usually freer from inclusions than the bundles. They occur between the main areas of ottrelite and may represent a 152 ('. I.. WHITTLE METAMOKPHK' ( < > XGLOM EB.ATE. second generation. They were necessarily formed after the groundmass was converted to a mosaic by granulation. Parallel grouping qfrutile (Irani*. — Thesame phenomenon is noticed in the rutile. Little yellowish-brown -rains of this mineral developed in the interspaces of the minerals composing the background tend, although made up of separate and sometimes isolated grains, to orient themselves parallel to one another, forming groups having prismatic outlines. These groups are only sparingly developed, but where observed they are gen- erally parallel to one another* and to the sehistosity of the rock, and are restricted in their occurrence, like the ottrelite individuals just described, to the most quartzose parts of the rock, which they enclose in the same manner as the ottrelite. ALTERATION OF OTT 11 ELITE INTO CHLORITE. Relation of the two Mineral*. — An interlamination of chlorite and ottrel- ite was mistaken at first glance for either the contemporaneous forma- Figuee 2.— Thin Section of Ottrelite. X 50. Showing alteration o( ottrelite to chlorite.— A overlapping plates oi ottrelite; B = bifurcating veins of chlorite allomorphosed after ottrelite and including cores of unaltered mineral ; C'= quartz and feldspar mosaic. (From a microphotograph.) * ( >wing to tin- great single refraction of rutile, their minute size, and tin- fart that they seldom make tin' entire thickness of tin • section, it is difficuN to detect the agreement or disagreement of their crystallographic position. RELATION OF OTTRELITE AND CHLORITE. 153 tion of these minerals or an infiltration of chlorite parallel to the basal cleavage of the ottrelite. Further investigation, however, showed that the chlorite as often traversed the ottrelite irregularly in bifurcating veins and enclosed parts of it (see figure 2). A study of the nature of these veins convinced me that the chlorite is an alteration product of the ottrel- ite. The edges of the veins where they traverse the ottrelite transverse to the basal cleavage are jagged, the saw-like teeth projecting along the composition faces or basal cleavage. The chlorite in such cases is dis- tinctly made up of little fibers which have arranged themselves parallel to one another and to one set of twinning lamella?. lanes of inclusion once continuous in the ottrelite now stop short against interlaminated areas of chlorite, showing the evident secondary nature of the latter min- eral. In other places the chlorite is developed along the basal cleavage of the ottrelite, leaves this cleavage and follows one of the prismatic cleavages, and then again follows the basal cleavage, making one con- tinuous line, thus producing steps, in much the same manner that garnet commonly undergoes this alteration. Optical Characteristics. — Cores of unaltered ottrelite remain in the chlo- rite, and the pleochroic zones, once in the parent, are seen again in the secondary mineral, while the relationship of maximum pleochroism of these zones to the greatest pleochroism of the chlorite is handed down as well. This metasomatic phenomenon has not been observed in other phases of the ottrelite-bearing conglomerate thus far studied by me. GROUNDMASS OF THE BOCK. Mineralogic Constituents. — The background of the rock is composed of quartz and feldspar as principal constituents. Feldspar. — The feldspar is fresh and glass}7, untwinned, and is prob- ably albite, but it is hardly abundant enough in the ottrelite bearing phases to make the rock a gneiss even in mineralogic composition ; and, structurally, a gneissic habit has been nowhere observed where ottrelite exists to any extent. Sericite. — Sericite is also abundant and occurs in minute prisms be- tween the interlocking quartz grains and generally inclosed by the albite but rarely by the ottrelite. It also incloses lines of rutile dots arranged parallel to its cleavage planes, and next to the ottrelite it is the last formed mineral. Anatase. — Associated with rutile in the groundmass are groups of stout and slender prisms and plates having a very high single and double refraction and a variable color, from brownish-yellow to blue, even in the same individual. These I identified as anatase. and for verification I 154 ('. L. WHITTLE — METAMOEPHIC CONGLOMERATE. studied the sections described by Diller.* Unlike the anatase there de- scribed, its occurrence in narrow prisms in this rock, together with its rutile inclusions, seem exceptional. The stouter prisms have terminal laces of an octahedron and range in size from one-fiftieth to three-iiftieths of a millimeter in length. As the stage is revolved the pleochroism seems only the intensification of the inherent color of the mineral — browns becomine: browner and blues becoming bluer. The presence of rutile in- clusions shows the anatase to have formed after that mineral and sug- gests the probability of its being a paramorphic product of the rutile inclusions. Rutile. — Rutile dots and prisms exist in multitudes inclosed by all other minerals of a secondary nature. They are so extremely minute that even in a very thin section they focus in six or more different planes. In General. — All traces of original clastic material in the rock have disappeared ; feldspar detritus, if it once occurred, has been converted into a mosaic of quartz, sericite, biotite and probably albite, and the detrital quartz has been granulated. The existing feldspar is the char- acteristic untwinned glassy variety carrying quartz and serecite inclu- sions so common throughout this horizon, and was formed after the granulation of the rock, since granulation could not have taken place without straining or crushing it. Nearly all the quartz is sprinkled with rutile inclusions, but it is noticeable that the larger areas have less of them and may be cores that have escaped granulation. Its presence, however, in such abundance militates against the probability of any of the quartz being allothegenic and indicates rather its secondary nature. In the same way quartz may inclose plates of micaceous ilmenite, but does not inclose sericite. There is evidence of a second period of this crushing force indicated by a faint wavy extinction in the feldspar in some instances, and by the bending and breaking of ottrelite prisms. ORDER OF CRYSTALLIZATION. We have then in this rock ottrelite, chlorite, feldspar and quartz, and the three titanium-bearing minerals, ilmenite, rutile and anatase. What is their genetic order of development? This is a difficult question to answer without more data, and is particularly difficult in the cases of the ottrelite and rutile. The relative position of the former mineral can be determined easily, but the source of the solution introducing it is not readily discovered. Ottrelite was formed alter the rock had undergone metasomatic and dynamic changes that converted its clastic feldspar into " \ii;it:is .ils l'ni\ ;iiicllmit;s|irve. This second crushing is probably to be cor- related with that which broke the ottrelite prisms in the ottrelite schist. Alteration of clastic Feldspars. — The alteration of detrital feldspars, prin- cipally microcline, to quartz, sericite, biotite and albite is well shown. This change takes place about the edges of the grains, along cleavage planes emphasized by pressure, and along irregular cracks. Lines of in- clusions in the clastic quartz serve to separate it from that resulting from the alteration of feldspar, the latter being always clear and glassy. These are commonly liquid-filled cavities with characteristic gyrating bubbles of carbonate dioxide, but in both the clastic microcline and secondary albite they are even more plentifully distributed. Liquid cavities in the quartz may have, besides the bubble, a single prism of some indetermin- able doubly refracting mineral or an apparent cube, which, however, is also doubly refracting. One of the thin sections (number 699) has a large pebble of microcline, three-fourths of an inch long, which retains its original water-worn out- line, excepting at its ends, where it is partially crushed. Lines of sericite, biotite and quartz traverse it regularly along emphasized cleavage planes and irregularly about grains resulting from granulation. Thousands of minute dots of hematite or limonite are distributed through it, and there is a tendency for them to be arranged in lines normal to the basal cleav- age of the feldspar. It is these that give the flesh color to the mineral in the hand specimen. Other interpositions are numerous rhombs of siderite, exhibiting all stages between the pure mineral and its pseudo- morphous resultant, limonite. These or their limonite representatives occur throughout the rock, but they are noticeably more abundant in the clastic feldspars. Their distribution indicates their formation after the feldspar Avas deposited in the rock, and if this be the case, there Avere two periods of alteration of the microcline — one during Avhich siderite or some iron-bearing carbonate was a stable alteration product under the conditions of environment, and a second during which the carbonate itself changed to limonite, not contemporaneously Avith the development of sericite, but posterior to that change and probably after the rock came under the operation of surface disintegrating influences. Sericite in minute hexagonal plates and prisms terminated by basal planus are scattered through it and seem to have resulted from a direct alteration of the feldspar without the aid of its introduction in solutions from other parts of the rock. Liquid cavities are not nearly so numerous as in the secondary feldspars. The interdependence of the different phases assumed by minerals, KiO ('. L. WIIITTLK -MKTAMOKl'IIK' CONGLOMERATE. upon all the varied factors going to make up their complex environment' and the correlation of these phases oiler, it seems to me. one of the most interesting fields of research to he found in the petrographic and chem- ical history of a rock. Clearing Action of growing Sericite. — Surrounding the pebble and along lines traversing it, as well as about crystals of siderite, there are con- formable zones of microcline free from inclusions of iron ] >r< (ducts. These are associated with the development of siderite and sericite, and, wher- ever lines of movement in the latter mineral traverse microcline or plagio- clase pebbles carrying interpositions, on either side of them there are r ' v •/■ ''•':■ ^x X-\" V&v*-* • SWiSSi ."X ■X y ■X:^:*? s&?* :sf/VWvV Figure 4. — r/iiw Section of microcline Pebble. Showing clearing action of sericite. (Drawing from a microphotograph.) parallel belts from which they have been removed. The border zone of the pebble has its folia of sericite running parallel to it. As the sericite grew as a product of dynamic metamorphism, it acted like a sponge, removing the inclusions and forcing the iron into a new combination, probably biotite. Figure 4 represents a triangular area of microcline illustrating this. In the central part there is an area, a, carrying the usual number of inclusions. Outside of this there is a zone, a', free from iron inclusions: then there is a parallel line of sericite prisms,/*, outside of which there is another parallel zone, c, also free from inclusions, and this is surrounded by the mass of the pebble d. The correspondence of ALTERATION OF THE FELDSPARS. 1G1 the optical orientation, even to the minutest twinned lamellae, is iden- tical on either side of the line of sericite, and the feldspar appears very fresh as compared with that not thus cleared of its inclusions. Its polari- zation colors are much more uniform in the cleared areas, and the greater the amount of the impurities and the more unequal their distribution, the greater the variety of mottled, tinted colors under crossed nicols. In case there are two lines of sericite close together, the interspace may he entirely cleared (see a', figure 5). In attempting to interpret correctly the cause of the outer clear rim about feldspar pebbles only two hypotheses need be considered — it is either secondarily deposited feldspar or is produced by some subsequent action that eliminated the interpositions. If secondary, then the outlines of the feldspar areas having inclusions are too jagged, and concave sur- faces are too common to have been the result of ordinary attrition, while the possibility that the new feldspar was added so as to change their out- line to that of normal pebbles is very improbable. In the case of the largest pebble in the section glassy feldspar accompanied by sericite folia follows the outer part of the pebble for a distance, then penetrate into the interior, following lines of sericite. Bordering areas of the back- ground not containing sericite have no complementary clear zone in the feldspar. Interior lines of sericite and their accompanying dependent zones are only explainable in one way. To assume that they are sec- ondary growths necessitates the subsequent displacement of the feldspar clastic a distance equal to the cleared areas and a consequent probable displacement of its optical continuity. As a matter of fact, all parts extin- guish as a unit, the conformity of the positions of the twinning lamellae on either side of the serecite indicating their original crystallographic and optical continuity. Examples of apparent secondary enlargements of clastic feldspar are becoming so commonly described that it may be well in the future to bear in mind this phenomenon, which simulates so closely that of genuine enlargement and which may have led to misin- terpretations in the past. Alteration of clastic Microcline into Plagloclase. — In connection with the study of secondary feldspars in metamorphic rocks, it is interesting to note the trend of certain phenomena observable in the granulated end of this large pebble mentioned above where secondary albite and clastic microcline are intermingled. Dr Wolff has lately called attention to a possible relationship between detrital areas of feldspar and secondary albites,* and the facts here observed substantiate his interrogative hy- pothesis. With but very few exceptions in the Vermont rocks studied by me have I noticed secondary feldspars free from inclusions of seri- *Metamorphism of Clastic Feldspar in Conglomerate Schist: Bull. Mus. Comp. Zool., \<>l xvi, no. id, p. ls:i. 162 C. L. WHITTLE METAMORPHIC CONGLOMERATE. cite and quartz. These minerals may be distributed throughout the feldspar, but there is a marked tendency for them to occur in groups in the central part, and the outline of groups is rudely conformable to that of the inclosing mineral. An explanation of this phenomenon has never been offered that appears entirety satisfactory. It seems, however, that we must be on the right track if we remember that the minerals, quartz, sericite, biotite and plagioclase, are the commonly recognized products of the decomposition of feldspar that has been subjected to the influence of dynamic forces, while at the same time the presence of quartz, sericite and albite making the groundmass of the rock would be referred at once to such an origin by all who are familiar with the ordinary microscopic phenomena observable in metamorphosed sedi- •mentary rocks. Many feldspars (see those described below from East Clarendon, Vermont) have interpositions of all other minerals occurring in the rock, but the history of their immediate origin and growth is not the same as for those under present consideration. Figure 5 is taken from the granulated portion of the above-mentioned feldspar and exhibits diagrammatically an area under the microscope covered by a number 5 objective : a is a portion of the normal microcline pebble filled with inclusions ; a1, the same, with its interpositions removed by the development of dynamic sericite, i i and k h ; a2, areas of elastic microcline included in secondary plagioclase, c ; and b are minute prisms of serecite grouped in the plagioclases, but impinging against the micro- cline on one side in the upper area. At d are cleavage lines, emphasized by strain, showing abrupt disap- pearance of inclusions along a line corresponding in direction to the basal cleavage in the microcline h h and i i ; e, rhombs of limonite pseudo- morphs after siderite; g, small liquid cavities arranged in lines parallel to lines of hematite inclusions in the feldspar generally ; o, faint traces of the double twinning of microcline occurring in the plagioclase. Two fad a in particular are intended to be brought out : First, the grouping of seri- cite prisms in the center of the lower plagioclase and their contact with the clastic feldspar in the upper; second, the occurrence of isolated areas of microcline in the plagioclase a2 and the conclusions to be drawn there- from. The plagioclase is known to be secondary, as it occupies areas in and includes portions of granulated microcline once continuous. Sericite is developed along the lines h h and i /, which are cleavage partings. The linear area of microcline, a2, which is isolated, is optically oriented with a1 and has been separated from its parent along the basal cleavage. Plagioclase surrounds and traverses it, dividing it into isolated areas, but all oriented with one another. It seems to me that this is a case of pla- gioclase forming about and from an area of microcline. The evidence in favor of this is complete if all the data in the upper plagioclase are taken ALTERATION OF THE FELDSPARS. 163 into consideration. The linear distribution of the microcline inclusion and its optical relation with a are such that it manifestly was once a part of the feldspar pebble. It is improbable that it could have been moved in separate pieces from the line i i without having its crystallographic and optic orientation disturbed. The twinning lamellae of the several parts correspond with one another and with those in a\ while the ex- tinction of c is not in parallelism with either set of twinned lamella? in a2. The plagioclase c, resulting from the alteration of the microcline, Figure 5.— Thin Section of microcline Pebble. Showing alteration of elastic microcline to plagioclase. ramifies through a2, apparently absorbing it, and at the same time caus- ing the development of sericite about and in it. This will be alluded to again when the areas of sericite b are considered. The arrangement of the fluid cavities g1 in lines parallel to the lines of hematite inclusions in the microcline does not seem to be accidental, but seems rather to in- dicate the operation of a grinding influence of the inclusions as the new feldspar formed and absorbed the old. Cleavage lines d, which are par- allel to i i, also seem to be connected in some way with the cleavage in XXIV— Bum. Ueol. Soc. Am., Vol. 4, 1892. 164 C. L. WHITTLE — METAMORPHIC CONGLOMERATE. the pebble, as though the plagioclase, as it replaced the microcline, took on a crystallographic position, controlled by old planes in the latter that had been emphasized by dynamic movements, in which one cleavage is parallel to P or M in the microcline. Along these cleavage lines, at o, there are faint indications of twinning, after the albite and pericline laws. Plagioclase may have replaced old microcline twinning lamellae, itself twinning after the same law, so that we may have the original twinning of the microcline handed down to its alteration product, plagioclase. The upper group of sericite inclusions, b, stops short in a plane against these cleavage lines, extends across the plagioclase to the left, and impinges against the microcline, which at this point is not crushed or strained, while the feldspar on all other sides of the upper area is granulated. Does not the area defined by these inclusions represent original micro- cline, now replaced by plagioclase, the k going into the sericite? So complex have been the conditions of environment that it is very difficult to interpret correctly, if at all, many phenomena exhibited in metamorphosed rocks, but in this case it seems to be legitimate to sup- pose that for a time the conditions were such that, as the plagioclase formed from the microcline, sericite was developed. Afterwards the intro- duction of new factors began. Sericite was no longer developed, while plagioclase continued to form both from the microcline and by addition from other parts of the rock, the growth taking place in all directions ex- cepting where the area of inclusions abuts against the microcline which had escaped granulation. Where this growth took place uniformly in all directions the inclusions are seen to occupy a central group in the plagioclase as in the lower area. The linear area of microcline, cr, with its associated sericite prisms, is an intermediate stage between original clastic feldspar and the completed change b. ' In this connection Dr Wolff remarks : " It does not seem possible to explain all these cases of mere outward growth of the feldspar grains by addition of fresh feldspar of the same species to the core, but rather by an actual replacement of the detrital core by the feldspar of the enlarge- ment."* Strongly contrasted as to immediate origin are the secondary feldspars found in another phase of this conglomerate horizon and those occurring in a phyllite in Massachusetts. CHLORITE SCHIST AND PHYLLITE. Their Plications built into secondary AlbiteS. — The differences in the envi- ronment of growing secondary feldspars and their consequent histories are seen when the above case is compared witli the porphyritic feldspars * Metamorphism of Clastic Feldspar in Conglomerate Schist: Bull. Mus. Com p. Zool., vol. xvi, no. 10, p. 182. CHLORITE SCHIST AND PHYLITE GROUNDMASS. 165 occurring in the chlorite schist found at East Clarendon, Vermont, and the phyllites of Greylock mountain, situated southwest of North Adams, Massachusetts. In the occurrence at the first-named locality the feldspar (albite), which occurs as single individuals or simple twins, a fourth of an inch across, was formed after the rock had been metamorphosed from an original shale to a chlorite schist and mountain-making forces had rear- ranged the minerals composing the rock into minute crenulations. Composition of the Ground/mass. — The groundmass of the schist is com- posed of granular, gneissic quartz and feldspar, much sericite and chlorite marking its foliation, as essential constituents, and as accidental minerals there are innumerable rutile dots and prisms, prisms of tourmaline and little black plates, probably ilmenite. All these, including the minute plications of the schist, have been built into the albite as it grew. Quartz droplets are arranged in sharp serratures, the continuation of the corru- gated lines outside the crystals; but the sericite and chlorite, particu- larly the former mineral, seem to have been eliminated by the growing albite forcing them to one side or by the chemical solution which de- posited the feldspar attacking and dissolving them. The chlorite is occasionally included; the sericite rarely. Rutile, ilmenite and tour- maline are also enclosed. In detail the outlines of the crystals are very jagged, the feldspar projecting in tongues into the background along the schistosity; but, considered as a whole, they are well-defined prisms. The colorless inclusions are by no means limited to quartz, for many give imperfect hyperboke and are secondary feldspars of a younger genera- tion. Nothing now remains in the rock that can be said to be of clastic origin, and certainly after the rock had been converted into a chlorite schist and crenulated, as we find it to-day, no detrital feldspar could have been left to serve as nuclei or furnish material for the large, last-formed porphyritic albites. Solutions with the necessary elements must have been derived from some extraneous source. The occurrence of the albites in the Greylock phyllites collected by Dale and described by Wolff* have much the same history, only secondary albites there have been enlarged by a tertiary growth of the same mineral. The Assuring and occasional faulting of the large albites from East Clarendon is to be correlated with the faulting of the secondary tour- malines and ottrelite prisms above described and indicate a second period of mountain-building forces. My thanks are due to Dr Wolff, who has given me many valuable suggestions during the preparation of this paper. *Ibid., p. 183. Cambridge, Mass., March, 1892. Explanation of Plate 2. Secondary Enlargement of clastic Tourmaline. Figure 1.— Secondary enlargement of elastic tourmaline pebble, showing prismatic planes and slight development of terminal planes. Partially included sericite prisms and occasional inclusions of quartz grains in new growth. Figure 2. — Secondary enlargement of clastic tourmaline. The core is free from interpositions ; the secondary mineral has abundant inclusions of gneissic quartz aud feldspar. Many of the fissures of the core abut abruptly against the new mineral, snowing two periods of straining. The growing tourmaline is seen to have attacked a clastic area of plagioclase, penetrating it irregularly and absorbing sericite previously developed along cleavage lines. (106) BULLETIN OF THE GEOLOGICAL SOCIETY OF AMERICA Vol. 4, pp. 167-178, pl. 3 February 27, 1893 PHASES IN THE METAMORPHISM OF THE SCHISTS OF SOUTHERN BERKSHIRE* BY WILLIAM H. HOBBS {Read before the Society August 16, 1892) CONTENTS Page Introduction 167 Beds represented within the Area 167 Evidences of orographic Disturbances 168 Porphyritic Minerals of the Schists resulting from metamorphic Action 169 The Minerals and their Association 169 Porphyritic Feldspar 169 Granophyre Structure in Feldspar 170 Its Origin 171 Secondary Enlargements of Feldspar 171 Their Origin 173 Garnet and its secondary Enlargements 173 Staurolite 174 Reactionary Rims of Staurolite and Magnetite about Garnet 174 Tourmaline and its secondary Enlargement 175 Porphyritic Biotite 176 Ottrelite. 176 Summary and Conclusions 177 Introduction. Beds represented within the Area. — In southwestern Berkshire county, Massachusetts, and in northwestern Litchfield county, Connecticut, is an area in which non-calcareous schistose rocks alternate with limestones which are in part micaceous, dolomitic, graphitic, pyroxenic, tremolitic or quartzitic.f Though the schists are the "mountain rock," they are found in the valleys as well and are frequently inclosed as islands in * Published with the permission of the Director of the United States Geological Survey. fThe area has been described and mapped by Professor J. D. Dana : On Taconic Rocks and Strat- igraphy, with a Geological Map of the Taconic Region. Am. Jour. Sci., 3d ser., vol. xxix, pp. '205- ■i-ii, pp. 4;;7-M3, pl. ii. XXV— Bum,. Geol. Soc. Am., Vol. 4, 1892. (167) 168 W. H. HOBBS METAMORBHISM OF BERKSHIRE SCHISTS. the limestone. The rocks here described occur in portions of the town- ships of Egremont, Sheffield and Mount Washington, in Massachusetts, and of Canaan and Salisbury, in Connecticut. They have been studied areally and structurally in the field and petrographically in the labora- tory. The full report of the investigation will appear elsewhere.* The area includes three beds of schist separated by beds of limestone, besides the thin layers of the former which are sometimes found within the limestones near the contact. The lowest of these schist beds is asso- ciated with quartzite and gneiss, and is more lacking in uniformity of character than the others. It incloses numerous veins of coarse pegma- tite and is specially rich in tourmaline, though this mineral is also found in the two other horizons. The next younger schist is separated from the one just mentioned by a dolomite, which is always very crystalline, and at many localities con- tains white pyroxene, tremolite or phlogopite. It moreover contains layers of graphitic rock and of canaanite.f The schist horizon itself is quite variable in character, but is frequently distinguished by the occur- rence of macroscopic garnets and staurolite. The upper schist bed is separated from the last mentioned by a lime- stone in which neither sahlite, tremolite nor canaanite has been found. The schist itself is free from the macroscopic garnets and staurolite characteristic of the central bed. In common with both the other beds it contains porphyrinic crystals of feldspar, but here they seem more generally to have glistening cleavage surfaces. Especially in the Mount Washington area this bed shows facies that are quite sericitic or chloritic, the latter with magnetite often in octahedra as big as a pea. Ottre- lite, though not restricted to this horizon, is more frequently found here than in either of the others. Though the rocks of the three non-calcare- ous beds have a preponderance of feldspar, they are structurally schists and they are so designated, as it is convenient to distinguish them from typical gneisses in adjacent territory. Notwithstanding characteristic differences can be pointed out, serving to distinguish the three beds when regarded as units, individual hand specimens from each often show re- semblances more striking, so that it is generally impossible to refer a specimen to a definite bed on the basis of petrographic character only. Evidences of orographic Disturbances. — Typically metamorphie minerals abound in all beds, but especially in the central schist bed and the dolo- mite underlying it. The beds have been thrown into sharp folds, most frequently reversed, with resulting shear planes and secondary foliation at many localities. *The work here referred to forms part of an investigation conducted by Professor Raphael Pumpelly for the United States Geological Survey, t American Geologist, vol. xv, 1892, p. 45. porphyritic constituents of the schists. 169 Porphyritic Minerals of the Schists resulting from metamorphic Action. The Minerals and their Association. — It is my object in this paper espe- cially to describe the so-called porphyritic constituents of the schists that have been developed or modified by metamorphic agencies. Under this head are included feldspar (largely an acid plagioclase), garnet, stauro- lite, tourmaline, biotite and ottrelite. Other Constituents present in greater or less quantity are sericite. quartz, graphite, chlorite, magnetite, ilmenite, pyrite, nbrolite, calcite, rutile. sphene (and leucoxene), zircon and apatite. In nearly all specimens there is a matrix made up of vary- ing amounts of feldspar, quartz and a micaceous mineral, which is in some cases a silvery mica (sericite) ; in other instances sericite with bio- tite or chlorite. Associated with these minerals are accessory graphite, ore material, etc. Almost without exception porphyritic feldspars occur in the matrix, usually many times larger than the feldspar grains com- posing it.* In addition to the modifications of the rock arising from the micaceous constituents present, petrographic variations consist mainly in the character of the porphyritic feldspar and in the presence or absence of the other porphyritic constituents, viz: garnet, staurolite, tourmaline, biotite and ottrelite. The central schist bed has furnished most of the specimens in which the structures I shall describe were observed, though such structures do not seem in all cases to be restricted to that bed. Porphyritic Feldspar. — The porphyritic feldspars appear under a num- ber of modifications. In certain facies of the rock they are more or less oval in shape and inclose with more or less uniformity blades of seri- cite, particles of graphite, ore material or tourmaline. They are com- monly either simple individuals or simple twins. They quite resemble in sections the beautiful photomicrograph which is figure 8 of the paper by AVolff on "The Metamorphism of Clastic Feldspar in Conglomerate Schist." f Though these feldspars may show no marked evidences of strain, many instances of polysynthetic twinning have been observed, and the occasional localization of the lamella? about cracks in the individual would indicate that the twinning is the result of internal mechanical movement. The twin lamella1 allow of the determination of the feldspar as an acid plagioclase. Dynamic metamorphism lias at other localities been more intense, as evidenced in sections where the granulation of the feldspars may be * See descriptions of similar feldspars in the schistose and conglomeratic rocks of lloosao moun- tain and elsewhere. (Pumpelly: The Relation of Secular Rock-Disintegration to Certain Transi- tional Crystalline Schists. Bull. Geol. Soc. Am., vol. ii, 1891, pp 209-224. Wolff: Metamorphism of Clastic Feldspar in Conglomerate Schist. Bull. Mus. Comp. Zool., vol. xvi,1891, pp. 173-183, pis. i-ii.) t Bull. Mus. Comp. Zool., vol. xvi, 1891, pp. 173-183, pis. i-ii. 170 W. H. HOBBS — METAMORPIIISM OF BERKSHIRE SCHISTS. seen. This may be largely peripheral, as in a specimen (number 3230) * from near Ore Hill, or it may include nearly the entire crystal, as in a number of thin sections (number 3224) from Miles mountain. Such pronounced granulation seems, however, to be most developed in the vicinity of shear planes, and is accompanied by a stretching and tearing of the other constituents. Figure 1, A shows the effect of this action on two adjacent garnets (number 3230). Granophyre Structure m Feldspar. — Those structures which 1 desire here more especially to emphasize, however, seem to be found farther removed from shear planes, and concern phases of metamorphism where mechan- ical movement has been a minimum. In such localities the feldspars have frequently a mottled appearance, like D in figure 1 (numbers 3111, 3326, 3328, 3463). __s C- Figure 1.— Examples of Deformation and modified Growths of Minerals in Schists. A = stretched garnets. B = secondary growth of tourmaline ; the oval core has brown tones, the enlargement blue or plum tones; the cloud}7 material near the junction is probably graphite. C= zonal structure in tourmaline. D = mottled feldspar. E = parallel growth of ilmenite and chlorite. The included areas sometimes take the form of curving canals, at others polygonal outlines, and, in short, exhibit all the peculiarities of the micropegmatite or granophyre structure. Hexagonal outlines char- acterize many of the areas, and there can be little doubt that they are in these cases quartz (number 3463). The inclosed quartz extinguishes alike over considerable areas, but sometimes shows several orientations within a single crystal of feldspar .f The feldspars which show this structure exhibit in many cases the min- imum of crushing and but little effect of stress, while in other cases the granophyre structure coexists with a pronounced granulation and exhi- bition of secondary twinning. In the latter ease the structure is very complicated, and it is difficult to distinguish the secondary quartz from the mosaic of feldspar, it was frequently observed (in those cases where but little deformation could be made out) that the granophyre occupies the center of a crystal, leaving a clear rim. *The numbers of sections are those of the Uniti'.l States Geological Survey collection. •f-Cf. Iddings, Obsidian Cliff, Yellowstone National Turk . Seventh Ann. Rep. V. 8. God Sur., 1888, p. 275, plate xv, fig. 5. ORIGIN OF THE GRANOPHYRE STRUCTURE. 171 Its Origin. — The question of the origin of the granophyre in these doubt- less clastic rocks is a difficult one. It is a question that deserves further study, and I hope later to be able to throw a little more light on the problem. For the present it can be said that the relation of the inter- grown quartz to the quartz outside, as exhibited in a number of sections lends no support to the view that the granophyre structure has been pre- served from some detrital grains which have an igneous origin, but that it is of a secondary nature, being developed in the already formed rock. The usual interpretation of granophyre structure to indicate an igneous origin for the rock in which it occurs is no longer tenable. Irving in 1883* described micropegmatite in a number of granitic porphyries and augite syenites from Lake Superior, the secondary nature of which was evident from its quartz being oriented like the areas of secondary quartz lying without the feldspars. Sornewhat similar cases have been described by Judd.f In a recent memoir by Julius Romberg^ on the petrographic characters of an extensive series of Argentine granites the granophyric structures are described in much detail with the aid of beau- tiful plates. The author raises the question of their secondary origin through weathering, and adduces many facts which make it probable that this is their origin. In some of the feldspars which show the mottled structure in the rocks now under consideration it can be determined that the inclosed areas are feldspar of a somewhat different composition (microperthite structure). This is particularly well shown in the instance of a feldspar core having a rim which polarizes yellow, the core polarizing gray. A set of fhottlings in the core give the same yellow tint as the rim and extinguish with it. This would seem to show that the original feldspar core had been partially replaced by a feldspar of different composition, which composes the rim entire. This view is quite in harmony with Wolff's deductions concerning the feldspars in the conglomerate schist of Hoosac mountain.|| Secondary Enlargements of Feldspar. — Secondary enlargements of feld- spar seem to be quite common in the rocks under investigation, and they have been found at localities widely separated. § Occasionally these en- *The Copper-bearing Rocks of Lake Superior: Monograph V, U. S. Geol. Survey, 1883, p. 114, plates xiv, xv. f On the Growth of Crystals in Igneous Rocks after their Consolidation : Quart. Journ. Geol. Soc. vol. xlv, 1889, pp. 175-18G. pi. vii. Ibid., vol. xlii, 1886, p. 72. X Romberg, Petrographische Untersuchungen an argentinisehen Graniten,.mit besonderer Be- rucksichtigung ihrer Structur und der Entstehung derselben : Neues Jahrbuch f. Mineralogie, etc., Beilage-Band viii, 1892, pp. 314-323, 374-378, plates ix-xii. !| Loe. cit. See also Lehmann, Jahresbericht der Schlesischen Gesellschaft fi'ir Vaterlandische Cultur, 1880, pp. 119-120. ttrelite and [lraenite Schist in New England : Bull. Mus. Comp. Zoo)., vol. xvi, 1890, pp. 159-165. I An < ittrelite-bearing Phase of a Metamorphic Conglomerate in the Green Mountains : Am. Jour. Sci., 3d sci-., vol. xliv, 1892, pp. 274-275. |1 Etude* sur l'origine de l'Ottrelite, ire Etude, I'Ottrelite dans 1'' Salmien superieur: Ann. Sor. Geol. Nord, Lille, vol. xv, L888, pp. L85-318. SUMMARY AND CONCLUSIONS. 177 show that a general movement occurred in the rock subsequent to the formation of the ottrelite, tending to bring the ottrelite crystals parallel to the schistosity. Professor Gosselet ascribes the development of the ottre- lite to heat, of which the cause is unknown* The spaces left behind the mineral by its movement become filled either at the time or subsequently by muscovite, quartz and oxide of iron, giving rise to peculiar tufts going- out from the mineral. Besides the crystals of ottrelite, M. Gosselet de- scribes with great care in the same rocks somewhat irregular rounded areas (noyaux) of cloudy, in part doubly refracting, material, surrounded by one or more zones, differing in some respects from the core, which he believes to be the remains of more elementary forms of ottrelite rather than crystals — globulites. Summary and Conclusions. From the foregoing, it may be asserted with much probability that the minerals of a porphyritic nature which occur in the schists, viz., feldspar, garnet, staurolite, tourmaline, biotite and ottrelite, were developed in originally clastic rocks as a result of the orographic disturbances to which they have been subjected. Internal mechanical movement seems to have played only a subordinate role in their formation, as shearing brings about a crushing and tearing of the constituents not generally observable in the sections. The development of the porphyritic constituents seems therefore to be due to a partial recrystallization of the rock as a result of what I would call static metamorphism — i. e., metamorphism in which pressure is the important factor, in contrast to internal movement, though heat and a mineralizer were important adjuncts. The universal dis- tribution of the porphyritic feldspars might indicate that they require a less intense metamorphism for their development than do garnet and staurolite, and this is probably true, though it cannot be asserted that some of these feldspars are not detrital grains like a portion of those de- scribed by Wolff.f Evidence has been given to show that the garnet developed largely before the staurolite, and that the latter probably re- quires for its formation more intense metamorphic action. The stauro- lite crystals have been developed, at some expense to the garnet, for iron, and probably also alumina and silica. This is shown by the crown of staurolite crystals about garnet in the June mountain schist. This fact, taken in connection with the secondary enlargements of feldspar, garnet, and tourmaline, and the probability of enlargements in the case of stauro- lite, indicates that the metamorphism which these schists have suffered *" La formation de Pottrelite est du a une production de chaleur dont il faudra chercher la cause." Loc. cit., p. 203. fBulI. Mus. Comp. Zool., vol. xvi, 1891, p. 17.">. 178 W. II. HOBBS — METAMORPHISM OF BERKSHIRE SCHISTS. was not a continuous process, but occurred in stages, of which there must have been several. It was in one of the later of these stages that the staurolite was developed. The importance of the enlargement of mineral fragments in clastic rocks as a factor in their alteration by metamorphism, has been empha- sized by Irving and Van Hise in their papers on the rocks of the Lake Superior region. This study presents a somewhat different phase of the subject and adds an instance of their occurrence in rocks which have been more profoundly metamorphosed. The investigation here outlined is not completed. The interesting problems of the chemical nature of the reactions involved in the development of the feldspars and their secondary enlargements, and of the other porphyritic constituents, will require for its solution a separation and chemical examination of the dif- ferent constituents. In conclusion, I would acknowledge my indebtedness to Dr G. H. Williams and Dr J. E. Wolff for valuable suggestions and criticism. Explanation of Plate. Sections of garnetiferous porphyritie Schist from the southeast Slope of Mount Washington, showing secondary Growths of Feldspar. Locality (number 3104) on road between Joyceville and Plantain Pond. Figure 1. — A = Secondary growth of feldspar, of which the core has a rounded outline. B = Feldspar growth with two distinct enlargements indicated by different extinction angles. The core has a micropegmatite structure. Crossed nicols. X 77. Figure 2. — A = Simply twinned feldspar core with an untwinned enlargement. Crossed nicols. X 48. BULL. GEOL. SOC. AM. VOL 4, 1892. PL. 3. SECTIONS OF GARNETIFEROUS PORPHYRITIC SCHIST. BULLETIN OF THE GEOLOGICAL SOCIETY OF AMERICA Vol. 4, pp. 179-190 February 27, 1893 CONTINENTAL PROBLEMS Annual Address by the President, G. K. Gilbert (Read before the Society December 30, 1892) CONTENTS Page Introduction 179 Differentiation of continental and oceanic Plateaus 180 Rigidity versus Isostasy 182 Nature of density Differences 183 What caused the continental Plateau? 183 Why do continental Areas rise and fall? 186 Are Continents permanent? 187 Do Continents grow ? 187 Summary 190 Introduction. — For a decade attention has been turned to the continents. Through the distribution of animals and plants Wallace has studied the history of the former connection and disconnection of land areas. Theo- ries of interchange of land and water have been propounded by Suess and Blytt. By means of geodetic data Helmert has discussed the broad relations of the geoid to the theoretic spheroid. Darwin has computed the strength of terrestrial material necessary to sustain the continental domes. James Geikie, treating nominally of coast lines, has considered the shifting relations of land and sea, and a half score of able writera have debated the question of continental permanence. The American Society of Naturalists, now holding its annual meeting at Princeton, N. J., devoted yesterday's session to the consideration of such evidences of change in the geography of the American continent as are contained in the distribution of animals and plants. The intercontinental congresses auxiliary to the World's Fair next summer are to be devoted to the dis- cussion of continental and intercontinental themes ; and a committee, at the head of which stands one of our vice-presidents, invites the geologists of the world to assemble for the consideration of those broader questions of earth structure and earth history which affect more than one hemi- XXVII— Bull. Gkol. Soc. Am., Vol. 4, 1892. (179) 180 G. K. GILBERT — CONTINENTAL PROBLEMS. sphere. This occasion, too, in which, after three years' sojourn in the land of the raccoon and 'the opossum, we return to the land of the sable and the beaver, brings forcibly to mind the continental extent of our society and its continental field. It is not strange, then, that the conti- nents have seemed to me a fitting theme of which to speak to you to-day. Realizing not only the breadth and grandeur, but the inherent difficulty of the subject, I do not hope to enlarge the contribution the decade has made, nor shall I attempt to summarize it ; neither is it my desire to anticipate the discussions of the World's Fair congress. It is my pur- pose, rather, to state, as clearly as I may, some of the great unsolved problems which the continents propound to the coming intercontinental congress of geologists. Differentiation of continental "n'l oceanic Plateaus. — It is one of the para- doxes of the subject that our ideas as to the essential character of the ♦ 30,000 FT.r- ♦ 20.000 FT. ♦ I0.000 FT. SEA LEVEL I 0,000 FT. 2 0,000 FT. ■30,000 FT. CONTI NENTAL PLATEAU OCEANIC PLATEAU Figure \.— Generalized Profile, showing relative Areas of the Earth's Surface at different Heights and . Depths. continents have been greatly modified and clarified by the recent explo- ration of the sea. The work, especially, of the " Challenger " and the " Blake " in delineating and sampling the bottom of the ocean has given new definitions, not only to the term " deep sea," but also to the term " continent," as they are employed by students of terrestrial mechanics and of physical geography. To the continental lands are now added the continental shoals, and the depth of the deep sea is no longer its sole characteristic. Look for a moment at this generalized profile of the earth's surface. It expresses in a concise way the relations of area to altitude, and of both to the level of the sea. Murray, to whose generaliza- tions from the "Challenger" dredgings and soundings the student of continents owes so much, has computed, with the aid of the great body of modern data, the areas of land and ocean bed contained between cer- CONTINENTAL AND DEEP SEA PLATEAUS. 181 tain contours, fourteen in number * and from his figures I have con- structed the profile. Vertical distances represent heights, and horizontal distances represent terrestrial areas. The full width of the diagram from side to side stands for the entire surface of the earth. The striking feat- ures of the profile are its two terraces or horizontal elements. Two-fifths of the earth's area lies between 11,000 and 16,000 feet beneath the ocean, constituting a vast submerged plateau, whose mean altitude is — 14,000 feet. This is the plateau of the deep sea. One-fourth of the earth's area falls between the contour 5,000 feet above tbe ocean and the contour 1,000 feet below, and has a mean altitude of + 1,000 feet. This is the continental plateau. The two plateaus together comprise two-thirds of the earth's surface, the remaining third including the intermediate slopes, the areas of extreme and exceptional depth, and the areas of extreme and exceptional height. Thus in the broadest possible way, and in a manner s s Figure 2.— The continental Plateau as related to the Western and Eastern Hemispheres. practically independent of the distribution of land and water, we have the ocean floor clearly differentiated from the continental plateau. It is at once evident that for the discussion of the greater terrestrial problems connected with the configuration of the surface, and especially of the problems of terrestrial mechanics, we must substitute for the continents, as limited by coasts, the continental plateau, as limited by the margins of the continental shoals. It does not follow from the profile, which, as I have said, represents only the relation of extent to altitude, that all districts of continental plateau are united in a single body, and in point of fact they are net completely united; but the greater bodies are brought together, and the only outlying district is that of the Antarctic continent. Running a line * John Murray: On the height of the land and the depth of the ocean. Scottish Geographical Mag., vol. iv, 1888, p. 1. 182 G. K. GILBERT — CONTINENTAL PROBLEMS. along the edge of the continental shelf where a gentle slope is exchanged for a steep one, and passing freely, as occasion may require, from the coast down to the line of 1,000 fathoms, a continental outline is produced in which North America and Eurasia are united through the shoals of the Arctic ocean, and in which Australia and the greater islands of the East Indies are joined to southwestern Asia. Antarctica alone stands separate, being parted from South America by a broad ocean channel, imperfectly surveyed as yet, but believed to have a depth of between 1,000, and 2,000 fathoms. The lower plateau, or the floor of the deep ocean, is less continuous, being separated by tracts of moderate depth into three great bodies, coinciding approximately with the Pacific, Atlan- tic and Indian oceans. Rigidity versus Isostasy. — The first of our continental problems refers to the conditions under which the differentiation of the earth's surface into oceanic and continental plateaus is possible. How are the continents supported ? Every part of the oceanic plateau sustains the weight of the superjacent column of water. At the same level beneath the conti- nental plateau each unit of the lithosphere sustains a column of rock both taller and denser than the column of water, and weighing about three times as much. The difference between the two pressures, or the differential pressure, is about 12,000 j:>ounds to the square inch, and this force, applied to the entire area of the continental plateau, urges it down- ward and urges the oceanic plateau upward. Referring again to the dia- gram in figure l,the entire weight of the continental plateau, pressing on the tract beneath it, tends to produce a transfer of material in the direc- tion from left to right, resulting in the lowering of the higher plateau * and the raising of the lower. To the question, how this tendency is counteracted, two general answers have been made : first, that the earth, being solid, by its rigidity maintains its form ; second, that the materials of which consist the continental plateau and the underlying portions of the lithosphere are, on the whole, lighter than the materials underlying the ocean floor, and that the difference in density is the complement of the difference in volume, so that at some level horizon far below the sur- face the weights of the superincumbent columns of matter are equal. The first answer regards the horizontal variations of density in the earth's crust as unimportant; the second regards them as important. The first may be called the doctrine of terrestrial rigidity ; the second has been called the doctrine of isostasy. At the present time the weight of opinion and, in my judgment, the weight of evidence lie with the doctrine of isostacy. The differential pressure of 12,000 pounds per square inch suf- fices to crush nearly all rocks, and it may fairly be questioned whether there are any rock masses which in their natural condition near the sur- CRUST AL DENSITIES. 183 face of the earth are able to resist it. The samples of rock to which the pressures of the testing machine are applied have been indurated by dry- ing ; but it is a fact familiar to quarrymen that rocks in general are softer as they lie in the quarry below the water-line than after they have been exposed to the air and thoroughly dried. It is probable, therefore, that rocks lying within a few hundred or a few thousand feet of the surface are unable to resist such stresses as are imposed by continents. At greater depths we pass beyond the range of conditions which we can reproduce in our laboratories, and our inferences as to physical conditions are less confident. The tendency of subterranean high temperatures is surely to soften all rocks, and the tendency of subterranean high pressures is prob- ably to harden them. It is not known which tendency dominates; but if the tendencies due to pressure are the more powerful, we are at least assured by the phenomena of volcanism that their supremacy admits of local exception. Nature of density Differences. — If we accept the doctrine of isostasy and regard the material under the continents as less dense than that under the ocean floors, the question then arises whether the difference in den- sity is due merely to a difference in temperature or whether it arises pri- marily from differences in composition. This, which may be called the second problem of the continents, is so intimately related to the one which follows that we may pass it by without fuller statement. What caused the continental Plateau ? — The problem of the origin of the continents remains almost untouched. Those who have propounded theories for the formation of mountain ranges have sometimes included continents also, but as a rule without adequate adaptation to the special conditions of the continental problem. So far as I am aware, the subject has been seriously attacked only by our second president, Professor Dana. He postulates a globe with solid nucleus and molten exterior, and pos- tulates, further, local differences of condition, in consequence of which the formation of solid crust on the liquid envelope was for a long period confined to certain districts. In those districts successive crusts were formed, which sunk through the liquid envelope to the solid nucleus, and by their accumulation built up the continental masses. The re- maining areas were afterward consolidated, and sul >s<>< |uent co< >ling shrunk the ocean beds more than it shrunk the continental masses because their initial temperatures (at the beginning of that process) were higher.* That the philosophic mind may find satisfaction in this explanation, it appears necessary to go behind the second postulate and disc-over what were the conditions which determined congelation in certain districts long before it began in others. Can it be shown that the localization of * James P. Daua: Manual of Geology, 2d edition, New York, 1874, p. 738. 184 G. K. GILBERT — CONTINENTAL TROBLEMS. congelation, having been initiated by an otherwise unimportant ine- quality, would be perpetuated by any of those cumulative processes which are of such importance in various departments of physics ? And can it be shown that such a process of continent-building would segre- gate in the continental tract certain kinds of matter, and thus institute the conditions essential to isostatic equilibrium? To the first of these questions no answer is apparent, but I incline to the opinion that the second may be answered in the affirmative. If we assume the liquid envelope to consist of various molten rocks arranged in the order of their densities, and if we assume, further, that their order of densities in the liquid condition corresponds to their order of densities in the solid con- dition, then the successive crusts whose heaping built up the continents would all be formed from the lightest material, and the isostatic condi- tion would be satisfied. It was the fashion of the last generation of physical geographers to study the forms of continents as delimited by coasts, seeking analogies of continental forms with one another, and also with various geometric figures, especially the triangle. The generalizations resulting from these studies have not yielded valuable ideas, and the modern student is apt to smile at the effort of his predecessor to discover the ideal geometric figure where the unbiased eye sees only irregularity. But barren as were those studies I am not satisfied that their method was faulty ; and as a physiographer I have such appreciation of the ideas that sometimes grow from studies of form that I have attempted to apply the old method to the new conception of the continental plateau. Confessing in advance that my only result has been negative, I nevertheless recite what I have done, partly because negative contributions to an obscure subject are not entirely valueless, and partly with the thought that the forms whose meanings I failed to discover may nevertheless prove significant to some other eyes. What I did was to draw upon a globe the outline of the continental plateau and then view it from every direction. Afterwards I developed the figure upon a plane surface, employing for that purpose a mode of projection which is probably novel. As this mode is not susceptible of mathematical formulation, and therefore will not find place in the litera- ture of cartography, I may be pardoned for applying a trivial name and calling it the orange-peel projection. The name almost explains it. Con- ceive the continental plateau to be outlined upon a spherical orange and the rind of the orange to be divided by a sharp knife along the sinuosi- ties of the outline; conceive then that the portion of the rind thus cir- cumscribed is peeled from the orange and is spread upon a flat surface, the different parts being stretched and compressed so as to pass from A STUDY IN FORM. 185 spherical form to plane with the least strain of the rind. The resulting shape is delineated in figure 3. Figure 4 shows the form assumed by the complementary part of the orange peel, which represents, of course, that portion of the ocean outside the continental shoals. In each diagram Figure 3. — The continental Plateau, developed on a plane Surface. the positions of the poles, north and south, are represented by the letters N and S. From the study of these figures, and especially from their study as delineated on the globe, it appeared possible that a portion of the continental plateau might belt the earth as a great circle. The dis- covery of such a belt would be important, for by assuming that it was N Figure I. — Oceanic Area complementary to the continental Plateau, developed on a plane Surface. originally equatorial we might be led to new hypotheses of continental development. In a rotating liquid sphere the only differentiation of sur- face condition we can readily conceive is that between equatorial and polar regions, and if such differentiation were sufficient to cause or local- 1SG G. K. GILBERT CONTINENTAL PROBLEMS. ize continental elevations, then these elevations would constitute either two polar tracts or else an equatorial belt. Moreover, I have been in- duced by recent studies of the physical history of the moon to suspect that the earth may at one time have received considerable accessions from without, and that these accessions were made to the equatorial tract. If these suspicions are well founded, peculiar characters may have been given to a tract having the form of a belt. So for a double reason I was led to compare the outline of the continental plateau with a great circle- To this end a great circle was chosen, coinciding as nearly as possible with the line of greatest continental extension, and the projection was so •modified as to render the locus of that great circle a straight line. The result appears in figure 5, where the straight line is the projection of the hypothetic ancient equator; and j-ou will probably agree with me that it gives little support to the suggestion that the principal line of conti- nental elevation was originally equatorial. Figure 5. — Area of continental Plateau, developed with Reference to a great Circle. Why do continental Areas rise and fall f — A fourth problem refers to con- tinental oscillations. The geologic history of every district of the land includes alternate submergence under and emergence from the sea. To what extent are these changes due, on one hand, to movements of the sea and, on the other, to movements of the land, and what are their causes? With American geologists the idea, recently advocated, that the chief movements are those of the ocean finds little favor, because some of the most important of the changes of which we are directly cognizant are manifestly differential. Our paleozoic map pictures a sea where now are Appalachian uplands, and uplands where now are low coastal plains and oceanic waters. In Cretaceous time the two margins of what are now the Great Plains had the same height, or at least the western margin was no higher than the eastern ; but now the western margin lies from four thou- sand to six thousand feet above the eastern, and the intervening rock mass appears to have been gently tilted without important internal dis- tortion. Such geographic revolutions are not to be explained by the shifting of the hydrosphere nor by its dilatation and contraction. Neither can they be ascribed to isostatic restoration of an equilibrium deranged OSCILLATION, PERMANENCE, GROWTH. 187 through the transfer of masses by erosion and sedimentation, for that hypothetic process is essentially conservative. Neither is it easy to be- lieve that the two margins of the plains have differed, since the Creta- ceous, to the extent of one mile in their radial contraction due to secular cooling of the globe ; nor is it easy, at least for the disciple of isostasy, to believe that such a change can have resulted from the localization of deformation consequent on the slowing of the earth's rotation. Each of these processes may have been concerned, but I conceive that the essen- tial factor still awaits suggestion. Our knowledge of surface processes, as compared to subterranean, is so full that the field of plausible epigene hypotheses may be exhausted, but the vista of hypogene possibility still opens broadly. Are Continents permanent ? — The doctrine of the permanence of the con- tinental plateau, enunciated long ago by Dana and more recently advo- cated, with a powerful array of new data, by Murray and Wallace, has made rapid progress toward general acceptance. Nevertheless its course is not entirely clear, and among the obstacles still to be overcome is one whose magnitude is perhaps magnified for the American student by prox- imity. All who have studied 1 iroadly the stratigraphy of the Appalachian district have concluded that the sediments came chiefly from the east; and the detailed Appalachian work of the past decade is disclosing a complicated history, in which all chapters tell of an eastern paleozoic land, and some chapters seem to testify to its wide extent. At some times the western shore of this land lay east of the site of the Blue Ridge, and there is serious doubt whether the existing belts of coastal plain and submerged continental shelf afford it sufficient space. For the present, at least, the subject of continental permanence must be classed with the continental problems. Do Continents grow? — According to my own view, there is yet another, a sixth, continental problem deserving the attention of the World's Fair intercontinental congress. We have been told by the masters of our science, and their teaching has been echoed in every text-book and in every class-room, that through the whole period of the geologic record the continents have grown ; not that the continental plateaus have been materially extended, not that the pendulum has moved always in one direction, but that the land area has, on the whole, steadily increased. From this doctrine there has been no dissent — and possibly there should be no dissent — but the evidence on which it is founded appears to me so far from conclusive that I venture to doubt. The evidence employed consists partly in the general distribution of formations as shown by the geologic map and partly in inferences drawn from certain formations which contain internal evidence that they orig- XXVIII-Bull. Geol. Soc. Am., Vol. 4, 1892. 188 G. K. GILBERT — CONTINENTAL PROBLEMS. inated on coasts. With the aid of such data are drawn the outlines of ancient ocean and land at various geologic dates, and from the compari- son of these outlines continental growth isinferred. In passing from the formation boundaries of the geologic map to the oceanic limits of the charts of ancient geography, allowance is made for the former extent of non-littoral formations beyond their present boundaries. Tins allowance is largely conjectural, and the range of possible error is confessedly great. In passing from the observed limits of littoral formations to the coast lines of ancient geography little or no allowance is usually made for the former extent of the formations, and I conceive that great possibility of error is also thus admitted. During a period of oceanic transgression over the land all portions of the transgressed surface are successively coastal, and the coastal deposits they receive are subsequently buried by off-shore deposits. When, therefore, littoral beds are found in remnants of strata surviving the processes of degradation, it is indeed proper to infer the proximity of ancient coasts during their formation, but the in- ference that they represent the limit of transgression for that epoch may be far from the truth. For these reasons it appears to me that the spe- cific conclusions which have been reached with reference to the original extent of various formations are subject to wide uncertainties; and if this be granted, then but brief attention to a simple law of denudation is necessary to show that the general conclusion may be illusory. The process of degradation by aqueous agencies is chiefly regulated, not by the thickness of formations, hut by the height to which they are uplifted. Thus the present extent of most formations is determined in large part by crustal oscillations subsequent to their deposition. As formations are progressively eroded, the underlying and older cannot be attacked until the overlying and younger have been carried away, and so the outcrops of the older of necessity project beyond the boundaries of the younger. The process of vague inference, making indefinite allowance for the un- known quantity of eroded strata, nearly always assigns to the older for- mation, which projects visibly beyond the newer, a greater original extent. It appears to me thus possible that the greater part of the data from which continental growth is inferred maybe factitious and mislead- ing. Furthermore, inference, such as it is, deals with only one phase of the problem. It is applied to the incursions of the sea upon the land, but it is not applied to the excursions of the land upon the sea. Just as we infer from stratified rocks the presence of the sea, so also we infer from unconformities the sea's absence; and to the student of ancient geography the two classes of evidence are equally important. But the strata, spread widely over the surface of the land, are conspicuous phenomena, while DO CONTINENTS GROW? 189 unconformities are visible only here and there and are usually difficult of determination. For this reason the data from unconformity have never been assembled. Essays toward ancient geogra | >1 iv have dealt only with the minima of ancient land, never with its maxima, and the ques- tion of continental growth cannot be adequately treated while half of the history is ignored. We may borrow a figure from the strand of a lake. As the waves roll inward, each records its farthest limit by a line upon the sand, and each obliterates all previous wave lines which it overpasses. The observer who studies the transient record at any point may find a series of lines, of which the highest is the oldest and the lowest is the newest, and he may infer that the lake level was higher when the first wave left its trace, and that the water is receding from the land. But if he continue his observations through many days and fix monuments to record from time to time the lowest land laid bare between the waves, he may dis- cover that the highest wave line and the lowest record of ebb correspond in time with the play of the largest waves, and that the lowest wave line and the highest record of ebb correspond to the play of smaller waves, and thus reach the conclusion that the lake level has remained unchanged. In the study of Time's great continental strand Ave are not even able to observe directly the wave lines of rhythmic transgression, but infer their positions from data often ambiguous, and of the lower wave limits, the lines of maximum regression, we are absolutely ignorant. It may be true that it priori considerations afford a presumption in favor of continental growth, but such presumption should not be per- mitted to give color to evidence otherwise neutral ; and, moreover, it is not impossible to discover an a priori presumption in favor of continental diminution. Assuming that hypogene agencies cause continental areas to rise above the ocean, the work of epigene agencies constantly tends to remove the projecting eminences and deposit their material about their margins, so as to extend the area of the continental plateau. Thus we have a strong a priori presumption in favor of continental growth. On the other hand, if we admit the principle of isostatic equilibrium, then the continental eminences have low density ; and as they are worn away by epigene processes the material which rises from below to restore them has greater density and maintains a somewhat less altitude. The pro- cess of isostatic restoration tends thus toward the permanent leveling of continents, and if the hypogene initiative should cease the continents would ultimately be reduced to ocean level, and finally, through pro- cesses of solution, to a level below the ocean ; so, assuming the initiative processes of the under earth to be of finite duration, the work of terres- trial degradation, combined with isostatic restoration, should afford a 190 G. K. GILBERT — CONTINENTAL PROBLEMS. continental history characterized in an earlier stage by growth and in a later stage by decadence. In our ignorance of subterranean forces we should use such a priori considerations only as a means for the sugges- tion of hypotheses. As they have doubtless served to promote the theory of continental growth, they should also he permitted to indicate the pos- sibility of continental retrogradation. Summary. — The problems of the continents have been touched to-day so briefly that a summary is almost superfluous. The doctrine of isos- tasy, though holding a leading position, has not fully supplanted the doctrine of rigidity. If it be accepted, there remains the question whether heat or composition determines the gravity of the ocean beds and the levity of continents. For the origin of continents we have a single hy- pothesis, which deserves to be more fully compared with the body of modern data. The newly determined configuration of the continental mass has yielded no suggestion as to its origin. The cause of differential elevation and subsidence within the continental plateau is unknown and has probably not been suggested. The permanence of the continental plateau, though highly probable, is not yet fully established ; and the doctrine of continental growth, though generally accepted, has not been placed beyond the field of profitable discussion. Thus the subject of continents affords no less than a half dozen of great problems, whose complete solution belongs to the future. It is not altogether pleasant to deal with a subject in regard to which the domain of our ignorance is so broad ; but if we are optimists we may be comforted by the reflection that the geologists of this generation, at least, will have no occasion, like Alexander, to lament a dearth of worlds to conquer. BULLETIN OF THE GEOLOGICAL SOCIETY OF AMERICA Vol. 4, pp. 191-204 March 24, 1893 COMPARISON OF PLEISTOCENE AND- PRESENT ICE-SHEETS BY WAR REX UPHAM [Read before the Society December 29, 1892) CONTENTS Page Existing Ice-sheets and Glaciers 191 The Antarctic Ice-sheet 192 The Greenland Ice-sheet 192 The Malaspina Glacier or Ice-sheet 194 The Mnir Glacier 196 Inferences from Comparisons of present and Pleistocene Ice-aheets 198 Probable surface Slopes and Thickness of the Pleistocene Ice-sheets of North America and Europe 19S Probable Rates of Er< >si< >n by Pleistocene Ice-sheets 199 Subglacial and englacial Transportation of Drift 199 Rapidity of final Ablation of the Ice-sheets 200 Modes of Deposition of the englacial Drift 201 Origin of Forest Beds between Deposits of Till 201 The Ice Age viewed as a continuous and geologically brief Period 202 General Consideration of the Question 202 Probable Synchronism of Glaciation in North America and Europe 203 Relation of the Ice Age to human and geologic History 204 Existing Ice-sheets and Glaciers. The guiding principle of geologic investigation, brought out most clearly by Lyell, requires us to seek the explanation of past changes of the earth by observation and study of agencies which are now in operation, pro- ducing similar changes during the present epoch. From such studies of the Swiss glaciers, Agassiz, Forbes, Tyndall and others have given to us the theory of the formation of the drift by land ice, so that the compara- tively small district of the Alps supplied the clue for deciphering the records of the latest completed chapter of the geologic history of north- western Europe and the northern half of North America. Glaciers of other regions in the eastern hemisphere, notably of the Himalayas and XXIX-Bull. Geol. Soc. Am., Vol. 4, 1892. " (191) 192 W. TJPIIAM — PLEISTOCENE AND PRESENT ICE-SHEETS. of Norway, have also contributed much to our knowledge of the ice-sheets of the Pleistocene or glacial period. The vast ice-sheets of that time, however, are adequately exemplified at the present day only by the Antarctic and Greenland ice-sheets, less completely and on a much smaller scale by the yet very instructive Malaspina glacier, and in some respects they may be profitably compared with the Muir glacier, which is the most fully studied ice-field of America or perhaps of the world. The Antarctic Ice-sheet. — Land ice surrounds the south pole to a distance of 12 to 25 degrees from it, covering, according to Sir Wyville Thomson, about 4,500,000 square miles. Its area is thus slightly greater than that of the Pleistocene ice-sheet of North America, which covered about 4,000,000 square miles, while the confluent Scandinavian and British ice-sheets appear to have enveloped no more than 2,000,000 square miles, including the White, Baltic, North and Irish seas, whose areas were then occupied by the continental mer de glace. Whether the Antarctic ice- sheet covered an equal or greater extent in the Pleistocene period, con- temporaneous with the glaciation of now temperate regions, we have no means of knowing. Along a portion of its border of perpendicular ice- cliffs Sir J. C. Ross sailed 450 miles, finding only one point low enough to allow the upper surface of the ice to be viewed from the masthead. There it was a smooth plain of snowy whiteness, extending as far as the eye could see. That this ice-plain has a considerable slope from its cen- tral portions toward its boundary is shown by its abundant outflow into the sea, by which its advancing edge is uplifted and broken into multi- tudes of bergs, many of them tabular, having broad, nearly flat, tops. As described by Moseley in " Notes by a Naturalist on the Challenger" these bergs give strange beauty, sublimity and peril to the Antarctic ocean, upon which they float away northward until they are melted. Many parts of the borders of the land underlying this ice-sheet are low and almost level, as is known by the flat-topped and horizontally strati- fied bergs, but some other areas are high and mountainous. Due south of New Zealand the volcanoes Terror and Erebus, between 800 and 900 miles from the pole, rising respectively about 11,000 and 12,000 feet above the sea, suggest that portions or the whole of this circumpolar continent may have been recently raised from the ocean to form a land surface, which on account of its geographic position has become ice-clad. The Greenland Ice-sheet. — Inside its border of mountains Greenland is enveloped by an ice-sheet which lias a length of about 1,500 miles, from latitude 60° 40' to latitude 82°, with a probable average width of 400 miles or more, giving it an area of 600,000 square miles. On the easf this ice-sheet in some places stretches across the mountains, and the coast- consists of its ice-cliffs; and on the west glaciers flow from the inland ice WORK OF ARCTIC EXPLORERS. 193 through gaps of the mountains to the heads of the many fjords and bays, where the outflowing ice is broken into bergs of every irregular shape and borne away by the sea. One of. these ice-streams, discovered and named by Kane the Humboldt glacier, is 60 miles wide where it enters Peabody bay, above which it rises in cliffs 300 feet high. The altitude and slopes of the Greenland ice-sheet have been deter- mined by Nordenskiold, Peary, and Nansen. Nordenskiold's journey in July, 1870, to the east from the head of Aulatsivik fjord, near latitude 68° 20', is estimated to have extended about 35 miles upon the ice-sheet, and the altitude reached was 2,200 feet. From nearly the same starting point, Nordenskiold, in July, 1883, went onto the ice-sheet about 73 miles, to a height of about 4,950 feet ; and two Lapps, traveling with the peculiar snowshoes called " ski," advanced a probable distance of 45 or 50 miles farther, where the barometers indicated a height of 6,386 feet. Land in the interior, free of ice and bearing vegetation, which Norden- skiold hoped to reach, was not found ; and no nunatak, or projecting top of hill or mountain, above the ice surface has been yet discovered more than 40 or 50 miles inside the ice-covered area. Lieutenant R. E. Peary, of the United States Navy, in June and July, 1886, accompanied by Christian Maigaard, made the next important ex- ploration of the inland ice, going eastward from the head of Pakitsok fjord, on the northeastern part of Disco bay, in latitude 69° 30'. They advanced to a distance of about 100 miles from the edge of the ice, at- taining an altitude of about 7,500 feet. In concluding the narrative of this journey* after describing the needful outfit, Peary remarked: "To a small party thus equipped, and possessed of the right mettle, the deep, dry, unchanging snow of the interior ... is an imperial highway, over which a direct course can be taken to the east coast." It was also suggested that the unexplored northern shore lines of Greenland may be most readily mapped by expeditions across the high inland ice. This sagacious suggestion Peary has since in part fulfilled by his very success- ful expedition from May 15 to August 6 of this year, in which he crossed the northwestern and northern parts of this ice-sheet, reaching altitudes of 5,000 to 8,000 feet, and determining approximately the northern bound- ary of the ice from Petermann fjord to the eastern coast at Independence bay, in latitude 81° 37' and longitude 34° west from Greenwich. In August and September, 1888, Dr Fridtjof Nansen, with five com- panions, crossed the ice-sheet of Greenland from east to west between latitude 64° 10' and 64° 45'. The width of the ice there is about 275 miles, extending into the ocean on the east, but terminating on the west *"A Reconnoissance of the Gfreenland Inland [ee," Bull. Am. Geog. Soc, vol. xix, pp. 201-2-'^ September 30, 1887. 194 W. UPHAM — PLEISTOCENE AXI> PRESENT ICE-SHEETS. about 14 miles from the head of Ameralik fjord and 70 miles from the outer coast line. For the first 15 miles in the ascent from the east, rising to the altitude of 1,000 meters, or 3,280 feet, the average gradient was nearly 220 feet per mile. In the next o5 miles an altitude of 2,000 meters, or 6,560 feet, was reached; and the average gradient in this distance, be- tween 15 and 50 miles from the margin of the ice, was thus about 94 feet per mile, or a slope very slightly exceeding one degree. The highest part of the ice-sheet, about 112 miles from the point of starting, was found to have an altitude of 2,718 meters, or about 8,920 feet. Its ascend- ing slope, therefore, in the distance from 50 to 112 miles was about 38 feet per mile. Thence descending westward, the gradients are less steep, averaging about 25 feet per mile for nearly 100 miles to the altitude of 2,000 meters, about 63 feet per mile for the next 52 miles of distance and 1,000 meters of descent, and about 125 feet per mile for the lower western border of the ice* But Greenland has not always been thus ice-enveloped. During the middle or earlier portions of the Tertiary era forest trees belonging to a temperate flora extended northward in western Greenland to the Arctic circle. Going much farther back to inquire the origin of this great island, we find that it is an outlier of the North American plateau of Archaean rocks, which comprises also Ellesmere land, the eastern part of North Devon, Baffin land, Labrador and the country around Hudson bay, stretching thence southwestward to lakes Huron, Superior and Winnipeg, and westward to Athabasca, Great Slave and Great Bear lakes, and to Coronation gulf of the Arctic sea. The greater part of the Arctic archi- pelago, however, consists of Paleozoic strata. During long Mesozoic and Tertiary ages of higher altitude of these regions subaerial stream erosion formed the channels which divide the Arctic islands, the basin and valley of Hudson bay and strait and those of Baffin bay and Davis strait, which now by subsidence separate Greenland from the mainland. More ample oceanic circulation, carrying warmth from tropical and temperate latitudes to the Arctic sea, was probably the cause of the formerly luxuriant vegeta- tion of Greenland ; but during the ensuing Pleistocene period its ice-sheet was for some time even more extended and deeper than now, as is shown by the glaciation of the rock surface high up on the sides of the fjords. The Malaspinet, Glacier or Ice-sheet. — The comparatively small Malaspina ice-sheet, stretching from the Saint Elias range to the shore of the Pacific ocean, has been described as follows by its principal explorer, Professor I. C. Russell, after his two expeditions of 1890 and 1891 : f *The First Crossing of Greenland, 2 vols., 1890. f" Mount Saint Elias and its Glaciers," Am. .lour. Sci., III, vol. xliii, pp. 169-182, with map, March, 1892. The report of the first expedition, in 1890, is given by Russell in the National Geographic Blagazine, vol. iii, pp. 53-203, with 19 plates, and Y/< in a i Irs inijircxxii.s, " Liotium punctatum, " Cumlia, sp. undet., " *Lunatia ((cell ana, " fRingicula carta, " fPanopsea concentrica, " fCuculaea truncata, " fArca breweriana, '' f 7 '/ • igo nia ; eq 1 1 wostata , ' ' Trigonia, related to evansana,% fPecten operculiformis, Gabb. f Cardinal (Lmvicardium) annula- tum, Gabb. fCorbula traskii. fMytilus quadratics, Gabb (?) fLeda translucida, " *Pleuromya laevigata, Whiteaves. Rhynchonella, sp. undet. ~f Nemo don vancouverensis, Meek. FOSSILS FROM TEXAS SPRINGS.* ^Ammonites hoffmanni, Gabl). * Ammonites breweri, " Action rina californica, " Gyrodes, sp. undet. *Belemnites impressus, Gabb. Liocium punctatum, " Fusus aratus, " *Lunatia avellana, '' Scalaria albensis (_?). D'Orb. *Ringinella polita, Gabb (?). *Anisomyon meekii, " t^4?ra breweriana, " f Trigonia sequ icostata, " Trigonia related to evansana, J fPecten operculiformis, Gabb. '[Trigonia leana, " fCorbula traskii. "fTellina hoffmanni, Gabb. f Mactra ashburneri, " "\Chinone varians, " Rhynchonella, sp. undet. ^Tellina mathewsonii, Gabb. fMeekia radiata, " ~\Meckia navis, " •jjfggfcta «//^, " Mytilus lanceolatus, Sowerby (?). jPanapn a concentrica, Gabb. Concerning this collection Mr Stanton, in his report dated December 17, 1892, says : " It is evident that all the fossils in both these lists belong to one fauna, and probably to a very limited zone, and the)' will he so considered in making com- parisons with described faunas. | Probably not described. INTERGRADATION OF THE SHASTA AND CHICO. 211 " This collection leaves no room for doubt that the faunas of the Shasta and Chico groups are so intimately blended that they cannot be separated. Horsetown is a well known Shasta locality, from which the types of some of Gabb's Shasta species were collected, yet in this small collection, containing twenty-one species from this place, ten species belong to the Chico fauna as described by Mr Gabb. Combin- ing the collections from these localities, there are thirty-six species enumerated, of which ten have been described as coming from the Shasta group, eighteen from the Chico group, and eight are doubtful or undecided." * So far as I have been able to learn, about seventy species and a dozen genera not represented by determinable species have already been rec- ognized in the Shasta series of California. Of these fossils certainly more than one-fourth, and probably nearly one-half, continue upward into the Chico beds, and clearly indicate that the Horsetown and Chico beds are much more closely related than has been supposed. f When we take into consideration, at the same time, both the strati- graphic and faunal evidence, there can be no doubt that the Horsetown and Chico beds were formed in one period of continuous sedimenta- tion. Relation of the Horsetown and Knoxville Beds. — In Tehama county, Cal- ifornia, where the contact between the Horsetown and Knoxville beds is well exposed, their relation can be studied to great advantage. Along Elder creek, just north of the fortieth parallel, at the eastern base of Yallo Bally, the unaltered fossiliferous Cretaceous strata have an appar- ent thickness of nearly 30,000 feet.J The whole series, including the Chico and Shasta groups, dips eastward away from the Coast range with remarkable uniformity and appears to he one continuous series of sedi- ments from top to bottom without a perceptible interruption. In the lower 19,900 feet its only fossil found is Aucella. These sedimentary rocks; the Knoxville beds, are limited below by serpentines resulting from the alteration of peridotitic eruptives such as form a considerable portion of the Klamath mountains and Coast range. In the upper 3,900 feet of the Elder creek section Chico fossils occur abundantly, while in the inter- mediate 6,100 feet Horsetown fossils have been found. The latter are best exposed in the Eald hills between Paskenta and Lowrey's, where Aucella occurs abundantly in the basal portion, associated with Ammon- ites batesii, Trask ; A. ramosus, Meek.; A. traskii (?), Gabb; Ancyloceras percostatus, Gabb ; Rhynchonella, n. sp. ; Siliqua, sp. undet. Although these fossils were not actually seen together with Aucella in the same rock exposure, yet they were seen so near together throughout a great * See also Mr Stanton's paper which immediately follows, p. '22.',, et seq. fjt is important to rememlier in this connection that the collections have been made almost wholly by geologists while studying the stratigraphy, and not by paleontologists who were en- deavoring to determine the relations of the faunas. J; Am. Jour. Sci., 3d ser., vol. xl, 1890, p. 47<>. See also Bull. Geol. Soc. Am., vol. 2, p. '_'n7. 212 J. S. DILLER — GEOLOGY OF CALIFORNIA AND OREGON. thickness of conformable shales and sandstones that the writer regarded them as not only contemporaneous but intermingled and belonging to the same fauna. On Elder creek, therefore, the evidence clearly indi- cates that the Horsetown beds are younger than the Knoxville, and that between them there is a stratigraphic and fauna] continuity. Mr Becker and the writer* claimed that at Riddles, Oregon, AueeUa is associated with ammonites and other forms of Horsetown age. The writer visited Riddles four times, and, in company with Mr Will Q. Brown, examined nearly all of the fossiliferous rocks of that region, but has never been able to obtain AueeUa and Horsetown fossils from exactly the same exposure. The rocks containing these fossils, however, are so intermingled and related to each other structurally that there can be no doubt that the fossils all belong to the same fauna. The valley of Cow creek is eroded out of a more or less modified synclinal of Cretaceous rocks. The older Aucella-henrmg strata are upon the sides. The strata in which Horsetown forms are most abundant occur near the middle of the valley, in the immediate vicinity of Riddles, where Aucella also occurs. The whole set of strata appears to be conformable. The following forms have been identified by Messrs White and Stan- ton in the collections made by Messrs Becker, Brown and the writer near Riddles, Oregon : Aucella concentrica, Fisher. Pleuromya laevigata, Whiteaves. Amninriilrs tra*kii, Gabb. Pecten operculiformis, Gabb. " batcsii, " " Californicus, " " brcweri, " Cardita translucidum, " Belemnites impressus, " Area breweriana, " In northern California the writer has found Ammonites traskii and A. batcsii in the lower half of the Horsetown beds only, A. brcweri in the upper half of the Horsetown beds, Pleuromya laevigata, Pecten operculi- f or mis and Belemnites throughout the Horsetown beds, and the last two, Cardita translucidum and Area breweriana, in both Shasta and Chico beds.f * Bull. Geol. Soc. Am., vol. 2, pp. 201-207. fMr Will Q. Brown, who, under the writer's supervision, mapped a large part of the Cretai us rooks in Jackson and Douglas counties in Oregon, has recently made an important contribution of new evidence. A collection which he generously made and transmitted at his own expense shows Aucella and an Ammonitt in the same hand specimen, so there can be no doubt concerning their association. Professor Hyatt has examined the specimen, and reports. December, 1892, that " the Ammonites could by its external whorls be referred to either of the two groups Cosmoceras of the upper Jura or Hoplitcs of the Cretaceous. By digging into the specimen enough of one of the inner whorls was exposed to indicate that the A mmonites is one of the Cryptoa ras groups of HopliU s, and probably a true Cretacic species." Professor Hyatt adds that, as he has not yet l d able to find any species of this group with an aperture, his opinion stated above is only pnn isional, but the evidence so far goes to show that one of the forms of Aucella occurs with a Cretaceous Ammonites. The Ammonites, however, is very distinct from anything yet discovered in the Horsetow a beds else where, it occurs in the basal portion of the beds which occupy Cow creek valley. INTERGRADATION OP THE KNOXVILLE AND HORSETOWN. 213 From both stratigraphic and paleontologic points of view, therefore, the evidence strongly supports the opinion that the Knoxville and Horse- town beds in northern California and Oregon are a successive and con- tinuous conformable series of sediments laid down without perceptible interruption. Since the Knoxville beds pass upward without interruption into the Horsetown beds and the latter in the same way grade into the Chico beds, we arrive at the conclusion contained in the first proposition of the thesis, namely : The Cretaceous strata of northern California and Oregon, embracing the Chico, Horsetown and Knoxville beds, or, in other words, the Chico and Shasta beds, are an essentially conformable and continuous series of sediments formed without a distinct interruption. For this series Mr Stanton and 1 have agreed to use the name Shasta-Chico series. Distribution and Composition of the Shasta-Chico Series. — The distribution of the Knoxville beds in the Coast range south of the fortieth parallel is described, so far as yet known, chiefly by Becker, Turner and Fair- banks in a number of papers* They are well developed on Elder creek. If we place the upper limit so far up as to include all the .l>"v//a-bearing strata, they extend, according to Fairbanks, as far northward as Cold fork. Tehama county, near the Shasta county line. At that point the present writer has observed the Shasta group to rest unconformably upon the metamorphic rocks, and the unconformity is conspicuous. The Horsetown beds have been definitely recognized only a few miles south of the fortieth parallel, but in the opposite direction they have been traced a long distance. From Elder creek, where they conformably overlie the Knoxville beds, they extend northward far beyond the latter, unconformably overlapping the older metamorphic rocks, to Horsetown and Texas springs, nearly as tar north as Redding. This overlapping is well shown in the Horsetown beds themselves. Ammonite* ramosus and A. batesii were found on the South fork of Elder creek near Aucella and in conformable strata far beneath the latest strata, containing Aucella. The writer has not found these ammonites to extend above the middle portion of the Horsetown beds. In the vicinity of Ono, on the North fork of Cottonwood, they are common near the uncon- formable contact between the Cretaceous and metamorphic rocks, but have not yet been discovered as far north so Horsetown, where only the upper members of the Horsetown beds occur. Ammonites hoffmanni and A. breweri, which occur at Horsetown and farther southward just above *G. F. Becker: Bulletin 19, U. S. Geol. Survey; U. S. Geol. Survey Monograph xiii: and Hull. Geol. Soc. Am., vol. 2, pp. 201-208. W. II. Turner • Bull. Geol. Soe. Am., vol. 2, pp. 399-401. H.W.Fairbanks: American Geologist, vol. ix, p. 159, March, 1892 ; ib., vol. xi, p. 69, February, 1893. XXXII— Bum.. Geol. Soc. Am., Vol. 4, 1892. 214 J. S. DILLER GEOLOGY OF CALIFORNIA AND OREGON. the latest A. ramorus and A. batesii, belong to the upper half of the Horse- town beds and extend much farther northward in its series, overlapping the older raetamorphic rocks. From the North fork of Cottonwood creek the Horsctown beds extend far westward, crossing the range between Yallo Bally and Bully Choop mountains along the Hay fork road, and an isolated fossiliferous area of them nearly five square miles in extent occupies Bedding creek basin in Trinity county, at the northwestern base of the Bully Choop mountains. Everywhere beyond the limit of the Knoxville beds the Horsctown beds rest, with a marked unconformity, directly on the metamorphic rocks. The Chico beds have a wide distribution in southern California, and to the northward underlie the Sacramento valley, with outcrops on both sides. At Elder creek, on the western side of the valley, the Chico beds rest conformably on the Horsetown beds. They extend north- ward, holding the same relation to the Horsetown beds until near Bed- ding, where the Horsetown beds run out and the Chico beds rest uncon- form ably on the metamorphic rocks. This unconformable contact be- tween the Chico beds and older metamorphic rocks, including at least Carboniferous, Triassic and Jurassic strata, has been traced around the northern end of the Sacramento valley, and, by way of the Great bend of Pit river, Mount Shasta, Henley and Ashland, farinto ( Oregon. There is good reason for believing that the Chico beds which extend beneath the lavas of the southern portion of the Cascade range connect with those recognized on Crooked river, Oregon* At a number of places in the Klamath mountains there are remnants of Cretaceous rocks in which these mountains were once enveloped, but this covering has nearly disappeared by erosion. To enter into the de- tails of their distribution Avould lead beyond the proper limits of this paper. Let it be sufficient to say that their distribution shows that the Klamath mountain region was almost, if not wholly, beneath the sea during the closing days of the Cretaceous. f On Elder creek, in Tehama county, California, the Chico, Horsetown and Knoxville beds are all present. The Knoxville beds extend from this place only a few miles to the northward ; the Horsetown beds ex- tend beyond them in that direction at least 25 miles, while the Chico beds stretch still further in the same direction far into Oregon. The Cre- taceous section thins out rapidly in the same direction by the successive dropping out of the earlier beds. On Elder creek the Cretaceous is ap- parently over 20,000 feet thick, at Ono 8,800 feet, and further northeast- * Bulletin 33, U. S. Geol. Survey p. 19. fSince the paper on fche geology of Lassen peak was written i Eighth Ann. Rept. ('. s. Geol. Sur- vey, p. 411,412) the subsidence has i o found much greater Hum was a! firs! supposed, so that the Cretaceous island may have wholly disappeared near the end oi thai period. TRANSGRESSION OF THE CRETACEOUS SEA. 215 ward still less. In none of the sections, however, has the exact top of the Cretaceous been seen. Since these beds are all marine and form one continuous series of sediments, it follows, from their distribution, that during their period of deposition the sea was transgressing what is now the northern portion of California. That the sea was transgressing during the Cretaceous is clearly shown also by the character of the Cretaceous sediments. Before the deposition of the Shasta group the Klamath mountains, composed of Jurassic, Tri- assic and Paleozoic rocks, more or less metamorphosed, had been dry land, exposed to weathering for a sufficiently long time to allow the sec- ular disintegration of a mass of surface rock to form the residuary deposits which have become the sediments of the Shasta group. In some cases the deposits of the Shasta group bearing fossils rest upon the residuary deposits and rotten rock from which they were derived, and the line of contact is not easily recognized. This is the case on the southeastern border of the Klamath mountains, in Shasta county, Cali- fornia, between Ono and Igo, where micaceous sandstone at the base of the Shasta group so closely resembles the rotten diorite on which it rests that until the presence or absence of fossils is determined one is in doubt which rock he may be examining* Near at hand, too, by the present streams, there are coarse shore con- glomerates, including the gravels of the Cretaceous streams which flowed down from the Klamath mountains on the northwest into the ancient bay of the Sacramento valley, and one is surprised to find some evidence that the valleys of the embouching streams of early Cretaceous times are still occupied by streams. This may be true to a very limited extent, but it is noticeable in the upper tributaries of the North Fork of Cottonwood creek near Ono. From this point the Cretaceous rocks extend westward, and the later members of the series lap up over the Yallo Bally and Bully Choop ridge, the main divide of the Klamath mountains, crossing to the' west- ern slope, where they appear well characterized by fossils in Redding creek basin of Trinity county. In all cases the Cretaceous sediments immediately in contact with the metamorphic rocks are of local origin. When they are coarse the contact is plain and the unconformity so well pronounced as to be beyond question, but where the sediments are fine there may appear to be a gradual transition from the older metamorphic rocks to the Cretaceous. For reasons already given, however, I am hilly convinced that in northern California and Oregon it is chiefly apparent and rarely if ever real.f It would be expected that the unconformable *See observations by Dr Dawson in Geol. Survey of Canada, Rept. of Progress, 1877-78, p. luG B. He describes the same sort of phenomena at the base of the Cretaceous on the Skagit t Incases where the Cretaceous strata have been metamorphosed a transition from the unaltered to the altered portions without an intervening unconformity would be expected. 216 J. S. DILLER — GEOLOGY OF CALIFORNIA AND OREGON. contact immediately underneath the Knoxville beds would be Less con- spicuous than that between the Horsetown beds and the metamorphic rocks or between the Chico and the metamorphics. This would follow from the fact that the Knoxville beds, having been deeply buried by later sediments, were subjected to more intense metamorphic action, which tends to render the original contact less evident. In Siskiyou county, California, upon the eastern slope of the Klamath (Scott) mountains, adjoining Shasta valley, there are a number of impor- tant exposures of Cretaceous rocks. Dr D. Ream, of Yreka, kindly fur- nished me a section of the rocks penetrated by Mr King's well at the salt works in Shasta valley, where over 500 feet of fossiliferous sandstonewas observed beneath the lavas of Shasta valley. The same rocks are exposed at the surface near Yreka and on Willow creek, where they contain Chico fossils. On the edge of Shasta valley the Cretaceous strata dip to the eastward and lap up over the lower slopes of the Klamath (Scott) mountains, which lie upon its western border. The tilting evidently occurred at the time the Klamath mountains were upheaved, and the unconformably overlapping Cretaceous strata have since been nearly all eroded. A few conspicuous remnants, however, are still there to tell the tale. The best of these are at Cave rock, three miles north of Gazelle, and near the summit on the road from Yreka to Fort Jones. The last is at an elevation of 2,000 feet above Shasta valley and over 5,000 feet above the sea. The mass is about 400 feet in thickness, and the conglom- erate at its base is composed chiefly of white quartz and unassorted angu- lar fragments of schistose rocks like those in place near by. Although fossils were not found at either of these localities, there can be scarcely a doubt that they represent the overlapping Cretaceous strata from the foot of the same slope. In Douglas county, Oregon, along Olalla creek, slates have been found containing . I uct lla alone, and the rocks are considerably metamorphosed. At Buck mountain, a few miles further southeast and twelve miles west of Riddles, AuceUa occurs alone in coarse, pebbly sandstone, which has a slightly metamorphic aspect. This appearance, however, is due not so much to actual metamorphism since deposition as to the fact that the rock is composed chiefly of residuary material removed but a short dis- tance from its original position: consequently its contact with the oldgr metamorphic rocks is not sharply defined. The same is true at some localities, but not all, about Kiddles, in the valley of Cow creek, where both AuceUa and Horsetown fossils occur in abundance. Still further eastward, on Grave creek, an area of Shasta beds occurs. AuceUa is absent, and there are some Chico forms present, with thoseof the Shasta group, so that the horizon must be near the top of thai group. These EXTENT OF THE CRETACEOUS SEA. 217 fossiliferous strata are in part coarse conglomerates of local origin and, according to the observations of Will Q. Brown, as well as of the writer, are clearly unconformable to the metamorphic rocks. Twelve miles further in an easterly direction, near Jacksonville, and elsewhere in Jackson county, < )regon, the Chico rocks, now called Horse- town by Mr Stanton, rest directly with a marked unconformity on the metamorphics. in Oregon, therefore, the evidence, although less complete, is entirely in harmony with that of northern California, and we are led to the con- clusion stated in the second proposition of the thesis, namely: While the Sliasta-Chico series was being deposited the region was gradually subsiding and the sea transgressing to the eastward in northern Cali- fornia and Oregon. This subsidence continued until the sea reached the western base of the Sierra Nevada, near the fortieth parallel, and all or nearly all that part of California north, northwest and west of Lassen peak, as well as almost the whole of Oregon, was beneath its waters. The occurrence of the Cretaceous in Washington, excepting that on Sucia, Orcas and Ship Jack islands, near Vancouver, lias hitherto beena matter of considerable doubt. Its determination has been based largely upon certain casts which were supposed to have been of Baeulites. Ac- cording to Willis,* the Cretaceous of northwestern Washington is com- paratively thin and rests directly on metamorphic rocks, which are pre- ( 'retaceous and probably of Paleozoic age. While in Seattle I obtained from Mr E. W. P. Guye a well-preserved Baculile, which Mr Stanton determined as Baeulites chicoensis. It was ob- tained on the Snoqualmie river, three miles below the falls, and shows the presence of the Chico at that point. The rock is unaltered and lies between the Puget group and the metamorphics. At the same time my attention was called to a bowlder found in Seattle ; it is composed chiefly of Aucclhi and was in all probability transported from the Cascade range. The rock is unaltered and closely resembles some of the Aucella-bea,rmg rock about Kiddles. In the collection of Professor T. Condon at the state university, Eu- gene, Oregon, there is a large fragment of rock f containing a multitude of robust shells of Aucella. It came from Vashon island, near Tacoma. Dr DawsonJ reports /4Mce/Za-bearing rocks oh the Skagit north of the international boundary. It is believed that they extend south into Wash- ington and have furnished the bowlders referred to. There can be no doubt that the Shasta-Chico series is represented in *Tenth Census, vol. xv, 18SC, p. 761. t Tliis is probably the same material that Becker and White refer to in U. S. Geol. Survey Monograph xiii, pp. 202, 232. X Geol. Survey ot Canada, Report of Progress, 1877-78, p. 10G B. 21S .1. S. DILLER — GEOLOGY OF CALIFORNIA AND OREGON. the Pugel sound region, but of its extent scarcely anything is known. Further northward, however, the same series is extensively developed in Vancouver and Queen Charlotte islands, as well as within the interior portion of British Columbia, where it lias been described by Dr Selwyn, Dr Dawson, and Mr Richardson in the reports of the Canadian geologic survey. From an extensive knowledge of the facts, Dr Dawson concludes that in early Cretaceous times the immediately post-Triassic elevation had been followed by a subsidence of the land, resulting in the reoccu- pation by the open sea of a great area near the Pacific coast and north of the fifty-fourth parallel, spreading eastward in a more or less connected manner completely across the present position of the Cordilleras. The Gold ranges, and probably also many other insular areas, continued to exist as dry land. As local terrestrial conditions are recurrent through- out a great thickness of strata, it is obvious that the subsidence was continuous or nearly so and was followed pari passu by sedimentation. Dr Dawson says : "About the stage in the Cretaceous which is represented by the Dakota group, however, a much more rapid downward movement of the laud occurred. This is marked by the occurrence of massive conglomerates, which have been recognized in many places in the southern part of the interior of British Columbia, as well as westward to the Queen Charlotte islands."* Dr Dawson calls attention to the tact that west of the axis of the Coast ranges the area of Cretaceous sedimentation was transgressively extending southward, the local base of the Cretaceous being found at suc- cessively higher stages in the system in that direction, till at a time, which is believed to have corresponded with the Laramie of the plains, the sea invaded the Puget sound region. The invasion of the sea in British Columbia was contemporaneous with that of northern California and Oregon just described, and possibly also with that which carried Aueetta around the southern end of the land barrier into Mexico.f Tertiary. The Tejon beds are now generally regarded as representing the earliest Tertiary deposits of California ami Oregon. In noddle California these beds are well represented. They are not only conformable with the( !hic( >. lint have been considered to form, with the Chico, a continuous series of strata, deposited without any interruption in the process of sedimenta- tion. This is unusual, for generally a fauna! and stratigraphic break occurs between the Cretaceous and Tertiary. * Am. .lour. Sri., .",.1 sit., vol. xxxviii, 1880, p. 120; Transactions of the Royal So< iety of Canada, vol. viii, sect, iv, 1S!H>, pp. 8, •>. See also S. F. Emmons, Bull. Geol. Sue. Am., vol. 1, p. 278. fNeues Jarb. fur Min., Geol. u. Pal., ls'ju, ii bund, p. l'v:;. DISTINCTION OF TPIE CHICO AND TE.TON. 219 Lindgren has recognized the Tejon in the Sacramento valley as far northward as Marysville buttes * In the Coast range Whitney, on Gabb's observation, reports the Tejon nearly as far northward as Round valley, Mendocino county* Similar coal-bearing strata containing fossil leaves have been observed by the present writer at Hyampome, Cox's bar and Redding creek basin, in Humboldt and Trinity counties, but the evidence that these strata are really Tejon is not convincing ; they are rather more probably Miocene. With the exception of the locality at Marysville buttes, no molluscan fossils of Tejon age have been found in northern California, and it has generally been regarded as absent. In Oregon, however, the case is very different. The Tejon, well char- acterized by an abundance of marine fossils, is represented by at least 2,000 feet of strata. Professor Condon has reported it at Cape Arago by Coos bay, and at Albany. Dr C. A. White has recognized it at Astoria, where it has since been studied by Dr W. H. Dall. Profess* >r ( !< mdon called my attention by letter to an excellent exposure of fossiliferous Eocene on the South fork of the north Umpqua, where Mr Will Q. Brown and the writer have made several collections. At least 1,000 feet of Eocene si rata are there exposed. They contain throughout abundant shells of Cardiia planicosta, with other fossils, and rest directly upon an irregular surface of metamorphic rocks. From this point the Eocene beds have been traced southwestward nearly to Coos bay, and fossils have 1 teen collected at Cleveland, Lookingglass, Olalla and Table mountain. At the last two localities they rest on the upturned edges of the Shasta-Chico series. The unconformity at the base of the Tejon group in Douglas county, Oregon, is in some cases conspicuous and in all eases well defined, and it appears that the Shasta-Chico series was not only folded but considerably eroded before the beginning of deposition of the Tejon in that region. With such a physical break, faunal continuity between the Chico and the Tejon of Oregon could hardly be expected ; but, to test this point as far as possible with the collections now at hand, I requested Mr Stanton to carefully examine the collections of Tejon from Oregon and Washing- ton for Chico species. In response Mr Stanton sent lists of all the species collected at a number of localities, and remarks :f " You will notice that there are a few species among them that have been re- ported from both the Chico ami the Tejon. For example, Pholadomya namta, < '//- lichna costata ami Turriiella chicoenm. There are also some others that closely re- semble Chico species, but which I believe to be distinct, such as Mactra ashburneri and DentaMum stramineum. We have the two species last named from Chico locali- ties, and, on direct comparison with the related Tejon forms, there is no difficulty *Geol. Survey of Cal., Fa]., vol. ii, p. xiii. f January '.>, 1893, » 220 J. S. DILLER — GEOLOGY OF CALIFORNIA AND OREGON. in pointing out recognizable differences. None of the other doubtful species arc represented in any of our collections from Chico localities. '•It is therefore safe to say that your collections do not show any commingling of the Chico and Tejon faunas, and I may add that, so far as I have examined them, none of the other collections in the National Museum show such blending."' All of the facts yet known indicate that in Oregon and northern Cali- fornia there is a fannal and stratigraphic break between the Chico and the Tejon. Pre-Cretaceous Elevation of the Klamath Mountains and Sierra Nevada. The existence of a large land area in northwestern California and south- western Oregon in early Cretaceous times is clearly indicated by the com- position and distribution of the Cretaceous rocks of that region. The geologic date of the uplift must have been considerably earlier than the beginning of the Shasta-Chico epoch in order to allow the secular disin- tegration of the surface rocks to furnish the Cretaceous sediments for the invading sea. Since the writer's paper on the geology of the Taylorville region was published, our knowledge of the distribution of the Jura-Trias and Car- boniferous in northern California has been considerably extended, and. as this distribution has an important bearing on portions of this paper, it is necessary to record it here. A large number of fossils were collected by the writer and James Storrs on and near Pit river by the western arm of the Great bend, and at many places near Cedar creek and Halcombs, on the toll and stage roads be- t ween Redding and Burney valley. The areal geologic work done at that time is shown in the Bend and Cedar formations in the northwestern corner of the Lassen peak atlas sheet, a preliminary edition of which i» now in proof. The fossils were all examined by Professor A. Hyatt. and in the descriptive text accompanying that sheet his conclusions con- cerning the age of the rocks are stated. Both the Jurassic and Triassic of the Taylorville region are well represented in Pit river valley and add another strong argument, showing that the Klamath mountains of north- western California are composed in large part of the same rocks as the Sierra Nevada, f Along the western side of the Sacramento valley, near the basin on the Humboldt trail eight miles west of Pettyjohns, in Tehama county, * Almost thirty species have been identified from the Tejon of Oregon and Washington. t Mr Harold W. Fairbanks, who has published an article entitled "Tin- pre-Cretaceous Age of the Metamorphic Rocks of the California (cast Range" (Am. Geologist for March, 1892, vol. ix,"pp, 153-166 : also for Feb., 1893, vol. xi. pp. 69-84), kindly call f. 1 my attention to a number of new locali- ties in the Pit river region from which he had recently collected i'"s>il<. DISTRIBUTION OF JURASSIC FOSSILS. 221 fossils were found in a limestone. Mr Walcott, who examined the fossils for me, reported that only one genus, viz, Chasleles, could be identified, and from what is known of the rocks of that region he refers the lime- stone to the Carboniferous. This horizon had long been known fur- ther northward, near Bass' ranch, through the investigations of Trask and Whitney. Pentagonal and round erinoid .stems have been discovered by James Storrs in a limestone on Clear creek between Horsetown and Texas Springs. Professor Hyatt regards them as Triassic and probably of the same horizon as the Hosselkus limestone* At Texas Springs Mr Storrs found a limestone containing a large pen- tagonal erinoid stem, a spirifer and other brachiopods which Professor Hyatt regards as belonging within the Jura-Trias. The older rocks, upon which the Cretaceous strata of the western and northern borders of the Sacramento valley at the Pit river region rest with a conspicuous unconformity, are at least in part Jurassic, Triassic and Carboniferous in age. As bearing upon the general distribution of the Taylorville Jurassic, a collection of fossils made by Professor Condon on the upper waters of Crooked river, in the Blue mountains of Oregon, deserves mention. In lithologic character and fossils Professor Condon's specimens appeared to the writer to very closely resemble the Jurassic rocks of Taylorville. Professor Condon kindly loaned the specimens to be sent to Professor Hyatt, who confirmed this view and established another important locality of Taylorville Jurassic The discovery of Jurassic fossils on Pit river synchronous if not iden- tical with that of Taylorville has thrown new light on the pre-Cretaceous elevation of the Klamath mountains and the Sierra Nevada. Concern- ing some of these fossils Professor Hyatt says* they " include the same association of forms as the Mormon sandstone fauna, and, although the specimens are not all well preserved, I have little doubt that the rocks from which they came were synchronous with the Mormon sandstone of Taylorville." These Jurassic rocks were deformed and metamorphosed with the Triassic. Carboniferous and other portions of the auriferous slates. They are separated from the unaltered Cretaceous (Shasta-Chico series) of that district by a conspicuous unconformity. The same unconformity extends southwestward, by way of Bedding, Horsetown and Ono, along the western side of the Sacramento valley, into Tehama county, Califor- nia, and northward, by way of Yreka, Cottonwood creek and Ashland, far into Oregon. It is evident, therefore, that a great upheaval and met- * Letter of October 4, 1802. XXXIII— Bull. Geol. Soc. Am., Vol. 4, 1882. 222 .!. S. DILLEK — GEOLOGY OF CALIFORNIA AND OREGON. amorphism of the Klamath mountains and Sierra Nevada occurred soon after the close of the Taylorville Jurassic. How long a time interval is represented by the great unconformity between the Taylorville Jurassic and the Shasta-Chico series is not yet known, hut that the upheaval took place in the earlier part of the inter- val is most probable. The relation of the Mariposa beds to the Taylorville Jurassic, on the one hand, and to the Shasta-Chico scries, on the other, is yet a matter of doubt, but will soon be resolved by Mr Becker and his assistants, Messrs Turner and Lindgren, who are now making a thorough survey of the Gold belt of the Sierra Nevada. It is already evident from the researches of Mr Becker and Dr White that the faunas of the Mariposa and Knox- ville beds are closely related, and on this account the great fauna! and stratigraphic break corresponding to the great unconformity between Shasta-Chico series and the Taylorville Jurassic on Pit river might be expected at the base of the Mariposa beds. That an upheaval occurred at the close of the Jurassic of Taylorville is indicated by the distribution of Auccllu in northern California and Oregon. Accordingly the disturb- ance in the Mariposa beds would have to be referred* to a later epoch, either within the Aucella-beaxing series or to the close of the Chico or Miocene. Inter-Cretaceous-Tertiary Upheaval of the Klamath Mountains. The lower portion of the Shasta-Chico series is in general more dis- turbed than the upper or Chico portion. This is due to various causes, the principal of which is to be found in the fact that, as now exposed, the Shasta beds are nearer the centers of disturbance than the Chico. The Chico has been removed from the disturbed areas by erosion. On the western side of the Sacramento valley, along Elder creek, where the Shasta-Chico series is exposed, the whole series is tilted, but the Shasta beds in the western portion toward the Coast range arc some- what more disturbed than the Chico beds in the eastern portion ; yet the difference is not great and the change so gradual through a number of miles of well-exposed strata that we looked in vain for any break in the stratigraphy or fauna. The character of the strata had much to do in determining the amount of deformation. The shales of the Shasta-Chico series are generally more deformed than the sandstones and conglomerates of the same locality, 1 lecause less rigid. They predominate in the lower portion of the Shasta- *See paper by Mr S. F. Kmmons "On Orographic MmvuiniN in the Roeky Mountains," Hull. Oeol, Soc. Am., vol. 1, \>. 27'J. EFFECT OF STRUCTURE ON DEFORMATION. 223 Chico series, and were deeply buried beneath the Chico. As a conse- quence they were subjected to the more rigorous action of deforming forces. The Shasta-Chico series in northern California and Oregon is rarely vertical, and from that angle the clip ranges to nearly horizontal. The gentlest inclinations are in the Chico on the western side and around the northern end of the Sacramento valley, and always miles away from the disturbed lower portions of the same series. The geologic date of the disturbance next succeeding the pre-Cretaceous one just referred to is well marked in Oregon, where, as already described, the Tejon is unconformable upon the Shasta-Chico series. Near the unconformable contact the Tejon is not folded, so that the deformation of the Shasta-Chico series, which is conspicuous in that region, took place before the deposition of the Tejon, or about the close of the Cre- taceous. That this deformation was accompanied by upheaval is shown by the absence of Tejon in northern California and part of Oregon. This deformation and upheaval appear to have been of great extent to the northward, for the Cretaceous sea which once covered part of Oregon, Washington and a large portion of British Columbia was driven westward by it, in some cases beyond the present limit of the continent; and about this time, according to King, the Wasacht range was uplifted * Resume and Conclusions. The observations of Dr W. H. Dall have shown that the Wallala beds are a phase of the Chico and belong near the base of those beds, essen- tially in the position assigned to them by Dr White. The Chico and Horsetown beds, which were once supposed to be sep- arated by a long interval, are now known to be stratigraphically and faunally continuous, and are the result of an uninterrupted epoch of sedimentation. In the same way the Horsetown and Knoxville, which together form the Shasta beds, are shown to lie stratigraphically and faunally contin- *The date of the deformation of the Mariposa beds must yet be regarded as an open question. If, as argued by Mr Becker, later by Mr Fairbanks, and finally by Messrs Turner and Lindgren, who have mapped the region, the Mariposa beds are unconformably beneath tin; Chico, their deformation would appear 1" have antedated the deposition of the Shasta-I Ihieo scries, I'm- in the group of strata including lie- Mariposa, Knoxville, Horsetown and Chico beds the argument for faunal and stratigraphic continuity is weakest between the Mariposa and Knoxville beds. The faunal relation of the Mariposa and Knoxville beds, however, is so close, according to Mr Becker, as not to admit of a great physical break hetween them. If one exists it- is possibly local and of limited extent. This might still lie in accord with the facts observed in northern California and < Iregon, where no break has yet been observed within the Aucelta-bearing rocks. Numerous observers have called attention to the great mountain-forming epoch about the .lose of the Miocene. During that revolution tic Klamath mountains and tic Sierra Nevada were modified to a large extent. The geologic history referred to in this paper wholly precedes that disturbance. 224 J. S. DILLEK — GEOLOGY OF CALIFORNIA AND OREGON. uous, and it follows that the Shasta-Chico series is the result of contin- uous sedimentation. The distribution of the members of the Shasta-Chico series and the composition of those in contact with the older rocks, on which they rest unconformably, shows that during their deposition the northern parts of California and Oregon were gradually subsiding and the sea trans- gressing. In Oregon the Tejon rests upon the Shasta-Chico series unconformably, and the paleontologic evidence, so far as it goes, tends to show that there is a faunal break in that region between the Chico and the Tejon. At the close of the Taylorville Jurassic there was an upheaval, by which the Klamath mountains and the northern end of the Sierra Nevada were outlined and the land extended far northwestward into the Pacific. This upheaval was followed after a considerable interval by a sub- sidence, which brought in Aucella from the northwest and inaugurated the Shasta-Chico series. In northern California and Oregon the subsidence continued through- out that series, unless interrupted between the Mariposa and Knoxville epochs, and was brought to a close by another mountain-forming upheaval, which forced the sea far to the westward before the begin- ning of the Tejon. IT. S. Geological Survey, Washington, 1). C. BULLETIN OF THE GEOLOGICAL SOCIETY OF AMERICA Vol. 4, pp. 225-240 May 20, 1893 ON THE GEOLOGY OF NATURAL GAS AND PETROLEUM IN SOUTHWESTERN ONTARIO BY II. P. H. BRUMELL (Read before the Society December 29, 1892) CONTENTS Page The Areas under Consideration 226 Gas-producing A rea 221 > Oil-producing' Area 226 Authorities indicated 226 Geologic Section of the Areas 226 The geologic Formations involved 227 Detailed Description essential 227 Portage 227 Hamilton 227 Corniferous 228 Oriskany 229 Onondaga and Lower Helderherg 230 Guelph 231 Niagara 231 Clinton 232 Medina 232 Hudson River 234 Utica 234 Trenton and Black River 2:14 Geologic. Horizons in Ontario yielding I ras and Oil 235 Oil Wells in the Corniferous Limestone 235 Age and Depth 2:!.) Annual Output of Oil 235 Chemical Composition of the Oil 236 The Corniferous petroliferous over a wide Area 236 The Medina as an ( )il-producer 231 i Gas-hearing Horizons : Clinton, Medina and ( >thers 236 Localities indicated 236 Depth at which Gas is found 236 Records of twenty-eight Wells 237 Gas-bearing Bed of the Medina 237 XXXIV— Bull. Gj-.ui.. Soc. Am., Vol. 4, 1892. (225) 22G H. P. H. BRUMELL — GAS AND PETROLEUM IN ONTARIO. Page Daily Capacity of BOme of the Wells 237 ( >ther Localities 238 The Clinton as a < ias producer 238 The Niagara as a < fas-producer 238 ( Mlier ( las-bearing Formations L'.'is The Onondaga as a Gas-producer 23J) The Trenton as a < ras-producer 239 An unusual Occurrence of Gas 240 Forthcoming Publication on the Subject 240 The Areas under Consideration. Gas-producing Area. — In that part of Ontario lying south and west of a line drawn from Toronto to Collingwood, operations in search of gas and petroleum have been carried on for a number of years. They have re- sulted in the discovery of two gas-producing areas of considerable extent, viz. that in Essex county, in the vicinity of Kingsville and Ruthven, and that in Welland county, in the neighborhood of Sherkston. Nor are the wells of these two fields the only producing ones, for many isolated bor- ings^ such as those at Cayuga, Dunn ville' and Mimico, afford no incon- siderable flows. Oil-producing Area. — Petroleum has unfortunately been found in com- mercial quantities in but one county, that of Lambton, where there are two distinct pools, known as the Oil Springs and Petrolea fields. These pools have been drawn upon continuously since 1862, when the first flowing well was struck, in what is now known as the " upper vein." Fol- lowing closely upon this discovery were more extended operations, which brought to light the present oil horizon, known as the " lower vein." The upper vein having long been exhausted, the source of supply has for years been in the lower, wherein wells affording as much as 7,500 barrels per day have been sunk. Authorities indicated. — As I wish to treat more of the geologic than the historical side of the question, I will follow out the title of my paper, but before doing so cannot do better than refer those interested in the oil industry in Ontario to Dr Robert Bell's paper on " The Petroleum Field of Ontario,'' published in volume v, Transactions Royal Society of Canada, and to the report of the Division of Mineral Statistics and Mines, part S, Annual Report Canadian Geological Survey, volume iv, 1888-89. Geologic Section of the Areas. — There is in that part of the province under consideration a series of rocks, lying in almost undisturbed posi- tion, ranging from the Trenton to the Portage formation, with an approx- imate total thickness of 4,100 feet, as follows: STRUCTURE OP THE HYDROCARBON FIELDS. 227 Devonian Silurian Cambro-Silurian Formations. Approximate A mk_ thickness m ■' r . * i ncss inject. r Portage and Chemung Hamilton, about Corniferous Oriskany Lower Helderberg \ Onondaga J Guelph 140 Niagara Clinton Medina Hudson Liver Utica I Trenton \ Rnn I Black Liver / uuu 25- 200 100 350 350 160- 300 230 6- 25 15 300- 1,000 650 140- 160 150 100- 130 115 30- 150 00 600- sou 700 500- 000 700 300- 400 350 600- 750 075 Total. 4,125 The geologic Formations involved. ,, « Detailed Description essential. — To meet the requirements of this paper it is perhaps 1 tetter to describe, so Car as is known, the various formations in descending order. Portage. — The Portage in Ontario consists of a series of fissile Mack bituminous shales and is developed almost altogether in the county of Lambton, where it acquires, according to Dr T. Sterry Hunt, a thickness of 213 feet, as shown in a boring made at Corunna* These shales in a well bored at Sarnia show a thickness of 80 feet, and again, in a well sunk on lot 12, concession 10, Bosanquet township, they are seen to have a total thickness of 95 feet. In both of these instances it lies immedi- ately over the upper shale bed of the Hamilton formation, the upper limestone bed of which, found at Petrolea and elsewhere, is wanting. In the township of Dawn, and again east of Oil Springs, 7<> feet of black shales are found. In this instance they rest upon the upper limestone of the Hamilton. In a syncline lying between Petroleaand Oil Springs, and separating the two fields, 40 feet of black shales are found in a well drilled on Fox creek, the elevation of which is considerably less than that of Oil Springs. These shales in no instance afford oil, but are prob- ably the source of the considerable quantities of shale gas found in the overlying gravel ami sand. Hamilton. — Thewells in Petroleaand Oil Springs and the greater num- ber of those drilled in Lambton county show that the black shales of the 1 Report of Progress, Geol. Survey of Canada, 1866, p. _:I7. 228 H. T. H. BRUMELL GAS AND PETROLEUM IN ONTARIO. Portage group immediately overlie a limestone bed which constitutes the upper stratum of the Hamilton formation. This series of rocks consists of alternating beds of limestone and gray shales ( known locally as " soap- stone ") and has a thickness, according to a drilling made at Kingstone's mills, Lambton county, of 3% feet. Dr Hunt* speaks of this well as being important in showing the thickness in Ontario of the middle and upper Devonian, which, if we add to the 396 feet found here the 213 feet of rocks belonging to the Portage found at Corunna, is 609 feet. The record of the well at Kingstone's mills is as follows: Clay 14 feet, Black shale 50 feet, P. >rtage. Shales, soft, and limestone 39(5 feet, Hamilton. Limestone, hard 44 feet, Coin i tennis. At Petrolea the Hamilton is only 296 feet thick, as follows: Limestone (" upper lime ") 40 feet. Shale (" upper soapstone") . . 130 " * Limestone ("middle lime") 15 " Shale ('* lower soapstone ") 43 " Limestone (" lower lime ") 68 " At Oil Springs, 8 miles southward, the formation shows evidence of having thinned out, the thickness there being only 240 feet according to the following record of many wells drilled on the eastern side of the field : Limestone (" upper lime ") 35 feet, Shale (" upper soapstone ") 101 " Limestone (" middle lime ") 27 " Shale (" lower soapstone ") 17 " Limestone (" lower lime ") ahout 00 " Corniferous. — Underlying the so-called lower lime of the Hamilton is a series of bituminous limestones constituting the Corniferous formation — the source of the oil of Lambton county. Regarding the distribution of this formation in Ontario, the following description is given :f "The surface occupied by this formation in western Canada is probably between 0,000 and 7,000 square miles. A great part of this, however, is deeply covered with drift, so that the exposures are comparatively few. To the eastward this forma- tion is hounded by the outcrops already assigned to the underlying strata, the limits of which in many parts have as yet been hut imperfectly traced. The whole of the province to the west and south of this line belongs to the Corniferous forma- * Report of Progress, Geo]. Survey of Canada, 1866, p. 251. fGeology of Canada, 1863, p. 362. DEVONIAN FORMATIONS OF ONTARIO. 229 tion, with the exception of a belt of higher Devonian rocks which crosses the country from Lake Huron to Lake Erie and divides the region into two areas. These newer strata occupy a saddle-shaped depression in the great Cincinnati anti- clinal, which runs nearly east and west through the peninsula, while the course of this depression or synclinal is nearly north and south from Plympton, on Lake Huron, to Orford, on Lake Erie. The belt of higher rocks has a breadth of only about twenty-five miles on the anticlinal between the Thames and Sydenham rivers, but on either side it spreads to the northeast and to the southwest along the shores of the two lakes." In two wells, those of London and the " Test well," at Petrolea, the Corniferous is shown to have an approximate thickness of about 200 feet, consisting throughout of hard gray limestone. In all wells where this formation has been struck the rocks appear to have been of uniform character and to consist of white or grayish limestones holding nodules and layers of chert. Oriskany.— The Oriskany formation is but slightly developed in Ontario, being entirely wanting in most of the wells sunk to or beneath its horizon ; again, owing to the carelessness of drillers, its presence may not have been noted. In the townships of Oneida and north Caynga, in Haldi- mand county, it is exposed and forms beds of sandstone aggregating at the most twenty-five feet in thickness. In many of the records obtained from drillers mention is made of a sandstone at about the summit of the Onondaga, but in most cases close inquiry has proven these statements to be fallible, the so-called sandstone being generally a granular dolomite. However, in two wells at least there is strong, evidence of a sandstone occurring at a point near the position occupied by the Oriskany. One of these was a well drilled at Dresden, Camden township, Kent county, wherein the following record was met with, according to the driller: Surface deposits 43 feet. Shale, black 180 " Limestone 12 " Shale ("soapstone") 172 " Limestone 75 " Sandstone 44 " Again, in a well sunk near Dresden, on lot 3, concession 2, Camden township, the following section was, according to the driller, obtained : Sn [face deposits 00 feet, Shale, black 20 " Limestone 30 Shale (" soapstone ") 204 " Limestone 117 Sandstone -10 230 II. P. II. BRUMELL — GAS AND PETROLEUM IN ONTARIO. Onondaga and Lower Hdderberg. — Beneath the Oriskany, when present, and usually directly underneath the Corniferous limestone, is a long series of limestones, dolomites, marls, shales, gypsum, and salt constitut- ing the Onondaga, which for convenience can be made to include the Lower Helderberg. This formation acquires a thickness, in the salt region of Huron county, of at least 1,500 feet, according to the following very accurate record made by Dr T. Sterry Hunt* of a well sunk at Gloderich by Mr Henry Attrill,- of that place: /•'( i I. Inrlies. Surface deposits 7S U Dolomite, with thin limestone layers 278 3 Limestone, with corals, chert and beds of dolomite 27(3 0 Dolomite, with seams of gypsum 24."> 0 Variegated marls, with beds of dolomite 121 () Rock-salt, first bed 30 11 Dolomite, with marls toward the base 32 1 Rock-salt, second bed 25 4 Dolomite G 10 Rock-salt, third bed 34 10 Marls, with dolomite and anhydrite 80 7- Rock-salt, fourth bed 15 5 Dolomite and anhydrite 7 0 Rock-salt, fifth bed 13 6 Marls, soft, with anhydrite 135 G « Rock-salt, sixth bed ' G 0 Marls, soft, with dolomite and anhydrite lo2 0 Total depth . . : 1,517 0 As to what is the greatest actual thickness of the formation it is im- possible to say, as data regarding its lower measures are wanting. In none of the records obtained has there been definitely noted the red and greenish shales indicative of the base of the formation in New York state. According to the records of wells sunk for gas in Bertie township, Wel- land county, it has there a total thickness of 390 feet, consisting of gray and drab dolomites, black shale and gypsum, and in a well at Petrolea it was found to be 905 or more feet thick, as follows : Limestone, hard, white 500 feet. Gypsum SO " Salt and shale 105 " Gypsum SO " Salt and shale 140 " The formation may be thicker, as drilling ceased in the salt and shale. * Report of Progress, Geol. Survey of Canada, 1S70- 77. SILURIAN FORMATIONS OP ONTARIO. 231 Guelph. — Underneath the Onondaga, is met with, over a considerable portion of the province, a series of yellowish to brown and in places bituminous dolomites, having a probable thickness of not more than 160 feet and known as the Guelph formation. These beds have been pierced in many wells in Ontario, but efforts to obtain from drillers definite in- formation as to their thickness and character have been useless, nor has it been found possible to draw any distinction, in records of wells so far obtained, between the dolomites of this formation and the gray dolomite of the Niagara, which immediately underlies it. In the wells of the Bertie township, Welland county, gas field are found about 240 feet of dolomites of Guelph and Niagara age, and in number 1 well sunk by the Port Colborne Natural Gas Light and Fuel company in Humberstone town- ship, Welland county, there are found, according to the driller, 30 feet of shaly dolomite and 188 feet of brown dolomite, with dark-blue shales toward the bottom. In the town of Paris a well was sunk in which 99 feet of Guelph dolomite was found immediately underlying the Onon- daga. The boring was not continued beyond this depth, so it is impos- sible to say what thickness the formation attained at this point. Niagara. — The Niagara formation, the upper beds of which are com- posed of dolomites, as stated above, has a probable thickness in Welland county of about 140 feet, made up of gray dolomites reposing upon about 50 feet of dark shale. It extends throughout the province in a north- westerly direction to Cabotshead, where, according to the Geology of Canada, 1863, it would have a thickness of about 450 feet, and is com- posed of a whitish subcrystalline limestone. On the Welland canal, near Thorold, is seen the following section in ascending order:* Bluish-black bituminous shale 55 feet. Bluish-gray argillaceous limestone 8 " Dark bluish bituminous limestone 8 " Light and dark -gray magnesian limestone 20 " Bluish bituminous limestone 7 " Total 104 " This section does not include two 10-foot beds of bluish-gray magne- sian limestone which maybe of Clinton age, though toward their summit holding two species of fossils characteristic of the Niagara series in New York, nor does it reach the summit of the formation. In Essex county the beds met with in the various wells sunk near Kingsville and Ruth- ven at a depth of from 1,000 to 1,100 feet consist of a light yellowish-gray vesicular dolomite which is probably of Niagara age. It is from this dolomite that the lame flows of gas have been obtained. I Geology of Canada, 1863, p. 322. 161 II. P. II. BRUMKLL — GAS AND PETROLEUM IN ONTARIO. Clinton. — The Clinton, on entering Canada through the Niagara penin- sula, consists of a band of green shale 24 feet thick underlying IS feet of limestone, though in the wells of the Provincial Natural Gas and Fuel company in Bertie township the shales are apparently entirely wanting, the formation consisting, it is said, of 30 feet of white crystalline dolomite, which is grayish toward the base. In number 1 well of the Port Col- borne company there were found beneath the dark shales, indicative of the base of the Niagara. 72 feet of marls and dolomites, which are in all probability attributable to the Clinton. The formation appears to thicken toward the northwest, gradually diminishing again, as proved by the ex- posure which trends to the north from Hamilton toward Collingwood, a little south of which it takes a sweep to the westward. In Wentworth county, in the township of Flamborough West, the Clinton is seen to rest upon about 8 feet of whitish sandstone, constituting the " gray band," which is apparently missing in Welland county, but on the northern extension of the formation proves a very conspicuous feature, forming a terrace upon which the' shale and limestone of the upper part of the Clinton occur. In the many records of wells drilled in the interior of the province evidence is wanting to estimate the thickness or character of the Clinton, though in one, that of a boring at Waterloo, there were said to have been found 114 feet of blue shale lying immediately above red shale undoubtedly of Medina age. In all probability there have been included in this 114 feet the dark shales of the Niagara. Medina. — Following immediately upon the Clinton and, where present, the sandstone of the gray band is a great thickness of red and white sandstones and red and green shales which constitute the Medina. This formation has its greatest thickness in the Niagara peninsula, gradually diminishing toward the north, where, at Cape Commodore, in Grey county, there are seen beneath the Clinton limestone 109 feet of red and green shales resting upon strata of the Hudson River formation. In number 1 well, drilled in Port Colborne by the Port Colborne company, the measures penetrated for a distance of 770 feet were — Red shale, with thin bands of white sandstone 50 feet. Red and white sandstone 53 " Soft red shale, with bands of gray and green G07 " Total 770 " Drilling ceased at this point at a distance of at least 200 feet above the base of the formation, as in a well on lot 6, concession 15 of Bertie town- ship, there were found 1,000 feet of strata attributable to the Medina. The best record of the upper beds of the formation is that of the bottom SILURIAN FORMATIONS OP ONTARIO. 233 of number 1 well, drilled by the Provincial company, on lot 35, conces- sion 3, Bertie township, and which is as follows: Red sandstone , 55 feet. Red shale 10 " Blue shale 5 " White sandstone 5 " Bine shale 20 " White sandstone (" gas-n >ck ") 1(3 " Total , Ill " Throughout the gas-fields of Bertie and Humberstone townships this section of the upper bods of the formation appears to lie unite constant, only very slight variations being noted. The most marked is that in number 9 well, drilled by the same company, and wherein was found — Red sandstone 55 feet. Red shale 10 " Blue shale 5 " White sandstone .• 20 " Illue shale 12 " Total 102 " The second white sandstone bed beneath was penetrated only four feet. in a well sunk on lot 11, concession 7, Barton township, Wentworth county, and about forty miles to the northwest of the above-mentioned, there were found 595 feet of red shale, with bluish bands, lying imme- diately above the bluish shales of the Hudson River. Again, a few miles northwest of this place, and at the insane asylum in Hamilton, there were said to have been found 634 feet of red shale, and at Dundas, three miles north of this, in a well sunk in the valley and begun in the Medina, there were found 400 feet of red shale, in both instances resting upon the Hudson River shales. To go back to the eastward again, there were found in a well at Saint Catharines .548 feet of red shale. This does not, however, show the entire thickness of the measures, which in a well at Thorold, eight miles southward, proved to be 930 feet thick, as follows : Red sandstone 30 feet. Shale 57 " Gray sandstone 30 Red shale 813 " Total 930 " XXXV— Bull. Geol. Soc. Am., Vol. 4, 1882. 234 II. P. IT. BKUMELL — GAS AND PETROLEUM IN ONTARIO. Many other records of wells bored into or through this formation are at hand, which go to show that it varies locally as to thickness, yet con- stantly diminishes toward the north. Of the formation in the western part of the province but little is known, as west of London, where it con- sists of 500 feet of red shale, it has not been reached in the borings thus far put down. Hudson River. — The Hudson River, which is next met with, plays a very unimportant part in the geology of gas and oil in Ontario, and con- sists, in that part of the province under consideration, of a series of shales and limestones immediately underlying the red and green shales of the Medina. Unfortunately the great area of its supposed exposure north of Toronto is overlaid with drift, but where the exposures are to be seen they consist, as in the township of Toronto, Peel county, " of a scries of bluish-gray argillaceous shales enclosing bands of calcareous sandstone sometimes approaching to a limestone and of variable thickness.'1 * These sandstone bands are slaty in places, though at times having a solid thickness of a foot. The formation has been reached in a considerable number of wells — among others, those at Saint Catharines, Thorold, number 14 of the Provincial company, in Bertie, all in the Niagara peninsula; Swansea and Mimico, near Toronto; Toronto, Hamilton, Brantford and London, where it was penetrated for 150 feet and found to consist of limestone and shale. In the wells at Swansea and Mimico there were found 440 and 493 feet respectively of bluish-gray shale. This does not of necessity represent the total thickness of the formation at these points, as boring began upon it immediately beneath the surface deposits, in the Thorold well, where the formation was met with at depth, it was found to consist of 700 feet of blue shale, and at Saint Catharines it had a similar character and thickness. It is quite probable that in the various borings limestone was found, though on account of its shaly character it was termed shale by the drillers. Utica. — The Utica formation, upon which the Hudson river rests, is found, wherever met with in drillings, to consist of a series of dark-brown bituminous shales, becoming in places bluish toward their base, and having a thickness of from 200 to 400 feet. Of its exact thickness in any well it is very difficult to speak, on account of the similarity between its upper members and the lower strata of the Hudson river. Trenton and Black River. — Beneath the Utica shales there is met with a thick series of bluish limestones, which constitute the Trenton forma- tion, including also the Black River. This series, which is regarded as the Mecca of all Ohio drillers, has proved itself, in Ontario, to be com- *Geology of Canada, 1863, p. 212 SILURIAN FORMATIONS OF ONTARIO. ZOO paratively barren of gas or oil. Of its productive properties, however, more will be said later. In eastern Ontario it covers a large area, but west of Toronto and Collingwood the series is overlaid by the Utica an 1 newer formations, with the exception of a small area in the vicinity of Collingwood, where it is seen to consist of bluish limestone, having a slight dip to the southwest. In the few wells wherein it has been reached the character of the rocks is apparently unchanged, though its thickness varies considerably. For instance, at Whitby, east of Toronto, it has a thickness of 600 feet; at Toronto, 585 feet; Swansea, 602 feet; Colling- wood, 553 feet, and Saint Catharines, 667 feet, in all of which places the formation was entirely traversed, the drillings, with the exception of the well at Saint Catharines, ceasing on the striking of the Archean rocks immediately beneath. In the case of the boring at Saint Catharines the drill, penetrated 27 feet of white quartzose sandstone, which may be Pa- leozoic or belong to the arkose beds. Geologic Horizons in Ontario yielding Gas and Oil. oil wells in the corniferous limestone. Age and Depth. — Of the occurrence of petroleum in Ontario but little can be said. In Lambton county, where it has been produced for 30 years, it is found in the Corniferous limestone at a depth of about 475 feet, the record of a well bored near the Imperial refinery, Petroleaj being as follows : T, „, , Thickness in Formation. Strata. ^gej Surface deposits 104 f Limestone 40 | Shale 130 Hamilton -J Limestone 15 | Shale 4:5 I Limestone 68 „ .c i Limestone, soft 40 Corniferous 1 Limesti me, gray, oil rock zo Depth 465 Annual Output of Oil. — Some 3,000 wells are now producing and afford about 800,000 barrels per annum, making the average daily production about two-thirds of a barrel per well. The oil is dark-colored and of from 31° to 35° Baume in gravity; nor is it an oil that can be easily refined, on account of the considerable proportion of sulphur it contains in a form as yet undetermined. 236 H. T. II. BRUMELL — GAS AND PETROLEUM IN ONTARIO. Chemical Composition of the Oil. — According to returns received from the refineries for the year 1880 it has a commercial content of — Benzine and naphtha L6 per cent. Illuminating oil 3S.7 " Paratfine, gas and other oils and wax L'."i.."> " Waste (coke, tar and heavy residuum) :}4.4 " 100.0 The Corniferous petroliferous over awide Area. — While the Corniferous af- fords commercial quantities of oil only in Lambton county, explorations have proved it to he petroliferous over a wide extent of country, including the northern part of Kent, the eastern part of Middlesex, and southern part of Oxford. In the county of Essex oil has been found at two points, presumably in the Niagara or upper strata of the Clinton. At Comber, in this county, small quantities of heavy black oil were found in a hard limestone at 1,270 feet, and again at Walker's well number 2, on lot 8, concession 6, Colchester township, oil similar in appearance and gravity was found at 1,000 feet in a brownish limestone. This well is said to have pumped five barrels per day. THE MEDINA AS AN OIL-PRODUCER. The only other formation wherein oil has been struck is the Medina, in which, in Humberstone township, Welland county, it has been noted in two wells. These are on lots 11 and 12, concession 3, and are said to have flowed four and two barrels each per day respectively. The oil occurs in the second white sandstone bed, about 100 feet beneath the summit of the formation. The oil is of light claret color, of about 45° Baume gravity, and is apparently free from sulphur. Further work in search of this oil has not yet been undertaken. GAS-BEARING HORIZONS: CLINTON, MEDINA AND OTHERS. Localities indicated. — Gas is found in large quantities at two horizons only, viz, one, which is still doubtful though in the neighborhood of the Clinton, in Essex county; and in the Medina, in Welland. In the former county, in the vicinity of Ruthven, Gosfield township, there have been sunk several wells, in three of which were found huge quantities of gas, in each ease emanating from a gray vesicular dolomite at a depth of about 1,000 feet. Depth at which Gas is found. — In Welland count}', wherein the gas field covers a much greater area than that of Essex, the gas is found almost entirely in the Medina sandstone, about 100 feet below the summit of the formation and at a depth of about 830 feet. The record of number 1 DEPTH AND CAPACITY OF WELLS. 237 Thickness in feet. 9 well, drilled on lot -'55, concession 3, Bertie township, by the Provincial Natural Gas and Fuel company, is a follows : Formation. Strata. Surface deposits • Corniferous Dark-gray limestone Onondaga Gray and drab dolomites, black shales and gypsum. . Guelph and Niagara. . . Gray dolomite Niagara ... Black shale Clinton White crystalline dolomite, gray toward bottom. . . Red sandstone Red shale Blue shale White sandstone Blue shale White sandstone (" gas-rock ") Medina. Total . 390 240 50 30 55 10 5 5 20 16 846 Records of twenty-eight Wells. — In the above well 2,000 ,000 cubic feet of gas per day were struck at a depth of 836 feet, or six feet in the second white sandstone bed. This company have drilled some thirty wells, the records of which do not differ materially from that given above, though capacity varies greatly, as may be seen from the following table : Number of the well. 1. 9 Cubic feet per day. . 2,050,000 375,000 600,000 . 2,200,000 3 -1 5 8,500,000 6 70,000 7 3,000,000 8 47,000 .9 3,500,000 10 4,500,000 11 300,000 12 5,500,000 13 300,000 14 5,000 Number of the well. Cubic feet per day. 15 50,000 16 12,500,000 17 2,500,000 18 2,000,000 19 1,500,000 20 300,000 21 None. 22 2,600,000 23 30,000 25 500,000 26 2,750,000 27 None. 28.-. Limited. Gas-bearing Bed of the Medina. — In all of these wells, with the exception of number 22, the entire flow was obtained from the second white sand- stone bed of the Medina; nor are these the only wells producing large quantities of gas from that horizon, as shown below. Daily Capacity of some of (he Wells. — The largest gas well is that known as Coste number 1, drilled by the Ontario Natural Gas company on lot 7, concession 1, of Gosfield, and carried to a depth of 1,021 feet, wherein 238 n. j'. n. brumell — gas and petroleum in Ontario. at 1,017 feet a flow of gas equal to 10,000,000 cubic feet per day was found. Another was drilled by the Citizens' Gas, Oil and Piping com- pany of Kingsville on the road allowance aboui 55 yards west of the above-mentioned well, and afforded 7,000,000 feet per day, from a rock similar in character and depth to that in Coste number 1. On lot 7, concession 1, of Gosfield. the Citizens' company again drilled and found gas to the extent of 2,500,000 cubic feet per day, and I understand that the Ontario company have been quite successful in a boring made southeast of their Coste number 1, having obtained there a heavy flow, estimated at 7,000,000 feet per day. All efforts to find gas north and northwest of this group of wells have been futile, the beds being found to be flooded with salt water. Other Localities. — Among other lesser producers may he mentioned Carrolls, in Humberstone township, which afforded 1,000,000 cubic feet per day. At Cayuga, in Haldimand county, west of Welland, a consid- erable flow was found in the Medina as well as at Dunnville, about mid- way between Port Colborne and Cayuga. In wells bored to or through the Medina north and northwest of Welland, and the wells mentioned above, the formation has been found to be practically barren of gas, the only boring wherein it Avas noted being at Beeton. where in a soft sand- stone just beneath the surface deposits a small quantity occurred. The Clinton a* a Gas-producer. — The Clinton in a small number of wells has afforded large quantities of gas, the most marked instances being those in Welland count}r, known as Near's, Reebe's and Hopkins' num- ber 2, each of which produced 400,000 cubic feet per day, and the Mu- tual company's well, which produced 1,500,000 cubic feet. These wells are all in that district wherein the Medina is so productive, a fact that rather tends to suggest that the gas is adventitious. Outside of this count}7 the Clinton has not as yet produced a single cubic foot of gas. Exception must, of course, be taken to this statement if it be proved that the productive horizon in Essex county is in that formation. The Niagara as a das- producer. — In Welland county the Niagara also is a large producer of gas. well number 22 of the Provincial company affording 1,850,000 cubic feet per day from the limestones of the upper part of the formation, while in a well sunk a few miles north of this, at Niagara Falls South, a flow of 50,000 cubic feet was obtained in the shales beneath the limestone. OTHER GAS-BEARING FOli.VATIOXS. There now remain to be spoken of only three formations which have afforded gas, though only as yet in small quantities. They arc the Onondaga, the Trenton, and a sandstone of age anterior to the latter. GAS FROM THE TRENTON AND ONONDAGA. 239 The Onondaga as a Gas-producer. — The occurrence of gas in the Onon- daga, even in the small quantities noted, is unique. At Blyth, Huron county, and in the midst of a considerable number of wells bored in the salt region, a well was drilled which afforded, according to the driller, the following record : Surface deposits 104 feet. Limestone 300 (?) 346 " " Black shale " 100 " "Hard rock" 170 " Shale 105 " Rock-salt 00 " Total 1,215 " In the black shales considerable quantities of gas were obtained, not, however, sufficient to he of commercial value. The Trenton ax a Gas-producer. — The Trenton formation has not as yet afforded any considerable quantities of gas, though pierced at many points, the most westerly being Stratford, where it was found at 2,360 feet and penetrated for 24 feet, where a heavy flow of salt water caused the abandon- ment of the work. Coining eastward, the point where it was next struck was on lot 16, concession 15, Brantford township, Brant county, where it was reached at a depth of 1,950 feet and a small quantity only of gas obtained at its summit. At Dundas, near Hamilton, in Wentworth county, it was struck at 1,43!) feet and found to he barren. Again, at Thorold, Welland county, about 40 miles east of Hamilton, the Trenton was struck at 1,905 feet and penetrated for 525 feet, where a very small How of gas was noted. About S miles north of this, at Saint Catharines, it was again reached, being struck at 1,506 feet and found to be barren, although the entire formation was traversed. Again east of Thorold and on lot 6, concession 15, of Bertie township, it was struck at 2,525 feet in well number 14 of the Provincial company, wherein it was traversed for 195 feet without affording gas. The foregoing three wells are the only ones in which the Trenton was reached south of Lake Ontario. On the northern side, however, it has been met with in all wells drilled close to the lake shore. In Toronto several wells were sunk, operations com- mencing upon the Hudson River formation and the drilling continued deep into or through the Trenton without finding gas; but at Mimico, about 8 miles west, three wells have afforded small quantities, the great- est flow being about 50,000 cubic feet per day. In and around Colling- wood several wells, beginning in the upper beds of the formation and continued to its base, afforded small Hows, the greatest being about 6,000 cubic feet per day. 240 II. P. ir. BRUMELL — GAS AND PETROLEUM IN ONTARIO. It will thus be soon that in Ontario the Trenton as a large producer has proved so far anything but successful. Even at lunulas, on the crown of the Dundas anticlinal, no gas was found. There, however, re- mains in the western and southwestern portion of the province a large area as yet untouched, wherein it may afford large quantities and prove of as great value as it has further southward, in Ohio. The following table exhibits the position of the Trenton in southwest- ern Ontario in regard to tide level. Locality of well. Toronto, Swansea . . . Mimico Collingwood, City. . . Delphi. Dundas Saint Catharines. . . . Thorold Provincial company, numbei 14 Brant ford Stratford Elevation of well above tide. Feet. About 347 250 592 600 300 .297 517 About 020 672 1,185 1, Elevation of summit of Trenton. Feet. — 296 — 44:; Begun on + 552 — 1,130 — 1,21)'.) — 1,388 - 1,905 -1,278 - 1,175 Thickness of Trenton. E < t. 602 Trenton. flii7 Elevation of base of Trenton. Feet. — 898 Not reached. + 39 Not reached. ....do — 1,876 Nut reached. .do .do .do I las in Tren- ton— cubic feet per day. None. A I .out 5,000 " r,,ooo " 0,000 None. None. Very small. None. Very small. None. Unfortunately no analyses or close examinations have as yet been made of the Trenton limestone in that part of the province under con- sideration, the only analyses available being those of specimens from quarries considerably to the east of the portion where it is under cover. An unusual Occur re ace of Gas. — A rather peculiar occurrence of gas is that found in the well near Saint Catharines. In this boring a yellow quartzose sandstone beneath the Trenton limestone was penetrated for seventy-seven foot and afforded a small quantity of gas, insufficient for commercial purposes. Forthcoming Publication on the Subject. In closing, I should like to draw attention to the fact that a detailed description of wells bored in Ontario, accompanied by maps and sections, is now in press and will shortly he issued by the Canadian Geological Survey. In this will be found a more or less complete narrative of bor- ing operations tip to the close of the calendar year 1890. BULLETIN OF THE GEOLOGICAL SOCIETY OF AMERICA Vol. 4, pp. 241-244 May 20, 1893 NOTES ON THE OCCURRENCE OF PETROLEUM IN GASPE, QUEBEC BY H. P. H. BRUMELL (Read before the Society December 30, 1892) CONTENTS Page Earlier History 241 The Locality indicated 2-11 The Oil-bearing Formation described 241 Former Knowledge concerning the Locality 242 Kecent Exploitation 243 History of later Operations not fully known 24 ' Notes on past and present Investigations 243 Continuation of Investigations probable 244 Earlier History, The Locality indicated. — Operations in search of petroleum have been carried on in a desultory manner for about 30 years in the vicinity of Gaspe basin, Gaspe county, Quebec, without as yet any economic result. The presence of oil at depth has, however, been proved through the efforts of " The Petroleum Trust," an English company, which has been operating on the southwest side of Gaspe bay, in the neighborhood of and to the south of Gaspe basin. The Oil-bearing Formation described.— in the eastern part of the Gaspe" peninsula there is a great thickness of sandstones resting conformably upon almost as great a thickness of limestones, the whole being of lower Devonian and possibly partly Upper Silurian age. According to Dr R. W. Ells* these sandstones have a thickness of about 3,000 feet, while the * Report of Progress, Geol. Survey of Canada, 1880-82, p. 5 D D. XXXVI— Bull. Geol. Soc. Am., Vol. 4, 1892. (241) 242 II. 1'. II. BRUMELL — PETROLEUM IX QUEBEC. underlying limestone is estimated at about 2,000 feet. These roeks are largely developed in the vicinity of Gaspe bay, where they form a scries of almost parallel anticlinals, on or near the axes of which the greater part of the exploratory work has been done. Dr R. W. Ells, in the report cited above, speaks of these anticlinals as follows : "The rocks of the series have a considerable development on the several rivers that How into Gaspe hay, where they lie in shallow basins, bounded by the anti- clinals, which bring into view the strata of the lower or Gaspe limestone series. These basins are at least four in number, the dividing anticlinals being known as the Haldimand, the Tar Point, the Point Saint Peter, and the Perce, the most southerly yet recognized. On the south side they rest upon rocks of the Silurian system. The whole formation may therefore be said to occupy a geosynclinal basin, the western limit of which has not yet been traced, but which will probably be found to be continuous with the basin recognized on the Cascapedia river, ami thence extending to the Metapedia." Former Knowledge concerning the Locality. — In the " Geology of Canada," 1863, page 789, the following mention is made of the various natural oil springs of the district. This includes probably all that was known of the occurrence of oil in Gaspe up to that date : "At the oil spring at Silver brook, a tributary of the York river, the petroleum oozes from a mass of sandstone and arenaceous shale, which dips southeastwardly at an angle of 13° and is nearly a mile to the south of the crown of the anticlinal. The oil, which here collects in pools along the brook, has a greenish color and an aromatic odor, which is less disagreeable than that of the petroleum of western Canada. From a boring which has been sunk in the sandstone to a depth of about 200 feet there is an abundant flow of water, accompanied with a little gas and very small quantities of oil. Farther westward, at about twelve miles from the mouth of the river, oil was observed on the surface of the water at the outcrop of the lime- stone. Petroleum is met with at Adams' oil spring, in the rear of lot B of York, nearly two miles east of south from the entrance of Gaspe" basin. It is here found in small quantities floating upon the surface of the water, and near by is a layer of thickened petroleum, mixed with mold, at a depth of a foot beneath the surface of the soil. A mile to the eastward, at Sandy beach, oil is said to occur, and, again, at Haldimandtown, where it rises through the mud on the shore. These three ocalities are upon the sandstone and on the line of the northern anticlinal which passes a little to the north of the Silver Brook oil spring. Farther, to the southeast, on the line of the southern anticlinal and about two miles west of Tar Point, which takes its name from the petroleum found there, another oil spring is said to be found, three-quarters of a mile south of Seal cove. On the south side of the Doug- lastown lagoon, and about a mile west of the village, oil rises in small quantities from the mud on the beach. A well has here been bored to a depth of L25 feel in the sandstone, which dips to the southwest at an angle of 10°, but traces only of oil have been obtained. Farther to the westward oil is said to occur on the second fork of the Douglastown river. Traces of it have also been observed in a brook RECENT OPERATIONS IN GASPE] 213 near Saint George's cove, on the northeast side of Gaspe hay. In none of these localities do the springs yield any large quantities of oil, nor have the borings, which have been made in two places, been as yet successful. The above indications are, however, interesting, inasmuch as they show the existence of petroleum over a considerable area in this region, some part of which may perhaps furnish availa- ble quantities of tins material." Recent Exploitation. History of biter Operations not fully knoion. — Regarding later operations but little is known, as owing to the distance from our usual fields of work and the disinclination of operators to impart information it has been found impossible to closely follow actual operations. However, this much is known, that oil has been found at some depth, though in small quantities. ■ Notes on past and present Investigations. — The following notes are gleaned from a report on mines and minerals of the province of Quebec recently prepared by J. Obalski, M E, supplemented by information obtained by the writer : At Sand}r Beach, on lot B, York township, two wells were sunk about 20 years ago, one of which is said to have afforded oil, and about a mile above Douglastown, on the southern side of the Saint John river, a well was sunk 125 feet without successful result. At Silver Brook two wells were bored to a depth of 800 and 900 feet respectively, both showing the presence of petroleum, and on the southern side of the York river, near Silver Brook, two borings were made by the Gaspe Oil company to a depth of 700 and 800 feet, in neither of which was oil struck. Subsequent to these a well was sunk at Sandy Brook to a depth of 700 feet, in which oil was found, though in small quantity. The oil, a specimen of which was collected in 1882 by the writer, was brought to the surface of a small pool by the water, which flowed in considerable quantity from the boring, and was a heavy black oil of about 25° Baume gravity. in 1888 the International Oil company of Saint Paul, Minnesota, sunk a shallow well, which was in 1889 deepened to 450 feet without finding oil. The lands and plant owned by this company Were in the same year taken over by "The Petroleum Trust." which lias since sunk five wells in the district. In one of these, bored at Seal cove, a short distance south of the crown of the Tar Point anticlinal, they have met witli a small quantity of high-grade oil. According to one of the drillers, the boring reached a depth of 3,000 feet, of which the upper 2,150 consisted of yellow and white sandstone, followed by 850 feet of bluish shaly limestone, in which, at a depth of about 2,600 feet from the 244 H. P. H. BRUMELL — PETROLEUM TN QUEBEC. surface, the oil was found. The oil, which is green in color, is of about 38° Baume gravity, has an aromatic odor, and is bright ruby red by transmitted light. Continuation of Investigations probable. — The company working at pres- ent expect to continue operations, the results of which, in view of the probable exhaustion in the near future of the Petrolea field in Ontario, will be watched with interest. BULLETIN OF THE GEOLOGICAL SOCIETY OF AMERICA VOL. 4, PP. 245-256 JUNE 8, 1893 THE FAUNAS OF THE SHASTA AND CHICO FORMATIONS BY T. W. STANTON (Read before the Society December 30, 1802) CONTENTS Page Historical Review , 245 Earliest Literature 245 Views of W. M. Gabb 246 The Tejon Controversy 246 Work of the Canadian Geological Survey 248 White's Classification of the California Cretaceous 249 Relation of Shasta and Chico Faunas 241> Identity of Faunas indicated 24!) Local Lists of both Faunas from northern California 250 Original Localities of Chico Fossils 253 Faunas of Queen Charlotte and Nanainio Formations 253 Correlation of Queen Charlotte Formation with the Shasta 253 Correlation of Nanaimo Beds with the Chico 254 The Shasta-Chico Fauna compared with the Fauna of the Blackdown Beds . . 254 Conclusions 255 Historical Review, Earliest Literature. — The earliest published opinion concerning the age of the beds now known as the Chico formation seems to be that of Dr J. B. Trask * who described Ammonites chicoensis and Baculites chicoensis in 1856. On account of the modern aspect of the fossils associated will: those species he referred the strata containing them to the upper Eocene. Shortly afterward Professor J. S. Newberry f discussed the same beds, *Proe. Cal. Aead. Nat. Sci., vol. i, 1850, p. 85. t Pacific R. R. Reports, vol. vi, pt. 2 [1857?], pp. 24, 25. The title-page bears the date 1855, but there is internal evidence that the volume was not published before 1857. XXXVII-Bui.l. Geoi.. Soc. Am., Vol. 4, 1892. (245) 240) T. W. STANTON SHASTA AND CHICO FAUNAS. and, while admitting the presence of modern types of mollusks, consid- ered that the cephalopods were stronger evidence of their Cretaceous age. He also stated that he had obtained a collection of fossils from Nanaimo, Vancouver island, that proved the Cretaceous age of the coal beds at that place. These fossils were placed in the hands of Professor P. B. Meek,* who soon afterward described them. Although at that time he thought that the entire collection came from Nanaimo, he believed that two dis- tinct horizons were represented. Many years afterward, when repub- lishing the descriptions with figures,t he stated that only those species which he believed to be the older came from Nanaimo, while the others were from Comox, northwest of Nanaimo, and from Sucia island. Those from the last two localities were thought to indicate about the horizon of the Fort Pierre shales, or number 4 of Meek and Hayden's upper Mis- souri section.'! In 1858 Dr B. F. Shumard § described three species of Cretaceous fossils from Nanaimo, and in 1861 Dr James Hector || published an account of the Nanaimo coal field, giving the evidence of its Cretace- ous age. Views of W. M. Gabb, — Up to this time both the geologic and the pale- on tologic work had been mainly preliminary, the latter based on very small collections brought in by explorers; and it was not until 18(34, when the first volume of the Paleontology of California was published, that any serious attempt was made to classify the Cretaceous formations of the Pacific coast or to present their paleontology in a systematic manner. In that volume Mr W. M. Gabb described about 260 species of fossils which he referred to the Cretaceous. In the introduction some general statements concerning the classification and correlation of the California Cretaceous were given by Professor J. D. Whitney ,^[ the state geologist, on the authority of Mr Gabb. All the Cretaceous beds on the Pacific coast were assigned to two divisions {A and 7>), winch were to- gether supposed to represent the Upper Chalk or White Chalk of Europe and the Fort Pierre and Fox Hills groups of the upper Missouri, although the Cretaceous of the latter region seemed to have no species in common with the California strata. The Tejon Controversy. — The publication of this volume precipitated a discussion between Messrs Gabb, Conrad and others as to the age of * Trans. Albany Institute, vol. iv, 1858-'64, pp. 36-49. i Bull. U. S. Geol. Snrv. Terr., vol. ii, 1876, pp. 351-374. [The same opinion is expressed in Professor Week's last work-, 1'. S. Geol. Surv. Terr., vol. ix, Invert. Paleontology, p. xxv. I Trans. St. Louis Acad. Sri., vol. i, 1858, pp. 123-125. || Quart. .Jour. Geol. Soc. Liond., vol. xvii, 1861, pp. 428-436. «| Paleontology of Cal., vol. i, L864, p. xix. EOCENE FACIES OF THE TEJON. 247 division "2?," now known as the Tejon formation, Mr Conrad asserting that it is Eocene and Mr Gabb as strenuously maintaining its Cretaceous age* On the one hand, the unquestionable fact that a number of the fossils are identical or closely related with species that elsewhere charac- terize the Eocene was regarded as proof of its Tertiary age ; while on the other hand, the presence of an ammonite (Ammonites jugalis) and the apparently close faunal and stratigraphic connection with the Cretaceous beds beneath were believed to prove its Cretaceous age. According to Mr Gabb's f statement in one of his controversial articles, 23 species of the 107 in division B are found in the underlying beds. When his list of common species is critically examined, however, it is seen that, with the exception of the Ammonites and perhaps two or three others, they all belong to genera that have lived from the Cretaceous or earlier to the 1 tresent time without undergoing much change. Professor Angelo Heil- prin \ has given a careful review of all the published evidence bearing on this question, and in preparing it he has studied a large part of Mr Gabb's original collections of California fossils. His article is a strong argument for the Eocene age of the Tejon and incidentally it throws considerable doubt on the accuracy of Mr Gabb's statements concerning the species that occur in both the Chico and the Tejon. Professor Jules Marcou§ and Dr C. A. White || have also referred the Tejon, or division B, to the Eocene, and this view is now generally accepted. While admitting its Tertiary age, both Dr White ^[ and Dr G. F. Becker,** after studying the subject in the field, have stated their belief that in southern California the Tejon, is only the upper part of an unbroken series, the Chico-Tejon, in which the sedimentation as well as the life was continuous from the Cretaceous into the Tertiary. In the second volume of the Paleontology of California, published in 1869, Professor Whitney ff again summarized Mr Gabb's latest views on the classification of the Cretaceous. Division B is named the Tejon and considered to be the probable equivalent of the Maestricht beds. Division ^1 is separated into three groups : the Martinez group, which is doubtfully separated from the one next below ; the Chico group, which ♦Conrad's articles arc in Am. Jour. Conch., vol. i, 18G5, pp. 3G2-305; vol. ii, 1866, pp. 97-100, and Am. Jour. Sci., vol. xliv, 1867, pp. 376-377. Gabb's replies may lie found in Am. Jour. Conch., vol. ii, pp. 87-92; Am. Jour. Sci., vol. xliv, 'pp. 226-229, and Proc. Cal. Acad. Nat. Sci., vol. iii, 1867, pp. 301- 306. fProc. Cal. Acad. Nat. Sci., vol. iii, 1867, p. 302. JProc. Acad. Nat. Sci. Phi la., 1882, pp. 195-214 ; Contributions to Tertiary Geol. and Paleont. of flic United States, 1884, pp. 102-117. g Bull. Soc. Geol. de France, tome xi, 1883, pp. 417-435. || Bull. 15, U. S. Geol. Survey, 1S85, pp. 11-17; Bull. 51, 1889, pp. 11-14; Bull. 82,1891, p. 193. U See references just given. ** Bull. 19, U. S. Geol. Surv., 1885. +t Pages xiii and xiv. 248 T. W. STANTON SHASTA AND CHICO FAUNAS. is correlated with the Upper Chalk or Lower Chalk and, it is thought, may prove to be the equivalent of both, is said to include all the known Cretaceous of Oregon and of the extreme northern part of California and the coal-hearing beds of Vancouver island; and the Shasta group, pro- visionally formed to include a series of beds of different ages below the Chico. According to Whitney "it contains fossils, seemingly represent- ing ages from the Gault to the Necomian, inclusive. . . . Few or none of its fossils are known to extend upward into the Chico group." Work of the Canadian Geological Survey. — In 1871 the geological survey of Canada began the work in British Columbia which has contributed greatly to our knowledge of the Mesozoic formations of the Pacific coast. It is beyond the scope of this paper to consider the detailed geologic description of the Cretaceous on Vancouver and Queen Charlotte islands and the mainland of British Columbia, as given by Mr James Richard- son* and Dr George M. Dawson. f These reports have shown that the Cretaceous attains thicknesses of over 5,000 feet on Vancouver island and of about 13,000 feet on Queen Char- lotte islands. The invertebrate fossils from both these areas have been described and fully discussed by Mr J. F. Whiteaves.| The most recently published conclusions of this author are that the larger part (divisions C, D, and E) of the Queen Charlotte islands section is the equivalent of the Shasta formation, and that the same horizon is represented in the northern part of Vancouver island and at several localities on the main- land of British Columbia; that the beds of the Nanaimo and Comox coal fields on the eastern coast of Vancouver island are more recent and referable to the Chico formation, and that none of these beds are older than the Gault. Previously Mr Whiteaves had expressed the opinion that the Shasta formation and its equivalents in British Columbia should be separated into two formations, referring the older beds, which are especially characterized by an abundance of Aucella, to the Necomian and the upper portion to the Gault; but additional collections showed such a blending of the faunas that they could not be separated and this view was abandoned. * Report on the coal fields of the east coast of Vancouver Island : Geol. Surv. Canada, Rept. of Prog. 1871-72, pp. 73-loit; Rept. on the coal fields of Vancouver and Queen Charlotte Islands : Ibid., 1872-'73, pp. 32-65. f For example— Report on the Queen Charlotte Islands: Ibid., 1878-79, pp. 1-101 B; On a Geologi- cal Examination of the northern Part of Vancouver Island : Ann. Kept. Geo). Survey < 'anada, 1886, pp. 1-107 B ; On the earlier Cretaceous Rocks of the northwestern Portion of the Dominion of Canada : Am. Jour. Sci., vol. xxxviii, 1889, pp. 120-127. t Geol. Survey Can. : Mesozoic Fossils, vol. i, pt. 1, Invertebrates from Queen Charlotte Islands, 1876; pt. 2, Fossils of the Cretaceous Rocks of Vancouver, 1879; pt. 3, Fossils of the coal-bearing deposits of Queen Charlotte Islands, 1884. See also Trans. Roy, Soc. Canada, vol. i, 1882, sec iv, pp. 81-86, and Cont. to Canadian Paleont., vol. i, pt. 2, 1889. USE OF DILLER'S COLLECTIONS. 249 White's Classification of the California Cretaceous. — DrC. A. White, whoso work on the Cretaeeous of California has already been referred to, also recognized two divisions in the Shasta, to which he gave the local names, Knoxville and Horsetown beds, although he believed them to be closely related ; and several species of the Horsetown fauna were afterward found associated in the same strata with Aucella, the characteristic fossil of the Knoxville beds, near Riddles, Oregon.* It may therefore be regarded as established that the Knoxville beds should not be considered distinct from the remainder of the Shasta formation, although they may usually be recognized by the great abundance of Aucella, a fossil that seems not to range into the upper part of the scries. The great apparent difference in the faunas of the Shasta and the < hico formations at the localities studied by him led Dr White to believe that there is a break between these two formations, representing a great time- hiatus.f although they are apparently conformable. The list of species assigned to each formation by Mr Gabb also seemed to justify this belief, but the sequel will show that the stratigraphic position and the vertical range of many of the species were very imperfectly known until quite recently. Relation of Shasta and Chico Faunas. Identity of Fauna* indicated. — Various members of the United States Geological Survey working in California and Oregon during the last few years have from time to time made small collections of Cretaceous fossils that have been submitted to Dr White for examination. The largest of these collections was received from Mr J. S. Diller in 1889, and was assigned to me for study and identification, under the direction and supervision of Dr White. The collection embraced small lots of fossils from about seventy-five different localities in northern California and southern Oregon, the most of which are in the valley of Sacramento river.;}; There were usually only a few species of fossils from each locality, as they were collected by the geologists in connection with other field-work and without any attempt at making exhaustive collections. The fossils were identified and those from each locality were, so far as practicable, assigned to tbe Shasta or to the Chico-Tejon, in accordance with the distribution of species in those formations given by Mr Gabb. But some of the locali- ties seemed to show a mixture of Shasta and Chico species, and when *See G. F. Becker, Notes on the early Cretaceous of California and Oregon : Bull. Geol. Soc. Am., vol. 2, 1891, pp. 204-205. fSee Hull. U. S. Geol. Survey, numbers 15, 22, 51 and 82. J For description of the geology of this region and further discussion of the paleontology see Mr Piller's paper, this volume, pp. 205-224. 250 T. W. STANTON — SHASTA AND CHICO FAUNAS. Mr Diller plotted all the localities on the map those that were assigned to different horizons were seen to be inexplicably mixed. Mr Diller at that time suggested that the two faunas were more closely related than had hitherto been supposed, but the evidence; did not then seem to be conclusive. Local Lists of both Faunas from northern California. — During the past held season Mr Diller had considerable collections made at Horsetown,* Shasta county, California, and at Texas springs, less than two miles east of Horsetown. These fossils, which have recently been studied, gave unquestionable proof of the blending of the Shasta, and Chico faunas. M i- 1 >iller says that the beds from which the fossils were collected at thes< i two localities are of no considerable thickness. Besides the nature of the matrix, the state of preservation of the fossils and the manner in which the species are commingled on hand specimens, all indicate that the entire collection came from the same horizon. I have therefore listed the fossils from both localities together, as follows : u u ^Ammonites hoffmanni, Gabb. * Ammonites breweri, *Diptychoceras Isevis, Ancyhceras (?) lineatus, " *Belemnites impressus, " Liocium punctatum, " *Lunatia avellana, Gyrodes. Fusus aralns, Gabb. *Anisomyon meekii, Gabb (?) Scalaria albensis (?), D'Orb., Whit- eaves. Actseonina califomica, Gabb. Cinulia. f Ringicula varia, Gabb. *Ringinella polita, " fPanopsea concentrica, " \Cucullasa truncata, \Nemodon Vancouver ensis, Meek. jTri(/onia sequicostata, Gabb. 'I'Trii/oiiia leana, Trigonia. fPecten operculiformis, Gabb. f Thetis annulata (Gabb) = Cardium (Lsevicardium) annulatum. 'I'Corbula traskii, Gabb. fMytilti* tjioidraius, Gabb (?) Mytilus lanceolatus, Sowerby. \Leda translucida, Gabb. *Pleuromya laevigata, Whiteaves. ~\Tellina hoffmanniana, Gabb. fTellina mathewsonii, " \Maetra ashbtirneri, " fChione varians, " fMeekia radiata, " fMeekia navis, " fMeekia sella, " Rhynchonella. *Mostofthe localities mentioned are shown on the sketch map prepared by Mr J. S. Diller, forming plate 1, page 205, of this volume. *fThe species belonging to Mr Gabb's Shasta fauna arc marked with an asterisk (*), those belonging t<> t h> ■ < h ieu u i 1 1 » an obelisk (t). The others have not been positively assigned to either horizon. Mr Gabb's nomenclature is used, in most- cases without revision, throughout this paper. HULEN CREEK AND ONO COLLECTIONS. 251 Of the 36 species in this list, the Paleontology of California gives 8 as coming from the Shasta and 18 from the Chico, while 2 of the others are doubtfully referred to the former and 2 to the latter. At least 12 of these species are also represented by identical or very closely related species in the Queen Charlotte islands (lower shales), and 7 are similarly repre- sented in the equivalent of the Chico on Vancouver island. It will be remembered that Horsetown is a typical and well known Shasta locality, and that the types of two of Mr Gabb's species were obtained there. Many of Mr Diller's localities for fossils are on Cottonwood creek and its branches, a few miles southwest of Horsetown. It will be instructive to group together some of these places and consider the fossils that were obtained from them. On Hulen creek, and near its mouth on Cotton- wood creek, the following were collected : Ammonites bated, Trask. Ammonite* hoffmanni, Gabb. . Immonites remondi, Turritella. Cytherea. Trigonia evansana, Meek. Trigonia tryoniana, Gabb. Nemodon Vancouver ends, Meek. Cucidlsea truncata, Gabb. Pecten opercuHformis, " This collection adds two Shasta and two Chico species to the Horsetown and Texas springs list. At and about Ono, California, mostly within a mile of the village, the following species were obtained : Ammonites bates!, Trask. Ammonite* breweri, Gabb. Ammonite* hoffnianni, " . Immonites remondi, Martesia clausa, Gabb. Tu/rnus plenus, l'~ Pleuromya laevigata, Whiteaves. Trigonia leana, Gabb. Ammonites (Phylhceras) ramosus, Trigonia sequicostata, (?) Meek. Ancyloceras remondi, Gabb. Belemnites impressus, Cinulia mathewsoni, Lunatia avellana, J'oln m ides diode mil, Ringinella polita, An eli nra. Nerinsea maudensis, Whiteaves. a a u a Trigonia evansana, Meek. Nemodon vancouverensis, " Plicatula variata, Gabb. Pecten open-id i form is, '* Avicula mucronata, Whiteaves. Pinna. Ostrea. Eriphyla. Most of the species in this list not contained in the preceding ones were originally described as from the Shasta. 252 T. W. STANTON — SHASTA AND CHICO FAUNAS. Localities at Gas Point post office and on Roaring river, not far dis- tant, yielded the following: Ammonites chicoensis, Trask. Turriteila seriaMm-granulata, Gabb, not Koemer. Nucula truncata, Gabb. On the Cold fork of Cottonwood creek the following collection was obtained : Bacidites chicoensis, Trask. Cucullsea truncata, Gabb. Belemnites impressus, Gabb. Pecten traskii, " (?) Neptunea hoffmanni, " Ostrea. Nucula truncata, " Terebratetta obesd, " Two of these species are common to Horsetown and Texas springs. Going a few miles farther southward, the first important localities are on Elder creek, on the line of one of Mr Diller's measured sections. Near Lowry's and at other places farther westward specimens of Aucella piochii, Cod))), were obtained, while a higher horizon about two miles east of Lowry's yielded the following species : Gyrodes excavata (Mi chelin), Whit- Venus lenticularis, Gabb. eaves. Tellina parilis, " Lunatia. Tellina ashburneri, '' Anchura californica, Gabb. Cucullcea truncata, " Dentalium stramintum, " Astarte conradiana, " (?) Thetis annulata, ■ " Pecten operculiformis, " Chione various, " Avicula. This lot shows a greater difference than any of the others, although it contains at least four species enumerated from other localities above given. Sufficient evidence has therefore been presented to show that all the species from the several localities mentioned very probably belong to one fauna. Near Redding, on Sacramento river, a large number of species were collected, many of which were not obtained at any of the above localities, but the presence there of such forms as Cucullsea truncata, Trigonia evan- sana, Pecten operculiformis, Corbula traskii, etc, make it probable that the beds belong to the same continuous series, though they may represent a somewhat higher horizon. Collections from several localities in Oregon that have always been referred to the Chico formation, such as Crooked river. Siskiyou moun- ABANDONMENT OF THE MARTINEZ GROUP. 253 tains, Ashland, and several places in Jackson county, indicate about the same horizon as that of the bed at Horsetown. Original Localities of Chico Fossil*. — In the second volume of the Pale- ontology of California there is a " Synopsis of the Cretaceous invertebrate fossils of California/' giving a complete list of the species then known, with the localities at which they had been obtained. For convenience in making comparisons I have made a list of the species reported from each locality there mentioned. Leaving out of consideration the locali- ties from which only from one to three species are reported, there are sixteen localities from winch Chico fossils were obtained. An examina- tion of the faunal lists from these places show that eleven of them may be referred without question to the Shasta-Chico fauna as represented at Horsetown and in the neighborhood of Cottonwood creek. These local- ities are: Benicia, Cottonwood creek, Crooked creek of the Des. Chutes (Oregon), Curry's. Jacksonville (Oregon), Martinez, mount Diablo, Ores- timba, Pacheco pass, Siskiyou mountains and Tuscan springs. The other five localities, viz, Chico creek, Cow creek, Folsom, Pence's and Texas Flat, yielded a greater proportion of species not contained in Mr Diller's collections from Shasta county, but there are several well marked Horsetown species reported from each of these localities ; and they are all so intimately related to the other Chico localities by means of species held in common with one or more of them that they cannot be regarded as belonging to another fauna. The Martinez group of Gabb has long since been abandoned as insep- arable from the Chico ; and. as Mr Diller has shown in his paper on the Cretaceous and early Tertiary deposits of this region,* the Wallala for- mation probably also belongs in the same series. Faunas of Queen Charlotte and Nanaimo Formations. Correlation of Queen Charlotte Formation with the Shasta. — The correla- tion of the Queen Charlotte formation (divisions C, D and E oi Dr Daw- son's section) with the Shasta has already been mentioned in speaking of Mr Whiteaves' work. The additions now made to the Horsetown fauna materially increase the number of species that occur in both the Shasta and Queen Charlotte formations. It should lie stated, however, that several genera of ammonites found on Queen Charlotte islands and not yet seen in the Shasta suggest a somewhat earlier period for the bed in which they occur. It would simplify the matter if it could be proved that these ammonites came from a lower horizon. It is worthy of note *Ante, pp. 205-224. XXX!VIII— Bull. Geol. Soc. Am., Vol. 4, 1882, 254 T. W. STANTON — SHASTA AND CHTCO FAUNAS. in this connection that the upper shales and sandstones, or division A •of the Queen Charlotte section, contain Inoceramus problemalicus, Schloth., a species that is characteristic of the Colorado formation in the Rocky mountain region and is not known to range higher than the Turonian in Europe. Correlation of Nanaimo Beds with the Chico. — The correlation of the Nanaimo.beds on Vancouver island with the Chico formation, taken in connection with the facts already given, implies that these beds are more closely related to the Queen Charlotte formation than has been supposed, and I think that a comparison of the faunas found in the three regions, California, Vancouver and Queen Charlotte, will give evidence of this relationship. The principal facts that seem to he opposed to this con- clusion arc that some of the species of B 'acuities and of Inoceramus found on Vancouver island are apparently closely related to species in the Montana formation of Nebraska. Colorado and elsewhere in the interior region, and that the plants found in the Nanaimo coal held are said to be of upper Cretaceous types. With the possible exception of the species just mentioned and a few others that have little diagnostic value, it is doubtful whether any of the species of the Shasta-Chico fauna occur in the upper Cretaceous beds east of the Rocky mountains.* The ammonites nearly all belong to genera that are not found in the upper Cretaceous of the interior region and differences almost as great might be pointed out in other classes of mollusks. These facts may readily be explained by supposing that the faunas lived contemporaneously in different oceans separated by a long conti- nental area, but they would also be equally ay ell explained if it could be proved that they were not strictly contemporaneous. The Shasta-Chico Fauna compared with the Fauna of the Black- down Beds. Mr Whiteaves has correlated the Queen Charlotte formation with the Gault, and as confirmatory of this reference it may be of interest to give the results of the comparison 1 have made with one of the English Cre- taceous faunas. In Sowerby's "Mineral Conchology " 4G species of Cretaceous fossils are described from the Blackdown beds of Devonshire, England. These beds have usually been referred to the Gault, though some authors now regard them (at least in part) as „ representing the lowest beds of the *See Dr C A. White's statement on this point in Bull. 15, U. S. Geol. Surv., pp. 27-29. CORRELATION WITH EUROPEAN DEPOSITS. 255 Cenomanian. Of the 46 species figured by Sowerby as coming from Blackdown, at least 23, or one-half of the entire number, are represented in the Shasta-Chico fauna by closely related species. These include such well marked forms as — From Blackdown- Astarte striata. Cuculhva costellata, Cucullsea fibrosa. Exogyra conica, Mytilus edentulus. Mytilus lanceolatus Thetis major. Thetis minor. Trigonia aliformis. Trigonia dxdalca. Trigonia spectabilis Turritella granxdata. Represented in California by — Eriphyla umbonata. (?) Nemodon vancouverensis. ( 'ucullsea truncata. Exogyra, parasitica. Mytilus lanceolatus. (?) Thetis annulata. Trigonia evansana. Trigonia leana. Turritella seriatim-gra n idata. (?) In addition to these the Blackdown beds contain a number of species belonging to the Venerida1 and Aporrhaidse, both of which groups are well represented in the Shasta-Chico fauna. In fact, so far as can be judged by figures and descriptions, the whole fauna of the Blackdown beds, if it had been found in the western part of the United States, would be referred to the Shasta formation and about to the horizon of the Horsetown beds. Whether the Chico beds above the fossil-bearing Horsetown horizon represent all the rest of the upper Cretaceous remains to be determined. The close relationship of their fauna to that of the underlying beds which has been compared with the Gault and Cenomanian, and its distinct- ness from the upper Cretaceous faunas east of the Rocky mountains representing the Turonian and Senonian of Europe seem to favor the view that a large part of the upper Cretaceous series is absent from the Pacific coast. Conclusions. ' In view of all these facts, it seems to me that the exact relationship of the Chico and Tejon formations and the extent to which their faunas are connected must still be regarded as an open question that can be solved only, if at all, after exhaustive collections have been made from both formations and thoroughly studied. 256 T. W. STANTON — SHASTA AND CHICO FAUNAS. The specific conclusions reached may thus he summarized : There is no fauna] break any where in the entire series of strata- that have been referred to the Shasta and Chico formations. Certain portions of the series are characterized by the abundance of particular species, e. g., AuceUa in the lower beds and several species and genera of ammonites in the Horsetown division ; but these sub-faunas are so bound together by connecting species that they cannot be regarded as really distinct, and I have therefore adopted Mr Diller's suggestion and called the whole the Shasta-Chico fauna. The age of this fauna, or at least of the portion found in the Horsetown beds, seems to be not more recent than the Cenomanian. BULL. GE10L. SOC. AM @sooo' Prominent Bed Rock fiiUs /Approximate course of Neocene ChajineC(rem.aiRLng) VOL. A. 1892. PL. 5. no'jo' t20* RECENT AND NEOCENE DRAI NAGE SYSTEMS v Of The Yuba and American Rivers, Sierra Nlvada, California. ao miles -j 3<) 110 JO' / rfpproAimate course of Neocene Channet (eroded) £tQorrect position and eleratton of Neocene Channei BULLETIN OF THE GEOLOGICAL SOCIETY OF AMERICA VOL. 4, PP. 257-298, PLS. 5-9 JUNE 19, 1893 TWO NEOCENE RIVERS OF CALIFORNIA BY WALDEMAR LINDGREN (Presented before Ihc Society December SO, 1892) CONTENTS Page Introduction 258 Review of Literature 25! » < )l (servations on Method of "Work 262 ( Outlines of Geologic History 263 Topography 263 Condition of the Sierra Nevada before and during the Gravel Period. 264 The volcanic Period 266 The Neocene Yuba River 268 The main River 268 From the Sacramento Valley to French Corral 268 The Nevada City and Grass Valley Channels 269 French Corral to North San Juan 270 North San Juan to Badger Hill 270 The North Fork ] 271 The Middle Fork 271 Badger Hill to North Bloomfield 271 North Bloomfield to Snow Point 272 The Derbec Channel 27:; The Forest City Channel 27:; Snow Point to Milton 271 Milton to Meadow Lake 276 The South Fork 277 Badger Hill to Dutch Flat 277 The Channel at Dutch Flat 282 The Liberty Hill Tributary ' 282 The Channel between Alta and Shady Run 283 The Neocene American Liver 284 The South Fork 284 From the Sacramento Valley to Diamond Springs 284 Diamond Springs to Newtown 285 Newtown to Pacific House 286 The North Fork 287 From the Junction to Jones Hill 287 Jones Hill to Bath 288 The Iowa Hill Channel 289 X XXIX— Bull. Gkol. Sue. Am., Vol. 1, 1892. (-57) 25S W. LINDGREN — TWO NEOCENE RIVERS OF CALIFORNIA. Page Bath to Ralstons 290 The Damascus and Last ( lhance Tributaries 291 < feneral character 291 From the Ralston Mine to Summit Valley 291 The lower Course 292 The Duncan Peak Tributary 293 The Canada Hill Tributary 293 The upper Course 293 Discussion of < rrades -"••I ( inclusions -"-IS Introduction. Tlie investigations of the United States Geological Survey in the Gold belt of the Sierra Nevada, carried out under the direction of Dr (i. V. Becker, with whose consent this paper is published, have included the geologic mapping of the country on topographic contour maps on the scale of 1 : 125,000, or about two miles to the inch. During the course of this mapping much information has been gained concerning the Neocene river channels, now largely covered by deep volcanic flows or cut away by subsequent erosion. The auriferous character of the accumulated gravels gives, as is well known, great practical importance to these channels. A large number of the productive Neocene gravel deposits occur in the watersheds of the present Yuba and American rivers, which were in- cluded in the area assigned to the writer. It has been found that these deposits are parts of two river systems which in a general way corre- spond to the two modern rivers now draining the same territory. It is the purpose of the present paper to indicate buiefly the direction of the principal forks of the Neocene Yuba and American rivers, to give a more accurate idea of the Neocene topography within this district, and to call further attention to certain channels which might prove re- munerative if opened by mining operations. The continuity of sonic of these can be asserted and their approximate position indicated. It is not proposed in this place to enter upon any elaborate discussion of the many and interesting questions connected with the accumulation of the gravels, nor is it the intention to describe in detail the often complex channel systems of any particular region* *The term "Neocene" has been used, < sistently with the nomenclature adopted by the Sur- vey, in preference to " Pliocene." The N ;ene comprises tin- Miocene .-mil Pliocene periods of the Tertiary era, between which, in the Sierra Nevada, no definite line can be drawn. It is, in. I I, very probable thai the first period of erosion, the gravel period mm. I tin- volcanic period repre- sent :i large pari of the time between the later Creti us and tin- later Tertian . bul there is no definite floral or faunal evidence t<> support this. work of whitney, le conte and others. 250 Review of Literature. For the first accurate information as to the geologic character and occurrence of the gravel beds we are mainly indebted to the former state geological survey of California under Professor J. D. Whitney. His volume on the Auriferous gravels * containing, besides his own extensive observations, the detailed notes of W. A. Goodyear and Professor W. H. Pettee, marks an epoch in the development of our knowledge of these Neocene deposits. The observations recorded in this book are in general accurate and trustworthy. The "review" at the end of the volume by Goodyear appears, in the light of later investigations, as very excellent indeed, and. while one may differ from some of his conclusions, it must be acknowledged that his views of the channels and of the general topography of the country over which they flowed are confirmed by more detailed and extended surveys. To these investigators belongs the credit of having established the fluviatile character and the age of the deposits, of having recognized the two important river sys- tems corresponding to the present Yuba and American rivers, and of having begun to outline the old drainage lines. Professor Whitney concludes that the Sierra Nevada has not undergone any important changes as to the general level and the grade of its channels, and that the carving of the canyons subsequently to the gravel period was prin- cipally caused by climatic changes. In 1886 Professor Joseph Le Conte published a paper on "A post- Tertiary elevation of the Sierra Nevada shown by the river beds," f in which no new observations were recorded, but which gave an impetus to the investigation by the introduction of a new theory, which, however, had already been suggested by Mr G. K. Gilbert in 18834 In subse- quent papers Professor Le Conte has further elaborated his views, § and in 1891 he published a paper on the " Tertiary and post-Tertiary changes of the Atlantic and Pacific coasts," || in which is found a concise state- ment of his present opinion, which is quoted in full: "The Sierra was formed, as we now know, by lateral crushing ami strata-folding at the end of the Jurassic. But during the long ages of the Cretaceous and Tertiary this range was cut down to a very moderate height, with gentle slopes eastward *.I. D. Whitney: "The Auriferous Gravels of the Sierra Nevada of California." Memoirs of tin.' Museum Comp. Zoo!., vol. <;, no. l, 1880. t Am. .lour. Sei., 3d series, vol. xxxii, 1886, \>. 167. {Review of Professor Whitney's "Climatic Changes;" Science, vol. i, 1883, pp. 141-142, 169-173, an. I 193-195. gForamore extended review of the literature regarding this subject the reader is referred to Mr II. W. Turner's "Mohawk Lake Beds." Bull. Phil. Soc. Washington, vol ix, April, 1891, pp. 385-410, II Bull. Geol. Soc. Am., vol. 'J, pp. 323-330. 260 W. LINDGREN — TWO NEOCENE RIVERS OF CALIFORNIA. and westward from a crest which was probably situated along a line just above the Yosemite and Hetch-Hetchy valleys, for there the erosive biting into the granite axis seems to be deepest. The rivers, by long work, had finally reached their base- levels and rested. The scenery has assumed all the features of an old topography, with gently flowing curves. The continental elevation" — previously described in the same paper — " of the Pliocene did not greatly affect the river slopes of this part. At the end of the Tertiary came the great lava streams, running down the river channels and displacing the rivers; the heaving up of the Siena crust-Mock on its eastern side forming the great favdt cliff there and transferring the crest to the ex- treme eastern margin; the great increase of the western slope and the consequent rejuvenescence of the vital energy of the rivers; the consequent cutting down of these to form the present deep canyons, and the resulting wild, almost savage, scenery of these mountains." Mr J. S. Diller, who has studied the geology of the northern end of the Sierra Nevada north of the fortieth parallel, holds similar views as to the age and elevation of the range. They were first set forth in his " Notes on the Geology of northern California,*'* which, however, does not in- clude any detailed discussion of the Tertiary river deposits on the west- ern slope. His conclusions may he best stated by quoting from a later paper on the " Geology of the Lassen peak district: "f "During the whole of the Cretaceous and the Tertiary the great belt of country lying east of the present Sacramento valley, embracing the region now occupied by the Sierra and a large portion of the Great Basin, was above the sea, and subjected to great degradation, which reduced it almost to its base-level of erosion. This gentle plain swept westward toward the ocean directly across the site of the present Sierra. That the north end of the Sierra country was a lowland during the Miocene, as already shown, is rendered perfectly evident by the character of its flora; and the relation of the Miocene conglomerate to the eastern escarpment north of Honey lake is such as to demonstrate that during the Miocene the Sierras were not yet in existence. Similar conditions continued through the Pliocene, for the Pliocene gravels on the western slope of the Sierras were evidently deposited while its in- clination was very gentle, before the Sierra region had attained any considerable elevation, and apparently also while it was yet a part of the Great Basin platform. * * * The faulting, by means of which the Sierra Nevada range was separated from the Great Basin platform, took place, in a geologic sense, very recently. The eastern escarpment of the range, at least in its northern portion, was evidently formed after the conclusion of the volcanic activity in its immediate vicinity." Since the above was written, Mr Diller has published a paper on the -• Geology of the Taylorville region,"^ in which he shows the Taylorville fault to be an overlhrust instead of a normal fault, as he had previously supposed. This change necessarily modifies his earlier views to some extent. ♦ Bulletin 33, U. S. Geol. Survey, L886. t Eighth Ann. Rep. V. 8. Geol. Survey, 1889, p. 128. | Bull. Geol, Soc. \m., vol. 3, p, 369. WORK OF BECKER, BEOWNE AND HANKS. 261 Dr (i. F. Becker, in his paper on '^Tlie Structure of a portion of the Sierra Nevada of California,"* considers the range to have existed as such during the Tertiary. From the analysis of the extensive fissure system discovered by him he draws the c melusion that no important tilting of the Sierra has taken place at or since the post-Miocene disturb- ances, but that the western slope of the range has been increased by dis- tributed faults along these systems. For the next and very important contribution to the actual knowledge of the Neocene channels one is indebted to Mr Ross E. Browne, who gave the results of his careful and detailed survey of the Forest Hill divide in the tenth annual report of the state mineralogist of California, 1890, pages 435-465 (with maps). Mr Browne's work includes an accurate topographic mapping of the contacts of the Neocene deposits and Hows with the bed-rock, surveys of all tunnels and mines, and determination of elevation of all important points. It is the first work of its kind, and stands as a model for the many similar ones which it is hoped the future will bring forth. It is gradually beginning to be recognized that de- tailed surveys are indispensable when works of such magnitude and cost are contemplated as the opening of important gravel channels. Both on the Forest Hill and Placerville divides large sums of money have been lost by neglecting a sufficiently extended topographic and geologic survey of the region in question. To Mr Browne belongs the credit of having first distinctly recognized the different systems of later channels (channels of tire volcanic period) as contrasted with the older pre-volcanic drainage system. In ( Jood year's notes from Forest Hill and Placerville the existence of such channels is, however, plainly implied. Mr Browne also gives a diagram showing the grades of the Neocene rivers with reference to the longitudinal axis of the Sierra with the view of ascertaining whether tilting of the range can be recognized in the grades of the Neocene channels. f He thinks more data are needed, but " that the evidence, as far as it goes, is against any considerable increase in the slope of the Sierra flank — decidedly against an increase large enough to account per se for the two thousand feet deeper cutting of the modern river." In the same report Mr John Hobson has carefully described and mapped the Iowa, Hill divide in a similar detailed way.J Mr Henry G. Hanks§ still appears to maintain a glacial or partly glacial origin of the gravels. I fear that in upholding this theory he is contending against very heavy odds. No evidence whatever of the ex- * Bull. Geol. Soe. Am., vol. 2, pp. <>1 and 7:;. fOp. eit,, p. 445. | Op. eit., p. 419. I Mining and Scientific Press, San Francisco, April 5, 1890, and following numbers. 262 \V. LINDGREN — TWO NEOCENE RIVERS OF CALIFORNIA. istence of Neocene glaciers has thus far been met with in the highest part of the range in this Latitude; nor is it likely, in view of the char- acter of the Neocene flora high up on the flank of the range, that such evidence will he found. Observations on Method ok Work. The help of a contour map is almost indispensable in order to ohtain a correct idea of the Neocene drainage and topography.* Each point of the contact lines between the bed-rock ami the super- jacent Neocene gravels or volcanic flows necessarily marks a point on the old surface of the region such as it was before hidden under Tertiary accumulations. A great number of these contact lines are usually ex- posed b}^ the canyons and creeks eroded since the close of the Neocene period, and each of them affords a section through a part of the Neocene surface. It will easily be conceded that if the elevation of a sufficient number of points on the contact lines were known, a contour map might be constructed of the Neocene surface, showing the topography and elevation above the sea, provided that no change in level or tilting had taken place in the interval. Even in such a case the map would he valuable as showing the relative topography, and if the existence and amount of the disturbance of the old surface could he ascertained by other means a correct map referred to the old sea level might he obtained from it. The bed-rock points that have been above the surface of the lava flows since the end of the Neocene — and there are many of them in the Gold Belt region — have often suffered a degradation difficult to measure, but probably in most cases not large. The flat tops of many of them show them to have formed a part of the Neocene surface, and the erosion, while scoring and furrowing their flanks, has not yet reached their summits. Many of the topographic features of the Neocene region may be directly read on the contour maps on which the geologic areas are outlined. If in a certain vicinity all the contact lines between lava and bed-rock run practically parallel with the contours and at the same elevation, the conclusion is easy that the Neocene deposit rested on a horizontal surface. provided no tilting has taken place since. If, again, the contact lines cross the contour lines in an irregular way and at considerable angles, the old surface was broken and irregular; with a sufficient number of contacts * Tin- part of the < told licit here under consideration Ins been mapped on tin- scale <>t l : 125,000, or :ii ii mi two mill's to the inch, with a contour interval of one hundred feet. It comprises the Smarts- vi lie, Colfax, Truckee, Sacramento, Placer ville, and Pyramid Peak sheets, and the topography has 1 n executed by Messrs h. M. Wilson, A. F. Dunnington, B. 11. Mc Kee, and M . E. I louglas under tin' charge pf Professor A. 11. Thompson. The geologic maps of the larger pari of tic area are finished and are now ready for publication. The Sacramento atlas short bas just been printed. ULL. GEOl. SOC. AM. 1Z 'J: nr — InJitn.H iSic&rd Tinxb. . 100' **K^_^fi/voonty 113' Wa.Uup£7F**Littyor}( aZndian.4 H. I bo ' fir i est) I Iowa Hill. \ (nearly level) aWiscons. H. Atyf/s '9 fan'kee.Oimj /* sf^Dg rJa ntlUt. VOL. 4. 1802. PL. 0. "« ~~°Bl«cksmithFlit teun Gulch. tiuttyr/ i * <*< '^ /oo "A/atvt Neocene Yuba and American Rivers, Sierra Nevada, California. » i 1 i « ) "J i3 ■ \ *0 miles V fZC'jo' w. fegjhga \ .'2 J SOUKCES OF ACCOMPANYING ILLUSTRATIONS. 2G3 the genera] drainage system may be made out. In the case of an old valley running across a recent creek or canyon, the angles of the contact lines with the contour lines on the opposite sides of the present gorge will easily and directly indicate the ancient trough. The accompanying map (plate 5) is reduced from atlas sheets of the United States Geological Survey. The elevations are partly taken from the very reliable observations of Messrs Pettee and Goodyear, partly from the maps of the United States Geological Survey, supplemented for short distances by my own aneroid determinations, and partly also from the surveys of Mr Browne. The channels where obliterated by erosion are marked by dotted lines; where remaining though generally hid- den under volcanic masses, by heavy black lines. It must be under- stood that in both cases the indicated position is only approximately correct and showing the probable course of the deepest depression. The grades given in plate 6 are affected by errors in distance and eleva- tion. The latter are believed not to be great, but the former are difficult to ascertain. An attempt has been made in measuring the distance to follow the probable curves of the rivers; nevertheless the grades are probably all a little too steep on account of underestimating distances, but thedill'crencesarenot, I think, large enough to be of much importance. The sections in plates 7 and 8 are taken from maps used in the field on the scale of 1 : 62.~>i K), or nearly one mile to the inch. In most cases it has been found necessary to enlarge the scale to 3,180 feet to the inch : only section L L is drawn on the scale of 6,360 feet to the inch. In all case3 the vertical and horizontal scales are equal. Outlines of Geologic History. Topography. — In this latitude the Sierra Nevada has two summits, separated by the Truckee valley and the deep basin of lake Taboo. The western summit, whose peaks rise from 8,000 to 10,000 feet above the sea. is also the divide between the Pacific and the Great Basin, while the Truckee river, draining lake Tahoe, has cut a deep canyon through the second or easterly summit on its way to the depressions of the Nevada deserts; on the eastern side of lake Tahoe the last-named summit at- tains even higher elevations than the principal divide. With the easterly summit and its escarpment this paper does not deal. On the Pacific slope, in the watersheds of the Yuba and American rivers, one may roughly distinguish three provinces: First, the foot-hill region, most frequently consisting of prominent ridges of diabase and amphibolite. Many of them, in Neocene times, projected boldly above the river beds, as shown, for instance, in the sec- 2G4 W. LINDGREN — TWO NEOCENE RIVERS OF CALIFORNIA^ tion A A. In this province the volcanic flows are not conspicuous. It is probable that the higher parts of the foothill region remained above them, and erosion to a great extent removed them from the lower parts. Second, the middle slopes, consisting chiefly of more or less altered sedimentary rocks, the auriferous slates. In this region the broad tables of Neocene lavas have largely effaced the pre-volcanic topography. Often, indeed, ridges of older rocks rise here also above the top of the gently sloping volcanic table-land, but as a rule they arc not prominent. Third, the region of high bed-rock peaks adjoining the divide, in which the character of a table-land, frequently noticeable even here. bec< >mes modified by prominent points of ante-Tertiary igneous and sedimentary rocks projecting conspicuously above the level of the Neocene flows. A glance at the map, on which only peaks of the older rocks are marked with their elevation in numbers, will make clear this distinction. At the divide there are many volcanic peaks, culminating in the extinct volcanoes of mount Lola. Castle peak and others which exceed 9,000 feel in height. The elevations of these volcanic peaks are not given on the map. Were the later volcanic masses removed along the divide the lowest passes would still be about 7,000 feet high. ( 'ondition of the Sierra X< vada before and during the gravel Period. — From the evidence accumulated it cannot be doubted that during the gravel period or the later part of the Tertiary the Sierra Nevada in this region formed a mountain range as distinct, if not as high, as at present. The two Neocene rivers headed near where the corresponding modern rivers begin now, in a region of lofty peaks and ridges. Their watersheds cer- tainly did not extend further eastward than the first summit, and in fact corresponded pretty closely with those of the modern rivers. On the Truckee sheet, at least, the Neocene divide coincides very nearly with the divide of to-day, and only unimportant changes can be noted. East of the divide there was an escarpment of moderate slope, and which is now exposed in many canyons to a height of 1,000 to 2,000 feet; it probably was much higher than this, but below a level of from (},<>( )0 to 7. "(Hi feel above the sea its slope is completely hidden under the immense accumu- lations of lavas Lying between the two summits north of lake Tahoe. The total height of this escarpment as it was before the eruption of the Neocene lavas should perhaps be measured from the bottom of hike Tahoe to the summit of the western divide, approximately 4,000 or 4,500 feet. There is, on the Truckee sheet, no evidence of any important post- volcanic fault along the western summit, nor is there any decided evi- dence that the steep eastern slope just mentioned represents a fault formed shortly beforcor during the volcanic period. This is illustrated by sections G G and L L (plate 7). .Many similar ones could be selected from the Truckee sheet. In G G a contact be- w 9***'r Vt(canic Kid^tt, flows sla/n Vrh Tic Jtoct l~, no Wtiit^ari SECTION N.W. SECTION " Scoo 15000' w looao SECTION. zoooo' 30000' •Sooc 10000' iSooo S.E Pinole PA.. SECTION DD , Proba-bte. po JtyLt/J If. Fork Yuba.Rit.itr /ln (ie.iL and Al&ece. £000' 1 000c' /SO00 A/W ifooo SECTIC Probab li p ositt «_>i-£ I tt N.Fork tVeiZer^r of cha-Pf* Scoo' JOOCi Mt.Lola. Zoooo Volcanic Riicji.ss flows tipping Ea.sltva.-ri 2SOO0 390*0 .7000' Zoooo' tSooo' 3oooo' iJiuLdt Pacific ty Grecct Ba-stn ■dne/eu'/t Grunitlj. ChUf GroLnUiirTfil^qts I Volcanic 10000 Ridges , tfOOOo' 60000 ' Bucktyt HUL /AyUrautiC mine) -irrT ~-~ ^ --■**^-— — ^vr * — - Zoooo' ZSooo' 30000' elev. ofchanntl. !>*«•__ I "daposils. N.W. 7000' &w 6S0O 7S00',-r--i ..- 6000' JOOO' ^SS-oo' 6soo'\ - 4 So 00' t>°o<>' \lfS00' ■ysoo'u Woo' Sood 20000" SECTION FF N.E Cisco Butte. 2000'MofSetiim puiaL 6soo'- — -i&oo^ SBeo1 1 50-Q.& So 00' •S. Fork IWtMerCf JihyoIiU. JSooc • Zoooo 1a/. LmJgrtr*. THE EROSION AND GRAVEL ACCUMULATION. 265 tween granite and andesite along which the section is laid runs for many miles nearly due eastward across the divide, thus exposing an excellent profile of the Neocene surface. The high volcanic ridges of mount Lola immediately northward are projected on the section. The slopes of the flows are eastward and westward from the central vents of the old vol- cano of Lola. In L L a section is made on a smaller scale across the divide showing the depression of the headwaters of the Neocene middle fork of the American river, east of which rises the old divide at Granite Chief. The river heads only a few miles northward and rises rapidly in this direction. The decided slope eastward from < Iranite ( Lief should be noted. That this slope was also that of the Neocene divide is proved by the contact lines of the andesitic masses with the underlying older rocks. This line is projected on the section from the ridges immediately north of it. From the ragged country in the region of their sources the rivers pursued their course down in broad valleys separate 1 by ridges which even in the lowest foot-hills sometimes reached an elevation of a thousand feet above the channels. The outlines of the ridges were usually com- paratively gentle and flowing; still, slopes of ten degrees from the channel to the summit were common and slopes as high as fifteen degrees occurred in the eastern part of the Sierra. The character of a region of old and continued erosion, commencing probably far hack in the Cre- taceous period, is everywhere plainly evident. In the center of the deep depressions is quite frequently found a deeper cut or " gutter," indicating a short period of more active erosive power just before the beginning of the gravel period. At this time, probably about the beginning of the Miocene period, the streams became charged with more detritus than they could carry and began to deposit their load along their lower courses, especially at places favorably situated, as, for instance, along the longitudinal valley of the South Yuba. Toward the close of the Neocene. gravels had accumulated all along the rivers up to a (present) elevation of about 5,000 or 6,000 feet; above this it is plain that erosion still con- tinued in places with great activity and furnished some of the materia] deposited in the lower parts of the streams. The coarse character of much of the gravel and the often remarkable absence of tine sediments in the beds point clearly to a somewhat rapid stream capable of carry- ing off a great deal of silt, and the accumulations are probably due to rapid overloading rather than to low grade of the rivers. The deep chan- nels were filled and the gravels encroached on the adjoining slopes, where they were deposited in broad benches. A maximum thickness of 500 feet of deposits was attained on the South Yuba, and of from 50 to 200 feel in the other parts of the lower rivers. En the lower and middle Siena some XL-Bum,. Geoi,. Soc. Am., Vol.. 4, 1802. 266 W. LINDGREN TWO NEOCENE RIVERS OF CALIFORNIA. of the rivers then meandered over floodplains two or three miles wide, above which the divides of bed-rock rise to a height of several hundred feet. In some instances low passes over divides were covered, and tempor- rary bifurcation and diversion of rivers into adjoining watersheds occurre< I . The volcanic Period. — At this time the first eruptions of rhyolite began from the first summit, from the volcanic center of Castle peak, they poured down the valleys, at first as molten flows, then as fine breccias and tuffs, and, being mixed with detrital material on their way, they arc finally found lower down as semi-volcanic sands, clays and gravels. These beds of mixed volcanic and sedimentary character, usually fine- grained and distinguished by a brilliant white color, have been collectively distinguished under the name of rhyolitic beds, and merge into the tuffs and massive rhyolites of the upper valleys. The rhyolitic flows usually confined themselves to the valleys and only in some instances flooded certain of the low passes. The maximum thickness of these flows near the summit is one thousand feet, but it rapidly diminishes westward. These masses of fine detritus flooded the lower slopes and compelled the rivers to seek new channels, still, however, in general confined to the old valleys. The waters at once began the work of cutting down in the clave}- and sandy masses. Then the period of the andesitic eruptions began, Dark-colored mud flows, at first sandy and clayey, again flowed down the valleys ; the divides began to be covered. Again the rivers were displaced and again they at once began their work of active erosion, cutting down not only through the accumulated silt to their former levels, but. wherever the intervals between the eruptions allowed it, down through the gravels sometimes deep into the underlying 1ied-n»ek. In some districts, especially on the American river, these intervolcanic channels cut and destroyed again and again the older deposits, pursuing a wholly independent course, although in general flowing in the same valleys. They have exactly the same characteristics as the modern rivers. It is important to note that they enable us to fix with accuracy the relative date of the change from the conditions of the Neocene to the conditions of to-day. Whatever causes produced this change, they began to act at this time. The intervolcanic channels were of an ephem- eral character; successive eruptive flows changed their direction, and it is to be expected that there were, as shown by Mr Browne, several dif- ferent systems of them. They occur principally in the watersheds of the American river where the interval between the first and the lasl andesitic flows seems to have been considerably larger than in the region of the Yuba. Cement channels, as the intervolcanic channels are often called. no doubt also occur in the latter, but as a rule they did not have time to cut down far into the rhyolitic beds before they were Idled and replaced CO _i a. CM CD CO O > UI u z o I- o UJ i SI s * 2 5 s "> •> CO ixl < < tr Q UJ o O UJ (3 z o i CO o \- o ui co 3 THE LAVA BEDS AND TUFFS. 267 by the last great andesitic flows. The intervolcanic channels, being no part of a permanent and established drainage, are not described or further discussed in this paper. These last flows, coming down in rapid succession from the volcanoes of Weber lake, of mount Lola, of Castle peak, and many others south- ward, flooded everything and covered up the lower and middle slopes to such an extent that only isolated peaks or ridges protruded above them_. Their character is peculiar; they consist of a gray or brown tuffaceous breccia, containing, in the foot-hills as well as in the high range, large, usually angular, bowlders of andesite. They came down the slope as successive mud Hows, setting soon to a hard and compact rock. Molten andesitic flows are found in the lava-flooded valley between the two summits, and also at some places west of the first summit, but they did not extend far down the western slope. The thickness of these flows ranges from over a thousand feet high up' to fifty or one hundred feet down toward the plains, where they are nearly always underlain by volcanic sands and conglomerates washed down from earlier flows winch had not reached so far down. The eruption of this tuffaceous breccia is assumed to close the Neocene period, and its flows form an important horizon by means of which the Neocene gravels may lie separated from the later Pleistocene accumula- tions. The age of the flows is indicated by the numerous plant impres- sions common in the clays of the rhyolitic beds, as well as in those of the older underlying gravels, and which, as well known, distinctly point to the Neocene period. Only rarely is there any difficulty experienced in distinguishing the Tertiary from the Pleistocene gravels. The length of the volcanic period may be roughly measured by the depths of the " cement channels " on the Forest hill divide. They have cut through about one hundred and fifty feet of loose detritus and, at most, one hundred feet of solid rock — not much more than a twentieth of the erosion since the close of the volcanic period. There have been no andesitic eruptions of later date than those de- scribed in the region now discussed, and the continuity of the last over- whelming lava, Hoods can be traced, almost uninterruptedly in places, from the plains of the great valley to the summits of the high Sierra,. When the volcanic activity ceased * the rivers began to seek their final channels, those of to-day. The general drainage was outlined by the *An eruption of massive basalt occurred in some parts of the Sierra Nevada subsequently to the andesitic eruptions and previously to the glaciation. In the region here considered only small areas of this Pleistocene basalt are found. Mr H. W. Turner has recently shown (Am Jour. Sci., 3d ser., vol. xliv, 1892, p. 455) the existence of ii basalt antedating the andesite in the northern part of the Sierra Nevada. This curlier basalt does not occur in the area described in this paper. 268 \V. LINDGREN — TWO NEOCENE RIVERS OF CALIFORNIA. ridges of older rocks still rising above the Hows, and to them is to be attributed the fact that the Neocene river system roughly corresponds to the present one; but over the large stretches of volcanic tables the rivers marked their new courses entirely independent of the older streams, now following them, now crossing them in a most irregular manner.* The Neocene Yuba River. the main river. Fromtln Sacramento Valley to French Coiral. At Smartsville, near Sacra- mento valley, a stretch of channel three miles Long has been preserved. Its character and grade are described in detail by Mr Pettee in the "Auriferous gravels," pp. 379-383. At Sicards Mat, ahout two miles lower down, on the northern side of the river, a fragment of the old channel remains, and three miles further down, on the southern side of the Yuba, the last trace of it is found, but it is not certain whether the elevation given at the last place represents the lowest channel. From here on it is buried under the more recent deposits of the great valley. It should be noted, in this place, that the areas of auriferous gravels indicated by Mr Pettee on the low rolling foot-hills west of Smartsville as Neo- cene and below the volcanic flows are in reality Pleistocene and rest on the andesitic breccia, and that they consequently have no signifi- cance in tracing the Tertiary channel. The gravels at Smartsville and Sicards Mat do not belong to the oldest Neocene deposits, for they contain a considerable amount of andesitic pebbles. They are, however, certainly Neocene, for at Smartsville they are covered by that sheet of andesitic tuffaceous breccia which, in the region under consideration, marks the close of the Neocene period. They must represent the Neocene river in its lower course, for both north and south of Smartsville rise bed-rock ridges, and this place affords really the only outlet possible for the channels of the upper course of the Yuba; the Neocene river broke through the harried of the great diabase area of Yuba county in a valley or canyon of somewhat gentler profile, hut almost as accentuated as that of the recent river. The ridges on each side rise to a height of one thousand feet or more above the old channel (see section A A). It might he objected that the channel at Smartsville was deepened during the intervolcanic period of erosion, and consequently no longer represents the bed of the prevolcanic river. * In the region described postvolcanic faults are ran' : those found have seldom more than 1 • 15 feet throw. The Tertiary deposits would greatly facilitate the recognition of any such faults of considerable throw, and I think the probability very slight that the slopes shown in the sections are to any noticeable degree influenced by such postvolcanic disturbances. THE LOWEE ANCIENT VALLEY. 269 This I do not think is compatible with the gentle curve made by the bottom of the old channel. The intervolcanic erosion cut sharp, strep canyons like those of to-day. The deepest "gutters"* in the Smarts- ville channel might perhaps have been carved by it and it probably swept away earlier accumulations of "white" or quartz gravel. From Smartsville to French Corral there is only one wav which the Neocene river could have followed, that of the present river canyon ; any other way would necessitate extremely improbable and sudden changes of grade. A scattered line of small deposits indicates that in all probability the old river, near the mouth of Deer creek, received a tributary of which one branch came from Nevada City and the other from Grass valley. Grades : Lowest point — Sicards Hat, 3-] miles, ('»<> feet per mile (?). Sicards flat — Timbuctoo, If miles, 100 feet per mile. Timbuctoo — Mooney flat,3 miles, 113 feet per milel Smartsville channel ). Mooiiey flat— French Corral, 1" miles, 7* feet per mile. The Nevada City and Grass Valley Channels. — In spite of the extensive erosion west of Nevada City and Grass Valley there is pretty good evi- dence that the channels of these places formed the old equivalents of the present Deer creek and connected with the main Vuha river a short distance above .Mooney Hat, three miles above Smartsville. The Nevada City channel evidently headed a few miles east-northeast of that city in the Harmony ridge, and is exposed in the East Harmony and Wesl Harmony drift mines ;f it runs westward with a steep grade, and, curving southward, emerges east of the Sugarloaf, in the old Manzanita diggings, and thence passes on to the hydraulic mines northwest of the city (American hill). From here on it is largely eroded away. .The large amount of gravel in the lower part of this channel is remarkable. The low divide toward the main river eastward formed a gateway through which some of the rhyolitic tuffs poured down toward Nevada City. Grades : Manzanita — West Harmony, about 76 feet to the mile. West Harmony — Harmony, about 190 feet to the mile. The Grass Valley channel is somewhat different in having a compar- atively small amount of gravel, it is covered with tuffs and volcanic sands, above which, as usual, lies thecompact tuffaceous andesitic breccia. It is separated from the Nevada City channel by a four-hundred feet high bed-rock ridge, culminating in Banner hill. The first point where ♦ "Auriferous Gravels," p. ;;s0. •(-These mines have been developed since Mr Pettee's visit to the place. 270 w. i.im><;i;kn — two neocene riveks of California. it is met with is at the " Buena Vista slide/"* a few miles east of Grass Valley : it is here covered by heavy masses of rhyolitic sand and tuffs— an overflow from the main South Yuba channel ; from here it passed by Krcs and Union hill across the eroded gap of Grass Valley, and thence on through the volcanic ridge down to Rough and Ready. The possi- bility is not excluded that this Grass Valley channel belongs to a some- what later period than that of Nevada City. ( trades : The average grade from the Manzanita diggings to supposed junction with the main Yuba near Mooney Hat, 16 miles, is 115 feet to the mile. The same from Buena Vista to the same junction, 16 miles, is about 1 22 feet to the mile. The actual grade of the Grass Valley channel from Buena Vista slide to Rough and Ready is about 72 feet per mile. This necessitates a heavy fall for the lower part of the Neocene Deer creek. French Corral la North San Juan. — Between these two points the channel is nearly continuous, and the volcanic beds once covering the gravel arc almost completely eroded. This part of the channel has been described in detail in "Auriferous gravels," page 190 et se

. 392. t Mr Pettee's distances vary somewhat from those here Adopted, which 1 have endeavored to measure along the probable curves of the stream. | Auriferous i rra\ els, p. 309 el seq. I Auriferous Gravels, p. 203, DEPOSITS OF TRIBUTARY CHANNELS. 273 of these points rises in a short distance 700 feet above the bottom of the channel. Grades : North Bloomfield to Backbone inlet, 3 miles, 152 feet per mile. Backbone inlet to Moores flat, 4J miles, 137 feet per mile. Moores flat to Snow Point, 21 miles, 87 feet per mile. The Derbec Channel — The Derbec shaft is sunk on a very different channel from that of North Bloomfield; it pays for drifting, which the main channel docs not, as a rule, and it carries a great many granite bowlders, which I think are derived from a hidden area under the volcanic flows rather than carried down from the granitic area above Washington. It has been mined for a distanee of 3,500 feet in an easterly direction from the shaft. It represents a tributary to the main channel, and I think it very probable that it connects under the lava with the Belief inlet, its course from there upward is very uncertain, as so much of it has been eroded. A connection with the Omega gravel area and others below that on the brink of the South Yuba canyon seems quite probable, but the problem is complicated by the existence of the deep Centennial channel on the Washington ridge, and more investigations are necessary before a final result can be reached. On the other hand, the Derbec channel undoubtedly joins the main channel at some place between North Bloomfield and the Backbone house. Grades : Derbec shaft to Relief, 3 miles, 115 feet per mile* From the Derbec shaft down to the main channel there is a pretty heavy grade of about 120 or 150 feet to be accounted for, hut the dis- tance, allowing for some curves, might have been nearly one mile. The Forest City ('limine!. — The channel between Orleans flat and Forest City is sufficiently known from Mr Pettee's notes. f Above Forest City the Neocene valley is continuous as far as City of Six, overlooking Downieville. From here it is not easy to trace it any further. Between Forest City and the Ruby mine there is, however, a break in form of a mass or dike of volcanic rock. At the Ruby nunc there are two channels, one lower connecting with the City of Six, and one upper running toward Forest City. The Bald Mountain Extension is mining a tributary from the northeast. In its former tunnel a basalt dike was found cutting across the andesitic breccia and showing that the eruption of the basalt masses of the Forest hill table mountain took place in tin vicinity. * Auriferous Gravels, p. 105. t [bid., p. 4;;:! e< seq. XLI— Buix. Of.oi.. Soc. Am., Vol. 4, 1892. s 274 W. LINDGREN — TWO NEOCENE RIVERS OF CALIFORNIA. Grade : From Orleans flat to Forest City, 51 miles, 70 feet per mile. Snow Point to Milton. — Mr Pettee regarded it as improbable that any stream ever came down to Snow Point from an easterly or northeasterly direction,* and evidently considered the Forest City channel as the main Neocene Middle Yuba. He states, regarding the country to the north- east of Snow Point,t that " it is thought b}r some that a channel will be traced from Haskell peak by way of Chips hill v. near Sierra City) to a junction with another channel coming from a more easterly direction, and that the two united follow a course under the lava by way of Amer- ican hill and Nebraska to some point near Forest City. . . . Others think that the high channel followed an independent course toward the south anil crossed the line of the present Yuba river near Milton with- out making any connection at all with the lower channel, which passes by Forest City." Mr C. W. Hendel, who is intimately acquainted with the mining industries of Sierra and Plumas counties, appears to have been the first to announce the former view as long ago as 1872, J but he carries his channel down from Plumas county by Beckwith pass and Cold lake somewhat regardless of grades and intervening bed-rock ranges. Mr Pettee states that his examination was hardly sufficiently extended to warrant the expression of any decided opinion, hut that, while he was not ready to assert that there were no old gravel channels, he did not think it proved that any existed in this vicinity. ^ The careful examination of the country between American hill and Milton cannot fail to convince any one of the existence of a decided trough or depression below the lava, so deep as to justify the conclusion that it represents the principal Middle Yuba during Neocene times. The outlet of this channel is undoubtedly found at or near American hill, on the southern bank of Wolf creek, while Nebraska and the gravels between the forks of Wolf creek represent tributaries to the main river. The gravel banks exposed at Bunker hill (near American hill) are about three hundred feet high, and the dee}) trough-like channel is clearly indicated. From the outlet at American lull there is hardly any other course possible, down stream, than across the eroded canyon of the Middle Yuba toward Snow Point. That a large channel ever passed across the Craniteville gap at Shand's hotel is, for a great number of reasons, not at all likely. The elevation of this gap is 4,625 feet. For at least ten miles above American hill the channel is hidden under the lava flow on tin- north side of the Middle Yuha. On the north- * Auriferous Gravels, i>. 401. flbid., p. 442. I [bid., p. 210. J Ibid., p. 44li. CHANNEL OF THE ANCIENT MIDDLE YUBA. 275 western side the bed-rock is very high, sometimes forming the crest of the divide between the North and Middle Yuba. On the other hand, the lava bed-rock contact runs very low on the slope of the canyon side, while it rises to considerable elevations on the opposite, southeastern side of the river. This relation is clearly illustrated in section D D (plate 7). For a long distance above American hill there is no indication that the chan- nel passes out from under the lava into the eroded canyon. Supposing a fairly uniform grade from Milton to American lull, it cannot emerge until about nine miles from Milton, and very possibly less. At any rate, the old channel for many miles above American hill would appear to offer an excellent field for drifting operations. It is easily accessible from the canyon of the Middle Yuba by moderately long tunnels, which, for instance, at the section D D would probably have to lie placed at an elevation of 5,000 feet. It is quite likely that the gravel in this channel would pay for drifting, especially as it would have received the debris from a part of the quartz mines south and southwest of Sierra City. An attempt to open up this channel was made at the Savage tunnel, about four miles above American hill, but it was abandoned long before com- pletion. Attention should he called to the deep valley through which the section shows the channel to have flowed. Those accustomed to profiles of equal horizontal and vertical scale will readily recognize the abrupt slopes of its sides. It is not probable that Pinoli peak lias suffered any large degradation since the Neocene times, as andesitic Hows cover it on the eastern side almost to the top. High bed-rock continues on the divide north of the Middle Yuba up to Milton, while the lava runs far down on the northern canyon slope. The detailed investigations in this region have not yet been completed, and just where the channel leaves the lava How and follows the eroded course of the present river is not quite certain. Neither to the north nor to the south is there, however, as far as I am aware, any possible outlet by which it could have turned from this course until Milton is reached. At Milton, however, there are both north and south of the Middle Yuba places with sufficiently low bed-rock to allow the Neocene river to deviate from its course parallel to the river. The first is about a mile southeast of Milton and forms the distinct outlet of the subsequently described Milton-Meadow lake channel; its elevation is not far from 5,950 feet. The second is northeast of Milton, where a gap appears to exist, with rapidly rising bed-rock on both sides. The approximate ele- vation of this gap, which I do not know from personal inspection, has been determined by Mr Pettee to be 5,938 feet.- It would seem to rep- * Auriferous Gravels, p. 112. 276 W. LIMA, REX — TWO NEOCENE RIVERS OF CALIFORNIA. resent a tributary coming down from the vicinity of Haskell peak. The high bed-rock ridges mar Haskell peak, the northern side of which have been examined by Mr H. W. Turner, preclude, except by assuming very large subsequent disturbances, any supposition that a channel could have flowed northward from Milton. Grades : American hill to Snow Point. 4' miles, 114 feet per mile. American hill to Milton, 11 miles, 107 feet per mile. Milton to Meadow Lake. — -Between these two places, a distance of 11 miles, there exists a deep channel entirely covered by volcanic rocks. 1 1 is easily traceable by means of a lower flow of rhyolite and by means of conspicuous bed-rock ridges rising on either side. The highest of these is English mountain, through which the section E E is laid. It shows that in some places, at least, the bed-rock peaks rise to a height of 2,000 feet above the ancient rivers* The outlet of this channel is, as mentioned above, about one mile southeast of Milton, at the base of a high andesitic bluff underlain by rhyolite; it does not seem as if this rhyolite flow had extended much farther in a westerly direction from here. An attempt has been made to open the channel in this place ; an old tunnel is still visible, but I do not know how the enterprise succeeded. Some coarse wash gold is said to have been found in this vicinity ; there is no evi- dence of any considerable amount of gravel. So far up as this the old rivers probably did not accumulate much more gravel than the present streams do now in bars and stretches of slight grade. Whether the channel would pay for drifting is a doubtful question. The distinct inlet of this channel is found between Fordyce and Meadow lakes at an elevation of nearly 6,700 feet. It is clearly indi- cated by the trough-shaped depression filled with rhyolite ("white lava ") between the high granitic hills west of Meadow lake and the slate ridges of the main divide about two miles to the northeast. It would seem almost certain that this part of the ancient stream — east of Meadow fike — would be auriferous ; the detritus from the Meadow lake quartz mines must have been swept down into this trough. Whether aurifer- ous enough for drifting is another question. No gravel is visible at this point; moraines cover, however, a great deal of the ground here and obscure somewhat the relations between lava and bed-rock. The course of the stream above this point is not known ; its uppermost course has been swept away by the erosion of the North creek. High granite ridges rise southward and eastward ; in fact we are now near tic source of the Neocene river; the Neocene divide is only live or six miles \ shoulder projecting from English m tain, which lias 1 n somewhat exaggerated in the drawing, produces the impression ofa terrace. Such a terrace or bench does nol exist in reality. EXCEPTIONALLY HEAVY GKAVEL DEPOSITS. 277 distant and its lowest passes eastward were at least one thousand feet higher than the stream at Meadow lake. Grade : Meadow lake to Milton, 11 miles, 73 feet per mile. THE SOUTH FORK. Badger I fill to Dutch Flat— From Badger hill to Dutch Flat or Gold Run extends, about parallel to the axis of the Sierra, a series of extraor- dinarily heavy gravel deposits, largely denuded of their volcanic cap and especially adapted for mining by the hydraulic process. It formed a part of the old " blue lead," that mysterious stream which was formerly believed to have flowed north and south along the Sierra with a supreme disregard for grades and high slate ridges. The true relations of the deep channelin these deposits have been extensively discussed, especially in the "Auriferous gravels ; " but Mr Pettee, who carefully examined the gravel mines along this line, was unable to form an opinion which could reconcile the apparently conflicting facts of grades and directions. Mr Pettee stated* his belief that no deep channel will ever be found be- tween Badger hill and Grizzly hill, but afterward suggested f that a con- nection existed between Blue Tent and Badger hill by way of Grizzly hill : " It seems most probable that this portion of the gravel field represents a broad estuary or lake-like expansion of water at the junction of two streams or where two streams by the filling up of their channels and the covering of the low inter- vening ridges became practically one. If this latter view is correct, it is not im- possible that there may once have been a current from Grizzly hill toward Colum- bia hill even if the slope of the deep bed-rock is just in the opposite direction." Mr Pettee^ ^ee^s confident that no deep channel exists between Blue Tent and Scotts flat. He did not. however, examine the intervening ground. The continuity of the deep flat channel between Quaker hill and Dutch Flat is not denied, but he believes that there is also a deep channel with slight grade between Dutch Flat and Indiana bill, which would complicate matters greatly, for the channel at Indiana hill drains directly toward the deep channel of the Neocene American river. After stating the facts based upon his excellent barometrical measure- ments, which 1 have extensively used in this paper, Mr Pettee says: "It does not seem possible that there was ever a deep channel flowing in either direction between Quaker hill and Indiana hill. Dutch Flat or Thompson hill must have stood at a parting of the Mays, and it is very probable that there was another such parting between You Bet and Red Dog." * Auriferous Gravels, p. 393. t [bid., p. 415. J; Auriferous Gravels, p. 413. 278 W. LINDGREN — TWO NEOCENE RIVERS OF CALIFORNIA. As a possibility, he mentions in another part of the volume* that the Red Dog channel may have found an outlet along the present Green- horn river in a southwesterly direction. The first question to be disposed of is whether or not there is a con- tinuous channel between Dutch Flat and Indiana hill with a southward grade, as Mr Pettee thinks. It is admitted that there is a deep channel coming down along the Dutch Flat diggings, and that the elevation of this is 2,848 feet at Thompson hill. A short distance south of this. Squires canyon crosses the gravel area connecting Dutch flat and Indiana hill at an elevation of about o,050 feet, or 200 feet above the bed-rock in the low channel of Thompson hill. Regarding the place Mr Pettee f says that "Where the gravel range is crossed by Squires canyon the country rock is seen on each side with a width of about 500 feet of gravel and tailings in the bottom of the canyon. How much more slate was visible before the accumulation of gravel began it is not easy to determine, but it appears as if the slate did not extend entirely across " . . . The result which I reached after two careful examinations was that the bed- rock does extend entirely across the supposed gap, and this effectually disposes of any deep channel connecting Dutch Flat and Indiana hill. The slate proper does not begin until further down the canyon. The bed-rock at the disputed place is the soft and decomposed gabbro of Dutch Flat, which in places looks very much like clay. There are a great many other considerations which favor the same result. The gravel areas of both Plug Ugly and Jehoshaphat hills between Squires canyon and Dutch Flat canyon have the distinct character of inclined benches above the main channel, through which benches a supposed connection south- ward could only have been effected by a deep and improbable gorge. Dutch Flat and Indiana hill were evidently separated by a, low divide corresponding to the present American-Yuba divide. When the deep channel was filled up with gravel masses the stream began to deposit its load on the adjoining broad inclined benches. Finally even the divide was covered by the gravels, and a bifurcation might have taken place in the latter part of the gravel period by means of which some of the waters of the Yuba found their way over to the American watershed. If the Tertiary deposits and flows were removed from the region between Dutch Flat and Badger hill an old longitudinal valley would be exposed to view with a high ridge rising both on the eastern and the western side. It cuts the strike of the probably ( arboniferous clay slates and siliceous slates at a small angle. The lateral ridges are in part com- posed of harder siliceous rocks, in pail of softer clay slates. The only out- '■■ Auriferous Gravels, p. it:'.. tAurii'erous Gravels, p. 153. FLOWS OF VOLCANIC MUD. 279 lets along this line westward are the narrow canyons cut by the present ] Jear, Steep Hollow, G reenhorn and South Yuba rivers. Through none of these canyons is there the remotest possibility that the ancient river passed westward. High bed-rock is exposed in each case on both sides of the gap cut by the recent rivers, and not even the smallest remains of any Neocene deposits are met with for some distance below any of the supposed gaps. Any such supposition would, moreover, necessitate ex- tremely improbable and curious bifurcations. Along the whole line, Dutch Flat to Badger hill, there are gravels accumulated to an excep- tional depth and extent. Above these gravels rest, at many places, the remnants of an eroded Mow of rhyolitic tuffs and sands. They are firs! met with in Canyon creek, about five miles above Alta. They are ex- posed at Shady run, at Alta, at You Bet, at Hunts hill, at Buckeye bill and at Quaker hill. Again, they are exposed at Seotts Hat, on the north- ern side of Deer creek, and, finally, at Blue Tent, where their volcanic character begins to be less apparent, being largely mixed with other detrital material; but everywhere they form a sheet perhaps a, hundred feet thick and resting on several hundred feet of gravel. The continuity and the direction of these Hows of rhyolitic mud are distinctly and unmistakably indicated on the geologic map. Coming down the old channel along the upper course of Canyon creek, they flowed in a southwesterly direction, passing Alta, and Dutch Flat, down to You Bet. Turning here with the valley, they flowed northward by Quaker hill to Blue Tent. Between Blue Tent and Badger hill the vol- canic masses are completely eroded and the underlying gravel beds exposed. Mr. Pettee traced the deep channel northward as far as Hunts hill, or even, with a somewhat uncertain elevation, to Quaker hill. If he had examined the relations at Seotts Hat and the country between Seotts flat and Blue Tent, I am confident he would have arrived at the same conclusion which has been reached here. At Seotts Hat there is the most ample evidence that a very large channel crosses Deer creek, with rapidly rising rim-rock on the east and west. The creek has not quite