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THE COLOR OF THE OCEAN 


Report of the Conference 


on August 5-6, 1969 


Sponsored by 


Earth Survey Office 
Electronics Research Center 
National Aeronautics and Space Administration 
Cambridge, Massachusetts 


Held at the 


Woods Hole Oceanographic Institution 
Woods Hole, Massachusetts 


Compiled by 


William I. Thompson, III 


Harth Survey Office 
Electronics Research Center 


THE COLOR OF THE OCEAN 


Contents 
Conference Participants ...... 
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Roswell Austin, Some Observations on Water Color on the . 
Continental Shelf 


Maurice Blackburn, Applications to Fishery Oceanography .. . 

Myron Block, New Instrumentation Concepts . 

CSOrGe CAPE ‘oo 6 6 0 ofo) oo) 6 oo! 0 6 6:0 oo 8 oo 6 6 
G, tho CGilawrkes Gs Co yale, ehael Co dip Monster 5 o 
Spectral Measurements from Aircraft of Back- 
seattered Light from the Sea in Relation to 


Chlorophyll Concentration as a Possible Index 
of Productivity 


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Mahlon Kelly, Aerial Photography for Study of Near-Shore .... 
Biotic Distributions Distributions 


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10-1 


Contents (Continued) 
C. J. Lorenzen, The Biological Significance of Surface 
Chlorophyll Measurements 


Peyoul MEISE 5 5°56 6 5 4.0.6 00.6 610.60 0056.90.00 


William Merrell, Apollo Photography and Multisensor . 
Aircraft Data 


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QO. Lyle Tiffany, 


Nolan UyAleie 5 6. 


Morris Weinberg, 


Peter White .. 


Charles Yentsch 


Preliminary 


Notes on Thermal Mapping and 


Multispectral Sensing in Oceanography... . 


Ocean Irradiance Measurements Using an Inter- 
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e ° ° ° e ° ° ° e ° ° ° e e ° e e e ° ° ° e 


So IX leslie eyacl Co So liaciela, MN Waoceerccholanle 4 5 4 
Means of Obtaining Monochromatic Spectra of Marine Algae 


L. E. DeMarsh, Color Film as an Abridged .... 
Spectral Radiometer 


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15-1 


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17-1 


18-1 
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26-1 


27-1 


28-1 


29-1 
30-1 
31-1 


31-2 


31-5 


THE COLOR OF THE OCEAN 


August 5-6, 1969 


Woods Hole, Massachusetts 


Participants 


Raymond Alfaya 

Science Engineering Research Group 
Long Island University 

P.O. Box 400 

Greenvale, N. Y. 11548 


Roswell Austin 

Visibility Laboratory 

Scripps Institution of Oceanography 
San Diego, Calif. 92152 


Maurice Blackburn 
Scripps Institution of Oceanography 
La Jolla, Calif. 92037 


Myron Block 

Block Engineering, Inc. 
19 Blackstone St. 
Cambridge, Mass. 02109 


George L. Clarke 

Harvard Biological Laboratory 
18 Divinity Ave. 

Cambridge, Mass. 02138 


Alfred Conrod 

Experimental Astronomy Laboratory 
Massachusetts Institute of Technology 
265 Massachusetts Ave. 

Cambridge, Mass. 02139 


Kirby Drennan 

U.S. Fish & Wildlife 
239 Frederick St. 
Pascagoula, Miss. 39567 


Gifford C. Ewing 
Woods Hole Oceanographic Institution 
Woods Hole, Mass. 02543 


Frank Hebard 

Bureau of Commercial Fisheries 
75 Virginia Beach Dr. 

Miami, Fla. 33149 


ay 


Rudolph Hollman 

Dept. of Meteorology and Oceanography 
New York University 

Bronx, N. Y. 10468 


George Huebner 

Dept. of Oceanography 

Texas A & M. University 
College Station, Tex. 77843 


N. G. Jerlov 

Dept. of Physical Oceanography 
University of Copenhagen 
Dénmark 


Mahlon G. Kelly 

Dept. of Biology 

New York University 

University Heights, N. Y. 10453 


Glenn Larson 

Electronics Research Center 

National Aeronautics and Space Admin. 
575 Technology Square 

Cambridge, Mass. 02139 


Leonard N. Liebermann 

Dept. of Physics 

University of California, San Dieqgo 
La Jolla, Calif. 92038 


Carl Lorenzen 
Woods Hole Oceanographic Institution 
Woods Hole, Mass. 02543 


Paul Maughan 

Bureau of Commercial Fisheries 
C Between 18th & 19th NW 
Washington, D. C. 20001 


William J. Merrell, Jr. 
Dept. of Oceanography 

Texas A & M University 
College Station, Tex. 77843 


Michael Miller 
Electronics Research Center 


National Aeronautics and Space Admin. 


575 Technology Square 
Cambridge, Mass. 02139 


Richard €. Ramsey 

TRW Systems 

One Space Park 

Redondo Beach, Calif. 90278 


Donald Ross 

Philco-Ford Corp., WDL Division 
3825 Fabian Way 

Palo Alto, Calif. 94303 


Peter M. Saunders 
Woods Hole Oceanographic Institution 


Woods Hole, Mass. 02543 


John D. Sherman II] 


Spacecraft Oceanography Project Office 


Naval Oceanographic Office 
Washington, D. C. 20390 


Raymond C. Smith 

Visibility Laboratory 

Scripps Institution of Oceanography 
San Diego, Calif. 92152 


Robert Spiers 
Lanagley Research Center 


National Aeronautics and Space Admin. 


Hampton, Va. 23365 


Joachim Stephan 
Battelle Institute 
505 King Ave. 
Columbus, Ohio 43201 


Robert E. Stevenson 
Bureau of Commercial Fisheries 


Galveston, Texas 7/7550 


Martin J. Swetnick 


National Aeronautics and Space Admin. 


Office of Space Applications 
Washington, D. C. 20546 


0. Lyle Tiffany 

Aerospace Systems Divisio- 
Bendix Corporation 

3300 Plymouth Rd. 

Ann Arbor, Michigan 4w¥&los 


John Tyler 

Visibility Laboratory 

Scripps Institution of Oceanography 
San Diego, Calif. 92152 


Morris Weinberg 

Block Engineering, Inc. 
19 Blackstone St. 
Cambridge, Mass. 02109 


Peter G. White 

Electronic Systems Dept. 
TRW Systems 

One Snace Park 

Redondo Reach, Calif. 90278 


Charles Yentsch 

Nova University 

College Ave. 

Ft. Lauderdale, Fla. 33314 


FOREWORD 


In our invitation to the conference, "The Color of the Ocean," which 
was held in Woods Hole, Massachusetts, on the 5th and 6th of August, 1969, 
we described the topics to be considered as follows: 

1. Upwelling radiance of the ocean with special reference 

to color. Applications to physical oceanography and 
to biological problems, including primary productivity, 
fisheries, pollution, currents, bottom studies, etc. 

2. The physical basis of upward radiance, scattering and 

absorption in the sea. 

3. Instrumentation, data reduction and interpretation. 

We explained that our eventual goal was to use spectrophotometry and 
photography as an aid in aerial and satellite reconnaissance of the ocean 
to locate distinct water masses and areas of high biological productivity. 

This report presents the remarks and presentations given at the 
conference as well as papers and thoughts contributed by the participants 


after the meeting. 


George L. Clarke 

Professor of Biology, Harvard University 
Associate in Marine Biology, 

Woods Hole Oceanographic Institution 


Gifford C. Ewing 
Senior Scientist 
Woods Hole Oceanographic Institution 


vi 


SUMMARY CONCLUSION 


Recognizing that a series of earth resources technology satellites 
will be orbited in the early 1970's, this conference recommends that the 
quantitative measurement of the color of the oceans should be one of the 
prime objectives of one or more of the on-board remote detection systems. 

We believe that such measurements, in addition to differentiating 
between water masses, will assist in the assessment of oceanic biological 
productivity, bottom topography and related hazards to navigation, coastal 
ecology of the bottom biota, and certain kinds of waterpollution. Such 
an assessment is essential to management of oceanic resources on a national 
and world-wide basis. 

lt is recommended that: 

1. The satellite color measurement system meet the following 
resolution specifications: 

|] mile spatially 

100 angstrom spectrally 

10 days temporally 
The required sensitivity will vary over fairly wide limits, being lowest 
over coastal areas and highest over the high seas. Color contrasts to be 
found over the open ocean are exceedingly small and are further degraded by 
atmospheric transmission. Although further investigation will be needed to 
specify the required sensitivity with certainty, present indications are that 
this is physically attainable and can be achieved in the next few years by 
reasonable advancement of the art. More detailed recommendations of 


specifications are presented in the conference review publication. 


Val at 


2, A substantial "ground truth" program of measurement must be 
instituted promptly which is primarily aimed at the understanding of the 
eauses and interpretation of ocean color, and how this is degraded by 
atmospheric scattering and by surface, waves, foam and glitter. This 
must be so planned that meaningful correlations will come from the data 


acquired during the experimental orbital missions. 


SUPPLEMENTAL REFERENCES 


Oceanography from Space. Ed. by G. C. Hwing. 
POG ng Lee Coit > (Oia Was WMSesalloaliliwy Ot) CoOlchwuie wiiage 


Oceanographic Explorations from Aircraft, 
Manned Orbital and Lunar Laboratories, Woods 
Hole, Mass., 24-28 Aug. 1964. 


OCSAMS stieON SOECSs Ila ly Bo Ge Bacheileyy. 
Ing NEO TEiicl Iho Clases 5, eOe> Oi Sy\moOsSaviian 


on Status of Knowledge, Critical Research Needs, 
and Potential Research Facilities Relating to the 
Study of the Oceans from Space, Houston, Tex., 
GwL® Puls COs 4 L69. 


Bailey, J. S. and P. G. White, (1969), Remote 
sensing of ocean color, Advances in Instrumentation, 
Wolk, Qa a Aes S46 NUNS JNeeSeSsaloral Number A70-18592. 


WalaL al 


Raymond Alfaya 
Science Engineering Research Group 
Long Island University 
Greenvale, New York 

This group is engaged in remote sensing research, in the area 
of multispectral color aerial photography. They have develoned their 
own four-lens multispectral aerial camera which simultaneously exposes 
four spatially identical black and white negatives through different 
optical filters. Using a specially designed additive color viewer, a 
corresponding set of four black and white positives are combined, by 
superposed projection, to produce an additive color display. Because 
this technique permits precise, independent control of the many 
individual variables in photography and viewing, it can distinguish subtle 
differences in the spectral reflectance of land and water masses, which 
are far too small to be detected by conventional color films. The 
group has also developed radiometric instrumentation and techniques for 
measuring reflectance spectra of ground and water taraet objects, to 


obtain the ground truth which is required for proper support of 


quantitative multispectral photography. 


NEST EA 


Roswell Austin 

Visibility Laboratory 
Scripps Institution of Oceanography 

Professional interests have been in the optical properties of 
the atmospheric and oceanic environments and their measurement. 
Main current interests are in the study of the visibility of submerged 
objects as seen from above, the assessment of sea state by the deter- 
mination of the fractional area of the sea surface covered by white 
water, and the determination and subsequent removal of atmospheric 
transmission effects in the remote optical sensing of properties of 


the ocean surface. 


SOME OBSERVATIONS ON WATER COLOR 


ON THE CONTINENTAL SHELF 


R. W. Austin 


NOTE: The original presentation relied heavily upon colored photographs 
obtained from Gemini and Apollo space missions and by the 
author from surface vessels. The following is considerably modi- 
fied and abbreviated as it is not feasible to use color printing in 


these proceedings. 


The author had the opportunity to make observations and measure- 
ments from a surface vessel along the very extensive continental shelf 
bordering the eastern coast of Asia from the Yellow Sea to the South China 
Sea. Subjective determinations were made of water color and physical 
measurements were made of the attenuation of the natural (diffuse) light 
field in the water and of the reflectance of the water (ratio of the upwell- 
ing to the downwelling illuminances). Information was obtained at over 
50 locations. 

Space photographs show marked local variations in water color, 
and presumably other optical properties, over small horizontal distances 
in the areas seaward from the mouths of rivers for many miles. Some of 
these rivers carry large quantities of silts having strong colorations. The 
measurements made from the surface vessel many miles from the coast 
confirmed the existence of many areas having higher than usual water re- 


flectance values and concomitant high values of attenuation. 


The diffuse attenuation coefficient, K, was plotted against 
the water reflectance, Ry/p and a definite correlation was obtained 
between the two properties with the clearer (low attenuation co- 
efficient) waters having generally low reflectance values and the 
turbid waters (high attenuation coefficient) generally showed higher 
reflectances. Figure 1 shows the defining relationships for K and 
Ru/pD- Figure 2 shows the relationship between the two properties 
and, additionally, shows that a correlation existed between these 
two parameters and the water color as subjectively determined by 


two observers. 


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Maurice Blackburn 

Scripps Tuna Oceanography Research Program, 
Institute of Marine Resources, 

Seripps Institution of Oceanography, 
University of California, San Diego 

La Jolla, California 92037 


My work is oriented to fishery oceanography. It involves the study of 
relations between pelagic fishes, their food supply, and the standing 
stock of chlorophyll. Examples are given in the abstract of my presen- 


tation, entitled "Applications to Fishery Oceanography". 


Applications to fishery oceanography 


What is the use of surface chlorophyll measurements in specifying and under- 
standing the distribution of surface fish? I propose to answer this question by 
giving the results of some of my own recent studies. 

During the years 1964-1966 I made a detailed study of the ecology of two 
species of tropical tuna along the west coast of Baja California, where these 
species occur from about June to December in each year. The results are in press 
in the Fishery Bulletin of the U.S. Fish and Wildiife Service. The following 
four figures show the main results. Hach figure shows: the surface isotherm 
at 20° C., below which temperature these tunas rarely occur; the area of maxi- 
mum standing stock of surface chlorophyll a; the area of maximum standing stock 
of the pelagic crab Pleuroncodes planipes, which in this area is the primcipal 
consumer of phytoplankton and the principal species that the tuna eat; and the 
areas in which tuna were caught by the fishermen. 

Figure 1 shows the situation off western Baja California at an early 
stage in the tuna season, such as July, or August in a cold year. The seasonal 
upwelling regime has begun to decay, whereby some waters have surface temperatures 
at or over 20° C., and tropical tunas can enter the area. Tongues of upwelled 
water protrude offshore from the coastal upwelling centers. They are rich in 
chlorophyll and herbivorous crabs, but too cold for tropical tunas (< ZO” Cs) 
except at the edges. On the other hand the warmer waters, where the temperatures 
are suitable for the tunas, are relatively poor in chlorophyll and tuna food. 

The tunas, therefore, are found at the boundary between the warm blue biologi- 


cally poor water and the cool green biologically rich water, and not elsewhere. 


Figure 2 shows the same area at a later stage, such as August in a warm 
year, when the tongues of upwelled water have become much warmer although they 
are still richer in chlorophyll and herbivores than any other waters. Tunas 
are now found in the middle of the tongues as well as along the edges, exploiting 
the richest areas of forage without any restriction imposed by unsuitable sur- 
face temperature. They are not found in the equally warm areas where biologi- 
cal material is scarce, however. 

Later still, as in September (Figure 3), tongues of upwelled water can no 
longer be recognized by their surface temperature, but they can still be recognized 
by their relatively high content of surface chlorophyll and herbivores. Tunas 
are found in these food-rich areas, and not elsewhere, although surface tem- 
peratures are suitable (> 20° C.) everywhere. 

Figure 4 shows the situation late in the tuna season (November), when all 
signs of upwelling have disappeared; thermal and biological conditions are 
rather uniform and suitable for tunas over large areas, and tuna occurrences 
are scattered through these areas. Later still, temperatures become unfavor- 
ably low throughout the whole area, and the tunas retreat to the tropics. 

In Figures 1 and 2 the areas of low temperature (< 20° C.) and high 
chlorophyll were broadly congruent, so that distribution of tuna food and tunas 
could perhaps have been specified from data on temperature only; but in Figures 
3 and 4 these distributions could not have been specified from temperature data, 
although they could have been specified from chlorophyll data. 

These studies supported a hypothesis, for which there was previous 
evidence as well, that two main ocean properties determine the distribution of 


tuna (and possibly other pelagic fish) at any particular time: namely 


2-5 


temperature, which sets limits of total range, and food supply, which determines 
the patchy distribution within the range limits. They also showed that surface 
chlorophyll is distributed like the tunas' supply off Baja California, and 
could therefore be used to specify areas in which tunas would be expected to 
occur (provided temperatures were suitable). 

One might expect less close relationships between distributions of surface 
chlorophyll and tuna food in other areas, where tunas are known to eat a greater 
variety of species, many of which are not herbivores. Nevertheless I have data, 
from cruises made at different seasons over a large area of the eastern tropical 
Pacific on EASTROPAC expeditions, which show that surface chlorophyll may be a 
good estimator of tuna forage, even in those situations. Figures 5 and 6, for 
opposite seasons, show the distribution of the standing stock of animals that 
skipjack tuna eat, in two different ways: as actually observed, and as esti- 
mated from a regression on surface chlorophyll measured at the same time and 
place. The agreement is at least fair: with more data and more understanding, 
it could probably be much improved. 

These remarks give an idea of what it may be possible to accomplish with 
a large and regular coverage of sea surface chlorophyll, such as might be 
obtained from aircraft or a satellite — namely, the ability to specify at 
short notice the areas of maximum concentration of food of tunas, and thus of 
the tunas themselves, and possibly the same for other kinds of pelagic fish. 

It may be more efficient to estimate the fish-food distributions from chlorophyll 
distributions, than to measure them directly. In many situations, data on sur- 


face temperature would be required as well. 


3-4 


Legends for M. Blackburn's Figures 


Fig. 1. Distribution of tropical tuna and environmental properties off 
Baja California: the situation early in the tuna season, when 
tongues of biologically rich upwelled waters are too cold for 
the tunas except at the edges. 


Fig. 2. Distribution of tropical tuna and environmental properties off 
Baja California: the situation later in the tuna season, when 
tongues of biologically rich upwelled waters are warm enough for 
tunas to penetrate. 


Fig. 3. Distribution of tropical tuna and environmental properties off 
Baja California: a later situation, like Fig. 2 except that 
the tongue of biologically rich upwelled water is not shown by 
the temperature. 


Fig. 4. Distribution of tropical tuna and environmental properties off 
Baja California: the situation late in the tuna season when 
no signs of upwelling remain. 


Fig. 5. Skipjack tuna forage on EASTROPAC Expedition, August-September 
1967, in ml./1,000 m2: (Above) as observed in net hauls; 
(Below) as estimated from a regression on surface chlorophyll. 


Fig. 6. Skipjack tuna forage on EASTROPAC Expedition, February-March 


WQS. alia, m1. /1,000 me: (Above) as observed in net hauls; 
(Below) as estimated from a regression on surface chlorophyll. 


5=5 


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AUGUST 1964 


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Figure 1. 


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AUGUST 1959 


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Myron Block 

Block Engineering, Inc. 
19 Blackstone Street 
Cambridge, Mass. 

New instrumentation concepts have been developed at Block that 
can have usefulness for oceanography. 

1. Fourier transformation spectroscopy -- 10,900 times improvement 
over former techniques of spectral measurement. 

2. Remote Raman spectroscopy technique -- quantitative high- 
resolution spectroscopy of gases and liquids. Uses pulsed laser light 
of certain pulse length, range gates the data, then does spectroscopy 
on return signal, measures parts/million of chemical composition. 

3. Technique to measure daytime fluorescence without seeing the 
effects of sunlight in same spectral region. 

4. Currently we are tying all this into a system called ''digilab"' -- 
computerized outputs of all sensors with operator using teletype input. 
For example, in interferometric spectrometry the system operates by 
"closed loop'' instrumentation, i.e., the system calibrates itself, 
wavelength scale is plotted, optimization takes place. 


We need to know something about depolarization of light in sea 


water. 


4-1 


George L. Clarke 


Associate in Marine Biology, Woods Hole Oceanographic Institution 
and Prof. of Biology, Harvard University. 


My special interest is in the application of light measurements 
to the biological problems of the sea. Light in the ocean is derived 
from the sun, the moon, and the sky, and also from the luminescent dis- 
charge of many kinds of marine organisms. The conditions of light in 
the sea control the growth of the primary plant producers and influence 
the behavior of many oceanic animals. The absorption, scattering, and 
spectral distribution of daylight passing through the water are modi- 
fied by dissolved and particulate matter, both living and non-living. 
Our present investigations are concerned with measurements from ship 
and aircraft of the spectrum of light back-scattered from beneath the 
surface. Changes in the spectra in space and time are under scrutiny 
as means for delineating water masses, detecting pollution, and evaluat- 
ing chlorophyll abundance as an index of productivity. A summary of our 


recent work on this subject is presented in this publication. 


Reprinted from Science, 


167, 


(1970) 


Copyright 1970 by the American Association 
for the Advancement of Science 


Reports 


Spectra of Backscattered Light from the Sea Obtained 
from Aircraft as a Measure of Chlorophyll Concentration 


Abstract. Spectra of sun and skylight backscattered from the sea were obtained 
from a low-flying aircraft and were compared with measurements of chlorophyll 
concentration made from shipboard at the same localities and at nearly the same 
times. Increasing amounts of chlorophyll were found to be associated with a rela- 
tive decrease in the blue portion of the spectra and an increase in the green. 
Anomalies in the spectra show that factors other than chlorophyll also affect the 
water color in some instances; these factors include other biochromes, suspended 
sediment, surface reflection, polarization, and air light. 


The penetration of daylight into the 
sea is of fundamental significance in 
the oceanic ecosystem because it con- 
trols the growth of the primary plant 
producers and the behavior patterns of 
many marine animals. Previous investi- 
gations have revealed great variation 
in the rates of light penetration due to 
differences in amounts and kinds of 
materials in the water. In addition, the 
spectral composition of the light be- 
neath the surface is altered by differ- 
ential absorption and scattering due to 
the water itself, and also to whatever 
dissolved and particulate matter (both 
living and nonliving) may be present 
(1). Because chlorophyll affects the 
spectrum in a characteristic way and 
because it is associated with living 
plants, spectral measurements of chlo- 
rophyll concentration may be used as 
an index of the amount of phytoplank- 
ton present. Regions with high phyto- 
plankton abundance can support large 
populations of herbivores and of suc- 
cessive links in the animal food chain, 
many of which are of economic impor- 
tance to man. Thus, abundant chloro- 
phyll indicates the presence of a po- 
tentially productive area (2). 

The spectral changes imposed on the 
downwelling daylight by natural waters 
and by the materials in them have been 
measured by lowering an upward- 
directed spectrometer in a watertight 
case to various depths (3). The up- 
welling, or backscattered, light that can 
be measured by employing the spec- 
trometer in the inverted position is 


20 FEBRUARY 1970 


found to have its spectrum similarly 
modified by its passage through the 
water. A portion of the backscattered 
light escapes upward through the sur- 
face, where it has been recorded by an 
inverted spectrometer suspended above 
the water from a ship and from air- 
craft (4). Allowance must be made for 
light reflected from the ocean surface 


10 
4 
9 1 — 600 ft 
2 — 1000 ft 
3 — 2000 ft 


4 — 5000 ft 
5 — 10,000 ft 


Percent of incident light 


ES ee joel ena weeere 
400 450 500 550 600 650 
Wavelength (nm) 


Fig. 1. Upwelling light as received at the 
indicated altitudes at Station S (Fig. 2) 
east of Cape Cod, 26 August 1968 be- 
tween 1345 and 1512 hours, E.D.T. 


5-2 


itself or scattered by the stratum of air 
above the water. 

The possibility thus exists that spec- 
tral measurements of backscattered 
light can be used to delineate water 
masses, to trace currents, and to deter- 
mine the abundance of chlorophyll, 
pollutants, or other significant materials 
in the water. Because measurements 
from aircraft or spacecraft can be 
made over extensive areas much more 
rapidly than from ships, they are 
especially suited to the study of small- 
scale, rapidly varying distributions of 
oceanic properties (5). Tests of some 
of these possibilities are reported here 
for water masses of widely different 
known chlorophyll concentrations off 
the New England coast. 

During the summers of 1967 and 
1968, records of the spectrum of back- 
scattered light from the ocean have been 
made from our research vessel Craw- 
ford and our C-54-Q research aircraft. 
The spectrometer used was designed 
by Peter White of TRW Systems, Inc., 
and described by L. A. Gore (6). R. C. 
Ramsey of TRW operated the instru- 
ment and took part in the reduction of 
the data and in the interpretation of the 
results. 

The TRW spectrometer is an electro- 
optical sensor of the off-plane Ebert 
type with an RCA 7265 (S-20 response) 
photomultiplier. The spectral range is 
400 to 700 nm with a spectral reso- 
lution of 5 to 7.5 nm, a scan time of 1.2 
seconds, and a field of view of 3° by 
0.5°. A continuous curve of the spec- 
trum is provided by a Sanborn re- 
corder for each scan. The spectrum of 
the incident light from the sun and sky 
was determined before and after each 
series of measurements by recording 
the light reflected from a horizontally 
placed Eastman Kodak “gray card” 
with a nonselective reflectivity of 18 
percent. A series of tests was made to 
detect changes in the spectral distribu- 
tion of incident light during the 3 
hours before and after noon due to 
changes in the sun’s altitude and to 
changes in sky conditions from clear 
to light cloudiness. Changes found were 
not great enough to affect significantly 
our investigation of the differences in 
backscattered light from the ocean. By 
taking advantage of the fact that light 
reflected from a plane surface at Brew- 
ster’s angle (approximately 53° from 
vertical incidence for normal sea 
water) is plane polarized with its vibra- 
tion plane perpendicular to the plane 
of incidence, we could reduce the light 


1119 


received as reflection from the water 
surface. We placed a polarizing filter, 
oriented at right angles to the major 
axis of polarization, over the receiving 
aperture of the spectrometer and tilted 
the instrument at Brewster’s angle (di- 
tected away from the sun). 

When we operated the spectrometer 
from our C-54-Q research aircraft, the 
signal that we wished to measure, 
namely, the spectrum of the light back- 
scattered from beneath the sea surface, 
was sometimes difficult to detect be- 
cause of interference from “noise” 
caused not only by surface reflection 
but also by “air light.” Air light is light 
that has been scattered to the instru- 
ment by the air and by material in the 
air between the sea surface and the 
aircraft. As the altitude of observation 
increases, the area of the sea from 
which light can enter the instrument 
enlarges, reaching the dimensions of 
about 52 by 9 feet (16 by 3 m) at 1000 
feet (305 m). Smaller irregularities in 
surface reflection or in the nature of the 
seawater will be averaged out. At the 
same time interference from air light 
will increase with altitude because of 
the greater path length through the 
atmosphere. The curves shown in Fig. 


1 were taken at altitudes ranging from 
600 to 10,000 feet (183 to 3048 m) over 
an area east of Cape Cod (Station S, 
Fig. 2), where the water was 200 m 
deep and the estimated chlorophyll 
content, although not measured at the 
time, was probably about 0.6 mg/m?. 
As altitude increased, the values for 
upwelling light received increased 
markedly and regularly in all parts of 
the spectrum. The remainder of the 
measurements reported here were made 
at an altitude of 1000 feet (305 m). 
Representative spectral measure- 
ments obtained over water with high 
chlorophyll content (about 4 mg/m', 
Buzzards Bay), with low chlorophyll 
content (about 0.3 mg/m%, north of 
the Gulf Stream), and with very low 
chlorophyll content (less than 0.1 mg/ 
m’, Sargasso Sea) are presented in Fig. 
3. The values for the backscattered 
light from these areas have been cal- 
culated as percentages of the incident 
light. The curves display characteristic 
differences in shape. For the water 
with high chlorophyll content the 
backscattered light rose from values 
mostly about 2.2 percent of the inci- 
dent light in the blue region of the 
spectrum to about 2.5 percent in the 


Fig. 2. The flight of the aircraft after leaving Nantucket on 27 August 1968 and 
the location of Stations A to E. Station S was occupied on 26 August. Representative 
temperatures measured from the aircraft flying at 305 m are shown to the left or below 
the flight path; representative chlorophyll concentrations in milligrams per cubic meter 
measured from the surface ship are shown to the right or above the flight path. 


1120 


By) 


green, and then dropped to about 0.3 
percent in the red. For water with low 
chlorophyll content the values were 
higher in the blue, dropped rapidly to 
much lower values in the green, and 
continued to drop in the red. Where 
chlorophyll content was very low, the 
backscattering was higher at all wave- 
lengths shorter than 500 nm and 
reached a maximum of 7 percent at 
400 nm. 

On 27 August 1968 -a more extensive 
survey of the changes in backscattered 
light from contrasting bodies of water 
was conducted during a flight from 
Buzzards Bay and Nantucket Sound to 
a point in the Sargasso Sea south of the 
Gulf Stream, then north on a 556-km 
transect that crossed successively the 
Gulf Stream, the slope water, a transi- 
tion zone, Georges Bank, Georges 
Shoals, and the southern part of the 
Gulf of Maine, and returned via Cape 
Cod Bay (Fig. 2). Records of the spec- 
trum were taken at frequent intervals 
with the TRW spectrometer, and a con- 
tinuous trace of surface temperature 
was obtained by P. M. Saunders by 
means of a Barnes infrared radiometer. 
A continuous record of the temperature 
and the chlorophyll concentration of the 
surface water was obtained from the 
R.V. Crawford by means of a thermistor 
and a continuous-flow Turner fluorom- 
eter (7). Water for this purpose was 
drawn from an intake valve through 
the hull of the vessel 2m below the 
surface. Analysis of these data shows 
that the surface temperature and the 
surface chlorophyll of the slope water, 
the Bank water, and the Gulf of Maine 
are statistically differentiated to a highly 
significant degree. We also have evi- 
dence from a previous study (8) that 
surface chlorophyll values may be use- 
ful as an index of biological productiv- 
ity. During four cruises in the Atlantic 
and Pacific, one of us (C.J.L.) collected 
91 samples, which covered a range of 
surface chlorophyll concentrations from 
0.04 to 28.3 mg/m?. Analysis showed 
highly significant correlations with mea- 
surements of the total chlorophyll in the 
euphotic zone and with the primary 
productivity of the phytoplankton in 
the waters studied. Temperature values 
obtained from the aircraft agreed close- 
ly with values obtained from the ship 
(see Fig. 2). Owing to the relative 
sterility of warm Gulf Stream water, the 
lower chlorophyll measurements tend 
to be associated with higher sea tem- 
peratures. 

A comparison of the spectra of the 
backscattered light as a percentage of 


SCIENCE, VOL. 167 


\ H — High chlorophyll 
\ 
4 L — Low chlorophyll 


——-— Very low chlorophyll 


Percent of incident light 


1 Tt 


500 550 600 
Wavelength (nm) 


Fig. 3. Data from the high and low 
chlorophyll curves plotted as percentage 
of the incident light and compared with 
data taken on the same day from an area 
with very low chlorophyll concentration 
south of the Gulf Stream. 


1 =r 
400 450 650 


Chier 
s LOCALE nig/m? SLOPE 
‘A SARGASSOSEA (<0.1) .0375 
B SLOPE WATER 0.3 .0210 
TRANSITION 0.6 .0119 
D GEORGES BANK 1.3 .0076 
E GEORGES SHOALS 3.0 .0038 


4.0 (To 7.0% at 400 nm) 
3.8 A 


nm 
a 
iF 
ot 


A: (<0-4) 


Percent of incident light 


fo} 
b 
T 


500 650 600 
Wavelength (nm) 
Fig. 4. Spectra of backscattered light mea- 
sured from the aircraft at 305 m on 27 
August 1968 at the following stations (Fig. 
2) and times (all E.D.T.): Station A, 
1238 hours; Station B, 1421 hours; Station 
C, 1428.5 hours; Station D, 1445 hours; 
Station E, 1315 hours. The spectrometer 
with polarizing filter was mounted at 53° 
tilt and directed away from the sun. Con- 
centrations of chlorophyll a were mea- 
sured from shipboard as follows: on 27 
August, Station A, 1238 hours; on 28 
August, Station B, 0600 hours; Station C, 
0730 hours; Station D, 1230 hours. 


20 FEBRUARY 1970 


=n n 
400 450 


the incident light at five localities along 
the flight path of 27 August is presented 
in Fig. 4. Simultaneous measurements 
from the aircraft and the ship were 
made in the slope water at Station B. 
The ship’s observations at Stations C, 
D, and E were not made until the fol- 
lowing day, but the range of chloro- 
phyll values was so great that the dif- 
ferences among the stations can be 
relied upon for the present comparison. 
Time did not permit the ship to reach 
the locality of the aircraft’s observation 
at Station A in the Sargasso Sea south 
of the Gulf Stream, but the chlorophyll 
content of the water there was almost 
certainly lower than in the slope water 
north of the Stream. Along the entire 
transect the shape of the spectral curves 
changed progressively as chlorophyll 
values increased from south to north. 
The percentage of backscattered light 
diminished markedly in the blue region 
and increased relatively in the green 
region, with an indication of an inflec- 
tion point at about 515 nm and with 
little change in the red region. This 
result agrees satisfactorily with the cal- 
culated values for the effect of increas- 
ing amounts of chlorophyll on ocean 
color presented by Ramsey (9). The 
change in shape with increasing chloro- 
phyll is reflected in decreased mean 
slope of the spectra. Anomalies in the 
shape and amplitude of these spectra, 
and of some taken on other occasions, 
make it evident that other factors play 
a role that merits further investigation. 
Our investigation shows that large dif- 

ferences occur in the spectra of the light 
backscattered from the ocean and that 
they can be recorded from aircraft. In 
the present instance, the slopes of the 
spectra correlate quite closely with dif- 
ferences in chlorophyll concentration. 
The discrepancies are believed to be 
due to difference in time within paired 
observations, to differences in surface 
reflection, to scattered air light, and to 
the presence in the water of material 
other than chlorophyll that affected the 
light selectively. If such interference 
can be eliminated, or identified and al- 
lowed for, spectrometric procedures 
from aircraft (and perhaps from satel- 
lites) will be of great value in the rapid 
investigation of oceanic conditions, in- 
cluding conditions important for biolog- 
ical productivity. 

GEORGE L. CLARKE 

GIFFORD C, EWING 

CaRL J. LORENZEN 
Woods Hole Oceanographic 
Institution, Woods Hole, 
Massachusetts 20543 


5-4 


10. 


12 


References and Notes 


. G. L. Clarke and E. J. Denton, in The Sea, 
M. N. Hill, Ed. (Interscience, London, 1962), 
pp. 456-468; G. L. Clarke, Oceanol. Int. 2, 
38 (1967); , BioScience 18, 965 (1968); 
N. G. Jerlov, Optical Oceanography (Elsevier, 
Amsterdam, 1968). 


. J. H. Ryther and C. S. Yentsch, Limnol. 


Oceanogr. 2, 281 (1957); G. C. Ewing, D. L. 
Inman, L. N. Liebermann, G. Newmann, D. 
P. Petersen, W. S. Wooster, C. S. Yentsch 
(Panel on Oceanography), Useful Applica- 
tions of Earth-Oriented Satellites (National 
Academy of Sciences, Washington, D.C., 
1969), vol. 5, pp. 44-54; J. H. Ryther, Science 
166, 72 (1969). 

. R. C. Smith and J. E. Tyler, J. Opt. Soc. 
Amer. 57, 589 (1967); J. E. Tyler and R. C. 
Smith, ibid., p. 595. 

. J. D. H. Strickland, “The estimation of sus- 
pended matter in sea water from the air,” in 
Ms. Rep. Ser. (Oceanogr. Limnol.) No. 88 
(Fisheries Research Board of Canada, 1967); 
G. L. Clarke, G. C. Ewing, A. Conrad, R. 
M. Alexander, G. Mayer, in Summary of In- 
vestigations Conducted in 1967 (Ref. No. 68- 
32, Woods Hole Oceanographic Institution, 
1968); G. L. Clarke, in Remote Sensing in 
Ecology, P. L. Johnson, Ed. (Univ. of Georgia 
Press, Athens, 1969). 

. G. C. Ewing, Deep-Sea Res. 16 (Suppl.), 35 
(1969). 

. L. A. Gore, unpublished report (Electronic 
Systems Division, TRW Systems, Inc., 1968). 

. C. S. Yentsch and D. W. Menzel, Deep-Sea 
Res. 10, 221 (1963); O. Holm-Hansen, C. J. 
Lorenzen, R. W. Holmes, J. D. H. Strick- 
land, J. Cons. Cons. Perma. Int. Explor. Mer 
30, 3 (1965); C. J. Lorenzen, Deep-Sea Res. 
13, 223 (1966). 

. C. J. Lorenzen, unpublished manuscript (1969). 

. R. C. Ramsey, unpublished final report (Elec- 

tronic Systems Dept., TRW Systems, Inc., 1968), 

Supported by NASA contract NASA 12-631 

and by Office of Naval Research contract 

ONR 241. We thank the crews of our research 
ship and aircraft; we also thank Miss Anne 

Bowen, Mr. Carl Fontneau, and Mr. Robert 

E. Frazel, research assistants. Contribution 

No. 2394 of the Woods Hole Oceanographic 

Institution. 


December 1969 


Alfred Conrod 
Measurement and Systems Laboratory 
Massachusetts Institute of Technology 
Cambridge, Massachusetts 
We are instrumentation makers and engineers and are involved 


here at this conference to provide machines, develop user requirements. 


The bulk of our work is in optical instrumentation. 


Kirby Drennan 
U. S. Fish & Wildlife 
Pascagoula, Miss. 

In recent months we have been looking at the problem of direct 
detection, identification and quantification of pelagic fish stocks 
through the use of remote sensors. Several approaches are being taken 
in an effort to establish those characteristics of fish schools which 
can be observed through the use of remote sensors and to define the 
sensor requirements and to develop a sensor system which will enable us 
to assess the resources of large oceanic areas. These include multi- 
spectral photography, studies of the reflectance spectra of individual 
fish and fish schools, measurements of the absorption spectra of 
fish oil films, studies to determine the application of low-level-light 
sensors, such as image intensifiers, to detect the bioluminescence 
associated with most fish schools, and in October a series of tests will 
be conducted with a pulse-gated laser system. A rather extensive 
photographic program was carried out at Pascagoula which resulted in 
several hundred aerial photographs of fish schools of various species. 
Black and white, color, and color infrared films with various filter 
combinations were used in this program. An effort is now being made to 
correlate the photographic imagery with the catch data and sonar soundings 
obtained during the field operation. 

In September of 1968, the Pascagoula base and TR Systems, under 
contract to Pascagoula, obtained spectral reflectance measurements of 
fifteen schooling species in the Northern Gulf of Mexico. Observations 


were made on single fish and fish schools inside an impoundment using a 


7-1 


recently developed TRW water color spectrometer. These data indicate 
that, in general, the reflectances are separable on a species basis and 
are different from sea water reflectance. The natural phenomenon of 
bioluminescence which is stimulated in ubiquitous marine organisms by 
the movement of fish schools appears to offer a promising solution to 
the problem of locating and possible identifying and quantifying fish 
schools at night. In recent months, we have used an airborne image 
intensifier/television system at altitudes of 5,000 feet to detect 
fish-stimulated bioluminescence, the intensity of which was far below 
the threshold of the human eye. Therefore, we are interested not only 
in the physical, chemical and biological factors which affect the color 
of the ocean, but also the effect that these factors have on the production 


and transmission of light within the sea. 


Gifford C. Ewing 
Woods Hole Oceanographic Institution 
Woods Hole, Massachusetts 

Of the various oceanographic parameters that one might attempt to 
measure remotely from satellites, color has the unique advantage of 
reacting to the bulk properties of the ocean, thus giving an estimate 
of its biological and chemical construction. Although this information 
is limited to the upper 10-20 meters of the sea, less than 1% of the 
total volume, nevertheless this is the part that is of most direct 
concern to the majority of mankind. That relatively little is known 
of the distribution of sea color is due in part to the fact that it jis 
distributed in fairly small patterns and varies with the biological 
activity at a relatively high rate so that the low sampling rate 
available to ships is inadequate to observe the day-to-day changes. 

Satellite oceanography is inherently directed toward observing the 
upper layers of the sea, the part that is stirred by the wind and lit by 
the sun. No matter what ingenious ways may be devised for probing deep 
beneath the surface, it seems unlikely that such regions will be naturally 
amenable to exploration by satellite technology. In other words, we are 
concerned here with a specialized description of a severely limited layer 
of the ocean. 

Fortunately, the layer of the ocean exposed to the overview is far 
more significant than the above considerations suggest. For one thing, it 


the part of the ocean that overwhelmingly concerns the everyday affairs of 


mankind. It is the site of waves, storm surges, the rise of tide, and 
the secular changes of sea level. It covers the continental shelves 
where oil and minerals are being recovered. It is the part of the sea that 


most concerns sailors, because of currents, destructive waves, dangerous 
shoals, or drifting ice. |t impinges on the beaches, harbors, and estuaries 
that are important for industry, recreation, and human habitat. It includes 
the zone that supports the photosynthesis upon which the whole biological 
resource of the sea depends. Not only is this the only part of the ocean 
that directly touches the lives of most of mankind, but, conversely, it 
is mostly at these superficial depths that man acts on the sea by activities 
such as dredging and fishing, or by contamination with chemical pollutants. 

The overview is equally important to the scientific understanding of 
the marine environment and its multifarious interrelations with the land 
and atmosphere, which exert a crucial, though somewhat less direct influence 
on the human environment. Virtually all the energy that controls its inner 
workinas flows across this boundary, and all the water types that constitute 
the ocean's anatomy have their genesis at the surface, in a reaion of 
exposure to sun and sky and wind. Like the sediments of the earth's crust, 
the sea is composed of tilted strata that outcrop somewhere at the surface. 
Consequently, a complete mao of all these surface outcrops must contain 
information about all deep-water masses of the sea. Geometrically, the 
ocean has approximately the proportions of a sheet of letter paper, and, 
like a sheet of paper, much of its information content is written on its 
face, exposed to view from afar. 

In spite of these obvious advantages, oceanographic exploration 
from the air is in a very rudimentary stage of development. Compared 
with forestry, agriculture, terrestrial geography, and meteorology, 


techniques such as aerial photography and infrared radiometry have as yet 


found little application to oceanography. The reasons are varied and 
complex, including the limited operatina range of aircraft, lack of 
suitable sensors, and the special difficulties of acquiring oceanic ''ground 
truth.'' But more fundamental than all these is the inability of 
oceanographers to make efficient use of surface maps of the ocean, if 

such data were readily available and free of error. Although the idea 
that the sea derives its constitution and motive force at the air/sea 
boundarv is well established in oceanographic theory, in practice the 

data of oceanic observation have usually been obtained and analyzed in 
vertical sections. As a result, the instruments, data-handling routines, 
analytic methods, and, in fact, the oceanographers themselves are all 
oriented toward vertical rather than horizontal aggregates of information. 
To establish the basis for satellite oceanography will require a gestation 
period that may be measured in years or decades, depending on how much 
effort is invested in this sector of the science. It will not be easy to 
combine such unrelated technologies as space science and oceanography, 

and it will not occur spontaneously as it has in agriculture or geography, 
where air mapping has long been established. Above all, it will require 

a much greater effort in establishing the validity of data acquired from 
satellites than is commonly recognized. For many applications, such as 

in agriculture, ''ground truth'' can be established by a few flights over 
selected areas that have been well surveyed. But in oceanography one deals 
with rapidly changing conditions. For example, high sea states cannot be 
scheduled months in advance, nor do they persist long enough to permit the 
leisurely coordination of air and surface activities to record their 


physical descriptions. 


8-3 


The great strength of the satellite observatory is its ability to look 
at the world ocean on a time scale that is small compared with that of 
many important dynamic processes. This ability is greatest in the case of 
satellites in earth-synchronous equatorial orbit, but even in low polar 
orbits of several hundred miles altitude the entire ocean can be overflown 
at intervals of less than one day. 

A large assortment of color photographs obtained during the Gemini 
flights is available at NASA headquarters and at the Manned Spacecraft 
Center in Houston. Some of these photographs have appeared in nonscientific 
popular magazines, and NASA has published them in an atlas. These pictures 
show that space resolution jis not limiting from these low orbits. The 
color photography shows that the color contrast is adequate for many 
purposes, such as delineating plumes of silt, mud, pollutants, and oily 
slicks off river mouths and estuaries, and showing areas of shoal water. 
Some information about the conditions of the sea surface can be obtained 
from its reflective properties. It is probable that the visibility of the 
Gulf Stream reported by Glenn on MA-6 was due to differences in the slopes 
of the wavelets rather than to differences in the water color itself. By 
suitable filtering, it is even possible to photograph the bottom at 
controlled optical depths, thus providing some information about shallow 
depth contours, where the color contrasts are very large. 

Over the open sea, color photography has not, as yet, produced much 
information of scientific value. Due to atmospheric effects and to the 
film-processing methods in use, the high seas are shown as brilliant blue, 


devoid of any recognizable color features. Whether this is all that can be 


8-4 


done with color photography over the ocean from satellite altitudes, we 
do not know. If this is the case, its usefulness will be limited to 
applications close to shore or in shallow water. Only spectroscopic 
methods would then be of value in mapping water color in deeper water. 

Light irradiatina the sea surface undergoes reflection and refraction. 
The reflected portion is polarized in the usual way, that is, the component 
of the electric vector parallel to the sea surface predominates in the 
reflected light and, at Brewster's angle, is virtually the only component 
present. This can be made use of to select either the reflected skyliaht 
or the backscattered sunlight upwelling through the water surface, 
depending on whether the desired information relates to the shape of the 
reflecting surface or to the optical properties of the bulk water. The 
refracted portion penetrates the sea and, in the absence of scattering, is 
eventually extinguished by absorption. In reality, the light is scattered 
by particles of all sizes, from molecules through the larger colloidal 
particles and up to large bubbles or, in shallow water, by the bottom. On 
the high seas, about 5 percent of the incident light is backscattered upward 
toward the sky. This is about equal to the skylight reflected at near- 
incident angles and severalfold larger than the fraction of reflected 
light passing through a suitably oriented polarizing filter. 

The backscattered light so recovered, having been subjected to 
absorption and spectral scattering along a path length that varies with 
the distribution of scatterers in the sea, is markedly different in color 
from the incident ''white'' light. In clearest ocean water, the effective 
path length is quite lona and the upward scattered light is strongly blue, 


with a dominant wavelenath of 4000 A and a quite pronounced saturation or 


8-5 


excitation purity. In coastal regions the water contains many colored 
absorbers, both inside the bodies of transparent plankters, and as 
solutes of tannins, chromatins, carotenoids, chlorophyll, and many other 
"foreign'' compounds. In addition, suspended particles of very fine mud 
scatter the light selectively and add to its color. As a result, the 
transparency of the water is much decreased, and the dominant wavelength 
shifts through green into the yellow (at 5700 A ) or even into brown. 

The distinctive color of water jis a familiar observation and leads to 
such names as the Black Sea, the Red Sea, the White Sea, the Azure Sea, 
and the Vermillion Sea. Although water color was used by the earliest 
navigators to locate familiar water masses and associated current systems, 
modern navigators depend on more ''scientific'' (i.e., less natural) methods. 
For the most part, oceanographers rely on the temperature and salinity of 
the water and more particularly on their correlation to identify water 
masses of different origin. Water color is used only as a measure of 
biological activity, past and present. For example, Steemann-Nielsen 
found that ''the distribution of water color in the open ocean outside 
influence of land must be closely similar to the quantitative distribution 
of plankton algae." (Fig.1) 

In air reconnaissance of the ocean, temperature is the only parameter 
that currently serves as a discriminant of water masses. Thus it is easy 
to distinguish the Gulf Stream water from the adjacent slope water by its 
temperature contrast. But for more subtle differences, this will hardly 
suffice. Surface temperature is auickly altered by air temperature and by 


radiation, so that water masses having very different histories can have 


identical temperatures. As an alternative to the correlation of 
temperature and salinity, it is suggested that the correlation of 
temperature and color might serve to distinguish different water masses. 

An example of the spectral variation of the backscattered light 
measured at a flight altitude of 500 ft is shown in the accompanyina 
figure,” To emphasize chromaticity as distinct from briaghtness, the 
spectra are presented in terms of their normalized trichromatic 
coefficients. (As usual, the blue coordinate is omitted.) The color 
of the ocean water is shown by its relation to the liaht reflected from 
a neutral gray card. The displacement of the color toward the green 
and yellow, relative to the clear ocean water, is also shown. The 
figure shows the sites over which the spectra were obtained. 

If equipment of requisite sensitivity can be developed, it may be 
possible to see significant ocean-color differences at satellite 
altitudes and thus to add an observable parameter which, correlated with 


temperature, will make subtle features detectable over the high seas. 


8-7 


Figure Captions 


igure 1. A series of charts of the South Atlantic Ocean. 
(a) Distribution of color of the sea (After Schott); 


(b) Distribution of phosphate in niyo fine in the upper 
5O-m layer; 


(c) Distribution of plankton organisms, thousands/ 


liter, in the upper 50-m layer, (After Hentschel 
and Wattenberg, 1930); 


(d) Distribution of zooplankton (metazoa), numbers 
per 4 liters, in the upper 50-m layer (After 
Hentschel, 1955); 

(e) Distribution of organic gross production in 
summer, g. C/ m“/day; and 


Ge) Dials bution ot vannuale met produc talon 1s G/m* 
E. Steemann-Nielsen, Galathea Rept., Vol. 1, 
Wee ZO5 Wide TSH719)6 


After National Academy of Sciences, Useful Applicat- 
ions of Earth-Oriented Satellites, Vol. 5, Ccean- 
ography, National Academy of Sciences, National 
Research Council, Washington, DC, 1969. 


Reference: 


Figure 2. Example of spectral variation of backscatter light 
Mmeasunedatyauilachit alt it udem ot SOON tac (WHO 


Report, unpublished). After the reference given 
alia Wdabers' 1g 


LEGEND 

O% deep blue 
0-2%biue 

24 2-S%bluegreen 
m1 >S %green 


LIL RR 
IY a 


ae) 


Kf 560} 


Ly 


MCL ROW AIG GORPIPUCTIEN fF (CVE) 


G) CLEAR 
(2) REDDISH 


a (3) BEACH 


8 a : (4) MEADOW ©5000 @ 


040° 4 (6) TURBID 


CAPE COD 
Pea. (6) CLEAR 


o 560 


MAX. TRANS. rs Nt 
CLEAR SHORE WATER 


oe a ae “De 
aN? B00 © 
eee (-)3 
Sat eee 6 610 x 
\ (REFERENCE 0620 “Oo 
i. ae GREY CARD oe 
2 Om 
3 Fa MAXOmRANS: 
oo 


; CEE ARE Sil OGEAIN 


ae 4 6 8 
UDMA OMAIHG CORAM GUEWY (GEE) : 


CHROMATICITY DIAGRAM 
Figure 2. 


8-10 


Frank Hebard 
Bureau of Commercial Fisheries 
Miami, FL 33149 
The major research effort at the Tropical Atlantic Biological Laboratory 
is the study of tuna distribution in the Tropical Atlantic Ocean and to 
determine how their distribution is affected by the physical and biological 
features of the ocean. During a recent cruise to west African waters 
(September-December, 1968), an attempt was made to use satellite derived 
APT data and ship-borne infra-red sea surface temperature data to supplement 
routine oceanographic observations in the location of the Gabon-Angola oceanic 
front. This front, represented by the 24°C sea surface isotherm, undergoes 
a seasonalnorth-south migration and has been reported to affect the aggrega- 
tion of tunas. 
The front was located and its migration followed during the cruise by 
monitoring changes in the location of the 24°C sea surface isotherm 
as determined by thermometer and by infra-red sensors aboard ship. 
One-hundred twenty-three (123) Essa 6 APT transmissions were received and 
photographed aboard ship and an attempt was made to relate the distribution 
of the Gabon-Angola front to features revealed on these photographs. 
We were unable to use the satellite photosto locate the Gabon-Angola 
oceanic front, probably because the temperature gradient associated with 
the front was not strong enough to affect cloud formation. In areas of 
upwelling where a strong temperature occurred, the photos 
showed that there was an effect on cloud distribution. 
In the future we will continue in our effort to monitor from aircraft 
and from satellite both physical and biological oceanographic conditions 
by means of remote sensing techniques. Of particular interest is the 


sea surface temperature, distribution of currents, distribution of fresh 


9-1 


water runoff from selected streams, monitoring phytoplankton and 
zooplankton standing crops, and location of tuna schools as a means 


of reducing search time for the fishermen. 


Rudolph Hollman 

Dept. of Meteorology and Oceanography 
New York University 

BRON No Vo 

Over the past years we have made a studv of the albedo of the 
sea surface, that is, the ratio of the unward radiant flux to the 
downward radiant flux, over the rather broad spectral band of 
approximately 0.35u to 2.5u. The instrumentation consisted of two 
Epnly pyranometers, a oyrheliometer, and a photocell. The two 
pyranometers were mounted back-to-back on a gimbal mounting affixed 
to a lona boom that was extended over the bow of the research vessel. 
The upright pyranometer sensed the total downward radiant flux 
(irradiance) or alobal radiation and the inverted pvranometer sensed 
the upward radiant flux from the sea surface. The ratio of these 
two irradiances is defined as the albedo. The pyrheliometer measured 
the direct solar radiation so that the difference between the global 
and the direct radiation yields a measure of the diffuse sky radiation. 
The calibrated photocell was mounted on a float and provided a measure 
of the upward radiant flux due to scatterina within the water. These 
measurements were largely carried out over the waters of Eastern Lona 
Island Sound. 

The results of these measurements show that the backscattered 
light contributes sianificantly (25 to 50%) to the albedo. We know 
that the albedo depends unon the solar altitude but we found the albedo 
also depends upon the state or condition of the atmosphere, that is, 


cloud conditions, turbidity, etc. An index of the state of the atmosphere 


10=1 


is the amount of sky radiation present in the global radiation. The 
measurements also indicate that the reflectance of sky radiation is 
not constant but depends upon the solar altitude and the angular 
distribution of the sky radiation itself. These results agree with 
the results derived from Kimball's data for the distribution of sky 


radiation. 


10-2 


George Huebner 
Dept. of Oceanoaraphy & Meteorology 
Texas A & M University 
Colleae Station, Texas 

For about four years we have had a program in remote sensing 
for oceanography sponsored by the Navy Oceanographic Office and Office 
of Naval Research. Personally, | am interested in the microwaves area-- 
microwave parameters of the ocean. Our program has used NASA data and 
photo data from ships. Recently, we were funded in a program investigatina 
sensors planned for orbiting vehicles and various ways to employ these 
even in cases not specifically designed for oceanogravhy. | am here to 


learn about interests and efforts in color photography of the ocean to 


aid this project goal. 


11-1 


NEw iGiey Jel lov, 
Institute of Oceanography 
University of Copenhagen 
Denmark 

The Institute of Oceanography is five years old and has two 
specialties: 

1. Turbulent diffusion of the sea 

2. Optics of the sea 

These are related because diffusion is studied by optics. 
Observations are made of attenuation, scatterina, polarization and 
fluorescence of the sea. Optics are used to characterize water 
masses and study their snreading in the sea. The distribution of 


scattering particles mav be related to primary production. 


Quantameter work. 


12-1 


Mahlon G. Kelly 
Department of Bioloay 
New York University 
University Heights, N. Y. 

My interest in light in the ocean started about seven years ago. 
At first this interest concerned the distribution of bioluminescence, 
but since has shifted to the use of aerial photoqraphy for studying 
coastal regions. Many benefits are to be gained by using such methods. 
The large-scale distribution of bottom cover has been much neglected 
in studies of bottom ecoloav, and photography aids areatly in studying 
this very important aspect of coastal areas. 

| have been studying bottom biota at locations in the Bahamas, 
near Miami, and in the Florida Keys, and am now starting work on the 
distribution and ecoloqy of suspended materials in polluted coastal 
areas. The work has benefited greatly from the help and cooperation 
of instrumentation engineers and workers interested in coastal land use. 


It is such cooperation that will allow optimal use and design of remote 


sensing techniques. 


AERIAL PHOTOGRAPHY FOR STUDY OF NEAR-SHORE BIOTIC DISTRIBUTIONS 


by 


Mahlon G. Kelly 


Although coastal areas contain some of our more valuable resources, 
synoptic study of the large-scale distribution of shallow-water bottom 
features is verv difficult because over-lying water limits survey and 
sampling. Surprisingly, although technology is available for photo- 
graphing through the water to depths of more than 100 feet, little use 
has been made of such photography for the study of biological resources 
and of marine ecology. Nonetheless, it is the biological features that 
are most immediately and drastically affected by pollution and man's 
activities along our coasts. Synoptic photography of shallow-water 
bottom biota needs to be developed to monitor and study environmental 
conditions and change. 

Color photomosaics have been obtained of approximately 200 square 
miles of shallow water area on the west edge of the Bahama Banks south 
of Bimini and in Biscayne Bay, south of Miami, Florida. These mosaics 
allowed identification and mapping of the major biotic cover on the bottom. 
This would have been nearly impossible using conventional survey techniques. 
In addition, distributional features were identified that could only be 
detected using the perspective obtained with remote photogranhy. Although 
some of these features are incompletely explained, they show important 
relationship to such environmental conditions as water depth, sediment and 
bottom geology, current scouring, wave exposure, etc. Also, man-made 
effects such as siltation due to dredging operations, canal drainage, and 


the effects of thermal outflow from power plants were reflected in the 


13-2 


types and distribution of the plant communities. 

Although there is some possibility that spectral signature analysis 
may help in studying these distributions, this approach is limited by 
the selective and variable spectral absorption and scattering of sea-water; 
any signatures are modified by the overlving water. Photoaqraphy is 
limited by the absorption of available light by the water and by contrast 
and resolution reduction due to turbid light backscatter. Nevertheless, 
bottom features may be resolved at considerable depths even in relatively 
turbid waters. 

Although instrumental analysis of photography and images and multi- 
spectral photography may be of value, their use is at present limited by 
the lack of even the most fundamental knowledge of large-scale distributions 
of the bottom biota. Backaround information is needed in primary photo- 
interpretation usina tone, hue, texture, and pattern recognition before 
more advanced technologies may be applied to their fullest, although 
photoenhancement techniques, instrumental analysis and multispectral 
photography may be invaluable as aids to interpretation. In short, sea- 
based photointerpretive studies are badly needed under diverse conditions 
to provide a backloa of information on the application of large-scale 
vhotography to the study of coastal biological resources. 

We are continuing work in the clear waters off Florida as well as 
in the very disturbed conditions near New York City. It is hoped that 
studies in such diverse conditions will prove valuable both to marine 
ecologists and to those concerned with management and monitoring of the 


conditions near our coasts. 


13=3 


Note: 

The presentation given above was an informal and slightly expanded 
version of a paper presented at meetings of the American Society of 
Photogrammetry, June 9-11, 1969, and published in the Seminar preceedineas | 
The abstract given above is identical to that of the previously presented 


paper. 


Reference 
1. Kelly, M. G., 1969. Aerial Photography for the Study of Near-Shore 
Ocean Biology, in: New Horizons in Color Aerial Photography, Seminar 


Proceedings. American Society of Photogrammetry, pp. 347-355. 


13-4 


Leonard N. Liebermann 
Department of Physics 
University of California, San Dieao 


The NASA-National Academy of Sciences Study Panel on Oceanography 


asked us to rate what could be done 
We found the following results were 
1. Global heat-budget studies 
2. General circulation of the 
3. Analysis and prediction of 


4, Analysis and prediction of 


from satellites for oceanography. 
obtainable: 

of the surface layer, 

ocean, 

sea-surface temperature, 


sea-surface roughness and sea state, 


5. Description of ocean-wide distribution of surface productivity. 


Conclusion: 


1. One of the most rewarding, 


nractical studies will be that of 


the color of the ocean. We made instrumentation for measuring 


chlorophyll by means of 6750 & band 


consisting of a spectroscope, 


prism and vibrating mirror, slit scanned spectrum by a photocell.... 


sinusoid wave, looked for second harmonic in vibrating mirror. 


2. What can be learned about the nature of waves by photography? 


Using transparent points of sea surface photos, as a hologram, one 


obtains patterns showing the spectrum of wave lengths. 


3. Measurements of wave heights by laser beam froma satellite 


may be feasible if power requirements can be met. 


14-1 


MAY 


viet 


C. J. Lorenzen 
Woods Hole Oceanographic Institution 
Woods Hole, MA 


The Biological Significance of Surface 
Chlorophyll Measurements 


The possibility of obtaining surface or near surface measurements 
of chlorophyll by remote sensing raises the question of the ecological 
importance of these measurements. Certain measurements, i.e., euphotic 
zone chlorophyll and/or productivity, are of much greater interest and 
importance in biological studies of the ocean. 

It is possible to test the correlation of surface chlorophyll con- 
centration with these other parameters with data on hand and this was 
done. The data was obtained from both the Atlantic and Pacific Oceans 
and covered the range of values one might reasonably expect to encounter 


in the oceans. The values are: 


euphotic zone 10-91 meters 

surface chlorophyll 0.04-28 mg m3 

euphotic zone chlorophyll 7.0-277 mg ae 

primary production 0.06-11 em C ware day oh 


The data was transformed into the natural logarithm and entered into 


Least Squares Regression. The results are summarized below. 


1s 


TABLE 1. n F HORS 
Ika 1 Coil = S.49) -- O262 Im Suet, Gn, Sil 398%«* 0.82%% 
iin DoOPKOELe Zone = S546 = O529) ihn Suvee, Gm, 91 388% 0.81** 
lim, jorealineeyy jorcorel 5 = gs} 45 OAS} iin, Suieie, Clnil. 87 99%% 0.54%** 


The conclusion of this exercise is: 

Surface chlorophyll estimation on a continuous basis is a worth- 
while objective, since it is a reasonable good estimator of euphotic 
zone chlorophyll and euphotic zone primary productivity. 

The measurement of either A loeeanaln or productivity in the ocean 
is of great ecological importance, and the point doesn't have to be dis- 
cussed here. Let it be sufficient to say that in some circumstances 
chlorophyll measurements may help to delineate areas where certain fish 
resources might be found (see comments by Blackburn), depending on 
meeting certain biological restrictions. On the other hand, obtaining 
chlorophyll information regularly over large areas of the ocean would 
be very interesting and helpful in solving certain problems involved 
in the study of food chain ecology. 

One other interesting feature of the statistical analysis was the 
strong relationship between surface chlorophyll and euphotic zone depth 
(the depth to which 1% of the surface irradiance reaches). Apparently, 
most of the extinction of visible light in the ocean can be related 


to chlorophyll (contained within algae). 


15-2 


Paul M. Maughan 

Special Assistant for Marine Resources 
Bureau of Commercial Fisheries 
Washington, DC 20240 

Bureau of Commercial Fisheries remote sensing programs, such as the 
space-photo interpretation of Dr. Robert Stevenson's at Galveston and the 
fishery intelligence program of Mr. Kirby Drennan's at Pascagoula, are 
coordinated through the BCF Central Office in Washington, D.C. 

The remote sensing programs are proceeding in two study areas: iL) 
direct detection of fish stocks in their natural environment and, 2) 
indirect detection of fish stocks using a knowledge of the physical parameters 
(such as areas of upwelling and convergence zones) to determine where fish are 
without actually observing the fish. Current plans are to investigate newer 
remote sensing techniques and to specify "fish sensors" for the proposed 
oceanographic satellite. There is no doubt that a real benefit to the 
fishing industry can be made through observations from a satellite system. 

One study at Oregon State University currently in progress which BCF 
is sponsoring, is observing the well-defined Columbia River plume flowing 
south along the Oregon coast and an adjacent area of upwelling, and relating 
these to the presence of albacore tuna. The first of three phases is now 
underway and involves the use of multi-spectral photography, IR (PRT5 ) 
temperature data, and standard color photographs from aircraft. OSU 
scientists have found major color differences between the plume and ocean 
water. Nimbus III HRIR satellite data will be used to determine the sea 
surface temperature. In conjunction with the albacore study, a forecast 
network issues a daily bulletin to the tuna fleet. This study is a combina- 
tion of applied and basic research and has a real monetary advantage to the 


fishing industry. 


16-1 


William J. Merrell, Jr. 
Department of Oceanography 
Texas A & M University 
College Station, Texas 

| am interested in identifying physical parameters and features 
in the ocean through color photography and other remote sensors. 
My most recent work has been related to identifying oceanographic 
features in Apollo photography and in multisensor data taken in 
Mexico and Brazil with NASA aircraft. 

(The following is taken from a letter dated August 24, 1969 
from W. J. Merrell to G. C. Ewing.) 

"Apollo VI (See Notes 1 and 2 on p. 17-3) 

This was an unmanned flight, so we have the highest percentage 
of photographs over the deep ocean. Although there also seemed to be 
a high percentage of cloud cover, some frames definitely show evidence 
of color boundaries. The Texas A & M team (Paris, Chmelik, Merrell, 
and Arnold) mention one (frame 1495) in a paper to be published in the 
final Apollo VII report. (This was turned in to NASA over a year ago 
and has not been released yet.) Frames 1499-1501 and frames 1495-97 
definitely show some sort of color variation or boundary. The overlap 
of the frames is very nice in that it gives added assurance that the 
feature is not due to some mishap in the development of the photoaraph. 
Dr. Stevenson's slides were probably taken from one of these sequences. 
The location of these color features is at least 700 kilometers offshore. 

"Apollo VII 

There are no photographs which show color boundaries because there 
are no vertical photographs in the deep ocean that are not almost 


completely cloud covered. 


lial 


"Apollo IX (See Note 3 on p. 17-4). 

Although few photographs of the deep ocean were taken, a definite 
color formation is present in one. Frame 3588 was taken from 107 N.M. 
at 12°N and 50°W. | believe that the white streak in the center of the 
photograph is a result of some error in the development of the photography 
and not a feature in the ocean or atmosphere. | reviewed satellite 
pictures of contrails from aircraft and found them to be much thinner 
and having a shadow. However, this brings up the question of why the 
astronaut took the photograph, as no other photographs were taken offshore 
without interesting cloud formations, etc. Perhaps the change in the 
glitter pattern caused by a convergence zone or wind shear zone caught 
his eye. It seems to be toward the center of the photograph. Anyway, 
the color feature | referred to is on the right-hand side of the 
photograph and appears to be in the general form of a large eddy. 

| believe that color boundaries in the open ocean have definitely been 
recorded in the previously mentioned Apollo photographs. How general 
these few photographs are of the total world ocean is impossible to say. 
No good satellite photographs are available for the Central Pacific Ocean. 
(lt was night in the Pacific when the Apollo V! photographs were taken.) 
| am sure that some may argue that the color boundaries | have mentioned 
may be from the outflow of the Amazon or froma large buildup of floating 
material sometimes found in these regions of the Atlantic and are not 
indicative of the color changes and boundaries in the world ocean. This 
may be true; but as of now, it is impossible to prove. | believe the 
important facts to be considered when we review these photographs are 


that they were taken far from shore and definitely seem to describe ocean 


17-2 


features solely by changes in ocean color. More missions are needed to 
answer the general question of how common these color boundaries are in 
the world ocean and more specific questions such as why do these color 
boundaries usually appear in photographs which also record what seems to 
be a convergence zone or roughness boundary. A satellite color sensor 
Similar to the one discussed at the workshop could help answer these 
questions if it were utilized over the central portions of the ocean." 
Notes Added by Compiler: 
Note 1 
NASA photographs are available from: 

Jo Ing Wierukeyy,; Inae. 

2321 4th Street N.E. 

Washington, DC 20002 

(202) 526-5000 
Give the photo number and spacecraft flight. The prices vary but are 
around $3.00 for a glossy print to $0.35 for a 35 mm slide. Super slides 
are around $3.00. Mr. Merrell gives the numbers of several good photographs. 
Wore 2, (Wee5 WS), USS), 
AS6-2-1495, AS6-2-1496, AS6-2-1501, AS6-2-1502 

These photographs of the Atlantic Ocean were taken from the Apollo 6 

spacecraft, an unmanned, orbiting vehicle, on April 4, 1968. Solar time 
for each photograph was 1011, 1013, 1027, 1030, respectively; spacecraft 
altitude was approximately 190-192 kilometers. The camera used was a 


J. A. Maurer, 70 mm. with a Kodak Ektar, 76 mm, f/2.8 focal length lens. 


WISD 


The film used was Eastman Kodak, Ektachrome, SO-121 high resolution aerial, 
70 mm. The camera was operated by automatic control and was mounted inside 
the cabin of the spacecraft. 
Note 3, (May 8, 1970) 

The white streak in frame 3588 of Apollo IX has been identified as 


the wake of a nuclear submarine by the Navy. 


17-4 


Richard C. Ramsey 
TRW Systems 
One Space Park 
Redondo Beach, California 

| have been involved in ocean color for two to three years. In 
1967 | made a study on application of remote sensors to measurements 
of ocean color (Study of the Remote Measurement of Ocean Color, Final 
Report, Contract No. NASW- 1658, prepared for NASA Headquarters, 
Washington, D.C., 26 January 1968). 

"The general tasks envisaged at the beginning of the program were: 

Task 1 - Analysis 


Conduct analysis of the spectral variation of the optical 
characteristics of the sea water as viewed from a location 
in or above the earth's atmosphere. This analysis was to 
include evaluation of the effects of surface conditions. 
If necessary, simple laboratory tests using TRW owned 
equipment would be used to evaluate the effect of surface 
roughness. 


Task 2 - Definition of System Requirements 
Based on the analysis of Task 1, a set of requirements 
would be prepared for a system capable of measuring the 
spectral characteristics of water from a moving vehicle. 
Both aircraft and snacecraft would be considered. 
Task 3 - System Definition 
Based on the requirements of Task 2, a preliminary design 
of a system to best meet these requirements would be 
performed. This design would include specification of 
major components and a preliminary evaluation of weight, 
dimension, and power requirements. 
"It is felt that these tasks have been completed during this study. 
lt was not considered necessary to perform the laboratory tests of the 
effects of surface conditions because some previous measurement data were 


available in the literature and because of the difficulty in simulating 


real conditions.!! 


18-1 


In 1968 and 1969 | participated in airborne measurements of ocean 
color at Woods Hole, as renorted herewith by Clarke, Ewing and Lorenzen 
(Spectral Measurements from Aircraft of Backscattered Light from the Sea 
in Relation to Chlorophy!1 Concentration as a Possible Index of 
Productivity. George L. Clarke, Gifford C. Ewina and Carl J. Lorenzen, 
SCIENCE, jo. 4, Im aress.)) 

In correspondence with C. F.Hagelberg, 8 July 1969, | set forth 
"calculations [which] relate the visible spectrum of the total upwelling 
light from the ocean waters to the chlorophyll content of the water...... 
These calculations, which produce results that correlate well with measure- 
ments with the water color spectrometer, indicate that the use of a 


minimum of only two bands should result in a chlorophyll determination." 


18-2 


Donald S. Ross 

Philco-Ford Corporation 

Space & Re-entry Systems Division 
Palo Alto, California 


Primary interests lie in acquisition and data processing of all types of 
earth sciences aerospace imagery, but with particular emphasis on oceano- 
graphic subjects. Data precessing is accomplished by a variety of photo- 
graphic, optical and electronic techniques, whereby image grey levels are 
converted from analog to digital form to emphasize or suppress pre-selected 
sets of information. "Data processing" as used here includes enhancing 
images to aid visual interpretation, as well as quantizing grey levels for 
assessing luminance characteristics of the subject. Similar treatment is 
given to images taken in different spectral bands which are added to or sub- 


tracted from each other to enhance the information. 


For oceanographic applications, a typical example would be optical or 
electronic digitization of variations in scattered light intensity within 
the water (as recorded by the camera) and conversion of each level into 
highly contrasting colors, for relative water depth assessment. In another 
example, the image of the water surface, taken in an infra-red spectral band, 
would be combined in opposite sign (positive-to-negative masking) with an 
imace taken simultaneously in a blue or green spectral band, to suppress 
image information common to both spectral bands; in this case the image of 
the water surface. The remaining image is that of sub-surface illumination 
which is not recordable in the infra-red spectral band, but which is found 


in the blue and green bands. 


The photo-optical image enhancing methods retain, or even yield apparent 
improvement of, the inherent resolution of the input image; but laboratory 


processing time is required. Electronic false color image enhancement is 


done in real-time; however, while the resolution of the cathode ray tube 
enhanced color image is substantially better than commercial color television, 


it cannot provide the high resolution of the photographic process. 


The present and future activities of our group, relating to ocean color, 
include planning and flying 4-band multispectral photography with our own 
camera for the practical testing of suitable films, filters and processing 
chemistry, to improve the recording of small color changes in the water, and 
aid in the selection of spectral bands for maximum depth penetration. Con- 
tinuing programs include the separation, enhancement and analysis of Gemini 
and Apollo photography for oceanographic subjects such as bathymetry, sedi- 
ment flow patterns, shoreline discrimination, emphasis of water color changes 
for delineating current boundaries and areas of upwelling, enhancing bottom 


features and topography, clarifying wave diffraction patterns. 


Methods of enhancing color differences are also under continuous development 


and improvement in our laboratory. 


19-2 


Abstract of Formal Presentation: 


While the development of equipment capable of accurately measuring water 
color and chlorophyll concentrations from orbital altitudes is under way, 
it is recognized that considerable work, experimentation and time will be 


involved before reliable working devices can be orbited. 


In the meantime the contributions which existing imaging sensors can make 
to the detection and assessment of water color changes should be neither 


underestimated nor overiooked. 


The catalog of Gemini and Apollo 70 mm color photography contains hundreds 
of images which demonstrate in a most graphic way changes in water color 


in the open ocean and its shorelines. 


The changes in water color in many of these images are clearly associated 
with features such as currents, upwelling, sediments, depth variations, 
changes in bottom composition, and so forth. The value of these images 

lies in their ability to indicate important oceanographic phenomena, through 
variations in water color. For this form of interpretation, it is only 
necessary to detect and record a color change; it is not necessary to be 


able to measure it accurately in the radiometric sense. 


The natural color film images taken from space which provide the most 


4 


Sa 44 7 = 
useful in 


K 


Formation for oceanographic purposes (through variations in water 
color) depend on blue and green sensitive layers, to record the differences 


in the ratios of blue and green light in the water. 


However, hardware systems currently proposed for orbit do not include imaging 
sensors operating in spectral bands below 500 my, in the blue and blue-green 
region. The degrading effect on the atmosphere on image contrast below 500 mu 


has been considered to be so severe that images obtained in this spectral 


192 


region would be of little value. This is unfortunate, since a blue or blue- 
green band is essential (in addition to a green spectral band) for detecting 
water color differences of primary significance. The blue and blue-green 
spectral region is also where the attenuation of light in clear water is 


least, and greatest photo-optical depth penetration is possible. 


In the course of image enhancement work in our laboratory, numerous Gemini 
and Apollo natural color film images of oceanographic subjects have been 
color-separated by photo-optical means. It has been found that the blue- 
sensitive layer in these films contains substantial information despite the 


ffecets of the atmosphere. Examples are shown in Figures IA, B and 2A,B; 


i) 


where blue and green separations made from typical images, taken from orbital 


altitude, are compared. 


It is concluded that it is quite feasible to utilize a spectral band in the 
460-500 my region for remote sensing in oceanography; and if the many 
important oceanographic phenomena associated with water color are to be 
detected, it will be essential to record and couple this spectral band with 


a green record. 


U4 


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ah 


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So. Carolina, 


Georgia, 


ee Notel on p.17-3) 


(s 


Apollo 1X Color Photo 
Blue Separation 


Frame No. AS9-3148 


Georgia, So. Carolina, Savannah 
x (See Note 1 on P.17-3). 


AS9-3128 


Green Separation 


Apollo IX Color Photo 
Frame No. 


n 
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M 
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Apollo IX Color Photo 
Blue Separation 
Frame No. AS9-3128 


No, Carolina, Cape Lookout, Cape Hateras 


K(see Nete | on p- 17-3) 


Peter M. Saunders 
Woods Hole Oceanographic Institution 


| am a meteorologist with an interest in exchange processes 
between ocean and atmosphere. Currently Mr. Richard Payne and | are 
attempting to make a definite measurement of the short wave albedo of 
the ocean. Albedo is the ratio of the upward to the downward irradiance 
close to the sea surface. Upward irradiance has two components: 

1. Energy reflected from the surface, and 

2. Energy scattered internally which escapes through the 

surface. 
In our measurement program we separate these. Above the surface we 
measure total and diffuse downward and upward irradiance using pyra- 
nometers, and just below the surface we measure the backscattered 
irradiance on a transparent floating buoy. Broad band sensors are 
used, namely thermopiles with uniform sensitivity from .3 to 3 microns; 
thus, we measure the energy fluxes into and out of the ocean. 

On the theoretical side | have studied the interaction of 
electromagnetic waves with the sea surface, following the work of Cox 
and Munk. By extending their work to oblique viewing, where the 
problems of multiple reflections and shadowing are important, | have 
given an explanation of the existence of the ocean horizon, predicting 
the radiance contrast between the sea and the sky there. 

The theoretical studies (together with the experimental 
measurements) show that the following factors influence albedo: 

1]. Roughness 


2. Directionality or diffuseness of illumination. 


20-1 


We will compare theoretical surface reflection properties with 
our measurements, and attempt to relate the backscattered light within 


the ocean to other oceanic properties. 


20-2 


John W. Sherman, III 
Spacecraft Oceanography Project 
Naval Oceanographic Office (Code 7007) 

The Spacecraft Oceanography (SPOC) Project plans and recommends to 
NASA a program in remote sensing oceanography and coordinates air and 
spacecraft experiments for oceanographic users in the NASA Earth Resources 
Survey (ERS) Program. 

The critical areas of sensor application that are important to oceano- 
graphy are: (1) ocean color and (2) microwave exploration. In the area 
of ocean color, what needs to be experimentally accomplished must be docu- 
mented by meetings such as this and the appropriate aircraft remote sensors 
obtained. A critique is invited of instrumentation for space and aircraft 
sensors related to color measurements. In the ERS Program, for example, 
the Department of Agriculture is a clear "user" group, but there are 
13-17 government agencies involved in oceanography, with no one, single 
user. The SPOC Project attempts to act as the technical focal point for 
NASA in the ERS Program. Thus, the requested instrumentation critique 
is in reality an attempt to insure that oceanographic user requirements 


are met. 


A DLNBY 


Raymond C. Smith 
Visibility Laboratory 
Scripps Institution of Oceanography 
San Diego, California 

Lately, we have been measuring chlorophyll] content and total 
particulate matter simultaneously with our spectral irradiance data. 
Also, we have a new instrument which measures radiance distributions 


under water. The radiance distribution data allows many optical 


properties of natural waters to be calculated. 


22-1 


Robert Spiers 

Langley Research Center 

National Aeronautics and Space Administration 
Hampton, Virginia 

Our earth resources activities are identified with remote sensor 
problems of research organizations: 

1. Working directly with the U. S. Fisheries, we are developing 
a spectrophotometer to measure the reflectivity of fish schools and 
ocean water. Output: reflectivity vs. wavelength. An electronic 
signal processing technique is used to filter radiance noise from ocean 
measurements. 

2. Working with Virginia Institute of Marine Sciences, we wil] 
launch a balloon carrying four cameras with color filters to photograph 
Chesapeake Bay and the Atlantic. These photographs will be analyzed 
usina ship measurements of ground truth. 

3. Working with Old Dominion College, we will measure changes 
in off-shore bottom contours with time. 


4. We are employing PhD's from various disciplines to perform a 


preliminary design of ERS systems. 


235-1 


Joachim Stephan 
Battelle Institute 
Columbus, Ohio 

Remote sensing applications to biota and wildlife on and near 
Amchitka Island in the Aleutians are presently being studied. We are 
currently photographing areas from a low-flying helicopter near shore 
to determine species of the algae and to determine if man-made effects 
disturb any of this. With marginal weather photography prevalent, 


never above 1,000 feet altitude, we can distinguish different algae 


populations. 


24-1 


Robert E. Stevenson 
Bureau of Commercial Fisheries 
Galveston, Texas 

We are concerned with the interpretation of color photography 
from manned spacecraft to determine the significance of the view 
from space to the fisheries. We are working primarily toward the 
development of a satellite system to provide real time information 


to all users. My purpose here is to learn actual applications of 


color photography to this goal. 


25-1 


Martin J. Swetnick 
National Aeronautics and Space Administration 
Office of Space Applications 

At NASA headquarters, in the office of Space Science and 
Applications, | am responsible for the Earth Resources Survey Program 
Oceanography discipline. 

One of the functions of an Earth Resources Survey Program staff 
scientist is to prepare and provide material for selling the concept of 
satellite oceanography to NASA management, Conaress, and segments of the 
oceanographic community both within the government and the private sector. 

Interest in getting an Earth Resources Technology Satellite (ERTS) 
flight program underway as early as possible has been expressed by several 
members of Congress. Planning an ERTS oceanoagranhy mission will be 
somewhat difficult in view of the lack of a focal point for oceanographic 
activities within our qovernment. The identification of potential users 
of ERTS oceanography data is another problem that needs to be resolved. 

NASA is an R & D agency. One of the missions of NASA is to apply 
space technology to global synoptic observations of remote sensor techniques 
for use on satellites. It works with other agencies who can evaluate the 
capabilities of various remote sensors for providing data on ocean parameters 
Or processes. 

NASA plans to carry out an ERTS program calling for a series of 
four remote sensina missions. The first two satellites (ERTS A and B) 
will be directed toward landing mass observations. These satellites wil] 
carry a three-color hiah resolution television camera system and a multi 


channel imager. Although this instrument payload is not optimum for ocean 


26-1 


observations, there will be a need to determine whether it could provide 
some meaningful information about the oceans. The third satellite (ERTS C) 
will be used for ocean survey. Serious consideration will be given to the 
selection of remote sensors. This will involve discussion with interested 
people and potential users of the data. 

NASA relies on the Spacecraft Oceanography Project (SPOC) in 
NAVOCEANO for the daily technical administration and monitoring of the NASA 
funded research programs at universities, private organizations, and other 
government agencies and for coordinating the work of scientists, participating 
in the NASA aircraft missions supporting the checkout of remote sensors 
during overwater flights and, where possible, the acauisition of ground 


truth information. 


26-2 


O. Lyle Tiffany 

Chief Scientist 

The Bendix Corporation 
Aerospace Systems Division 


Our division of Bendix is working in the fields of thermal and multi- 
spectral imaging for earth resources. 

In instrumentation we make commercial thermal mappers with a variety 
of infrared detectors as options. We have built our own 9 channel visible 
and near infrared scanner which is now flying in a company Beechcraft. 
We are at the present time engaged in the design and fabrication of a 
24~channel scanner from the near ultraviolet through the visible and out 
to 13 microns in the infrared for the NASA Houston. 

On the research side we are flying our multispectral scanner and 
thermal mappers to collect data to be compared with ground truth for a 


variety of disciplines. 


27-1 


PRE LIMINARY NOTES ON THERMAL MAPPING AND 
MULTISPECTRAL SENSING IN OCEANOGRAPHY 


Resource survey missions for the purpose of exploring the value 
and utility of multispectral data are conducted at Bendix in a company air- 
craft which is a Beech D118. This aircraft is instrumented with an infrared 
scanner, anda 9-channel UV, visible, and near infrared multispectral 
scanner. The supporting equipment includes a 70-mm aerial survey type 
sequencing camera. The video from the infrared single channel thermal 
mapper and from the 9-channel multispectral scanner are recorded on 
wide-band FM tape. After the mission this tape is returned to the laboratory 
for detailed studies of the multispectral data which includes conversion toa 
digital format and statistical studies using a large computer such as the 
IBM 360. Imagery can be produced from the multispectral data using the 
film recorder in the laboratory directly from the tape recorded video. The 
data produced by a multispectral line scanner is particularly well adapted 
for studies of image enhancement and target classification because linear 
combinations of the electronic video can be formed using analog circuitry. 
The result of such linear combination can be fed directly to the film re- 
corder for the production of enhanced imagery. The particular formula 
used in forming any given linear combination is determined from a statistical 


study of the digital samples of the multispectral data. 


27-2 


The results from three different missions will be illustrated 
briefly in this talk. The first from the Thermal Mapper shows Boston 
Harbor in the infrared as observed during a night time flight at low water 
ebb tide. The other two examples are taken from multispectral missions. 
One is in the area of agriculture and the other in the area of limnology. 

On the morning of 11 June 1969 at 0230 hours a Bendix airplane 
equipped with a Thermal Mapper flew a total area cover mission of the 
Boston Harbor area. The time of the flight was selected to give coverage 
at low water slack tide. The detector in the mapper was an indium anti- 
monide device cooled with liquid nitrogen. It was operating unfiltered. 

In the absence of reflectance solar IR this gives thermal coverage out to 
about 5.5 microns. Figure 1 is a sample of this imagery. 

Excellent thermal contrast was obtained in the water of the harbor. 
In this imagery the dark areas correspond to warmer areas and the lighter 
areas correspond to cool spots. In general, the water was warmer than 
the land. When the complete set of data is assembled in an area cover 
mosaic the spatial distribution of the thermal mixing is expected to show 
the flow patterns into and out of the harbor as the tide flows. 

LARS, the laboratory for agriculture remote sensing at Purdue 
University, maintains a set of ground truth over a number of well defined 


flight lines in rural Tippicanoe County where Lafayette, Indiana is located. 


27-3 


Multispectral data was obtained over this test site on 13 November 1968 to 
evaluate the Bendix 9-channel scanner for use in crop classification studies. 
Six of the nine channels were recorded on the seven-channel analog tape 
recorder used at that time and subsequently played back in the electronic 
processing laboratory. A grey scale presentation of the reflectance in each 
wavelength region was in the resulting imagery. The reflectance range in 
each channel is known from preflight calibration and allows reflectance 
values to be placed on each resolution element on the ground. The analog 
processing laboratory allows any channel or combination of channels to be 
recorded on film and permits processing coefficients to be applied to any 
channel. The coefficients may be selected from digital data extracted 

from the original analog tape after computerized statistical analysis has 
been performed. In this way targets of interest are enhanced and the 
backgrounds suppressed. 

Two statistical methods were employed in an attempt to enhance 
the agricultural targets of interest. Before the data was analyzed it was 
submitted to processing to produce unenhanced imagery for selection of 
the areas to be sampled. Seven thousand digital samples of the selected 
areas were then obtained for which ground truth was available in the form 
of crop identification. The first statistical method applied was factor 


analysis. The linear combinations of the original data channels specified 


by factor analysis are intended to make it possible for the user to identify 
physical phenomena responsible for variation in the data to be identified 
with particular factors. Upon completion of this statistical analysis the 
processing coefficients thus specified were input to the analog processing 
unit. and film showing the variation in the first three factors was produced. 
The results of this factor analysis are shown in Figure 2. The ground 
truth collected by Purdue University identifies the dark areas in the 

factor 1 imagery as corn fields. In factor 2 the dark areas correspond to 
fields of bare soil. The second statistical analysis employed with respect 
to this data was multiple linear regression analysis. Samples of this 
imagery are shown in Figure 3. The middle strip identified at the top with 
the caption ''corn equals white'' corresponds rather well with the factor 1 
imagery from figure 2. Corn is enhanced in both cases. The sense of the 
enhancement is changed however so that in the case of regression, corn 
appears as the lighter color fields. With the aid of the ground truth, wheat 
fields were also identified. The regression analysis was performed to 
determine linear combinations which would enhance wheat fields. This is 
also identified in Figure 3. Finally, bare soil was enhanced in much the 
Same manner as found in Figure 2. Again, however, the sense of the 
enhancement is reversed so that bare soil appears as the light color in 


the regression imagery while it appears as a dark color in the factor 


25 


analysis imagery. 

More recently Bendix has been studying the apparent color change 
of water with water depth using the multispectral equipment. This data 
collection activity is being conducted in support of a data analysis program 
being conducted for the Electronics Research Center in Boston. This data 
was collected at Pentwater which is a small port on the eastern shore of 
Lake Michigan during the week of 21 July 1969. Lake Michigan was selected 
as a test site because the water is relatively clear and clean, making the 
bottom visible out to depths of perhaps 20-30 feet. It was also desired 
that the test site have a very uniform bottom in order to remove one of the 
variables from the experiment. The entire eastern shore line of Lake 
Michigan has an extremely sandy and uniform bottom. The currents flowing 
north and south along this shore provide an interesting structure for study 
with multispectral devices. Figure 4 illustrates this structure. The 
picture is an enlargement of 70-mm imagery from channel 4 of the multi- 
spectral scanner. The scanner was calibrated in sucha way that reflectance 
values ranging from 0 to 15% would completely fill the dynamic range of the 
video. The wavelength boundaries of channel 4 extend from about .56 to 
.62 microns. This range includes the wavelength which has the greatest 
water penetration in the visible region. The characteristics sandbar 
structure of the eastern shore of Lake Michigan is clearly visible in this 


pueituasey. 


27-6 


The NASA contract in support of which this data was collected 
has as its objective the quantitative measurement of water depth using 


multispectral video and multiple regression as the necessary tools. 


2t=1 


Figure 1 Thermal Imagery of Boston Harbor 


27-8 


FACTOR 1 FACTOR 2 FACTOR 3 


™ 
le 
t 
A~) 
& 
= 
' 
2 
= 
Cy 
s 
a 


Figure 2 Factor Analysis of Agricultural Data 


27-9 


WHEAT = WHITE CORN= WHITE 


BARE SOIL = WHITE 
rr. - 


= 
ot 
3 
s 
2 
> 


ALT. 5000 FT. TIME 1440 HR DATE 13 NOV. 1968 


Figure 3 Regression Analysis of Agricultural Data 


27-10 


Figure 4 Sand Bars in Lake Michigan 


27-11 


NPR 
aM 


ie 
Sa 
ee 


John E. Tyler 
Visibility Laboratory 
Seripps Institution of Oceanography 

Our group has been actively engaged in making measurements of spectral 
irradiance underwater for the last three or four years. We have accumu- 
lated a considerable body of data not only on radiometric data but also 
on other oceanic variables such as: chlorophyll concentration, primary 


productivity, total particulate matter, temperature profile and trans- 


mittance. 


We are interested in both biological and physical aspects of radiant 
energy in the sea. Our data give the energy available for photosynthesis. 
At the same time our data quantitatively specify the optical signature 
available underwater for the detection of surface chlorophyll from above 


the water. 


We now have pending two major publications; viz., a report on the 
results of an expedition conducted by 8.C.0O.R. Working Group 15, which 
will be published by The Office of Oceanography, UNESCO, Place de Fontenoy, 
Paris 7°, France, and a monograph entitled "Measurements of Spectral Irra- 
diance Underwater" to be published by Gordon and Breach Science Publishers, 


150 Fifth Avenue, New York,New York 10011. 


28-1 


PEO hou 
cee Gaul 
OHA tt 

MO ie Ne 

WOAH 


Morris Weinberg 
Block Engineerina, Inc. 
19 Blackstone Street 
Cambridge, Massachusetts 
| have not applied remote Raman spectroscopy to the sea surface. 
My role at Block is in data analysis, quantitative snectral analysis, 


field programs, etc. Quantitative analysis is remotely possible for 


surfaces and gases. 


29-1 


OCEAN IRRADIANCE MEASUREMENTS USING 
AN INTERFUROMBTER SPYCTROMETAR 
Before discussing the data, I'd like to briefly 
familiarize the reader with the mechanism of data reduction 
LO EUS Vex pekaMehitw i LM un basi lOti Shows stMelaceval: Wambo 
ESGOC|eSIN WISSC|| rsOse’ Oloyecishiquliarey elas Pate (Speer 0) eee 
MERE jOlOE Shows Bin Wincoirrecered wecduceiom, Os Sjecexrum 2O, Ae 
ANS jXOLME, AN WAWelenGiEn Seale iS SSezloll wSJnSdl lone elae OieeirinerceS 
scale (spectral radiant emittance) is not yet calibrated. 
(NOTE: “The wavelength Scale obtained from the antexterometer 
spectrometer 1s really linear in wave number. Therefore, in 
interpolating between wavelength points presented on each 
Spectrum this fact should be incorporated). The next plot 
SIMON TeloKS) Keliohe bray alialsjieraUlmlciole nalsisjoioyaliskc) |azubaKereaohay (one ielaKs) 14 92)Ul 
spectrometer used in the measurements. Bach UncomTGecucdmspeeeraumnt 
is divided by this function to properly display the actual 
data. Note that the instrument response function is “bell 


J 


shaped Thus, we would expect the final structure in the 
corrected spectrum to be somewhat modified from the uncorrected 


corrected 


i 
lee 
ry 
Qs 
# 
D 
cr 
De 
o 
Fh 
b 
2 
Ay) 
ed 


GENES} 5) | WAMS HAGE WS loOSSte TeViOLE Le 
Spectrum an this sek. The rinal comrected Spectrum has) ats 
SIMYOS MEE LEsl ig Elie AIOM EO COMLSECTCIOME: iO ILSLC—-Oik“val GW » 
attenuation,:nunb2r of HENS, | Sue. I should be quick to make 


two points: 


29-2 


1. Every spectrometer has an instrument function 
and this function should be removed before attempting diagnostics 
with the data. The interferometer spectrometer function closely 
resembles that of the photomultiplier tube, alone, since there 
Zee imo) Clisjioesiing Glemendess ReEMCe, a SSikoelay TebiaiesOm seSSeules- 

2.  Sinee instrument calibration corrections are 
required for quantitative spectroscopic studies, compute 
reduction of the data is really the most advantageous route 
to follow. Hence, the necessity of performing Fourier trans- 
formations on the computer in the case of this class of instruments 
poses no constraint since one would resort to the computer 
OVE elle Oeineie COrewOCERCMS. 

The enclosed figures contain the computer reduced 
spectra numbers 19-26. All of these spectra were obtained in 
75 seconds with attenuation factors ranging from approximately 
uO to 10". As you can see, the spectrometer was! hardly taxed 
during the experiment. 

Specena 9, 2s) and 24 wermeteaken ae che sumtace loi the 
water uSing the modified light shield basket: we brought. 
There was no glass bottom on the basket. fence, these three 
spectra measure the zero depth upwelling irradiance at Eel 
Pond during this time period. The measurements were taken 


at aboule an 80° depressiicom angle looking down iamto the water. 


29-9 


Spectra 20, 21 and 22 were taken at the surface of 
the water. These spectra would have contributions from 
upwelling and reflected light. Again, the depression angle 
of the spectrometer was 80°. 

Spectra 25 and 26 were obtained by depressing the 
spectrometer by about 80° and viewing ane gray card. These 
measurements indicate the downwelling irradiance at the ee 
of the measurements. The gray card is assumed to have 0.18 
diffuse reflectivity coefficient over the spectral response 
of the instruments. 

1. All spectra should be matched in wavelength scales 
when overlaying for comparison. 

2. The irradiance scales on all spectra have been 
normalized to ‘9 inches. Hence, structural details between 
spectra can be compared readily while quantitative irradiance 
differences are not well obtained by direct overlay. 

3. The weak structure residing on top of the broad 
spectra is probably noise and should be treated as such unless 
it has regular repeatability from spectrum to spectrum. 

© ° 

4. The data from 7000 A to 8000 A is noise domineted. 

Jo ABE slissic Sie, “aS Aintevinal CoOMenSeeaGy OL cle 
experiment is best validated lowe Conoainaine, 2S, ancl 26, ((cieeyy Care!) . 


A direct overlay shows almost identical spectral structure versus 


29-4 


wavelength between these two spectra. I would estimate the 
° 

Suga eo momse vats 500 0A to be 20/1. The arradiance varies 
by about a factor of 4 to 5 between these spectra. Most 
of this variation is probably due to cloud cover changes. TI 
would conclude that there as a high degree of Consistency in 
SJOSCSrweicall SGieiavCieureS slid tela) seesiilicatine Gleicels — G@llouiel| loners swelipaiclieaiosn 
does not appear to alter spectral shape. 

Go Was jssjoeie loy Smmed eimel Wyler ain elie wo wicinell Cis 
the Optical Society of America, 57, 589 (1967) will be used 
as a guide in validating the Woods Hole experiment. 

° 

7. Our average Gray Card irradiance value at 5000 A 
: 3 2 : , Sh 
1S Zod s< IO” WM Werties/emi Us Comsicleiciing a Chlincwse seizileGiemyaicyy 
Of the Gray Card of 0.18 we obtain a downwelling irradiance 

4 2 

wallue oi 1sS se dO" WW WecES/om” lM. Wyle, ie Cieeieens InAIKe, 

Sle vis 5 2 : ‘ 
OQOL IMAC 2 WEIS Ol 2 ox NO” WM WerkeES/em” (Mo I Wowllkel Joa Sineilaimacl 
EOMACCe pie Ehlsieractowm OF UO ditterence as paztivally beimedue 
(c@ Cube SrSineSs aie Ciloucl Gower (seidiajos, El seer Cre Si) Glial ielie 
TESHUALaLIMaLIONS) TEeeIcOIe OE 3 Oise 4! eis cl jo@Ssslolle Cinidone slim Cyl Cela losses 
due to the stacking of many neutral density AMCs, AIL aim 
ail, we could not havc hoped) for nuch) better resulces) any ehie 
short time period for the work. I'm very encouraged with 


this comparison. 


ZS) 


So Was AO BosorwoerCin Gajos ee BOO A and 4300 A 
ame neal vand) due jto aceual dijos) im the) /solac (spectral imradianee 
(see all spectra 19-26 for the intense absorption near 4000 A). 

25 MAS Sicivicewica il COMSLSESMEGY stOIe IAS WoO Owe Welieeue 
Spectra is excellent (compare 20, 21 ere DP) 6 

lO, WS TreseICMeMeES WeseneieLein On ZO=BQ icclingies Oweire a 
TAGEOIC OF AlOWUE 5.) Wale LAGEOI COMSArSS Taworeloly Wwatela ene 
Gray Card data and is probably due to changing cloud cover. 
Therefore, I would accept this variation as being real. 

ll,  COnesLceriag ZO as eae loSsst Woy OG WaESIe Sioxseierum 
and comparing with the Gray Card data (25 and 26) at 4500 A 
WO AAMC! Alig) aliceAGiAiMnGa Olt 65s) 5x 107 U wertes fone (i sE@ie ZO 
and an average of 3 x Oo [ uatis/on ue stone ZS Bincl ZOE  Siimce 
the Gray Card reflectance is known as 0.18 one concludes that 
the reflectance at the surface of the water is 0.04. Admittedly, 
many meteorological changes were taking place during this 
time period. Nevertheless, our value of 0.04 at 4500 h ecmpares 
AVOID Wali) Ive Ss Walwe O12 O.O9) tO Creer ale, 

12> Spectra, ZO=-22 are Yoecakiless”, Myler Closemyecd wine 
Same effect in his work. 

L3o Comijosiee ZO) eincl 25, Very lattle cGiikexenes soem 


between Gray Card and Too of Water in structural detail. 
\ t 


29-6 


I see no evidence of chlorophyll. Perhaps, if upwelling 
irradiance were subtracted from the reflected light from the 
SUNSESS Oi Clas Werecics ielaS O/aO A absorption would e seen. 

Hab WS SieeKewheslil ComneSinte sa telme UpalelSie \wielie@ie Glee 
compare almost identically (compare 19, 23, and 24). 

5° irradiance has!) very slaght Ta aCien in these 
Under Water data. The peak value changes from 36 to 52 u 
wakes fon” [BO cMOSe SjxeCcEras 2 Would Exyoecr a Ciseeiesic 
variation since the cloud cover changed over the time period 
from 1:15 to 1:45. Perhaps, we were inadvertently "shadowing" 
the water thus negating cloud cover changes. 

16. The Under Water spectra have a definite "peak" 

AE Bilaowlic Sloe A (Comoaire 19, 23 ame 24). 

7. Tt doubt 1f the irradiance values measured are 
truly upwelling. Tyler obtained a value of about 3 x 10° u watts/ 
ane uu for zero depth upwelling irradiance at Crater Lake while 

2 ° 
we obtained about 45 pw watts/fem won 19, 23 and 24 at 5000 A. 
Either the ocean upwelling irradiance is lower by a factor of 
50 or we were inaeed, shadowing the irradiance (see Statement 
WS) c 

IUB— UMMSeS ALS) = COAG ELLS Sieioice) EYOSOoeLOM Cyclone 
in the Under Water data that sets in near. 5500 A and attenuates 


°o 


the irradiance from 6900-7000 A. 


Zo) 


I certainly hope you find these spectra as interesting 
Ag Wwe GHGs Gl teladils Elias sor Suen 2 Saori joeievocl alia Winslclo 
to prepare and acquire the data, we should be happy to obtain 


Ela S|. THMEOIMNEN ESL Ie SHE Wain g 


29-8 


FIGURE 1 


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17 August 1968 


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17 August 1968 
BLOCK ENGINEERING, 


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Woods Hole, 


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17 August 1968 
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17 August 1968 


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Peter G. White 
TRW Systems 
One Space Park 
Redondo Beach, California 
The bulk of my activity deals with remote sensors--most for 
space vehicles, some for air and ground. My interest lies in 
ocean color, with studies beginning four years ago--studies of 
sensing problems, design and instrumentation specifically for ocean 


color measurements. Currently I am determining requirements of 


instrumentation for ocean color mapping systems. 


30-1 


ij , 


t Vastly bus ph ay tat te a 


a 


Charles S. Yentsch 

Physical Oceanographic Laboratory 
Nova University 

Fort Lauderdale, Florida 

Studies in our laboratory concern photochemical events that 
occur in Natural Ocean waters. The principal reaction is photosynthesis; 
however, we are becoming aware of other reactions that are driven by 
light energy. In the course of these studies we have developed 
photographic techniques which may be of interest to this group. 

To be brief, we have been able to convert three color densitometry 
values taken from common color film into monochromatic data (see papers 
by Baig and Yentsch and De Marsh in this volume). The technique depends 
upon establishment of a mean monochromatic curve for the images to be 
studied. In our case the image is the spectral absorption curve 
typical for marine phytoplankton. The dominance of chlorophyll «a 
absorption in these spectra allows the establishment of a mean curve 
where the deviation from the mean, at certain wavelengths is quite 
small. 

We have also examined the amount of light and its spectral 
characteristics, backscattered from the Bahamana Banks. These data 
show that the influence of bottom reflection is of prime importance 
to a depth of about 25 meters. Below this depth, total volume 


scattering from the water column is the important factor. 


31-1 


, Reprinted from APPLIED OPTICS, Vol. 8, page 2566, December 1969 
Copyright 1969 by the Optical Society of America and reprinted by permission of the copyright owner 


A Photographic Means of Obtaining 
Monochromatic Spectra of Marine Algae 


S. R. Baig and C. S. Yentsch 


Oceanographic Center, Nova University, Fort Lauderdale, 
Florida 33316. 
Received 16 July 1969. 


There are many cases in which it is time-consuming or difficult 
to measure routinely the visible absorption spectra of a large 
number of samples. Multivariate analysis of color photographs 
of the samples provides a simple method by which it is possible 
to reconstruct the spectra once the material of interest has been 
spectrophotometrically calibrated. It is then only necessary to 
take a photograph and measure the density of the three dye 
layers in the film with a three-color densitometer. From these 
data the absorption spectrum can be generated. 

The original application of characteristic vector analysis to 
photographic problems was made by Simonds. He was able 
to reconstruct any one of over 100 Hurter-Driffield curves 
(density vs log exposure) using the mean curve of the samples and 
four vectors and their corresponding scalar multipliers. The 
mathematical technique is outlined and an example calculated 
in his paper. 


2566 APPLIED OPTICS / Vol. 8, No. 12 / December 1969 


31-2 


Table |. Mean and Vectors. Linear Regression Formulas for 
Calculating Scalar Multiples from Log Exposure Values 


A(nm) Mean ee Visa V5" 
400 5S. 1 66.34 —3.185 — 14.08 
410 60.5 66.93 —8.025 —7.92 
420 61.8 68.33 —12.78 —4.10 
430 63.0 69.75 —18.17 —0.77 
440 61.9 aealets —21.25 0.26 
450 56.8 69.76 —18.11 1.398 
460 Pai) 68.02 —17.36 3.952 
470 50.7 68.07 — 14.10 9.262 
480 48.8 67.66 —12.65 6.771 
490 47.5 65.99 —10.67 6.281 
500 42.6 63.20 —4.889 3. 8d2 
510 op. Ll 57.97 Neo 2) 0.4849 
520 27.4 46.12 >. 981 —().2175 
530 22.8 39.438 he: 0.1375 
d40 20.0 28.41 8.484 2.656 
550 Noe 24.51 8.779 4.421 
560 16.8 24.33 9.102 4.546 
570 17.4 28.48 9.015 3.498 
d5S0 18.1 34.39 6.785 Teatit2 
590 18.6 38.09 7.008 1.439 
600 19.1 40.49 6.892 le 
610 20.6 43.98 7.009 1.682 
620 Pe) 47.18 6.745 2.156 
G30 ee) 47.61 6.512 2.300 
640 eri 49 85 8.219 ».226 
650 24.7 57.61 11.90 10.50 
660 29.5 60.73 11.59 14.33 
670 oto 68. 7$ 8.026 16.44 
680 36.3 68.15 6.065 13.37 
690 24.2 49.14 8.607 6 547 
700 1S PBS ars teas 0.2942 


“V, = 0.799 log exposure R + 0.133 log exposure G@ + 0.832 
log exposure B — 0.679. 

* Vo = 3.010 log exposure 2 + 1.887 log exposure GF — 3.192 
log exposure B + 0.596. 

“V3 = 3.625 log exposure 2 — 0.550 log exposure G — 2.683 
log exposure B + 0.650. 


We have successfully applied the technique to the reconstruc- 
tion of visible absorption spectra of a group of nine cultured 
marine algae. We filtered 50 ml of each culture onto a plain 
white gla---fiber filter, 25 mm in diameter. The absorption 
spectrum of each filtered sample was measured in a Beckman 
DK-1A_ specirophotometer according to Yentsch’s method.? 
Within 10 min a photograph was taken of each of the filtered 
algae. The film was Ivastman 5242, Ektachrome EF, type B; 
iHumination was by electronic flash with an 85B filter used over 
the 35-mm camera lens. A gray seale and a blank glass-fiber 
filter were also photographed for calibration and reference. The 
Welch Densichron was used to measure the tri-color densities. 
It was calibrated against a step wedge of known densities. The 
error in Measurement was 2:0.0f optical density. 

From the gray scale the ) log &£ curves are constructed for 
each of the three layers of the film. These provide a check on 
processing operations and film sensitivity (ASA speed). The 
18%, gray patch imaged with each filter is used to correct for 
inevitable variations in exposure. The first 18¢¢ gray patch is 
used as a standard for each roll of film. Any variations in the 
tri-color densities of subsequent patches are converted to log 


exposures. The same log exposure correction is made for the 
filterimage. In this way all filters are reduced to the equivalent 
exposire. 


The actual absorption spectra were subjected to characteristic 
vector analysis using an IBM 1130 computer. The operation 
in outline was as follows: 

(1) Write the r optical densities of the m algal spectra in 
rows, one spectrum per row. The r columns are then the optical 
densities at LO-nm increments. 

(2) Find the mean optical density of each column. 

(3) Subtract the mean optical density from all of the optical 
densities in the corresponding column. This array is called the 
n-row by r-colttumn mean corrected data matrix. ! 

(4) Prepare the transpose of the matrix generated in step 3. 
This new matrix has 7 rows and n columns. Each element 
a,,, of the step 8 matrix becomes the element a,,,, of the transpose. 

(5) Premultiply matrix 3 by matrix 4 (its transpose) to 
yield anv by 7 matrix. 

(6) Caleulate m eigen-vectors and -values of matrix 5. 
Weighing coefficients w,, are calculated by dividing each element 
of each vector by the corresponding root 10 yield an 1 X 7 matrix. 
Sealar multiples y,,,, ave caleulated by summing the products of 
Wy X (mean o.d.),,,. The scalar multipliers indicate how much 
of each vector is needed to add to the mean to reconstitute any 
particular absorption spectrum. Table I shows the average 
values and the three eigenvectors for a group of algae. 

The three-layer color film ean be thought of as a three-channel 
synchronous recording device. To see if three vectors are enough 
to account for all the variation among samples it was only nec- 
essary {0 see what percent of the trace of the determinant of the 
above matrix was accounted for by each root. The first root 
accounted for 92.286, the first two for 96.91°%. No substantial 
improvement was observed by increasing the number beyond 
three, which gave a total of 98.11% for the trace. 

The red, green, and blue (Wratten 92, 92, 94 filters) densities 
were converted to log exposure of each picture and these were 
regressed in {turn upon each of the three corresponding scalar 
multiples to give a least-square fit. Examples of reconstituted 
spectra and their fit with the original spectra are shown in (Fig. 
1. The scalar multiples for these fits are calculated from film 
densities. 


Good fits of the actual spectra were found for most algae be- 
cause of the dominance of chlorophyll a in determining the mean. 
It is noted that Jess perfect agreement is obtained in the region 
in which the accessory pigments, carotenoids, and chromopro- 
teins, absorb. The over-all fit of reconstructed spectra can be 


A 
\ 
/ » 589 VAN 605 
/ 
{ : c 
\ N 
5 f\ A 
\ Hi \ \ { \ 
o3 / \ \ 
: ) | / 
a O02 SG \ Sear 
irq 7 ¥ 
2 o1 Ke ~ ———————— e——_— — —— —SE 
a — 
= OGN/ZON 590 592 
2 Y/ \ 
3 = 
ost \ 
\ 
o4 \ 
\ 
o3 \ 
\ 
02 \ 
Aa 
400 500 600 700 400 500 600 70c 
WAVE LENGTH - (nm) 
Fig. 1. Absorption spectra of four marine algae. 589 is Nanno- 


chloris atomus; 590 is Aphanizamenon holsgatiewm; 592 is Por- 

phoridium sp.; and 605 is Phaeodactylum tricornutum. The solid 

line = measured spectra, and the dotted line = reconstituted 
spectra. 


December 1969 / Vol. 8, No. 12 / APPLIED OPTICS 2567 


31-3 


improved by deemphasizing the role of the accessory pigments. 
This can be done by increasing the step width to 20-50-nm in- 
crements in the region wherein they absorb. (Preliminary 
results with a much larger algal set indicate that only two vectors 
account for most of the variation. The 400-580-nm region was 
sampled in 20-nm steps. The 600-700-nm region was sampled 
in 5-nm steps. ) 

The usefulness of the method lies in its ability to produce 
visible absorption spectra of a large number of samples which 
must be examined simultaneously. The number of samples that 
can be examined simultaneously is only a function of film dimen- 
sion and image size, the inter- and intralayer diffusion of the dyes 
in the film providing a lower bound to image size. Camera and 
lens combinations establish an upper bound to film dimension. 

Subjects in which a visible change occurs with time are es- 
pecially amenable to this treatment. Instead of correlating 
film densities of photographs of a number of different subjects, 
one would be dealing with varying concentrations of the same 
subject. Once spectrophotometrically calibrated it would not be 
necessary, for example, to remove the subject from a transparent 


2568 APPLIED OPTICS / Vol. 8, No. 12 / December 1969 


aes 


enclosure. The film furthermore provides an accurate record of 
any visible change. An important advantage gained by the 
method is that the photograph can be taken in a fraction of the 
time needed for a spectrophotometric scan. Times of the order 
of 0.01 sec are usual. This permits surveillance of fast changing 
stationary subjects. If the scale of reproduction desired in the 
photograph is too large to permit a single photograph to be made, 
smaller areas may be photographed in a fraction of the time it 
would take to scan them spectrophotometrically. The photo- 
graphic technique has obvious advantages and is important in 
aerial surveillance, since it is possible to preserve a degree of 
micro-variation over wider areas. 

We thank LeRoy DeMarsh of Eastman Kodak Research 
Laboratories for his continuing assistance with this work. 

This work was supported by the National Science Foundation 
(#GB-7088) and the Atomic Energy Commission [#AT-(401)-3845]. 


References 


1. J. L. Simonds, J. Opt. Soc. Amer. 53, 968 (1963). 
2. C.S. Yentsch, Limnol. Oceanogr. 7, 207 (1962). 


Color Fiim as an Abridged Spectral Radiometer 

Spectral measurements are usec in many research’ problems. 
Can collor film be used to make these measurements? The answer 
is yes for some problems. In many instances the problem is 
not one of identifying one particular speetral curve from an 
infinaty of possible ones. More often one is working with a 
fairly well-defined population of possible spectral curves. ‘Two 
examples of such populations are the spectral absorbances of 
algae samples and the spectral distribution variations of natural 
Gaylight. 

A-collor film measures the amount of zed; sreen, and bime 
iignit 2c sees reflected from an object. These measurements; 
the red, green, and blue layer exposures of the film, then control 
the amount of cyan, magenta, and yellow dye that are formed in 
the layers. If we measure the spectral density curve of a film 
image and compare this curve with that of the original object, 
we usually find a poor correlation. Such a comparison is show 
in Fisure 1. The absorbance curve of an algae sample is show 


asea douved Wine wthe taln image as acsolva Tine. nis is 


iow 


obviously not the way to use a color filmi for’ spectral measuring 
device, although it has been tried. A color film does not need 
to produce a spectral matcn to the objects it records. Color 
films do attempt to produce an image whicn looks like the 
original object. 

HeGis walk a Glosieie Toole 2h “wlasksy ial lin’ ahmelers 5 Atos at al Mon 
image is produced by combining three dyes. This image of an 
aleae sample consisted of the dye amounts showm in Figure e. 

Ali the images produced by this film are produced with various 
amounts of these three dyes. When I want to measure the spectral 
density curve of a color-film image, I do not need to use a 
spectrophotometer. I know that the film image contains only 
three dyes. 1 can calculate, the amounts of) the ayes) in anvimage 
from three measurements--the red, green, and blue densities of 
the film sample. These analytical densitometry techniques are 
familiar to most photographic engineers. From the dye amounts 
and the spectral density curves of the individual dyes, I can 
compute the spectral density curve of the film sample. Thus I 
can construct the entire sneatral density curve from three measurements 


31-6 


This same idea can be applied to other spcctral meesuring 
problems. The question is, "Can the population of spectral curves 
being studied be analyzed as though it were being produced with 
combinations of three or fewer components?" To be more specific, 
"Can the pepMLersen of spectral data be matched with linear 
combinations of three basis curves?" Characteristic vector 
analysis can be used to answer this question. 


Simonds? 


has described the application of characteristic 
vector analysis to optical response data and illustrates in detail 
a procedure for callcullating echaracteristie vectors. Kor this 
analysis we first compute the average curve for the population 

and subtract this average curve from each of the samples in the 
population. An iterative procedure is then used to compute a 

set of basis curves or vectors. These vectors describe the var- 
iations of the population: about the average. A small number of 


characteristic vectors can often describe a complex set of data. 


In the procedure described by Simonds, one computes the vectors 


31-7 


in order of decreasing significance. ‘hat is, the first vector 
describes the largest part of the variation, and subsequent 
vectors describe smaller parts of the variability. 

Tre nques|TLOn" TOrNOuR Spe Curalemcasumimne | problemas, 
"Can the first three vectors describe our ponuletion of data with 
sufficient accuracy?" The average curve and the first three 
characteristic vectors for a population of algae curves® are 
shown in Figure 3. The values of these curves are shown plotted 
versus wavelength. These vectors can be thought of as the "dyes" 
which combine to make up the varicus algae spectral curves. 
These vectors fit the algae curves with a standard error of |) 203. 
Each of the spectral absorbance curves in the population can be 
matched by combining the average curve and some amount of each 


of the three vectors. 


ey Aint Lah Vigt Mo) Vey 3 V3% 


A 
A = the spectral absorbance curve (1) 
Y¥,,Yo,Y2 = the amounts of the vectors 


haracteristic vectors 


Q 


aU T — } 
Vip Voy Vay the 
The reconstruction of one of the algae curves is shoym in Figure 4. 


31-8 


Judd, MacAdam, and Wyszecki? have shown that the 
variations which occur in natural daylight (sunlight + skylight) 
Can be fitted with two characteristic vectors. The average 
eurve and the first two characteristic vectors for their data 


are shown in Figure 5. The spectral energy distributions of 622 


samples of daylight can be matched by linear combinaticns of these 


ue 


curves. 

Characteristic vector analysis reduces the dimensionality 
Of a set of data to a mingmum.  Kach of the daylight spectral 
distributions can be represented by a point in a two-dimensional 
Spacen  Hachwou mchelalacel absorbance weurves) Canube  Pepresenved 
by a point in a three-dimensional space. This is illustrated in 
Figure 6. The coordinates of this three-dimensional space are 
the vector amounts Y) -Yo-Y3. Three points are shoym plotted in 
Figure 6. The locations of each of these points is determined 
by how much of each of the vectors are required to match that 
sample. 

The spectral sensitivities of a color film define another 


three-dimensional soace. The coordinates of this three-space 


} 


(Figure 7) ere the red, green, and blue layer exposures of the 


Ss) 


film. Each of the algae samples when photographed will result 

in some red, green, and blue exposure and hence can be represented 
by a point in this space hid WS Chel raltqyel el wieelals ronal ici. Cin 
between these two three-dimensional spaces, then we can compute 


the vector scalars ¥1,Yo,Y3 MeO TNS scsi EGHYoOSswUeSsS Ih G5 18} 


( Yo | Sei oC j (2) 
ae 
One potential problem here is a situation where two samples have 
different spectral curves and hence plot at different points in 
the vector space, but give the same film exposures. Ine Swela 
metamers exist, there can be no transformation between the two 
coordinate systems. Assuming that a transformation can be 
found, we can compute the vector scalars from the film exposures 
and then construct the spectral curve from the vector amounts-- 
Y¥1,Yo,¥3 and’ the vectors V1;,Vo,V3 plus the average curve Av (Eq. 1). 
How can we calibrate a film to apply this aparece 
Hirst.) at) asinecessaryoto, Obtain ispeciticall ienicves (Oma) muUmMbe TNO 
Samples which represent the population to be studied. The number 
of samples required would depend on tne nature of tne population. 


31-10 


hree characteristic vectors and the amounts of the vectors 
required to matcl: cach sample are calculated from these data. 

The film exposures can be determined in one of two ways. If 

all the physical data are available, we can compute the film 
SxpPOSURes Gunecciiilive, I backine thei physical idaten svc ican photograph 
the calibreting samples’ and derive tne film exposures .by paoto- 
graphic photometry as shown in Figure 8. The transformation 
between the two coordinate systems can then be estimated by 
multiple regression analysis. 

The transformation between color film exposure and the 


algae vector space is shown in Equations 3. 


Ma = 0.7324*R + 0.2901*G + 0O.7944*B - 0.6980 
Yigg = SaMOhOMR ce LoVAMONG = S05) (nt) On (sisi) () 
Wa © -5.5420*R + 6.8750*G + 6.3600*B - 0.6450 


The algae curve showm in Figure 1 and a curve computed from film 
exposures is shown in Figure 9. The original curve is shown as 
a solid line, the reconstruction from film data as +. 

The transformation between film exposures and daylight 


vector space is shown in Equations 4. 


WaT =O 59 2023 — 25 (so0OuG ar) sjolOs, (Oss 


16.100*R - 19.360%*G + 6.6440*B 


Yo 
Sel 


TMhiemueeCOns Piewlets Oma Oman Carmine |CIMeICe Va CUE iIcOT sess O SMES 
is shown in Figure 10. 

These two examples illustrate a method whereby a color 
film can be calibrated and uses as an abridged spectral measuring 
device. It must be emphasized that this procedure must be used 
With Cau Nene Hach worobmern must De wanaly zed. and speci le icalmbicalie some 
derived for that problem. The four main requirements which must 
bel met Hor the application of this procedure are listed below: 

WG | Hvaver joxoyoibllencaiieya, Ont spectral curves must be specifiable. 

Only curves drawn from this population can be measured. 

Zs SUMRAISS Ceisieeoewoicahs icalo WoC comos ibis Cascio wale 

POpDUMa tony Om CURVES Wich Sumi CHent a aeceumalcive. 

3. The population of curves contains no metamers, in 

terms of the film spectral sensitivities. 

4, A transformation between the vector space and the 

film exposure space can be found. 
If more than three vectors are required to describe the population, 
@ color film cannot be used. A panchromatic black-and-white film 
exposed througn several narrow band filters could be used for 


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