PIOLOGY LIBRARY : m. A TEXT BOOK OP PHYSIOLOGY BIOLOGY LIBRARY G PRINTED BY C. J. CLAY, M.A. & SON, AT THE UNIVERSITY PRESS. PREFACE TO THE FOURTH EDITION. IN previous Editions of this work I endeavoured, by the use of small and large print, to distinguish between the more important and stable portions of Physiology, which ought to be made known to every one engaged in a serious study of the science, and the less settled, often controverted views which should be attacked by the more advanced students only. Experience however has taught me that the advantages of such a plan are more than counterbalanced by its disadvantages. I especially felt that the amount of space which I could fairly allow to the small print paragraphs was wholly insufficient to permit me to do justice to the conflicting views which I strove, in them, to expound. In this Edition accordingly I have made no attempt at any such distinction, and have used small print almost exclusively for the description of methods and apparatus. This step involving, as it necessarily did, the transference, into the body of the work, of some of the statements which previously had found their place in the small print 606165 vi PREFACE. portions, has given the volume, at first sight, the appear- ance of having been largely altered. This however is not the case. For good or for bad, the book remains very much as it was ; and though I have done my best to remove some of the many defects present in previous editions, I have been encouraged, by the favour with which those editions have been successively received, to persevere in the views which I have always held as to which are the parts of physiology most to be insisted on, and which may be lightly touched or wholly omitted ; and though I would still most strenuously repudiate the idea, put forward by some, that there is such a thing as a physiology for medical men, different from that physiology which is a part of science, I have tried to make this volume especially useful to medical students. My decision to do away with the small print portions of former editions has been largely determined by the fact that my former pupils, now my colleagues at Cam- bridge, have undertaken to join with me in treating these higher or advanced parts of physiology in a more extended and satisfactory form. And the hope that' the result of their labours will soon appear has led me, in this volume, to omit all references, and to use as little as possible the personal authority of the names of investi- gators. The fondness of students for the use of names of persons is as marked as the pertinacity with which they use them wrongly; and if any observer may feel aggrieved at his name being absent from an ordinary text- book, he may at least have the satisfaction of reflecting that the omission of all names does something to prevent others receiving the credit of his labours. PREFACE. vii I cannot say how much I am indebted to the con- tinued help of those friends who assisted me in former editions ; and I have also to acknowledge with gratitude the aid afforded me by Prof. C. S. Boy, to whose kindness I owe several of the new illustrations. The appendix on chemical matters, as in former editions, has been under the care of Mr Sheridan Lea; in this, which stands on a somewhat different footing from the rest of the work, references and names of authors have been retained. TRINITY COLLEGE, CAMBRIDGE, February, 1883. CONTENTS. PAGE INTEODUCTOEY 1 BOOK I. BLOOD. THE TISSUES OF MOVEMENT. THE VASCULAR MECHANISM. CHAPTER I. BLOOD, pp. 11—34. Sec. 1. The Coagulation of Blood . . . . -. . . . 13 Sec. 2. The Chemical Composition of Blood . . . * . . . 24 Sec. 3. The History of the Corpuscles . .V . ~ „ . . . 28 Sec. 4. The Quantity of Blood, and its distribution in the body ... 33 CHAPTER II. THE CONTRACTILE TISSUES, pp. 35 — 103. Sec. 1. The Phenomena of Muscle and Nerve 37 Muscular and Nervous Irritability, p. 37. The Phenomena of a simple muscular contraction, p. 39. Tetanic contractions, p. 48. Sec. 2. The Changes in a Muscle during Muscular Contraction ... 54 The change in form, p. 54. Electrical changes, p. 58. Chemical changes, p. 64. Thermal changes, p. 70. The changes in a Nerve during the passage of a Nervous Impulse, p. 72. Sec. 3. The Nature of the Changes through which an Electric Current is able to generate a Nervous Impulse 75 The action of the Constant Current, p. 75. Electrotonus, p. 77. Electrotonic Currents, p. 80. x CONTENTS. PAGE Sec. 4. The Muscle-Nerve Preparation as a Machine . . . . 83 The nature and mode of application of the Stimulus as affecting the amount and character of the Contraction, p. 83. The influence of the Load, p. 87. The influence of the Size and Form of the Muscle, p. 88. The work done, p. 89. Sec. 5. The Circumstances which determine the Degree of Irritability of Muscles and Nerves 90 The effects of severance from the Central Nervous System, p. 91. The Influence of Temperature, p. 93. The Influence of Blood Supply, p. 94. The Influence of Functional Activity, p. 95. Sec. 6. The energy of Muscle and Nerve, and the nature of Muscular and Nervous Action 98 Sec. 7. Other forms of Contractile Tissue 101 Unstriated Muscular Tissue, p. 101. Cardiac Muscles, p. 102. Cilia, p. 102. Migrating Cells, p. 103. CHAPTER III. THE FUNDAMENTAL PROPEETIES OF NERVOUS TISSUES, pp. 104 — 114. Automatic actions, p. 107. Eeflex actions, p. 109. Actions of sporadic ganglia, p. 112. Inhibition, p. 113. CHAPTER IV. THE VASCULAR MECHANISM, pp. 115 — 230. I. THE PHYSICAL PHENOMENA OF THE CIRCULATION .... 116 Sec. 1. Main general facts of the Circulation 117 The Capillary Circulation, p. 117. The flow in the Arteries, p. 120. The flow in the Veins, p. 127. Hydraulic principles of the Circu- lation, p. 128. Sec. 2. The Heart 135 The Phenomena of the Normal Beat, p. 135. The Mechanism of the Valves, p. 142. The Sounds of the Heart, p. 143. On the relative duration and special characters of the cardiac events, p. 146. The work done, p. 157. Variations in the Heart's Beat, p. 159. Sec. 3. The Pulse 161 n. THE VITAL PHENOMENA OF THE CIRCULATION .... 176 Sec. 4. Changes in the Beat of the Heart 178 The Mechanism of the normal beat, p. 180. Inhibition of the beat, p. 184. The effects on the circulation of changes in the heart's beat, p. 194. CONTENTS. xi PAGE Sec. 5. Changes in the calibre of the minute arteries. Vaso-motor actions . 197 Vaso-motor Nerves, p. 139. Vase-motor Centres, p. 212. The effects of local vascular constriction or dilation, p. 216. Sec. 6. Changes in tJie Capillary Districts 219 Sec. 7. Changes in the Quantity of Blood 224 Sec. 8. The Mutual Relations and the Co-ordination of the Vascular Factors 227 BOOK II. THE TISSUES OF CHEMICAL ACTION WITH THEIR RESPECTIVE MECHANISMS. NUTRITION. CHAPTER I. THE TISSUES AND MECHANISMS OF DIGESTION, pp. 233 — 311. Sec. 1. The Properties of the Digestive Juices 234 Saliva, p. 234. Gastric juice, p. 239. Bile, p. 247. Pancreatic juice, p. 250. Succus entericns, p. 255. Sec. 2. The act of secretion in the case of the Digestive Juices and the Nervous Mechanisms which regulate it 256 Sec. 3. The Muscular MecJianisms of Digestion 281 Mastication, p. 281. Deglutition, p. 282. Movements of the O3sophagus, p. 284. Movements of the stomach, p. 285. Move- ments of the small intestine, p. 286. Movements of the large intestine, p. 288. Defaecation, p. 288. Vomiting, p. 290. Sec. 4, The Changes which the Food undergoes in the Alimentary Canal . 292 Sec. 5. Absorption of tJie Products of Digestion 301 The Lymphatics, p. 301. Entrance of the chyle into the lacteals, p. 303. Movements of the chyle, p. 304. Lymph-hearts, p. 306. The course taken by the several products of digestion, p. 306. CHAPTER II. THE TISSUES AND MECHANISMS OP RESPIRATION, pp. 312 — 383. Sec. 1. The Mechanics of Pulmonary Respiration 314 The Rhythm of Respiration, p. 316. The Respiratory Move- ments, p. 319. Facial and Laryngeal Respiration, p. 324. Sec. 2. Clianges of the Air in Respiration 326 Sec. 3. The Respiratory Changes in the Blood 329 The relations of oxygen in the blood, p. 332. Hemoglobin ; its properties and derivatives, p. 333. Colour of venous and arterial blood, p. 338. The relations of the carbonic acid in the blood, p. 342. The relations of the nitrogen in the blood, p. 343. Sec. 4. The Respiratory Changes in the Lungs 344 The entrance of oxygen, p. 344. The exit of carbonic acid, p. 346. xii CONTENTS. PAGE Sec. 5. The Respiratory Changes in the Tissues . . . . . . 348 Sec. 6. The Nervous Mechanism of Respiration 358 Sec. 7. The Effects of Respiration on the Circulation 304 Sec. 8. The Effects of Changes in the Air breathed 375 The effects of deficient air. Anphyxia. Phenomena of asphyxia, p. 375. The circulation in asphyxia, p. 378. The effects of an increased supply of air. Apnoea, p. 380. The effects of changes in the composition of the air breathed, p. 380. The effects of changes in the pressure of the air breathed, p. 381. Sec. 9. Modified Respiratory Movements 382 Sighing, Yawning, Hiccough, Sobbing, Coughing, Sneezing, Laughter and Crying, p. 382. CHAPTER III. SECRETION BY THE SKIN, pp. 384 — 391. The nature and amount of Perspiration, p. 385. Cutaneous Eespiration, p. 386. The Secretion of Perspiration, p. 387. The Nervous Mechanism of Perspiration, p. 388. Absorption by the Skin, p. 390. CHAPTER IY. SECRETION BY THE KIDNEYS, pp. 392 — 414. Sec. 1. The Composition of Urine 393 Sec. 2. The Secretion of Urine 397 The relation of the secretion of urine to arterial pressure, p. 398. Secretion by the renal epithelium, p. 404. Sec. 3. Micturition 410 CHAPTER Y. THE METABOLIC PHENOMENA OF THE BODY, pp. 415 — 478. Sec. 1. Metabolic Tissues 416 The History of Glycogen, p. 416. Diabetes, p. 424. The History of Pat. Adipose Tissue, p. 426. The Mammary Gland, p. 429. The Spleen, p. 432. Sec. 2. The History of Urea and its allies 436 Sec. 3. The Statistics of Nutrition 443 Comparison of Income and Output, p. 446. Nitrogenous Meta- bolism, p. 449. The effects of Fatty and of Carbohydrate Food, p. 453. Sec. 4. The Energy of the Body 457 The income of energy, p. 457. The expenditure, p. 458. Tho (sources of Muscular Energy, p. 459. The sources and distribution of Heat, p. 461. Eegulation by variations in loss, p. 464. Regu- lation by variations in production, p. 465. Sec. 5. The Influence of the Nervous System on Nutrition . . . - 470 Sec. 6. Dietetics . 474 CONTENTS. xiii BOOK III. THE CENTRAL NERVOUS SYSTEM AND ITS INSTRUMENTS. CHAPTER I. SENSORY NERVES, pp. 481 — 489. CHAPTER II. SIGHT, pp. 490 — 555. PAGE Sec. 1. Dioptric Mechanisms 491 The Formation of the Image, p. 491. Accommodation, p. 493. Movements of the Pupil, p. 500. Imperfections in the Dioptric apparatus, p. 506. Sec. 2. Visual Sensations , 511 The origin of Visual Impulses, p. 511. Simple Sensations, p. 519. Colour Sensations, p. 524. Sec. 3. Visual Perceptions 535 Modified Perceptions, p. 536. Sec. 4. Binocular Vision 541 Corresponding or identical points, p. 541. Movements of the eye- balls, p. 542. The Horopter, p. 547. Sec. 5. Visual Judgments . 549 Sec. 6. The Protective Mechanisms of the Eye 554 CHAPTER III. HEARING, SMELL, AND TASTE, pp. 556—571. Sec. 1. Hearing 556 The acoustic apparatus, p. 557. Auditory Sensations, p. 559. Auditory Judgments, p. 565. Sec. 2. Smell .567 Sec. 3. Taste 570 xiv CONTENTS. " CHAPTER IV. FEELING AND TOUCH, pp. 572 — 584. PAGE Sec. 1. General Sensibility and Tactile Perceptions . . . . . 572 Sec. 2. Tactile Sensations 575 Sensations of Pressure, p. 575. Sensations of Temperature, p. 576. Sec. 3. Tactile Perceptions and Judgments 579 Sec. 4. The Muscular Sense 582 CHAPTER Y. THE SPINAL CORD, pp. 585—607. Sec. 1. As a Centre or Group of Centres of Reflex Action .... 585 Inhibition of Reflex Action, p. 590. The Time required for Reflex Actions, p. 5L3. Sec. 2. As a Centre or Group of Centres of Automatic Action . . . 595 Sec. 3. As a Conductor of Afferent or Efferent Impulses .... 598 CHAPTER VI. THE BRAIN, pp. 608—650. Sec. 1. On the Phenomena exhibited by an animal deprived of its Cerebral Hemispheres 608 Sec. 2. The Mechanisms of Co-ordinated Movements 614 Forced Movements, p. 620. Sec. 3. The Functions of the Cerebral Convolutions 623 Sec. 4. The Functions of other parts of the Brain 636 Corpora striata and optic thalami, p. 636. Corpora quadrigernina, p. 638. Cerebellum, p. 640. Crura cerebri and pons Varolii, p. 641. Medulla oblongata, p. 642. Sec. 5. The Rapidity of Cerebral Operations . . . . . . 643 Sec. 6. The Circulation in the Brain 645 Sec. 7. The Cranial Nerves 648 CHAPTER VII. SPECIAL MUSCULAR MECHANISMS, pp. 651 — 664. Sec. 1. The Voice 651 Sec. 2. Speech 657 Vowels, p. 657. Consonants, p. 658. Sec. 3. Locomotor Mechanisms 662 CONTENTS. xv BOOK IV. THE TISSUES AND MECHANISMS OF REPRODUCTION. CHAPTER I. MENSTRUATION, pp. 669 — 671. CHAPTER II. IMPREGNATION, pp. 672 — 673. CHAPTER III. THE NUTRITION OF THE EMBRYO, pp. 674 — 680. CHAPTER IV. PARTURITION, pp. 681 — 683. CHAPTER V. THE PHASES OF LIFE, pp. 684—694. CHAPTER VI. DEATH, pp. 695—696. APPENDIX. ON THE CHEMICAL BASIS OP THE ANIMAL BODY, pp. 697 — 770. INDEX, pp. 771—785. INTRODUCTORY. AMONG the simpler organisms known to Biologists, perhaps the most simple as well as the most common is that which has received the name of Amoeba. There are many varieties of Amoeba, and probably many of the forms which have been described are, in reality, merely amoebiform phases in the lives of certain animals or plants ; but they all possess the same general characters. Closely resembling the white corpuscles of vertebrate blood, they .are wholly or almost wholly composed of undifferentiated protoplasm, in the. midst of which lies a nucleus, though this is sometimes absent. In many a distinction may be observed between a more solid external layer or ectosarc, and a more fluid granular interior or endosarc; but in others even this primary differentiation is wanting. By means of a continually occurring flux of its protoplasmic substance, the amoeba is enabled from moment to moment not only to change its form but also to shift its position. By flowing round the sub- stances which it meets, it, in a way, swallows them ; and having digested and absorbed such parts as are suitable for food, ejects or rather flows away from the useless remnants. It thus lives, moves, eats, grows, and after a time dies, having been during its whole life hardly anything more than a minute lump of protoplasm. Hence to the Physiologist it is of the greatest interest, since in its life the problems of physiology are reduced to their simplest forms. Now the study of an amoeba, with the help of knowledge gained by the examination of more complex bodies, enables us to state that the undifferentiated protoplasm of which its body is so largely composed exhibits certain fundamental phenomena which we may speak of as ' vital.' F. 1 OF PROTOPLASM. 1. It is contractile. There can be little doubt that the changes in the protoplasm of an amoeba which bring about its peculiar ' amoeboid ' movements, are identical in their fundamental nature with those which occurring in a muscle cause a contraction : a muscular contraction is essentially a regular, an amoeboid move- ment an irregular flow of protoplasm. The substance of the amoeba may therefore be said to be contractile. 2. It is irritable and automatic. When any disturbance, such as contact with a foreign body, is brought to bear on the amoeba at rest, movements result. These are not passive move- ments, the effects of the push or pull of the disturbing body, proportionate to the force employed to cause them, but active manifestations of the contractility of the protoplasm ; that is to say, the disturbing cause, or ' stimulus/ sets free a certain amount of energy previously latent in the protoplasm, and the energy set free takes on the form of movement. Any living matter which, when acted on by a stimulus, thus suffers an explosion of energy, is said to be ' irritable.' The irritability may, as in the amoeba, lead to movement ; but in some cases no movement follows the application of the stimulus to irritable matter, the energy set free by the explosion taking on some other form than movement, ex. gr. heat. Thus a substance may be irritable and yet not contractile, though contractility is a very common manifestation of irritability. The amoeba (except in its prolonged quiescent stage) is rarely at rest. It is almost continually in motion. The movements cannot always be referred to changes in surrounding circumstances acting as stimuli ; in many cases the energy is set free in conse- quence of internal changes, and the movements which result are called spontaneous or automatic movements. We may therefore speak of the protoplasm of the amoeba as being irritable and automatic. 3. It is receptive and assimilative. Certain substances serving as food are received into the body of the amoeba, and there in large measure dissolved. The dissolved portions are subse- quently converted from dead food into new living protoplasm, and become part and parcel of the substance of the amoeba. 4. It is metabolic and secretory. Pari passu with the re- ception of new material, there is going on an ejection of old material, for the increase of the amoeba by the addition of food is not indefinite. In other words, the protoplasm is continually undergoing chemical change (metabolism), room being made for the new protoplasm by the breaking up of the old protoplasm into products which are cast out of the body and got rid of. These products of metabolic action have, in many cases at all events, subsidiary uses. Some of them, for instance, we have reason to think, are of value for the purpose of dissolving and effecting other INTRODUCTORY. 3 prelimiDary changes in the raw food introduced into the body of the amoeba ; and hence are retained within the body for some little time. Such products are generally spoken of as ' secretions.' Others which pass more rapidly away are generally called 'ex- cretions.' The distinction between the two is an unimportant and frequently accidental one. The energy expended in the movements of the amoeba is supplied by the chemical changes going on in the protoplasm, by the breaking up of bodies possessing much latent energy into bodies possessing less. Thus the metabolic changes which the food (as distinguished from the undigested stuff mechanically lodged for a while in the body) undergoes in passing through the protoplasm of the amoeba are of three classes : those preparatory to and culminating in the conversion of the food into protoplasm, those concerned in the discharge of energy, and those tending to economise the immediate products of the second class of changes by rendering them more or less useful in carrying out the first. 5. It is respiratory. Taken as a whole, the metabolic changes are pre-eminently processes of oxidation. One article of food, i.e. one substance taken into the body, viz. oxygen, stands apart from all the rest, and one product of metabolism peculiarly associated with oxidation, viz. carbonic acid, stands also somewhat apart from all the rest. Hence the assumption of oxygen and the excretion of carbonic acid, together with such of the metabolic processes as are more especially oxidative, are frequently spoken of together as constituting the respiratory processes. 6. It is reproductive. The individual amoeba represents a unit. This unit, after a longer or shorter life, having increased in size by the addition of new protoplasm in excess of that which it is continually using up, may, by fission t(or by other means) resolve itself into two (or more) parts, each of " which is capable of living as a fresh unit or individual. Such are the fundamental vital qualities of the protoplasm of an amoeba; all the facts of the life of an amoeba are manifesta- tions of these protoplasmic qualities in varied seouence and sub- ordination. The higher animals, we learn from morphological studies, may be regarded as groups of amoebae peculiarly associated together. All the physiological phenomena of the higher animals are simi- larly the results of these fundamental qualities of protoplasm peculiarly associated together. The dominant principle of this association is the physiological division of labour corresponding to the morphological differentiation of structure. Were a larger or ' higher' animal to consist simply of a colony of undifferentiated amoebae, one animal differing from another merely in the number of units making up the mass of its body, without any differences between the individual units, progress of function would be an 1—2 4 THE FUNDAMENTAL TISSUES. impossibility. The accumulation of units would be a hindrance to welfare rather than a help. Hence, in the evolution of living beings through past times, it has come about that in the higher animals (and plants) certain groups of the constituent amcebiform units or cells have, in company with a change in structure, been set apart for the manifestation of certain only of the fundamental properties of protoplasm, to the exclusion or at least to the complete subordination of the other properties. These groups of cells, thus distinguished from each other at once by the differentiation of structure and by the more or less marked exclusiveness of function, receive the name of 'tissues.' Thus the units of one class are characterized by the exaltation of the contractility of their protoplasm, their automatism, metabolism and reproduction being kept in marked abeyance. These units constitute the so-called muscular tissue. Of another tissue, viz. the nervous, the marked features are irritability and automatism, with an almost complete absence of contractility and a great restriction of the other qualities. In a third group of units, the activity of the protoplasm is largely confined to the chemical changes of secretion, contractility and automatism (as manifested by movement) being either absent or existing to a very slight degree. Such a secreting tissue, consisting of epithelium-cells, forms the basis of the mucous membrane of the alimentary canal. In the kidney, the substances secreted by the cells, being of no further use, are at once ejected from the body. Hence the renal tissue may be spoken of as excretory. In the epithelium-cells of the lungs, the protoplasm plays an altogether subordinate part in the assumption of oxygen and the excretion of carbonic acid. Still we may perhaps be permitted to speak of the pulmonary epithelium as a respiratory tissue. In addition to these distinctly secretory or excretory tissues, there exist groups of cells specially reserved for the carrying on of chemical changes, the products of which are neither cast out of the body, nor collected in cavities for digestive or other uses. The work of these cells seems to be of an intermediate character ; they are engaged either in elaborating the material of food that it may be the more easily assimilated, or in preparing used-up material for final excretion. They receive their materials from the blood and return their products back to the blood. They may be called the metabolic tissues par excellence. Such are the fat-cells of adipose tissue, the hepatic cells (as far as the work of the liver other than the secretion of bile is concerned), and probably many other cellular elements in various regions of the body. Each of the various units retains to a greater or less degree the power of reproducing itself, and the tissues generally are capable of regeneration in kind. But neither units nor tissues can reproduce other parts of the organism than themselves, much less the entire organism. For the reproduction of the complex INTRODUCTORY. 5 individual, certain units are set apart in the form of ovary and testis. In these all the properties of protoplasm are distinctly subordinated to the work of growth. Lastly, there are certain groups of units, certain tissues,. which are of use to the body of which they form a part, not by reason of their manifesting any of the fundamental qualities of protoplasm, but on account of the physical and mechanical properties of certain substances which their protoplasm has been able by virtue of its metabolism to manufacture and to deposit. Such tissues are bone, cartilage, connective tissue in large part, and the greater portion of the skin. We may therefore consider the complex body of a higher animal as a compound of so many tissues, each tissue correspond- ing to one of the fundamental qualities of protoplasm, to the development of which it is specially devoted by the division of labour. It must however be remembered that there is probably a distinct limit to the division of labour. In each and every tissue, in addition to its leading quality, there are more or less pronounced remnants or at least some traces of all the other protoplasmic qualities. Thus, though we may call one tissue par excellence metabolic, all the tissues are to a greater or less extent metabolic. The energy of each, whatever be its particular mode, has its source in the breaking-up of the protoplasm. Chemical changes, including the assumption of oxygen and the production complete or partial of carbonic acid, and therefore also entailing a certain amount of secretion and excretion, must take place in each and every tissue. And so with all the other fundamental properties of protoplasm ; even contractility, which for obvious mechanical reasons is soonest reduced where not wanted, is present in many other tissues besides muscle. And it need hardly be said that each tissue retains the power of assimilation. However thoroughly the material of food be prepared by digestion and subsequent metabolic action, the last stages of its conversion into living protoplasm are effected directly and alone by the tissue of which it is about to form a part. Bearing this qualification in mind, we may draw up a physio- logical classification of the body into the following fundamental tissues : — 1. The eminently contractile : the muscles. 2. „ „ irritable and automatic : the nervous system. 3. „ „ secretory, or excretory : digestive, urinary, and pulmonary, &c., epithelium. 4. „ „ metabolic : fat-cells, hepatic cells, lymphatic and ductless glands, &c. 5. „ „ reproductive : ovary, testis. 6. The indifferent or mechanical : cartilage, bone, &c. All these separate tissues, with their individual characters, are 6 INTEGRATION. however but parts of one body ; and in order that they may be true members working harmoniously for the good of the whole, and not isolated masses, each serving its own ends only, they need to be bound together by coordinating bonds. Some means of communication must necessarily exist between them. In the mobile homogeneous body of the amoeba, no special means of com- munication are required. Simple diffusion is sufficient to make the material gained by one part common to the whole mass, and the native protoplasm is physiologically continuous, so that an explosion set up at any one point may be immediately propagated throughout the whole irritable substance. In the higher animals, the several tissues are separated by distances far too great for the slow process of diffusion to serve as a sufficient means of commu- nication, and their primary physiological continuity is broken by their being imbedded in masses of formed material, the product of the indifferent tissues, which being devoid of irritability, present an effectual barrier to the propagation of molecular explosions. It thus becomes necessary that in the increasing complexity of animal forms, the process of differentiation should be accompanied by a corresponding integration, that the isolated tissues should be made a whole by bonds uniting them together. These bonds moreover must be of two kinds. In the first place there must be a ready and rapid distribution and interchange of material. The contractile tissues must be abundantly supplied with material best adapted by previous elabo- ration for direct assimilation, and the waste products arising from their activity must be at once carried away to the metabolic or excretory tissues. And so with all the other tissues. There must be a free and speedy intercourse of material between each and all. This is at once and most easily effected by the regular circulation of a common fluid, the blood, into which all the elaborated food is discharged, from which each tissue seeks what it needs, and to which each returns that for which it has no longer any use. The carrying on such a circulation of fluid, being in large measure a mechanical matter, needs a machinery, and calls forth an expendi- ture of energy. The machinery is supplied by a special con- struction of the primary tissues, and the energy is arranged for by the presence among these of contractile and irritable matter. Thus to the fundamental tissues there is added, in the higher animals, a vascular bond in the shape of a mechanism of circulation. In the second place, no less important than the interchange of material is the interchange of energy. In the amoeba the irritable surface is physiologically continuous with the more internal proto- plasm, while each and every part of the body has automatic powers. In the higher animal, portions only of the skin remain as eminently irritable or sensitive structures, while automatic actions are chiefly confined to a central mass of irritable nervous INTRODUCTORY. 7 matter. Both forms of irritable matter are separated, by long tracts of indifferent material, from those contractile tissues through which they chiefly manifest the changes going on in themselves. Hence the necessity for long strands of eminently irritable tissue to connect the skin and contractile tissues as well with each other as with the automatic centres. Similar strands are also needed, though perhaps less urgently, to connect the other tissues with these and with each other. To the vascular bond there must be added an irritable bond, along the strands of which, impulses set up by changes in one or another part, may travel in determinate courses for the regulation of the energy of distant spots. In other words, part of the irritable tissues must be specially arranged to form a coordinating nervous system. Still further complications have yet to be considered. In the life of a minute homogeneous amoeba, possessing no special form or structure, there is little scope for purely mechanical operations. As however we trace out the gradual development of the more complex animal forms, we see coming forward into greater and greater prominence the arrangement of the tissues in definite ways to secure mechanical ends. Thus the entire body acquires particular shapes, and parts of the body are built up into mechan- isms, the actions of which are to the advantage of the individual. Into the composition of these mechanisms or ' organs ' the active fundamental tissues, as well as the passive or indifferent tissues, enter ; and the working of each mechanism, the function of each organ, is dependent partly on the mechanical conditions offered by the passive elements, partly on the activity of the active elements. The vascular mechanism, of which we have just spoken, is such a mechanism. Similarly the urgent necessity for the access of oxygen to all parts of the body, has given rise to a complicated respiratory mechanism ; and the needs of copious alimentation, to an alimentary or digestive mechanism. Further, inasmuch as muscular movement is one of the chief ends, or the most important means to the chief ends, of animal life, we find the animal body abounding in motor mechanisms, in which the prime mover is muscular contraction, while the machinery is supplied by complicated arrangements of muscles with such indifferent tissues as bone, cartilage, and tendon. In fact, the greater part of the animal body is a collection of mus- cular machines, some serving for locomotion, others for special manoeuvres of particular members and parts, others as an assist- ance to the senses, and yet others for the production of voice, and in man, of speech. Lastly, the simple automatism of the amoeba, with its simple responses to external stimuli, is replaced in the higher animals by an exceedingly complex volition affected in multitudinous ways by influences from the world without ; and there is a correspond- ingly complex central nervous system. And here we meet with .: 8 CENTRAL NERVOUS MECHANISM. a new form of differentiation unknown elsewhere. While the contractility of the amoeba! protoplasm differs but slightly from the contractility of the vertebrate striated muscle, there is an enormous difference between the simple irritability of the amoeba and the complex action of the vertebrate nervous system. Except- ing the nervous or irritable tissues, the fundamental tissues have in ail animals the same properties, being, it is true, more acute and perfect in one than in another, but remaining fundamentally the same. The elementary muscular fibre of a mammal is a mass of differentiated protoplasm, forming a whole physiologically continuous, and in no way constituting a mechanism. Each fibre is a counterpart of all others ; and the muscle of one animal differs from that of another in such particulars only as are wholly subordinate. In the nervous tissues of the higher animals, on the contrary, we find properties unknown to those of the lower ones ; and in proportion as we ascend the scale, we observe an increasing differentiation of the nervous system into unlike parts. Thus we have, what does not exist in any other tissue, a mechanism of nervous tissue itself, a central nervous mechanism of complex structure and complex function, the complexity of which is due not primarily to any mechanical arrangements of its parts, but to the further differentiation of that fundamental quality of irrita- bility and automatism which belongs to all irritable tissues, and to all native protoplasm. In the following pages I propose to consider the facts of phy- siology very much according to the views which have been just sketched out. The fundamental properties of most of the ele- mentary tissues will first be reviewed, and then the various special mechanisms. It will be found convenient to introduce early the account of the vascular mechanism, and of its nervous coordinating mechanism, while the mechanisms of respiration and alimentation will be best considered in connection with the respiratory and secretory tissues. The description of the purely motor mechanisms will be brief; and, save in a few instances, confined to a statement of general principles. The special functions of the central nervous system, including the senses, must of necessity be considered by themselves. The tissues and mechanism of reproduction and the phenomena of the decay and death of the organism will naturally form the subject of the closing chapters. BOOK I. BLOOD. THE TISSUES OF MOVEMENT. THE VASCULAR MECHANISM. CHAPTEE I. BLOOD. BLOOD, when flowing in a normal condition through the blood- vessels, consists of an almost colourless fluid, the plasma, in which are suspended a number of more solid bodies, the red and white o ' corpuscles. Were we anxious to give a formal completeness to the classification of the various parts of the body into tissues, we might £0 speak of the blood as a tissue of which the corpuscles are the essential cellular elements, while the plasma is a liquid matrix. We might compare it to a cartilage, the firm matrix of which had become completely liquefied so that the cartilage-corpuscles were perfectly free to move about. In regarding blood as tissue, however, we come upon the difficulty that it, unlike all the other tissues, possesses no one characteristic property. The protoplasm of the white corpuscles is native un differentiated protoplasm, in no respect fitted for any special duty ; and though, as we shall see, the red corpuscles have a definite respiratory function, inasmuch as they are carriers of oxygen from the lungs to the several tissues, still this respiratory work is only one of the very many labours of the blood. It will be therefore far more profitable, indeed necessary, to treat of the blood, not as a tissue by itself, but_as the great means of com- munication of material between the tissues properly so called. Its real usefulness lies not so much in any one property of either its corpuscles or its plasma, as in its nature fitting it to serve as the great medium of exchange between all parts of the body. The receptive tissues pour into it the material which they have received from without, the excreting tissues withdraw from it the things which are no longer of any use, and the irritable, the contractile, and indeed all the tissues, seek in it the substances (including 12 BLOOD AN INTERNAL MEDIUM. [BOOK i. oxygen) which they need for the manifestation of energy or for the storing up of differentiated material, and return to it the waste products resulting from their activity. All over the body every- where there is so long as life lasts a double current, here rapid, there slow, of material from the blood to the tissues, and from the tissues to the blood. It, together with lymph (whether in the lymph-canals or in the interstices of the tissues), may, as Bernard has suggested, be regarded as an internal medium bearing the same relations to the constituent tissues that the external medium, the world, does to the whole individual. Just as the whole organism lives on the things around it, its air and its food, so the several tissues live on the complex fluid by which they are all bathed and which is to them their immediate air and food. From this it follows, on the one hand, that the composition and characters of the blood must be for ever varying in different parts of the body and at different times ; and on the other hand, that the united action of all the tissues must tend to establish and maintain an average uniform composition of the whole mass of blood. The special changes which blood is known to undergo while it passes through the several tissues will best be dealt with when the individual tissues and organs come under our considera- tion. At present it will be sufficient to study the main features, which are presented by blood, brought so to speak into a state of equilibrium by the common action of all the tissues. Of all these main features of blood, the most striking if not the most important is the property it possesses of clotting or coagulating when shed. SECT. 1. THE COAGULATION OF BLOOD. Blood, when shed from the blood-vessels of a living body, is perfectly fluid. In a short time it becomes viscid; it flows less readily from vessel to vessel. The viscidity increases rapidly until the whole mass of blood under observation becomes a complete jelly. The vessel into which it has been shed, can at this stage be inverted without a drop of the blood being spilt. The jelly is of : the same bulk as the previously fluid blood, and if forcibly removed, -— presents a complete mould of the interior of the vessel. If the blood in this jelly stage be left untouched in a glass vessel, a few drops of an almost colourless fluid soon make their appearance on the surface of the jelly. Increasing in number, and running together, the drops after a while form a superficial layer of pale straw-coloured fluid. Later on, similar layers of the same fluid are seen at the sides and finally at the bottom of the jelly, which, ^ shrunk to a smaller size and of firmer consistency, now forms a clot or crassamentum, floating in a perfectly fluid serum. The shrinking and condensation of the clot, and the corresponding increase of the serum, continue for some time. The upper surface of the clot is generally cupped. A portion of the clot examined under the microscope is seen to consist of a feltwork of fine granular fibrils, in the meshes of which are entangled the red and white corpuscles of the blood. In the serum nothing can be seen but a few stray corpuscles. The fibrils are composed of a substance called fibrin. Hence we may speak of the clot as consisting of fibrin and corpuscles ; and the act of clotting or coagulation is obviously a conversion of the naturally fluid portion of the blood or plasma into fibrin and serum, followed by separation of the fibrin and corpuscles from the serum. 14 COAGULATION OF BLOOD. [BOOK i. In man, blood when shed becomes viscid in about two or three minutes, and enters the jelly stage in about five or ten minutes. After the lapse of another few minutes the first drops Jof serum are seen, and coagulation is generally complete in from one to several hours. The times however will be found to vary according to the condition of the individual, the temperature of the air, and the size and form of the vessel into which the blood is shed. Among animals the rapidity of coagulation varies ex- ceedingly in different species. The blood of the horse coagulates with remarkable slowness ; so slowly indeed that many of the red corpuscles (these being specifically heavier than the plasma) have time to sink before viscidity sets in. In consequence there ap- pears on the surface of the blood an upper layer of colourless plasma, containing in its deeper portions many colourless cor- puscles (which are lighter than the red). This layer clots like the other parts of the blood, forming the so-called 'buffy coat.' A similar buffy coat is sometimes seen in the blood of man, in inflammatory conditions of the body. This buffy coat makes its appearance in horse's blood even at the ordinary temperature of the air. If a portion of horse's blood be surrounded by a cooling mixture of ice and salt, and thus kept at about 0° C., coagulation may be almost indefinitely postponed. Under these circumstances a more complete descent of the cor- puscles takes place, and a considerable quantity of colourless transparent plasma free from blood-corpuscles may be obtained. portion of this plasma removed from the freezing mixture clots exactly as does the entire blood. It first becomes viscid and then forms a jelly, which subsequently separates into a colourless shrunken clot and serum. This shews that the corpuscles are not an essential part of the clot. If a few cubic centimetres of the same plasma be diluted with 50 times its bulk of a 0'6 p.c. solution of sodium chloride1 coagu- lation is much retarded, and the various stages may be more easily watched. As the fluid is becoming viscid, fine fibrils of fibrin will be seen to be developed in it, especially at the sides of the containing vessel. As these fibrils multiply in number, the fluid becomes more and more of the consistence of a jelly ., and at the same time somewhat opaque. Stirred or pulled about with a needle, the fibrils shrink up into a small opaque stringy mass ; and a very considerable bulk of the jelly may by agitation be resolved into a minute fragment of shrunken fibrin floating in a quantity of what is really diluted serum. If a specimen of such diluted plasma be stirred from time to time, as soon as coagulation begins, with a needle or glass rod, the fibrin may be removed piecemeal as it forms, and the jelly stage may be altogether done away with. When fresh blood which has not yet had time to 1 A solution of sodium chloride of this strength will hereafter be spoken of as ' normal saline solution.' CHAP. 1.1 BLOOD. 15 coagulate is stirred or whipped with a bundle of rods (or anything presenting a large amount of rough surface), no jelly-like coagu- lation takes place, but the rods become covered with a mass of shrunken fibrin. Blood thus whipped until fibrin ceases to bef deposited, is found to have entirely lost its power of coagulation. Putting all these facts together, it is very clear that the phenomena of the coagulation of blood are caused by the appear- ance in the plasma of fine fibrils of fibrin. As long as these are scanty, the blood is simply viscid. When they become sufficiently numerous, they give the blood the firmness of a jelly. Soon after their formation they begin to shrink ; and in their shrinking en- close in their meshes the corpuscles, but squeeze out the fluid parts of the blood. Hence the appearance of the shrunken coloured clot and the colourless serum. Fibrin, whether obtained by whipping freshly-shed blood, or by washing either a normal clot, or a clot obtained from colourless plasma, exhibits the same general characters. It belongs to that class of complex unstable nitrogenous bodies called proteids which form a large portion of all living bodies and an essential part of all protoplasm1. It gives the ordinary proteid reactions. It is insoluble in water and in dilute saline solutions; and though it swells up in dilute hydrochloric acid, it is not thereby appreciably dissolved2. Coagulation then is brought about by the appearance in the; blood-plasma of a substance, fibrin, which previously did not exist • there as such. Such a substance must have antecedents, or anj antecedent — what are they, or what is it ? If blood be received direct from the blood-vessels into one- third its bulk of a saturated solution of some neutral salt such as magnesium sulphate, and the two gently but thoroughly mixed, coagulation, especially at a moderately low temperature, will be deferred for a very long time. If the mixture be allowed to stand, the corpuscles will sink, and a colourless plasma will be obtained similar to the plasma gained from horse's blood by cold, except that it contains an excess of the neutral salt. The presence of the neutral salt has acted in the same direction as cold : it has prevented the occurrence of coagulation. It has not destroyed the fibrin; for if some of the plasma be diluted with from five to ten times its bulk of water, it will coagulate speedily in quite a normal fashion, with the production of quite normal fibrin. If some of the colourless transparent plasma, obtained either by the action of neutral salts from any blood, or by the help of cold from horse's blood, be treated with some solid neutral salt, such as sodium chloride, to saturation, a white flaky somewhat sticky precipitate will make its appearance. If this precipitate be re- moved, the fluid is no longer coagulable. (or very slightly so), even though the neutral salt present be removed by dialysis, or 1 See Appendix. 2 For further details see Appendix. . 16 COAGULATION OF BLOOD. [BOOK i. Uts influence lessened by dilution. With the removal of the (substance precipitated, the plasma has lost its power of coagu- lating. If the precipitate itself, after being washed with a saturated solution of the neutral salt (in which it is insoluble) so as to get rid of all serum and other constituents of the plasma, be treated with a small quantity of water, it readily dissolves1, and the solution rapidly filtered gives a clear colourless filtrate, which is at first rfectly fluid. Soon however the fluidity gives way to viscidity, and this in turn to a jelly condition, and finally the jelly shrinks into a clot floating in a clear fluid; in other words, the filtrate clots like plasma. Thus there is present in cooled plasma, and in plasma kept from clotting by the presence of neutral salts, a something, precipitable by saturation with neutral salts, a some- thing which, since it is soluble in very dilute saline solutions, cannot be fibrin itself, but which in solution speedily gives rise to the appearance of fibrin. To this substance its discoverer, Denis, gave the name of plasmine. We are justified in saying that the coagulation of blood is the result of the conversion of plasmine I or some part of plasmine into fibrin. But there are reasons for thinking that plasmine is a mixture of at least two bodies. If sodium chloride be carefully added to plasma to an extent of about 13 per cent, a white flaky viscid precipitate is thrown down very much like plasmine. If after the removal of the first precipitate more sodium chloride, and especially if magnesium sulphate, be added a second precipitate is thrown down, less viscid and more granular than the first. The name fibrinogen is given to the former, paraglobulin to the latter. Both are proteids belonging to the globulin family2, the members of which while insoluble in distilled water are readily soluble in dilute solutions of neutral salts. According to some authors solutions of fibrinogen are characterized by their being precipitated, and coagulated 3 at a temperature of about 55° — 60° while solutions of paraglobulin are not so changed till the tempe- rature rises to 68° — 70°. There are also other differences (see Appendix). Both these substances are thrown down when plasma is saturated with sodium chloride so that the plasmine of Denis appears to be a mixture of fibrinogen and paraglobulin, and the question arises, Are both these concerned in the formation of fibrin ? Paraglobulin Jhoi only occurs as a constituent of plasma, but is found in considerable quantity in the serum left after clotting ; it forms as we shall see a large portion of the proteids present in 1 The substance itself is not soluble in distilled water, but a quantity of the neutral salts always clings to the precipitate, and thus the addition of water virtually gives rise to a dilute saline solution, in which the substance is readily soluble. 2 See Appendix. 3 See Appendix for the distinction between the coagulation of proteids by heat, and the coagulation due to the appearance of fibrin. CHAP, i.] BLOOD. 17 serum. Now the addition of serum will often bring about coagu- lation in fluids which, left to themselves, will not coagulate, the clot so formed being composed of fibrin with normal characters, and the artificial coagulation thus induced being in all other respects exactly like a natural clotting. Thus for instance bydrocele fluid, carefully removed without admixture of blood from a hydrocele, will in most cases remain fluid without any disposition to clot1. So also the serous fluid removed from the pericardial, pleural, or peritoneal cavities some hours after death in most cases shews no disposition to clot2. But these fluids, hydrocele or pericardial, though they do not clot spontaneously, will generally, upon the addition of serum or a little whipped blood, clot in a most unmis- takeable manner3. Now fibrinogen is certainly present in these fluids, and may be thrown down from them by the addition of sodium chloride or by other means ; and, since serum contains paraglobulin, it was at first thought that the absence of spontaneous coagulation in the untouched hydrocele or pericardial fluid was due to the absence of paraglobulin, which as we have seen is present with fibrinogen in the spontaneously coagulable plasma of blood, and that the coagulating effect of the addition of the serum was due to the paraglobulin it contained, the paraglobulin and fibrinogen acting in some way or other upon each other to produce fibrin. And this view was supported by the fact that paraglobulin precipitated from serum was, like the entire serum, efficacious in giving rise to a coagulation in fibrinogenous pericardial, or hydrocele fluids. It was soon found however that certain specimens of pericardial and even hydrocele fluid did not need the addition of the para- globulin to make them coagulate; that though they would not coagulate spontaneously they might be made to coagulate by adding to them a constituent of serum which was not paraglobulin but something else. Thus if serum, or indeed whipped blood, be mixed with a large quantity of alcohol and allowed to stand some days, the proteids present are in time so changed by. the alcohol as to become insoluble in water. Hence if the copious precipitate, after long standing, be separated by filtration from the alcohol^ dried at a low temperature not exceeding 40°, and extracted with' distilled water, the aqueous extract contains very little proteid matter, indeed very little organic matter at all. Nevertheless even a small quantity of this aqueous extract added alone to certain specimens of hydrocele fluid will bring about a speedy coagulation. The same aqueous extract has also a remarkable effect in hastening the coagulation of fluids which though they will eventually clot, do so very slowly. Thus plasma may, by the careful addition of a 1 In some specimens, however, a spontaneous coagulation, generally slight, but in exceptional cases massive, may be observed. 2 If it be removed immediately after death it generally clots readily and firmly, giving a colourless clot consisting of fibrin and white corpuscles only. 3 In a few cases no coagulation can thus be induced. F. 2 /T 18 FIBRIN-FERMENT. [BOOK i. certain quantity of neutral salt and water, be reduced to such a condition that it coagulates very slowly indeed, taking perhaps days to complete the process. The addition of a small quantity of the aqueous extract we are describing will however bring about a coagulation which is at once rapid and complete. The active substance, whatever it be, in this aqueous extract J exists in small quantity only, and its coagulating virtues are at ' Npnce and for ever lost when the solution is boiled. Further, there .'is no reason to think that the active substance actually enters $ into the formation of the fibrin to which it gives rise ; it seems, \ $J ^ tnout undergoing changes in itself, to act in some way or other N ^/ on the actual fibrin factors (fibrinogen and paraglobulin or one of /vjy\f them) and to convert them or part of them into fibrin. It appears to belong to a class of bodies playing an important part in physiological processes and called ferments, of which we shall have more to say hereafter. We may therefore speak of it as the fibrin- ferment, the name given to it by its discoverer Alex. Schmidt. Fibrin-ferment appears to make its appearance in blood soon after it has been shed, and like other ferments is apt to be entangled in and carried down by any precipitates which occur in blood. It is carried down by the plasmine, and hence solutions of plasmine coagulate spontaneously. It exists in serum, and is carried down with paraglobulin when that substance is precipitated. And hence arises the serious question whether the coagulating effects of serum or prepared paraglobulin on hydrocele or pericardial fluid are not, after all, due to the ferment present rather than to the paraglobulin. So that two views may be taken of the nature of coagulation. One1 teaches that fibrin arises from some mutual action of fibrinogen and para- globulin induced by the fibrin ferment ; the other2 that fibrin is formed through the conversion of fibrinogen alone by the agency of the ferment, paraglobulin either having nothing to do with the matter, or merely assisting by its presence in some indirect way. There can be no doubt that fibrinogen is an essential factor, that coagulation cannot take place without it and that it or some part of it actually becomes fibrin. There is equally no doubt that the presence of the fibrin-ferment is absolutely necessary. It is also more than probable that fibrin does not result from the union of fibrinogen arid paraglobulin, since the quantity of fibrin formed is not greater than that of either of these two substances used to produce it. But we still need further light as to the exact nature of the change produced by the ferment, the true characters of the ferment itself, and the part played by paraglobulin. In favour of the view that paraglobulin is not concerned in the matter, it is asserted, that fibrinogen cautiously precipitated from plasma by small quantities of sodium chloride so as to obtain 1 That of Alexander Schmidt, and his pupils and others. " That of Hammarsten, Fredericq and others. CHAP, i.] BLOOD. 19 it apart from paraglobulin, and then freed from ferment by repeated washing, will yield a solution not spontaneously coagulable, but clotting freely on the addition of ferment only. In favour of the view that the presence of paraglobulin is essential may be quoted the striking fact that certain specimens of hydrocele fluid may be met with which will not coagulate either spontaneously or upon the addition of ferment alone, but will coagulate upon the addition of paraglobulin and ferment. Such fluids may be supposed to contain fibrinogen only. And it has been argued that two substances have been confused under the name of fibrinogen : one coagulating at the same temperature as paraglobulin, and needing the cooperation of paraglobulin to form fibrin ; and another body, which may be thrown down from solutions of plasm ine or from blood at the temperature of 55°— 60° (the fluids thereby losing the power of coagulating), and which is fibrinogen already on its way to become fibrin, in fact a sort of nascent fibrin, capable of becoming actual fibrin in the total absence of paraglobulin. Lastly tbell presence_of a neutral salt, such as sodium chloride, appears to be essential to the process, coagulation not occurring even where all , three factors are present, if no neutral salt accompanies them. Awaiting further investigation we may for the present conclude that fibrin is formed by the conversion, through the agency of a ferment, of a substance fibrinogen, which forms part° of the plasm ine spoken of above, but the exact nature of that conversion and whether paraglobulin has any share in the matter, and if so what, must remain as yet undecided. This conception of coagulation as a chemical process between certain factors renders easy of comprehension the influence of various conditions on the coagulation of blood. The quickening influence of heat, the retarding effect of cold, the favourable action of motion and of contact with surfaces, and hence the results of whipping and the influence exerted by the form and surface of vessels, become intelligible. The greater the number of points, that is the larger and rougher the surface presented by the vessel into which blood is shed, the more quickly coagulation comes on, for contact with surfaces favours chemical union. So also the presence of spongy platinum, or of an inert powder like charcoal, quickens the coagulation of tardily clotting fluids, such as many specimens of pericardia! fluid. Having thus arrived at an approximative knowledge of the nature of coagulation, we are in a better position for discussing the question, Why does blood remain fluid in the vessels of the living body and yet clot when shed ? The older views may be at once summarily dismissed. The clotting is not due to loss of temperature, for cold retards coagu- lation, and the blood of cold-blooded animals behaves just like that of warm-blooded animals in clotting when shed. It is not due to loss of motion, for motion favours coagulation. It is not due to 2—2 20 INFLUENCE OF THE LIVING BLOOD-VESSELS. [BOOK i. exposure to air, whereby either an increased access of oxygen or an escape of volatile matters is facilitated, for on the one hand the blood is fully exposed to the air in the lungs, and on the other shed blood clots when received, without any exposure to the atmosphere, in a closed tube over mercury. All the facts known to us point to the conclusion, that when blood is contained in healthy living blood-vessels, a certain relation or equilibrium exists between the blood and the containing vessels of such a nature that as long as this equilibrium is maintained the blood remains fluid, but that when this equilibrium is disturbed by events in the blood or in the blood-vessels or by the removal of the blood, the blood undergoes changes which result in coagulation. The most salient facts in support of this conclusion are as follows. 1. After death, when all motion of the blood has ceased, the blood remains for a long time fluid. It is not till some time , afterwards, at an epoch when post-mortem changes in the blood and in the blood-vessels have had time to develope themselves, that coagulation begins. Thus some hours after death the blood in the great veins may be found perfectly fluid. Yet such blood has not lost its power of coagulating ; it still clots when removed from the body, and clots too when received over mercury without r^ i exposure to air, shewing that the fluidity of the highly venous blood is not due to any excess of carbonic acid or absence of oxygen. Eventually it does clot even within the vessels, but perhaps never so firmly and completely as when shed. It clots first in the larger vessels, but remains fluid in the smaller veins, for a very long time, for many hours in fact, since in these the same bulk of blood is exposed to the influence of, and reciprocally exerts an influence on, a larger surface of the vascular walls than in the larger veins. 2. If the vessels of the heart of a turtle (or any other cold- W blooded animal) be ligatured, and the heart be cut out and AT \ vJI$iace(^ in favourable circumstances so that it may continue to beat P> V^V as ^on£ a Per*°d as possible, the blood will remain fluid within •* *$^ ^he heart as long as the pulsations go on, i. e. for one or two days (and indeed for some time afterwards), though a portion taken away at any period of the experiment will clot very speedily. 3. If the jugular vein of a large animal, such as an ox or horse, be ligatured when full of blood, and the ligatured portion excised, the blood in many cases remains perfectly fluid, along the greater part of the length of the piece, for twenty-four or even forty-eight hours. The piece so ligatured may be suspended in a framework and opened at the top so as to imitate a living test-tube, and yet the blood will often remain long fluid, though a portion removed at any time into another vessel will clot in a few minutes. If two such living test-tubes be prepared, the blood may be poured from one to the other without coagulation taking place. The above facts illustrate the absence of coagulation in intact CHAP, i.] BLOOD. 21 or slightly altered living blood-vessels; the following shew that coagulation may take place even in the living vessels. 4. If a needle or piece of wire or thread be introduced into f VA> 'w the living blood-vessel of an animal, either during life or imme-; , !,"7', diately after death, the piece will be found encrusted with fibrin. 5. If in a living animal a blood-vessel be ligatured, the ligature being of such a kind as to injure the inner coat, coagu- lation takes place at the ligature and extends for some distance from it. Thus if the jugular vein of a rabbit be ligatured roughly in two places, clots will in a few hours be found in the ligatured portion, reaching upwards and downwards from the ligatures, the middle portion being the least coagulated. Clots will also be found on the far side of each ligature. The clots will still appear if the ligature be removed immediately after being applied, provided that in the process the inner coat has been wounded. If the ligatures be applied in such a way as not to injure the inner coat, coagulation will not take place, though the blood may remain for many hours perfectly at rest between the ligatures. So also when an artery is ligatured a conspicuous clot is formed on the cardiac side of the ligature. The clot is largest and firmest in the immediate neighbourhood of the ligature, gradually thinning away from thence and reaching usually as far as where a branch J" is given off. Between this branch and the ligature there is stasis ; the walls of the artery suffer from the want of renewal of blood, and thus favour the propagation of the coagulation. On the distal side of the ligature where the artery is much shrunken, the clot which is formed, though naturally small and inconspicuous, is similar. 6. Any injury of the inner coat of a blood-vessel causes a coagulation at the spot of injury. Any treatment of a blood-vessel tending to injure its normal condition causes local coagulation. 7. Disease involving the inner coat of a blood-vessel causes a coagulation at the part diseased. Thus inflammation of the lining membrane of the valves of the heart in endocarditis is frequently accompanied by the deposit of fibrin. In aneurism the inner coat is diseased, and layers of fibrin are commonly deposited. So also in fatty and calcareous degeneration without any aneurismal dilation there is a tendency to the formation of clots. Similar phenomena are seen in the case of serous fluids which coagulate spontaneously. If, as soon after death as the body is cold and the fat is solidified, the pericardium be carefully removed from a sheep by an incision round the base of the heart, the pericardial fluid may be kept in the pericardial bag as in a living cup for many hours without clotting, and yet a small portion removed with a pipette clots at once, and a thread left hanging into the fluid soon becomes covered with fibrin. The only interpretation which embraces these facts is that1 so long as a certain normal relation between the lining surfaces ofjj 22 SOURCES OF THE FIBRIN FACTORS. [BOOK i. the blood-vessels and the blood is maintained, coagulation does not take place ; but when this relation is disturbed by the more or less gradual death of blood-vessels, or by their more sudden disease or injury, or by the presence of a foreign body, coagulation sets in. Two additional points may here be noticed. 1. Stagnation of blood favours coagulation within the blood-vessels, apparently because the blood-vessels, like other tissues, demand a renewal of the blood on which they depend for the maintenance of their vital powers. 2. The influence of surface is seen even in the coagulation within the vessels. In cases of coagulation from gradual death of the blood-vessels, as in the case of an excised jugular vein, the fibrin, when its deposition is sufficiently slow, is seen to appear first at the sides, and from thence gradually, frequently in layers, to make its way to the centre. So in aneurism, the deposit of fibrin is frequently laminated. In cases where coagulation results from disease of the lining membrane, the rougher the interior, the more speedy and complete the clotting. So also a rough foreign body, presenting a large number of surfaces and points of attachment, more readily produces a clot when intro- duced into the living blood-vessels than a perfectly smooth one. We may perhaps go a step further, for there are certain weighty reasons for believing that in normal circulating blood all the fibrin- factors are not present in the plasma, and that a disturbance of the equilibrium between the blooid and the blood-vessels gives rise to coagulation by inducing changes in certain corpuscles, either the ordinary white corpuscles or corpuscles of a special kind, whereby one or more of the fibrin-factors are discharged into the plasma. 1. When blood is received direct from the blood-vessels into alcohol, the aqueous extract of the precipitate contains little or no fibrin-ferment. If the blood be allowed to stand a little while before being thrown into alcohol some ferment makes its appearance ; and the longer, up to clotting, that the blood stands before being treated with alcohol, the more efficacious is the aqueous extract of the precipitate. Fibrin-ferment therefore seems to make its appearance in blood after being shed. 2. When blood, kept from clotting by exposure to cold or through being retained by ligatures in a living blood-vessel, is allowed to stand till the corpuscles have sunk, the upper layers of the plasma, free from both red and white corpuscles, exhibit when removed very little power of coagulation and, upon examination, are found to contain a very small quantity only of fibrin-ferment. 3. We have reasons for thinking that when blood is shed, certain number of corpuscles, which we may speak of as w -f j^hite corpuscles, leaving it for the present uncertain whether J. substances, or acted upon by various galvanic currents^ contrac- tions are seen in the muscles to which branches of the nerve are distributed. ne > sti 38 MUSCULAR CONTRACTION. [BOOK i. The nerve like the muscle is irritable, it is thrown into a state of activity by a stimulus ; but unlike the muscle it does not itself contract. The changes set up in the nerve by the stimulus are not visible changes of form; but that changes of some kind or other are set up and propagated along the nerve down to the muscle is shewn by the fact that the muscle contracts when a part of the nerve at some distance from itself is stimulated. Both nerve 'and muscle are irritable, but only the muscle is contractile, i. e. manifests its irritability by a contraction. The nerve manifests its irritability by transmitting along itself, without any visible alteration :of form, certain molecular changes set up by the stimulus. We shall icall these changes thus propagated along a nerve, 'nervous impulses.' We have stated above that the muscle is irritable in the sense that it may be thrown into contractions by stimuli applied directly to itself. But it might fairly be urged that the contractions so pro- duced are in reality due to the fact that, although the stimulus is apparently applied directly to the muscle, it is, after all, the fine nerve-branches, so abundant in the muscle, which are actually stimulated. The following facts however go far to prove that the muscular fibres themselves are capable of being directly stimu- lated without the intervention of any nerves. When a frog (or other animal) is poisoned with urari, the nerves may be subjected to the strongest stimuli without causing any contractions in the muscles to which they are distributed ; yet even ordinary stimuli applied directly to the muscle readily cause contractions. If before introducing the urari into the system, a ligature be passed under- neath the sciatic nerve in one leg, for instance the right, and drawn tightly round the whole leg to the exclusion of the nerve, it is evident that the urari when injected into the back of the animal, will gain access to the right sciatic nerve above the ligature, but not below, while it will have free access to the whole left sciatic. If, as soon as the urari has taken effect, the two sciatic nerves be stimulated, no movement of the left leg will be produced by stimu- lating the left sciatic, whereas strong contractions of the muscles of the right leg below the ligature will follow stimulation of the right sciatic, whether the nerve be stimulated above or below the ligature. Now since the upper parts of both sciatics are equally exposed to the action of the poison, it is clear that the failure of the left nerve to cause contraction is not attributable to any change having taken place in the upper portion of the nerve, else why should not the right, which has in its upper portion been equally exposed to the action of the poison, also fail ? Evidently the poison acts on some parts of the nerve lower down. If a single muscle be removed from the circulation (by ligaturing its blood-vessels), previous to the poisoning with urari, that muscle will contract when any part of the nerve going to it is stimulated, though no other muscle in the body will contract when its nerve is stimulated. Here the whole nerve right down to the muscle has been exposed to the action of the CHAP, ii.] THE CONTRACTILE TISSUES. 39 poison ; and yet it has lost none of its power over the muscle. On the other hand, if the muscle be allowed to remain in the body, and so be exposed to the action of the poison, but the nerve be divided high up and the part connected with the muscle gently lifted up before the urari is introduced into the system, so that no blood flows to it and so that it is protected from the influence of the poison, stimulation of the nerve will be found to produce no con- tractions in the muscle, though stimuli applied directly to the muscle at once cause it to contract. From these facts it is clear that urari poisons the ends of the nerve within the muscle long before it affects the trunk, and it is exceedingly probable that it is the very extreme ends of the nerves (possibly the end-plates, for urari poisoning, at least when profound, causes a slight but yet distinctly recognisable effect in the microscopic appearance of these structures) which are affected. The phenomena of urari poisoning therefore go far to prove that muscles are capable of being made to contract by stimuli applied directly to the muscular fibres them- selves ; and there are other facts which support this view. This question of 'independent muscular irritability' was once thought to be of importance. In old times, the swelling of a muscle during con- traction was held to be caused by the animal spirits descending into it along the nerves; and when the doctrine of 'spirits' was given up, it was still taught that the vital activity of the muscle was something bestowed upon it by the action of the nerve, and not properly belonging to itself. We owe to Haller the establishment of the truth, that the contraction of a muscle is a manifestation of the muscle's own energy, excited it may be by nervous action, but not caused by it. Haller spoke of the muscle as possessing a vis insita, while he called the nervous action, which excites contraction, the vis nervosa. He used the word irritability as almost synonymous with contractility, a meaning which is still adopted by many authors. In this work we have used it in the wider sense, first employed by Glisson, which includes other manifesta- tions of energy than the change of form which constitutes a contraction. The Phenomena of a simple Muscular Contraction. If the far end of the nerve of a muscle-nerve preparation1, Figs. 1 and 2, be laid on the electrodes of an induction-machine 2, 1 By this is meant a muscle dissected out with some length of nerve attached to it, both being in a living condition, i.e. still irritable. The muscle generally used is the gastrocnemius of the frog, the attachment to the femur and a portion of the tendo Achillis, together with a considerable length of the sciatic nerve, being carefully preserved. 2 It may perhaps be worth while to remind the reader of the following facts. In a galvanic battery, the substance (plate of zinc for instance) which is acted upon and used up by the liquid is called the positive element, and the sub- stance which is not so acted upon and used up (plate &c. of copper, platinum, or carbon, &c.) is called the negative element. A galvanic action is set up when the positive (zinc) and the negative (copper) elements are connected outside the battery 40 MUSCULAR CONTRACTION. [BOOK i. the passage of a single induction-shock, which may be taken as a convenient form of an almost momentary stimulus, will produce no visible change in the nerve, but the muscle will give a short sharp contraction, i.e. will for an instant shorten itself, becoming thicker the while, and then return to its previous condition. If one end of the muscle be attached to a lever, while the other is fixed, the by some conducting material, such as a wire, and the current is said to flow in a circuit or circle, from the zinc or positive element to the copper or negative element inside the battery and then from the copper or negative element back to the zinc or positive element through the wire outside the battery. If the conducting wire be cut through, the current ceases to flow, but if the cut ends be brought into contact, the current is re-established and continues to flow so long as the contact is good. The wires or the ends of the wires, which may be fashioned in various ways, are called electrodes. When the electrodes are brought into contact or are connected by some conducting material, galvanic action is set up, and the current flows through the battery and wires; this is spoken of as "making the current" or "completing or closing the circuit." When the electrodes are drawn apart from each other, or when some non-conducting material is interposed between them, the galvanic action is arrested; this is spoken of as "breaking the current" or "opening the circuit." The current passes from the electrode connected with the negative (copper) element in the battery to the electrode connected with the positive (zinc) element in the battery ; hence the electrode connected with the copper (negative) element is called the positive electrode, and that connected with the zinc (positive) element is called the negative electrode. In an "induction machine" the wire connecting the two elements of a battery is twisted at some part of its course into a close spiral, called the primary coil. Thus in Fig. 1 -the wire x"' connected with the copper or negative plate c.p. of the battery, E, joins the primary coil pr. c., and then passes on as y'", through the "key" F, to the positive (zinc) plate z.p. of the battery. (In Fig. 9. p. 51) the direction of the current from x to y through the primary coil P is shewn by arrows; but in this figure complications are introduced which will be explained hereafter.) Over this primary coil, but quite unconnected with it, slides another coil, the secondary coil, s.c. ; the ends of the wire forming this coil, y" and x", are continued on in the arrangement illustrated in the figure as y' and y, and as x' and x and terminate in electrodes. If these electrodes are in contact or connected with conducting material, the circuit of the secondary coil is said to be closed ; otherwise it is open. In such an arrangement it is found that at the moment when the primary circuit is closed, i.e. when the primary current is "made" a secondary "induced" current is, for an exceedingly brief period of time, set up in the secondary coil. Thus in Fig. 1 when by moving the "key" F, y'" and x'" previously not in con- nection with each other, are put into connection and the primary current thus made, at that instant a current appears in the wires y" x" &c., but almost immediately disappears. A similar almost instantaneous current is also developed when the primary current is "broken," but not till then. So long as the primary current flows with uniform intensity, no current is induced in the secondary coil. It is only when the primary current is either made or broken, or suddenly varies in intensity that a current appears in the secondary coil. In each case the current is of very brief duration, gone in an instant almost, and may therefore be spoken of as " a shock," an induction shock ; being called a "making shock" when it is caused by the making, and a "breaking shock" when it is caused by the breaking, of the primary circuit. The direction of the current in the making shock is opposed to that of the primary current; thus in the figure while the primary current flows from of" to i/'", the induced making shock flows from y to x. The current of the breaking shock on the other hand flows in the same direction as the primary current from x to y, and is therefore in direction the reverse of the making shock. When the primary current is repeatedly and rapidly made and broken, the secondary current being developed with each make and with each break, a rapidly recurring series of alternating currents is developed in the secondary coil and passes through its electrodes. We shall frequently speak of this as the interrupted induction current, or more briefly the interrupted current. CHAP. TI.] THE CONTRACTILE TISSUES. 41 42 THE MUSCLE CURVE. [BOOK i. FlG. 1. DlAGBAM ILLUSTRATING APPABATUS ABBANGED FOB ExPEBIMENTS WITH MUSCLE AND NEBVE. A. The moist chamber containing the muscle-nerve preparation. (The muscle- nerve and electrode-holder are shewn on a larger scale in Fig. 2.) The muscle m, supported by the clamp cl, which firmly grasps the end of the femur/, is connected by means of the S hook s and a thread with the lever I, placed below the moist chamber. The nerve n, with the portion of the spinal column n' still attached to it, is placed on the electrode-holder el, in contact with the wires x, y. The whole of the interior of the glass case gl. is kept saturated with moisture, and the electrode-holder is so constructed that a piece of moistened blotting-paper may be placed on it without coming into contact with the nerve. B. The revolving cylinder bearing the smoked paper on which the lever writes. (7. Du-Bois Eeymond's key arranged for short-circuiting. The wires x and y of the electrode-holder are connected through binding screws in the floor of the moist chamber with the wires x', y', and these are secured in the key, one on either side. To the same key are attached the wires x" y" coming from the secondary coils s. c. of the induction-machine D. This secondary coil can be made to slide up and down over the primary coil pr. c. , with which are con- nected the two wires x'" and y'". x'" is connected directly with one pole, for instance the copper pole c. p. of the battery E. y'" is carried to a binding screw a of the Morse key F, and is continued as T/IV from another binding screw 6 of the key to the zinc pole z. p. of the battery. Supposing everything to be arranged, and the battery charged, on depressing the handle ha, of the Morse key F, a current will be made in the primary coil pr. c., passing from c. p. through x1" to pr. c., and thence through y'" to a, thence to 6, and so through yiv to z. p. On removing the finger from the handle of F, a spring thrusts up the handle, and the primary circuit is in consequence immediately broken. At the instant that the primary current is either made or broken, an induced current is for the instant developed in the secondary coil s. c. If the cross bar h in the du-Bois Eeymond's key be raised (as shewn in the thick line in the figure), the wires x", x', x, the nerve between the electrodes and the wires y, y', y" form the complete secondary circuit, and the nerve consequently experiences a making or breaking induction-shock whenever the primary current is made or broken. If the cross bar of the du-Bois Eeymond key be shut down, as in the dotted line h' in the figure, the resistance of the cross bar is so slight compared with that of the nerve and of the wires going from the key to the nerve, that the whole secondary (induced) current passes from x" to y" (or from y" to x"), along the cross bar, and practically none passes into the nerve. The nerve being thus "short-circuited," is not affected by any changes in the current. CHAP, ii.] THE CONTRACTILE TISSUES. 43 FIG. 2. The muscle-nerve preparation of Fig. 1, with the clamp, electrodes, and electrode-holder, are here shewn on a larger scale. The letters as in Fig. 1. The apparatus figured in Figs. 1 and 2 is intended merely to illustrate the general method of studying muscular contraction; it is not to be supposed that the details here given are universally adopted or indeed the best for all purposes. lever will by its movement indicate the extent and duration of the shortening. If the point of the lever be brought to bear on some rapidly travelling surface, on which it leaves a mark (being for this purpose armed with a pen and ink if the surface be plain paper, or with a bristle or needle if the surface be smoked glass or paper), so long as the muscle remains at rest the lever will describe an even line. When, however, a contraction takes place, as when a single induction-shock is sent through the nerve, some such curve as that shewn in Fig. 3 will be described, the lever rising with the shorten- Fio. 3. A MUSCLE- CURVE OBTAINED BY MEANS OF THE PENDULUM MTOQRAPH. To be read from left to right. 6 the a indicates the moment at which the induction- shock is sent into the nerve. commencement, c the maximum, and d the close of the contraction. Below the muscle-curve is the curve drawn by a tuning-fork making 180 double vibrations a second, each complete curve representing therefore ^rv °f a second. It will be observed that the plate of the myograph was travelling more rapidly towards the close than at the beginning of the contraction, as shewn by the greater length of the vibration- curves. ing of the muscle, and descending as the muscle returns to its natural length. This is known as the ' muscle-curve.' In order to make the ' muscle-curve ' complete, it is necessary to mark on the record- ing surface the exact time at which the induction-shock is sent into the nerve, and also to note the speed at which the recording surface is travelling. These points are best effected by means of the pendulum myograph, Fig. 4. In this instrument a smoked glass plate, on which a lever writes, forms the bob of a pendulum and consequently swings with it. The pendulum with the glass plate attached being raised up, is suddenly let go. It swings of course to the opposite side, the glass plate travels through an arc of a circle, and, the lever being stationary, the point of the lever describes an arc on the glass plate. The rate at which the glass plate travels, i.e. the time it takes for the lever-point to describe a line of a given length on THE MUSCLE CURVE. [BOOK i. FIG. 4. THE PENDULUM MYOGRAPH. The figure is diagrammatic, the essentials only of the instrument being shewn. The smoked glass plate A swings with the pendulum B on carefully adjusted CHAP, ii.] THE CONTRACTILE TISSUES. 45 bearings at C. The contrivances by which the glass plate can be removed and replaced at pleasure are not shewn. A second glass plate so arranged that the first glass plate may be moved up and down without altering the swing of the pendulum is also omitted. Before commencing an experiment the pendulum is raised up (in the figure to the right), and is kept in that position by the tooth a catching on the spring-catch b. On depressing the catch 6 the glass plate is set free, swings into the new position indicated by the dotted lines, and is held in that position by the tooth a' catching on the catch b'. In the course of its swing the tooth a' coming into contact with the projecting steel rod c, knocks it on one side into the position indicated by the dotted line c'. The rod c is in electric continuity with the wire x of the primary coil of an induction-machine. The screw d is similarly in electric continuity with the wire y of the same primary coil. The screw d and the rod c are armed with platinum at the points in which they are in contact, and both are insulated by means of the ebonite block e. As long as c and d are in contact the circuit of the primary coil to which x and y belong is closed. When in its swing the tooth a' knocks c away from d, at that instant the circuit is broken, and a 'breaking' shock is sent through the electrodes connected with the secondary coil of the machine, and so through the nerve. The lever I, the end only of which is shewn in the figure, is brought to bear on the glass plate, and when at rest describes a straight line, or more exactly an arc of a circle of large radius. The tuning-fork /, the ends only of the two limbs of which are shewn hi the figure placed immediately below the lever, serves to mark the time. the glass plate, may be calculated from the length of the pendulum, but it is simpler and easier to place a vibrating tuning-fork immediately under the point of the lever. If the vibrations of the tuning-fork are known, then the number of vibrations which are marked on the plate between any two points on the line described by the lever gives the time taken by the lever in passing from one point to the other. An easy arrangement permits the exact time at which the shock is sent through the nerve to be marked on the line of the lever. To avoid the confusion of too many markings on the plate the pendulum after describing an arc is caught by a spring catch on the opposite side. A complete muscle-curve, such as that shewn in Fig. 3, taken from the gastrocnemius of a frog, teaches us the following facts : 1. That although the passage of the induced current from electrode to electrode is practically instantaneous, its effect, measured from the entrance of the shock into the nerve to the return of the muscle to its natural length after the shortening, takes an appreci- able time. In the figure, the whole curve from a to d takes up about the same time as eighteen double vibrations of the tuning- fork. Since each double vibration here represents -^ of a second, the duration of the whole curve is ^ sec. 2. In the first portion of this period, from a to b, there is no visible change, no shortening of the muscle, no raising of the lever. 3. It is not until 6, that is to say after the lapse of IoU i.e. about -^sec., that the shortening begins. The shortening as shewn by the curve is at first slow, but soon becomes more rapid, and then slackens again until it reaches a maximum at c; the whole shortening occupying about -^ sec. 4. Arrived at the maximum of shortening, the muscle at once begins to relax, the lever descending at first slowly, then very . 46 THE MUSCLE CURVE. [BOOK i. rapidly, and at last more slowly again, until at d the muscle has regained its natural length ; the whole return from the maximum of contraction to the natural length occupying yj^, i.e. about -fa sec. Thus a simple muscular contraction, a simple spasm or twitch as it is sometimes called, produced by a momentary stimulus, such as a single induction-shock, consists of three main phases : 1. A phase antecedent to any visible alteration in the muscle. This phase, during which invisible preparatory changes are taking place in the nerve and muscle, is called the ' latent period '. 2. A phase of shortening or, in the more strict meaning of the word, contraction. 3. A phase of relaxation or return to the original length. In the case we are considering, the electrodes are supposed to be applied to the nerve at some distance from the muscle. Consequently the latent period of the curve comprises not only the preparatory actions going on in the muscle itself, but also the changes necessary to conduct the immediate effect of the induction-shock from the part of the nerve between the electrodes, along a considerable length of nerve down to the muscle. It is obvious that these latter changes might be eliminated by placing the electrodes on the muscle itself or on the nerve close to the muscle. If this were done, the muscle and lever being exactly as before, and care were taken that the induction-shock entered into the nerve at the new spot, at the moment when the point of the lever had reached a T>1> FIG. 5. CURVES ILLUSTRATING THE MEASUREMENT OP THE VELOCITY or A NERVOUS IMPULSE. (Diagrammatic.) To be read from left to right. The same muscle-nerve preparation is stimulated (1) as far as possible from the muscle, (2) as near as possible to the muscle ; both contractions are registered by the pendulum myograph exactly in the same way. In (1) the stimulus enters the nerve at the time indicated by the line a, the con- traction, shewn by the dotted line, begins at V ; the whole latent period therefore is indicated by the distance from a to &'. In (2) the stimulus enters the nerve at exactly the same time a; the contraction, shewn by the unbroken line, begins at b ; the latent period therefore is indicated by the distance between a and 6. The time taken up by the nervous impulse in passing along the length of nerve between 1 and 2 is therefore indicated by the distance between & and &', which may be measured by the tuning-fork curve below. N.B. No value is given in the figure for the vibrations of the tuning-fork, since the figure is diagrammatic, the distance between the two curves, as compared with the length of either, having been purposely exaggerated for the sake of simplicity. CHAP, ii.] THE CONTRACTILE TISSUES. 47 exactly the same point of the travelling surface as before, a curve like that shewn by the plain line in Fig. 5 would be gained. It resembles the first curve (indicated in the figure by a dotted line) in all points, except that the latent period is shortened : the con- traction begins rather earlier. From this we learn two facts : The greater part of the latent period is taken up by changes in tlie Nmuscle itself, preparatory to the actual visible shortening, for the two latent periods do not differ much. Of course, even in the second case, the latent period includes the changes going on in the short piece of nerve still lying between the electrodes and the muscular fibres. To eliminate this with a view of determining the latent period in the muscle itself, the electrodes might be placed directly on the muscle poisoned with urari. If this were done, it would still be found that the latent period was chiefly taken up by changes in the muscular as distinguished from the nervous elements. 2. Such difference as does exist indicates the time taken up by the propagation, along the piece of nerve, of the changes set up at the far end of the nerve by the induction-shock. These changes we shall hereafter speak of as constituting a nervous impulse ; and the above experiment shews that it takes some appreciable time for a nervous impulse to travel along a nerve. In the figure the difference between the two latent periods, the distance between b and 6', seems almost too small to measure accurately ; but if a long piece of nerve be used for the experiment, and the recording surface -be made to travel very fast, the difference between the duration of the latent period when the induction-shock is sent in at a point close to the muscle, and that when it is sent in at a point as far away as possible from the muscle, may be satisfactorily measured in fractions of a second. If the length of nerve between the two points be accurately measured, the rate at which a nervous impulse travels along the nerve to a muscle can thus be easily calculated. This has been found to be in the frog about 28, and in man about 33 metres per second. Thus when a momentary stimulus, such as a single induction- shock, is sent into a nerve connected with a muscle, the following events take place : 1. The generation at the spot stimulated of a nervous impulse, and the propagation of the impulse along the nerve to the muscle. The time taken up by this varies according to the length of the nerve but is always very short. 2. The setting up of certain molecular changes in the muscle, unaccompanied by any visible alteration in its form, constituting the latent period, and occupying on an average about y^th sec. 3. The shortening of the muscle up to a maximum, occupying about sec. 48 TETANIC CONTRACTIONS. [BOOK i. 4. The return of a muscle to its former length, occupying about ylfosec. We have given what may be considered the average duration l of each phase chiefly for the sake of shewing their relative propor- tions. But it must be borne in mind that the duration of a contraction differs in different animals and in different muscles of the same animal ; in the rabbit the more deeply coloured SQ^called "red" muscles have in their contraction a longer period than have the pale muscles. The duration may also differ in the same muscle under different conditions; moreover the duration of the several phases may vary independently. Temperature has a marked effect in varying the length of the muscle-curve, a higlTtemperature shortening, and a low temperature prolonging, the contraction, and especially the third phase or relaxation. Fatigue also lengthens the contraction as do also to a remarkable extent certain poisons such as veratrin. An increase in the load which the muscle is lifting, shortens the descending or return part of the curve and increases the length of the latent period. All such influences will be better studied when we come to speak more in detail of the changes which take place in a muscle during contraction. Their effects are only mentioned now in order that the reader may thus early learn to conceive of even a simple muscular contraction as a complex act, the several parts of which are variable, so that many differing forms of a muscle-curve may be obtained under different circumstances. Tetanic Contractions. If a single induction-shock be followed at a sufficiently short interval by a second shock of the same strength, the first simple FIG. 6. TRACING or A DOUBLE MUSCLE-CURVE. To be read from left to right. While the muscle2 was engaged in the first contraction (whose complete course, had nothing intervened, is indicated by the dotted line), a second induction-shock was thrown in, at such a time that the second contraction began just as the first was beginning to decline. The second curve is seen to start from the first, as does the first from the base-line. 1 The curve described in the previous text happened to have a rather long latent period, and the lengthening to be of shorter instead of longer duration than the shortening. 2 In this and the other curves of this section the tracings figured were taken from frog's muscle. CHAP, ii.] THE CONTRACTILE TISSUES. 49 contraction or spasm will be followed by a second spasm, the two bearing some such relation to each other as that shewn by the curve in Fig. 6, where the interval between the two shocks was just long enough to allow the first spasm to have passed its maxi- mum before the latent period of the second was over. It will be observed that the second curve is almost in all respects like the first except that it starts, so to speak, from the first curve instead of from the base-line. The second nervous impulse has acted on the already contracted muscle, and made it contract again just as it would have done if there had been no first impulse and the muscle had been at rest. The two contractions are added together and the lever raised nearly double the height it would have been by either alone. A more or less similar result would occur if the second contraction began at any other phase of the first. The combined effect is, of course, greatest when the second contraction begins at the maximum of the first, being less both before and afterwards. If in the same way a third shock follows the second at a sufficiently short interval, a third curve is piled on the top of the second. The same with a fourth, and so on. FIG. 7. MUSCLE THROWN INTO TETANUS, WHEN THE PRIMARY CURRENT or AN IN- DUCTION-MACHINE IS EEPEATEDLT BROKEN AT INTERVALS OF SIXTEEN IN A SECOND. To be read from left to right. The upper Hue is that described by the muscle. The lower marks time, the intervals between the elevations indicating seconds. The intermediate line shews when the shocks were sent in, each mark on it corresponding to a shock. The lever, which describes a straight line before the shocks are allowed to fall into the nerve, rises almost vertically (the recording surface travelling in this case slowly) as soon the first shock enters the nerve at a. Having risen to a certain height, it begins to fall again, but in its fall is raised once more by the second shock, and that to a greater height than before. The third and succeeding shocks have similar effects, the muscle continuing to become shorter, though the shortening at each shock is less. ^ After a while the increase in the total shortening of the muscle, though the individual contractions are still visible, almost ceases. At b, the shocks cease to be sent into the nerve ; the contractions almost immediately disappear, and the lever forthwith commences to descend. The muscle being lightly loaded, the descent is very gradual ; the muscle had not regained its natural length when the tracing was stopped. F. -i 50 TETANIC CONTRACTIONS. [BOOK i. When however repeated shocks are given it is found that the height of each contraction is rather less than the preceding one, and this diminution becomes more marked the greater the number of shocks. Hence after a certain number of shocks, the succeeding impulses do not cause any further shortening of the muscle, any further raising of the lever, but merely keep up the contraction already existing. The curve thus reaches a maximum, which it maintains, subject to the depressing effects of exhaustion, so long as the shocks are repeated. When these cease to be given, the muscle returns, in the usual way, at first very rapidly, and then more slowly, to its natural length. When the shocks do not succeed each other too rapidly, the individual contractions may readily be traced along the whole curve, as is seen in Fig. 7, where the primary current of the induction-machine was repeatedly broken at intervals of sixteen in a second. When the shocks succeed each other more rapidly, the individual contractions, visible at first, FIG. 8. TETANUS PBODUCED WITH THE OBDINABY MAGNETIC INTEBEUPTOB OF AN IN- DUCTION-MACHINE. (Eecording surface travelling slowly.) To be read from left to right. The interrupted current being thrown in at a the lever ristes rapidly, but at b the muscle reaches the maximum of contraction. This is continued till c, when the current is shut off and relaxation commences. may become fused together and lost to view as the tetanus con- tinues and the muscle becomes tired. When the shocks succeed each other still *more rapidly (the second contraction beginning in the ascending portion of the first), it becomes difficult or impossible to trace out the single contractions. The curve then described by the lever is of the kind shewn in Fig. 8, where the primary current of an induction-machine was rapidly made and broken by the magnetic interrupter, Fig. 9. The lever, it will be observed, rises at a after the latent period (which is not marked), first rapidly, and then more slowly, in an apparently unbroken line to a maxi- mum at about 6, maintains the maximum so long as the shocks continue to be given, and when these cease to be given, as at c, gradually descends to the base-line. This condition of muscle, brought about by rapidly repeated shocks, this fusion of a number of simple spasms into an apparently smooth, continuous effort, is known as tetanus, or tetanic contraction. The above facts are most clearly shewn when induction-shocks, or at least galvanic currents in some form or other, are employed. They are seen, however, whatever be the form of stimulus employed. Thus in the case of CHAP, ii.] THE CONTRACTILE TISSUES. 51 mechanical stimuli, while a single blow may cause a single spasm, a pronounced tetanus may be obtained by rapidly striking suc- cessively fresh portions of a nerve. With chemical stimulation, as when a nerve is dipped in acid, it is impossible to secure a momentary application; hence tetanus, generally irregular in character, is the normal result of this mode of stimulation. In the living body, the contractions of the striated muscles, brought about either by the will or by reflex action, are generally tetanic in character. Even very short sharp movements, such as a sudden jerk of the limbs, are in reality examples of tetanus of short duration. FIG. 9. THE MAGNETIC INTERBUPTOE. The figure is introduced to illustrate the action of this instrument as commonly used by physiologists. The two wires x and y from the battery are connected with the two brass pillars a and d by means of screws. Directly contact is thus made the current, indicated in the figure by the thick interrupted line, passes in the direction of the arrows, up the pillar a, along the steel spring b, as far as the screw c, the point of which, armed with platinum, is in contact with a small platinum plate on 6. The current passes from b through c and a connecting wire into the primary coil p. Upon its entering into the primary coil, an induced (making) current is for the instant de- veloped in the secondary coil (not- shewn in the figure). From the primary coilp the current passes, by a connecting wire, through the double spiral, m, and, did nothing happen, would continue to pass from m by a connecting wire to the pillar d, and so by the wire y to the battery. The whole of this course is indicated by the thick interrupted line with its arrows. As the current however passes through the spirals m, the iron cores of these are made magnetic. They in consequence draw down the iron bar e, fixed at the end of the spring 6, the flexibility of the spring allowing this. But when e is drawn down, the platinum plate on the upper surface of 6 is also drawn away from the screw c, and a similar platinum plate on the under surface of b is brought into contact with the platinum-armed point of the screw /, the screws being so arranged that this takes place. In consequence of this change the current can no longer pass from 6 to 52 TETANIC CONTRACTIONS. [BOOK i. c. On the contrary, it passes from b to /, and so down the pillar d, in the direction indicated by the thin interrupted line, and out to the battery by the wire y. Thus the current is 'short- circuited' from the primary coil; and the instant that the current is thus cut off from the primary coil, an induced (breaking) current is for the moment developed in the secondary coil. But the current is cut off not only from the primary coil, but also from the spirals m ; in consequence their cores cease to be magnetised, the bar e ceases to be attracted by them, and the spring ft, by virtue of its elasticity, resumes its former position in contact with the screw c. This return of the spring however re-establishes the current in the primary coil and in the spirals, and the spring is drawn down, to be released once more in the same manner as before. Thus as long as the current is passing along x, the contact of 6 is constantly alternating between c and/, and the current is constantly passing into and being shut off from p, the periods of alternation being determined by the periods of vibration of the spring 6. With each passage of the current into, or withdrawal from the primary coil, an induced (making and, respectively, breaking) shock is de- veloped in a secondary coil. When it has once been realized that an ordinary tetanic muscular movement is essentially a vibratory movement, that the apparently rigid and firm muscular mass is really the subject of a whole series of vibrations, a series namely of simple spasms, it will be readily understood why a tetanized muscle, like all other vibrating bodies, gives out a sound. That a contracting (tetanized) muscle does give out a sound, the so-called muscular sound, is easily proved by listening with a stethoscope to a contracted biceps, or by stopping the ears and listening to the contractions of one's own masseter and temporal muscles. When a muscle is thrown into tetanus by interrupted shocks applied directly to the nerve or to the muscle, the note is the same as that of the interruptor determining the number of the shocks. This is naturally the case, since the note of the muscle-sound is determined by the rapidity of the spasms or vibrations which go to make up the tetanus, and these are determined by the rapidity with which the stimulus is repeated. When a muscle is thrown into tetanus by the will or by reflex action or by direct stimulation of the spinal cord, in fact, in any way through the action of the central nervous system, the same note is always heard, viz. one of 36 to 40 vibrations per second, which however is probably a harmonic of a lower note indicating that the muscle is really vibrating 19 or 20 times a second. It need hardly be said that a single muscular contraction, a single vibration, cannot cause a muscular sound. The general observations which have been described in this section may, when proper precautions are taken, be carried out on a muscle-nerve preparation from a frog for a very considerable time after its removal from the body. After some hours however, or it may be days, the length of time varying according to circumstances, it will be found that no stimulus, however powerful, will cause any contraction, when applied either to the nerve or to the muscle. Both muscle and nerve are then said to have lost their irritability ; and a short time afterwards the muscle may be observed to pass into a peculiar condition known as rigor mortis, CHAP, ii.] THE CONTRACTILE TISSUES 53 in which it loses all the suppleness and extensibility characteristic of the living irritable muscle. The causes of this loss of irritability as well as the features and nature of this rigor mortis we shall study in detail presently. The muscles and nerves of a mammal, or indeed of any warm- blooded animal, lose their irritability, and the muscles become rigid in a very short time (it may be a few minutes) after removal from the body. Hence these are less suitable for experiments than the muscles and nerves of the frog, though their general phenomena are exactly the same. We must now attempt to study in greater detail the changes which take place in a muscle and nerve during the contraction of the former and the passage of an impulse along the latter, with a view to the better understanding of both events. SEC. 2. THE CHANGES IN A MUSCLE DURING MUSCULAR CONTRACTION. The Change in Form. We have seen that at the close of the latent period the muscle shortens, that is, each fibre shortens, at first slowly, then more rapidly, and lastly more slowly again. The shortening (which in severe tetanus may amount to three-fifths of the length of the muscle) is accompanied by an almost exactly corresponding thicken- ing, so that there is hardly any actual change in bulk. If a muscle be placed horizontally, and a lever laid upon it, the thickening of the muscle will raise up the lever, and cause it to describe on a recording surface a curve exactly like that described by a lever attached to the end of the muscle. There appears to be a minute diminution of bulk not amounting to more than one thousandth. If a long muscle of parallel fibres, poisoned with urari, so as to eliminate the action of its nerves, be stimulated at one end, the contraction may be seen, almost with the naked eye, to start from the end stimulated, and to travel along the muscle. If two levers be made to rest on, or be suspended from, two points of such a muscle placed horizontally, the points being at a known distance from each other and from the point stimulated, the progress of the contraction may be studied. It is found that the contraction starting from the spot stimulated, passes along the muscle in the form of a wave diminishing in vigour as it proceeds. The velocity with which this contraction wave travels in the muscles of the frog is about 3 or 4 metres a second ; and since it takes, in round numbers, from about 0-5 to *1 sec. for the contraction to pass over any point of the fibre, the wave-length of the contraction wave must be from about 200 to 400 mm. In the muscles of a mammal laid bare for the purposes of experiment the velocity does not seem to be very different from that in the frog; but in the intact muscles in their normal con- CHAP. IL] THE CONTRACTILE TISSUES. 55 dition in the living body, it is probably somewhat greater, and the wave also probably travels with undiminished velocity and vigour to the end of the fibre. In general, the velocity with which the contraction wave travels, like the duration and character of the con- traction, varies under different circumstances, being much influenced by temperature, by the action of drugs, and especially by those complex intrinsic changes which we speak of as fatigue or ex- haustion. Seeing that the extreme limit of the length of a muscular fibre is about 30 or 40 mm., it is evident that even when the stimulation begins at one end and the wave travels at the more rapid rate, the whole fibre is not only in a state of contraction at the same time, but almost in the same phase of the contraction wave. In an ordinary contraction occurring in the living body the stimulus is never applied to one end of the fibre; the nervous impulse which in such cases acts as the stimulus to the muscle, falls into the fibre at about its middle, where the nerve ends in an end-plate, and the contraction wave starting from the end-plate travels along the muscular fibre in both directions. In such a case therefore, still more even than in the urarised muscle stimulated artificially at one end, must the whole fibre be occupied at the same time by the wave of contraction. Changes in microscopic structure. When portions of living irritable muscle are examined under the microscope, contraction waves similar to those just described, but feebler and of shorter FlO. 10. MUSCULAB FIBRE UNDERGOING CONTRACTION. The muscle is that of Telephones melanurus treated with osmic acid. The fibre at c is at rest, at a the contraction begins, at 6 it has reached its maximum. The right-hand side of the figure shews the same fibre as seen in polarized light. (After Engelmann. ) 56 THE CHANGE OF FORM. [BOOK T. length, may be observed passing along the fibres. By appropriate treatment with osmic acid or other reagents, these short contraction waves may be fixed, and the structure of the contracted portion compared at leisure with that of the portions of the fibre at rest. In Fig. 10, representing a fibre of the muscle of an insect (in which these changes can be more satisfactorily studied than in vertebrate muscle), the contraction wave begins near a, and has reached about its maximum at b, while at c the fibre is at rest, the contraction wave not having reached it (or having passed over it, for the beginning and end of the wave are exactly alike). It will be seen that at b, each disc of the fibre is shorter and broader than at c. Further, while at c the dim band oc is conspicuous, and the light band y, with its accessory markings y ', is together lighter than the dim band x, at b in the fully contracted part of the fibre the dim band appears light as compared with the black line y occupying the middle of the previously light band. In the contracted muscle then there is a reversal of the state of things in the resting muscle, the light band (or part of the light band) of the latter in contracting becomes dark, and the dim band of the latter becomes by comparison light. Between rest and full contraction there is an intermediate stage, as at d, in which the distinction between rHm and bright bands seems to be largely lost. The subject however is one offering peculiar difficulties in the way of investigation, and while most, though not all, observers agree in the broad facts which have just been stated, there is great diversity of opinion concerning further details and especially as to the interpretation of the various appearances observed. The accessory markings in the middle of the light band have, in particular, been the subject of controversies into which we cannot enter here. When the fibre is examined in polarised light it is seen that the dim band is anisotropic, and the light band isotropic. This is the case during all the phases of the contraction. At no period is there any confusion between the anisotropic and isotropic material ; these maintain their relative positions, both become shorter and broader; but it will be observed that the isotropic substance diminishes in height to a much greater extent than does the anisotropic substance. The latter in fact appears to increase in bulk at the expense of the former. Relaxation. The shortening as we have seen is followed by a relaxation, the muscle returning to its original length. When an appropriate weight is attached to the muscle this return is generally complete, the curve speedily rejoining, as shewn in Fig. 3, the base line from which it started ; but when no load is used and the muscle therefore is acted upon by its own weight and that of a very light lever only, the return is incomplete ; the curve, though descending near to, fails to touch the base line and runs nearly parallel to it for some considerable distance. The relaxation is therefore obviously assisted by the extending force of the load ; CITAP. ii.] THE CONTRACTILE TISSUES. 57 but, nevertheless, is in the main the result of intrinsic processes going on in the muscle, the reverse of those leading to the shorten- ing. The return of the muscle to its elongated condition, is not a mere passive stretching, after the causes leading to the shortening have passed away; it like the shortening itself is a manifestation of activity. And hence we find that the complete- ness of the relaxation is dependent on the complex changes which we speak of as the nutrition of the muscle. Thus in their natural position in the living body, muscles, owing to their vigorous nu- trition, assisted by the fact that their anatomical disposition keeps them always on the stretch, return completely to their original length, after even powerful and prolonged contractions. In a muscle out of the body, on the other hand, even when loaded, re- peated successive contractions frequently result in the failure to achieve complete relaxation becoming very conspicuous ; and the tetanus curves, Figs. 6 and 7, shew very strikingly this shortcoming, which is often spoken of as the 'contraction remainder/ We may speak of the relaxation as the result of an elastic reaction, but only in the sense that the elastic qualities of the muscle, at any moment, are the expression of deep-seated and con- tinually varying molecular changes going on in the muscular sub- stance. And in this connection attention may be called to a peculiar physical character of contracting muscle. Living muscle at rest is very extensible, but when stretched returns after the extending cause has been removed, rapidly and completely to its former length. In physical language muscle is spoken of as possessing slight but perfect elasticity. It might be imagined that during a contraction this extensibility would be diminished in order that none of the resistance which the muscle had to overcome, no part of the weight for instance which had to be lifted, should be employed in stretching the muscle itself and thus lead to an apparent waste of energy. On the contrary we find that during a contraction there is an increase of extensibility ; thus if a muscle at rest be loaded with a given weight, say 50 grammes, and its extension observed, and be then while unloaded thrown into tetanus, and the load applied during the tetanus, the extension in the second case will be distinctly greater than in the first. During the contraction there is so to speak a greater mobility of the muscular molecules, and though this greater mobility may have its advantages, the loaded muscle has in contracting to overcome its own increased tendency to lengthen on extension before it can produce any effect on the weight which it has to lift. The elasticity and extensibility of the muscular substance is how- ever a complicated and difficult subject, and it will be sufficient to reassert that it is essentially a vital property, being dependent, like the irritability of the muscular substance, on certain nutritive factors. As the muscular substance becomes weary with too much work or impoverished by scanty nutrition, its elasticity suffers pari passu 58 MUSCLE CURRENTS. [BOOK i. with its irritability. The exhausted muscle when extended does not return so readily to its proper length as the fresh active muscle, and, as we shall see, the dead muscle does not return at all. Electrical Changes. Muscle-currents. If a muscle be removed in an ordinary manner from the body, and two non-polarisable electrodes1, con- z.s di.c FlG. 11. NON-POLABISABLE ELECTRODES. a, the glass tube; z, the amalgamated zinc slips connected with their respective wires; z. s., the zinc sulphate solution; ch. c., the plug of china clay; c', the portion of the china-clay plug projecting from the end of the tube; this can be moulded into any required form. nected with a delicate galvanometer of many convolutions, be placed on two points of the surface of the muscle, a deflection of the galvanometer will take place indicating the existence of a current passing through the galvanometer from the one point of the muscle to the other, the direction and amount of the deflection varying according to the position of the points. The 'muscle- currents' thus revealed are seen to the best advantage when the muscle chosen is a cylindrical or prismatic one with parallel fibres, and when the two tendinous ends are cut off by clean incisions at right angles to the long axis of the muscle. The muscle then presents a (artificial) transverse section at each end and a longi- tudinal surface. We may speak of the latter as being divided into two equal parts by an imaginary transverse line on its surface 1 These (Fig. 11) consist essentially of a slip of thoroughly amalgamated zinc dipping into a saturated solution of zinc sulphate, which in turn is brought into connection with the nerve or muscle by means of a plug or bridge of china-clay moistened with normal sodium chloride solution ; it is important that the zinc should be thoroughly amalgamated. This form of electrodes gives rise to less polarisation than do simple platinum or copper electrodes. The clay affords a connection be- tween the zinc and the tissue which neither acts on the tissue nor is acted on by the tissue. Contact of any tissue with copper or platinum is in itself sufficient to de- velope a current. CHAP. IT.] THE CONTRACTILE TISSUES. 59 called the * equator/ containing all the points of the surface midway between the two ends. Fig. 12 is a diagrammatic representation of such a muscle, the line ah being the equator. In such a muscle the development of the muscle-currents is found to be as follows. The greatest deflection is observed when one electrode is placed FIG. 12. DIAGRAM ILLUSTRATING THE ELECTRIC CURRENTS OF NERVE AND MUSCLE. Being purely diagrammatic, it may serve for a piece either of nerve or of muscle, except that the currents at the transverse section cannot be shewn in a nerve. The arrows shew the direction of the current through the galvanometer. ab the equator. The strongest currents are those shewn by the dark lines, as from a, at equator, to x or to y at the cut ends. The current from a to c is weaker than from a to y, though both, as shewn by the arrows, have the same direction. A current is shewn from e, which is near the equator, to /, which is farther from the equator. The current (in muscle) from a point in the circumference to a point nearer the centre of the transverse section is shewn at gh. From a to & or from x to y there is no current, as indicated by the dotted lines. at the mid-point or equator of the muscle, and the other at either cut end ; and the deflection is of such a kind as to shew that posi- tive currents are continually passing from the equator through the galvanometer to the cut end, that is to say, the cut end is negative relatively to the equator. The currents outside the muscle may be considered as completed by currents in the muscle from the cut end to the equator. In the diagram Fig. 12, the arrows indicate the direction of the currents. If the one electrode be placed at the equator ab, the effect is the same at whichever of the two cut ends x or y the other is placed. If, one electrode remaining at the equator, the other be shifted from the cut end to a spot c nearer to the equator, the current continues to have the same direction, but is of less intensity in proportion to the nearness of the electrodes to each other. If the two electrodes be placed at unequal distances e and /, one on either side of the equator, there will be a feeble current from the one nearer the equator to the one farther off, and the current will be the feebler, the more nearly they are equidistant from the equator. 60 MUSCLE CURRENTS. [BOOK i. If they are quite equidistant, as for instance when one is placed on one cut end x, and the other on the other cut end y, there will be no current at all. If one electrode be placed at the circumference of the transverse section and the other at the centre of the transverse section, there will be a current through the galvanometer from the former to the latter; there will be a current of similar direction but of less intensity when one electrode is at the circumference g of the transverse section and the other at some point h nearer the centre of the transverse section. In fact, the points which are relatively most positive and most negative to each other are points on the equator and the two centres of the transverse sections ; and the intensity of the current between any two points will depend on the respective distances of those points from the equator and from the centre of the transverse section. Similar currents may be observed when the longitudinal surface is not the natural but an artificial one ; indeed they may be witnessed in even a piece of muscle provided it be of cylindrical shape and composed of parallel fibres. * These 'muscle-currents' are not mere transitory currents dis- appearing as soon as the circuit is closed; on the contrary they last a very considerable time. They must therefore be maintained by some changes going on in the muscle, by continued chemical action in fact. They disappear as the irritability of the muscle vanishes, and are connected with those nutritive, so-called vital changes which maintain the irritability of the muscle. Muscle-currents such as have just been described, may, we repeat, be observed in any cylindrical muscle suitably prepared, and similar currents, with variations which need not be discussed here, may be seen in muscles of irregular shape with obliquely or otherwise ar- ranged fibres. And du Bois-Reymond, to whom chiefly we are indebted for our knowledge of these currents, has been led to re- gard them as essential and important properties of living muscle. He has moreover advanced the theory that muscle may be con- sidered as composed of electro-motive particles or molecules, each of which like the muscle at large has a positive equator and negative ends, the whole muscle being made up of these molecules in somewhat the same way, (to use an illustration which must not however be strained or considered as an exact one) as a magnet may be supposed to be made up of magnetic particles each with its north and south pole. There are reasons however for thinking that these muscle-currents have no such fundamental origin, that they are in fact of surface and indeed of artificial origin. Without entering largely into the controversy on this question, the following important facts may be mentioned. 1. When a muscle is examined while it still retains untouched its natural tendinous terminations, the currents are much less than CHAP, ii.] THE CONTRACTILE TISSUES. 61 when artificial transverse sections have been made; the natural tendinous end is less negative than the cut surface. But the tendinous end becomes at once negative when it is dipped in water or acid, indeed when it is in any way injured. The less roughly in fact a muscle is treated the less evident are the muscle- currents, and it has been maintained that if adequate care be taken to maintain a muscle in an absolutely natural condition no such currents as those we have been describing exist at all. 2. Englemann has shewn that the surface of the uninjured in- active1 ventricle of the frog's heart is isoelectric, i. e. that no current is obtained when the electrodes are placed on any two points of the surface. If however any part of the surface be injured, or if the ventricle be cut across so as to expose a cut surface, the injured spot or the cut surface becomes at once most powerfully negative towards the uninjured surface, a strong current being developed which passes through the galvanometer from the uninjured surface to the cut surface or to the injured spot. The negativity thus developed in a cut surface passes off in the course of some hours, but may be restored by making a fresh cut and exposing a fresh surface. Now, when a muscle is cut or injured the substance of the fibres dies at the cut or injured surface. And many physiologists, among whom the most prominent is Hermann, have been led by the above and other facts to the conclusion that muscle-currents do not exist naturally in untouched muscles, that the muscular substance is naturally, when living, isoelectric, but that whenever a portion of the muscular substance dies, it becomes while dying negative to the living substance, and thus gives rise to currents. They explain the typical currents (as they might be called) manifested by a muscle with a natural longitudinal surface and artificial transverse sections, by the fact that the dying cut ends are negative relatively to the rest of the muscle. Du Bois-Reymond and those with him offer special explanations of the above facts and of other objections which have been urged against the theory of naturally existing electro-motive molecules. Into these we cannot enter here. We must rest content with the statement that in an ordinary muscle currents such as have been described may be witnessed, but that strong arguments may be adduced in favour of the view that these currents are not ' natural ' phenomena but essentially of artificial origin. It will therefore be best to speak of them as ' currents of rest/ Negative variation of the Muscle-current. The controversy whether the " currents of rest " observable in a muscle be of natural origin or not, does not affect the truth or the importance of the fact that an electrical change takes place in a muscle whenever it enters into a contraction. When currents of rest are observable in a muscle these are found to undergo a diminution at the onset of a 1 Th* necessity of its being inactive will be seen subsequently. 62 NEGATIVE VARIATION. [BOOK i. contraction, and this diminution is spoken of as 'the negative variation' of the currents of rest. The negative variation may be seen when a muscle is thrown into a single contraction, but is most readily shewn when the muscle is tetanized. Thus if a pair of electrodes be placed on a muscle, one at the equator, and the other at or near the transverse section, so that a considerable deflection of the galvanometer needle, indicating a considerable current of rest, be gained, the needle of the galvanometer will, when the muscle is tetanized by an interrupted current sent through its nerve (at a point too far from the muscle to allow any escape of the current into the electrodes connected with the galvanometer), swing back towards zero ; it returns to its original deflection when the tetanizing current is shut off. Not only may this negative variation be shewn by the galvano- meter, but it, as well as the current of rest, may be used as a galvanic shock and so employed to stimulate a muscle, as in the experiment known as ' the rheoscopic frog.' For this purpose the muscles and nerves need to be very irritable and in thoroughly good condition. Two muscle-nerve preparations A and B having been made and each placed on a glass plate for the sake of insulation, the nerve of the one B is allowed to fall on the muscle of the other A in such a way that one point of the nerve comes in contact with the equator of the muscle, and another point with one end of the muscle or with a point at some distance from the equator. At the moment the nerve is let fall and contact made, a current, viz. the 'current of rest' of the muscle A, passes through the nerve; this acts as a stimulus to the nerve, and so causes a contraction in the muscle connected with the nerve. Thus the muscle A acts as a battery, the completion of the circuit of which by means of the nerve of B serves as a stimulus, causing the muscle B to contract. If while the nerve of B is still in contact with the muscle of A, the nerve of the latter is tetanized with an interrupted current, not only is the muscle of A thrown into tetanus but also that of J5; the reason being as follows. At each spasm of which the tetanus of A is made up, there is a negative variation of the muscle-current of A. Each negative variation in the muscle- current of A serves as a stimulus to the nerve of B, and is hence the cause of a spasm in the muscle of B ; and the stimuli following each other rapidly, as being produced by the tetanus of A they must do, the spasms in B to which they give rise are also fused into a tetanus in B. B in fact contracts in harmony with A. This experiment shews that the negative variation accompanying the tetanus of a muscle, though it causes only a single swing of the galvanometer, is really made up of a series of negative variations, each single negative variation corresponding to the single spasms of which the tetanus is made up. But an electrical change may be manifested even in cases when CHAP, ii.] THE CONTRACTILE TISSUES. 63 no currents of rest exist. We have stated (p. 61) that the surface of the uninjured inactive ventricle of the frog's heart is isoelectric, no currents being observed when the electrodes of a galvanometer are placed on two points of the surface. Nevertheless a most distinct current is developed whenever the ventricle contracts. This may be shewn either by the galvanometer or by the rheos- copic frog. If the nerve of an irritable muscle-nerve preparation be laid over a pulsating ventricle, each beat is responded to by a spasm of the muscle of the preparation. In the case of ordinary muscles too instances occur in which it seems impossible to regard the electrical change manifested during the contraction as the mere diminution of a preexisting current. Accordingly Hermann and those who with him deny the existence of 'natural' muscle-currents speak of a muscle as de- veloping during a contraction a ' current of action,' occasioned as they believe by the muscular substance as it is entering into the state of contraction becoming negative towards the muscular substance which is still at rest, or has returned to a state of rest. In fact, they regard the negativity of muscular substance as characteristic alike of beginning death and of a beginning contraction. So that in a muscular contraction a wave of negativity, starting from the end-plate when indirect, or from the point stimulated when direct stimulation is used, passes along the muscular substance to the ends or end of the fibre. We cannot however enter more fully here into a discussion of this difficult subject. Whichever view be taken of the nature of these muscle-currents, and of the electric change during contraction, whether we regard that change as a ' negative variation ' or as a ' current of action,' it is important to remember that it takes place entirely during the latent period. It is not in any way the result of the change of form, it is the forerunner of that change of form. Just as a nervous impulse passes down the nerve to the muscle without any visible changes, so a molecular change of some kind, unattended by any visible events, known to us, at present, only by an electrical change, runs along the muscular fibre from the end-plates to the terminations of the fibre, preparing the way for the visible change of form which is to follow. This molecular invisible change is the work of the latent period, and careful observations have shewn that it, like the visible contraction which follows at its heels, travels along the fibre from a spot stimulated towards the ends of the fibres, in the form of a wave having about the same velocity as the contrac- tion, viz. about 3 metres a second1. 1 In the muscles of the frog; but as we have seen having probably a higher velocity in the intact mammalian muscles, within the living body, and varying according to circumstances. 64 CHEMICAL CHANGES. [BOOK i. Chemical Changes. Before we attack the important problem, What are the chemical changes concerned in a muscular contraction? we must study in some detail the chemical features of muscle at rest. And here we are brought face to face with the chemical differences between living and dead muscles. All muscles, within a certain time after removal from the body, or while still within the body, after 'general' death of the body, lose their irritability. The loss of irritability, even when rapid, is gradual, but is succeeded by an "^event which is somewhat more sudden, viz. the entrance into the condition known as rigor mortis, the occurrence of which is marked by the following features. The muscle, previously possessing a r certain translucency, becomes much more opaque. Previously very extensible and elastic, it becomes much less extensible and at the same time loses its elasticity; the muscle now requires considerable force to stretch it, and when the force is removed, does not, as before, return to its natural length. To the touch it has lost much of its former softness, and becomes firmer and more resistent. The entrance into rigor mortis is characterised by a shortening or con- traction, which may, under certain circumstances, be considerable. The energy of this contraction is not great, so that when opposed, no actual shortening takes place. When rigor mortis has been fully developed, no muscle-currents whatever are observed. The onset of this rigidity may be considered as the token of the death of the muscle itself. As we shall see, the chemical features of the dead rigid muscle are strikingly different from those of the living muscle. If a dead muscle, from which all fat, tendon, fascia, and con- nective tissue have been as much as possible removed, and which has been freed from blood by the injection of saline solution, be minced and repeatedly washed with water, the washings will contain certain forms of albumin and certain extractive bodies, of which we shall speak directly. When the washing has been continued until the wash-water gives no proteid reaction, a large portion of muscle will still remain undissolved. If this be treated with a 10 p. c. solution of a neutral salt, ammonium chloride being the best, a large portion of it will become imperfectly dissolved into a viscid fluid which filters with difficulty. If the viscid filtrate be allowed to fall drop by drop into a large quantity of distilled water, a white flocculent matter will be precipitated. This flocculent precipitate is myosin. It is a proteid, giving the ordinary proteid reactions, and having the same general elementary composition as other proteids. It is soluble in dilute saline solutions, especially those of ammonium chloride, and may be classed in the globulin family, though it is not so soluble as paraglobulin. Dissolved in saline solutions it readily coagulates when heated, i.'e. CHAP. IL] THE CONTRACTILE TISSUES. 65 is converted into coagulated proteid1, and it is worthy of notice that it coagulates at a lower temperature, viz. 55° — 60° C., than does serum-albumin, paraglobulin and many other proteids ; it is precipitated and after long action coagulated by alcohol, and is precipitated by an excess of sodium chloride. By the action of dilute acids it is very readily converted into what is called syntonin or acid-albumin2, by the action of dilute alkalis into alkali-albumin. Speaking generally it may be said to be inter- mediate in its character between fibrin and globulin. On keeping, and especially on drying, its solubility is much diminished. Of the substances which are left in washed muscle, from which the myosin has thus been extracted by ammonium chloride solution, little is known. If washed muscle be treated directly with dilute hydrochloric acid, the greater part of the material of the muscle passes at once into syntonin. The quantity of syntonin thus obtained may be taken as representing the quantity of myosin previously existing in the muscle. The portion insoluble in dilute hydrochloric acid consists in part of the substance of the sarco- lemma, of the nuclei, and of the tissue between the bundles, and in part probably of certain structural elements of the fibres themselves. If living contractile frog's muscle, freed as much as possible from blood, be frozen3, and while frozen, minced, and rubbed up in a mortar with four times its weight of snow containing 1 p. c. of sodium chloride, a mixture is obtained which at a temperature just below 0° C. is sufficiently fluid to be filtered, though with difficulty. The slightly opalescent filtrate, or muscle- plasma as it is called, is at first quite fluid, but will when exposed to the ordinary temperature become a solid jelly, and afterwards separate into a clot and serum. It will in fact coagulate like blood-plasma, with this difference, that the clot is not firm and fibrillar, but loose, granular and flocculent. During the coagulation the fluid, which before was neutral or slightly alkaline, becomes distinctly acid. The clot is myosin. It gives all the reactions of myosin obtained from dead muscle. The serum contains ordinary serum-albumin, one or more pe- culiar proteids4 coagulating at a lower temperature than does serum- albumin, and extractives. Such muscles as are red also contain a small quantity of haemoglobin, to which indeed their redness is due. Thus while dead muscle contains myosin, serum-albumin, and other proteids and extractives with certain insoluble matters and certain gelatinous elements not referable to the muscle-substance 1 See Appendix. 2 Ibid. 3 Since, as we shall presently see, a muscle may be frozen and thawed again without losing any of its vital powers, we are at liberty to regard the frozen muscle as a still living muscle. 4 See Appendix. F. 5 66 RIGOR MORTIS. [BOOK i. [itself, living muscle contains no myosin, but some substance or (substances which bear somewhat the same relation to myosin that (the fibrin factors do to fibrin, and which give rise to myosin upon (the death of the muscle. "We may in fact speak of rigor mortis as characterised by a coagulation of the muscle-plasma, comparable to the coagulation of 'blood-plasma, but differing from it inasmuch as the product is not fibrin but myosin. The rigidity, the loss of suppleness, and the diminished translucency appear to be at all events largely, though probably not wholly, due to the change from the fluid plasma to the solid myosin. We might compare a living muscle to a 'number of fine transparent membranous tubes containing blood-plasma. When this blood-plasma entered into the 'jelly' stage of coagulation, the system of tubes would present many of the phenomena of rigor mortis. They would lose much of their suppleness and translucency, and acquire a certain amount of rigidity. There is however one very marked and important difference between rigor mortis of muscle and the coagulation of blood : blood •during its coagulation undergoes only a slight change in its reaction ; Ibut muscle during the onset of rigor mortis becomes distinctly acid. A living muscle at rest is in reaction neutral, or, possibly from some remains of lymph adhering to it, faintly alkaline. If on the other hand the reaction of a thoroughly rigid muscle be tested, it will be found to be most distinctly acid. This development of an acid reaction is witnessed not only in the solid untouched fibre but also in expressed muscle-plasma ; it seems to be associated in some way with the appearance of the myosin. The exact causation of this acid reaction has not at present been clearly worked out. Since the coloration of the litmus pro- duced is permanent, carbonic acid, which as we shall immediately state, is set free at the same time, cannot be regarded as the active acid, for the reddening of litmus produced by carbonic acid speedily disappears on exposure. On the other hand it is possible to ex- tract from rigid muscle a certain quantity of lactic acid, or rather of a variety of lactic acid known as sarcolactic acid1; and it has been thought that the appearance of the acid reaction of rigid muscle is due to a new formation or to an increased formation of this sarcolactic acid. But there is considerable doubt whether any such increase of sarcolactic acid does actually take place in rigor mortis. Hence though there can be no doubt that an acid reaction is established, we are not yet in a position to affirm positively the exact manner in which that reaction is produced, the complex nature of the muscular substance suggesting to the chemist several ways in which it might come about. Coincident with the appearance of this acid reaction, though as we have said, not the direct cause of it, a large development of carbonic acid takes place when muscle becomes rigid. Irritable 1 Bee Appendix. CHAP, ii.] THE CONTRACTILE TISSUES. 67 living muscular substance like all living protoplasm is continually respiring, continually consuming oxygen and giving out carbonic acid. In the body, the arterial blood going to the muscle gives up some of its oxygen, and gains a quantity of carbonic acid, thus becoming venous as it passes through the muscular capillaries. Even after removal from the body, the living muscle continues to take up from the surrounding atmosphere a certain quantity of oxygen and to give out a certain quantity of carbonic acid. At the onset of rigor mortis there is a very large and sudden! increase in this production of carbonic acid, in fact an outburst as itl were of that gas. This is a phenomenon deserving special attention.* Knowing that the carbonic acid which is the outcome of the res- piration of the whole body is the result of the oxidation of carbon- holding subtances, we might very naturally suppose that the in- creased production of carbonic acid attendant on the development of rigor mortis is due to the fact that during that event a certain quantity of the carbon-holding constituents of the muscle are suddenly oxidized. But such a view is negatived by the following facts. In the first place, the increased production of carbonic acid during rigor mortis is not accompanied by any corresponding in- crease in the consumption of oxygen. In the second place, a muscle (of a frog for instance) contains in itself no free or loosely attached oxygen : when subjected to the action of a mercurial air- pump it gives off no oxygen to a vacuum, offering in this respect a marked contrast to blood ; and yet, when placed in an atmosphere free from oxygen, it will not only continue to give off carbonic acid while it remains alive, but will also exhibit at the onset of rigor mortis, the same increased production of carbonic acid that is shewn by a muscle placed in an atmosphere containing oxygen. It is obvious that in such a case the carbonic acid does not arise from the direct oxidation of the muscle substance, for there is no oxygen present at the time to carry on that oxidation. We are driven to suppose that during rigor mortis, some complex body, containing in itself ready formed carbonic acid so to speak, is split up, and thus carbonic acid is set free, the process of oxidation by which that carbonic acid was formed out of the carbon-holding constituents of the muscle having taken place at some anterior date. Living resting muscle then, is alkaline or neutral in reaction, and the substance of its fibres contains a coagulable plasma. Dead rigid muscle on the other hand is acid in reaction, and no longer contains a coagulable plasma, but is laden with the solid myosin. Further, the change from the living irritable condition to that of rigor mortis is accompanied by a large and sudden development of carbonic acid. It is found moreover that there is a certain amount of parallel- ism between the intensity of the rigor mortis, the degree of acid reaction and the quantity of carbonic acid given out. If we suppose, as we fairly may do, that the intensity of the rigidity is 5—2 68 CHEMICAL CHANGES. [BOOK i. dependent on the quantity of myosin deposited in the fibres, and the acid reaction to the development if not of lactic acid, at least of some other substance, the parallelism between the three products, myosin, acid-producing substance, and carbonic acid, would suggest the idea that all three are the results of the splitting-up of the same highly complex substance. But we have not at present succeeded in isolating or in otherwise definitely proving the exist- ence of such a body, and though the idea seems tempting, it may in the end prove totally erroneous. We may now return to the question, What are the chemical changes which take place when a living resting muscle enters into a contraction? These changes are most evident after the muscle has been subjected to a prolonged tetanus ; but there can be no doubt that the chemical events of a tetanus are, like the physical events, simply the sum of the results of the constituent single contractions. In the first place, the muscle becomes acid, not so acid as in rigor mortis, but still sufficiently so, after a vigorous tetanus, to turn blue litmus distinctly red. The cause of the acid reaction like that of rigor mortis is doubtful ; but is in all probability the same in both cases. In the second place, a considerable quantity of carbonic acid is set free ; and the production of carbonic acid in muscular contrac- tion is altogether similar to the production of carbonic acid during rigor mortis. It is not accompanied by any corresponding increase in the consumption of oxygen. This is evident even in a muscle through which the circulation of blood is still going on, for though the blood passing through a contracting muscle gives up more oxygen than the blood passing through a resting muscle, the increase in the amount of oxygen taken up falls below the increase in the carbonic acid given out ; but it is still more markedly shewn in a muscle removed from the body. For in such a muscle both the contraction and the increase in the production of carbonic acid will go on in the absence of oxygen. A frog's muscle suspended in an atmosphere of nitrogen will remain irritable for some considerable time, and at each vigorous tetanus an increase in the production of carbonic acid may be readily ascertained. Moreover there seems to be a correspondence between the energy of the contraction and the amount of carbonic acid and the degree of acid reaction produced, so that, though we are now treading on somewhat uncertain ground, we are naturally led to the view that the essential chemical process lying at the bottom of a muscular contraction as of rigor mortis is the splitting up of some highly complex substance. But here the resemblance between rigor mortis and contraction ends. We have no evidence of the formation jiuring a contraction of any body like myosin. Now the contracted and rigid muscle differ essentially in the fact that while the former, as compared with living resting muscle, increases in extensibility and CHAP. IL] THE CONTRACTILE TISSUES. 69 loses none of its translucency, the latter becomes less extensible, less elastic, and less translucent. Corresponding to this marked differ- ence, we find myosin formed in the rigid muscle, but we cannot find it in the contracted muscle. The other chemical changes in muscle during a contraction have not yet been clearly made out. Indeed our whole information concerning the other chemical constituents of muscle is at present imperfect. The bodies which we have called extractives are numerous and varied. Among the nitrogenous crystalline extractives the most important is kreatin, which occurs to the extent of about '2 to •3 p. c., is an invariable constituent of muscle, and is found elsewhere only in nervous tissue, the kidney, and to a slight extent in the blood. As we shall hereafter see, great interest is attached tot this body inasmuch as it readily splits up into urea, and sarcosin, » and accordingly has been regarded as one at least of the antecedents ? of urea, which body is conspicuous by its absence from muscular \ tissue. The alkaline kreatinin into which kreatin is converted by the action of acids, and which appears in the urine, is apparently absent from muscle. The other nitrogenous crystalline bodies, which need not detain us now, are karnin, hypoxanthin (or sarkin), xanthin, inosinic acid, taurin and possibly uric acid1. Fats are present in considerable quantities both in the adipose tissue between the bundles of fibres and also as constituents of the muscular substance within the sarcolemma. The peculiar starch-like body, glycogen, of which we shall have to speak more fully in a later part of this work, is especially abundant in the muscles of the embryo at an early period, and besides, is so continually met with in the muscles of the adult that it may fairly be considered as a normal constituent of muscle to a variable extent, possibly from '5 to 1 p. c. A dextrin-like body has also been found, and at times glucose or an allied sugar. The cardiac muscular tissue contains the peculiar sugar, inosit. The ashes of muscle, like those of the red corpuscles, are cha-J racterised by the preponderance of potassium salts and of phos-j phates ; these form in fact nearly 80 p. c. of the whole ash. The general composition of human muscle is shewn in the following table of v. Bibra. Water 744'5 Solids Myosin and other matters, elastic ele- ments, &c., insoluble in water ... 155*4 Soluble proteids 19'3 Gelatin 207 Extractives and Salts 37'1 Fats 23-0 255-5 1 See Appendix. 70 THERMAL CHANGES. [BOOK i. Concerning the functional importance of these various bodies we have very little exact knowledge. Helmholtz shewed long ago that the effect of long continued contraction is to diminish the substances in muscle which are soluble in water, but to increase those which are soluble in alcohol. In other words, during contraction some substance or substances soluble in water are converted into another or other substances insoluble in water but soluble in alcohol. During or after rigor mortis, glycogen is converted into sugar, and it has been contended that a similar change takes place during contraction; but we are not, at present at all events, in a position to affirm that such a conversion is a necessary and integral part of the chemical transformations which lie at the bottom of a muscular contraction. We shall have occasion to treat more fully and from a different point of view, of the relations between muscular exercise and the quantity of urea discharged by the kidneys. Meanwhile we may state that not only does this all-important nitrogenous crystalline body appear to be absent from normal muscle, both during rest and after contraction, but we have as yet no adequate evidence that the contraction of a muscle is followed by the appearance in the substance of the muscle or in the blood passing through it of any new nitrogenous product, or by any increase in any of the nitrogenous extractives which we have mentioned as normally present in muscle. In fact all we know at present is that a contraction is followed by an increase in the discharge of carbonic acid, and by certain changes which lead to an acid reaction. Beyond this we are in the dark. Thermal Changes. The view however that chemical changes lie at the bottom of a muscular contraction, that the energy which takes on the form of muscular work arises from a metabolism of the muscular substance, is supported by a variety of considerations and especially perhaps by the fact, that the development of energy as muscular work, is accompanied by a development of energy as heat. Though we shall have hereafter to treat this subject more fully, the leading facts may be given here. Whenever a muscle contracts, its temperature rises, indicating that heat is given out. When a mercury thermometer is plunged into a mass of muscles, such as those of the thigh of the dog, a rise of the mercury is observed upon the muscles being thrown into a prolonged contraction. More exact results however are obtained by means of a thermopile, by the help of which the rise of temperature caused by a few repeated single contractions, or indeed by a single contraction, may be observed and the amount of heat given out approximative^ measured. CHAP, ii.] THE CONTRACTILE TISSUES. 71 The thermopile may consist either of a single junction in the form of a needle plunged into the substance of the muscle ; or of several junctions either in the shape of a flat surface carefully opposed to the surface of muscle (Heidenhain) the pile being balanced so as to move with the con- tracting muscle, and thus to keep the contact exact ; or in the shape of a thin wedge (Fick) the edge of which comprising the actual junctions is thrust into a mass of muscles and held in position by them. In all cases the fellow junction or junctions must be kept at a constant temperature. Fick calculated that the greatest heat given out by the muscles of the thigh of a frog in a single contraction was 3*1 micro-units of heat l for a gramme of muscle, the result being obtained by dividing by five the total amount of heat given out in five successive single contractions. It will however be safer to regard these figures as illustrative of the fact that the heat given out is considerable rather than as data for elaborate calculations. Moreover we have no satisfactory quantitative determinations of the heat given out by the muscles of warm-blooded animals, though there can be no doubt that it is much greater than that given out by the muscles of the frog. There can hardly be any doubt that the heat thus set free is' the product of chemical changes within the muscle, changes, which though they cannot for the reasons given above be regarded as simple and direct oxidations, may be spoken of in general terms as a combustion. So that the muscle may be likened to a steam- engine, in which the combustion of a certain amount of material gives rise to the development of energy in two forms, as heat and as movement, there being certain quantitative relations between the amount of energy set free as heat and that giving rise to move- ment. We must however carefully guard ourselves against pressing this analogy too closely. In the steam-engine, we can distinguish clearly between the fuel which through its combustion is the sole source of energy, and the machinery, which is not consumed to provide energy and only suffers wear and tear. In the muscle we can make no such distinction ; though the whole matter is not fully worked out, we have reason to think that the muscular fibre is not to be regarded as a machine which takes so to speak a charge of certain substances from the blood, and by inducing an explosion of these substances in itself gives rise to the energy of heat and movement. On the contrary the evidence goes to shew that it is the living contractile substance as a whole which is continually breaking down in an explosive decomposition and as continually building itself up again out of the material supplied by the blood. In a steam-engine only a certain amount of the total potential energy of the fuel issues as work, the rest being lost as heat, the proportion varying, but the work rarely exceeding one-tenth of the total energy. In the case of the muscle we are not at present in a position to draw up an exact equation between the latent energy 1 The micro- unit being a milligramme of water raised one degree centigrade. 72 CHANGES DURING A NERVOUS IMPULSE. [BOOK i. on the one hand and the two forms of actual energy on the other. "We have reason to think that the proportion between heat and work varies considerably under different circumstances, the work sometimes rising as high as one-fourth, sometimes possibly sink- ing as low as one twenty-fourth of the total energy, and obser- vations seem to shew that the greater the resistance which the muscle has to overcome, the larger the proportion of the total energy expended which goes out as work done. The muscle in fact seems to be so far self-regulating, that the more work it has to do, the greater, within certain limits, is the economy with which it works. Lastly it must be remembered that the giving out of heat by the muscle is not confined to the occasions when it is actually con- tracting. When, at a later period, we treat of the heat of the body generally, evidence will be brought forward that the muscles even when at rest are giving rise to heat, so that the heat given out at a contraction is not some wholly new phenomenon, but a temporary exaggeration of what is going on continually, at a more feeble rate. The Changes in a Nerve during the passage of a Nervous Impulse. The change in the form of a muscle during its contraction is a thing which can be seen and felt; but the changes in a nerve during its activity are invisible and impalpable. We stimulate one end of a nerve, and since we see this followed by a contraction of the muscle attached to the other end, we know that some changes or other, constituting a nervous impulse, have been propagated along the nerve ; but these are changes which we cannot see. Nor have we satisfactory evidence of any chemical events or of any pro- duction of heat, accompanying a nervous impulse. We may fairly suppose that some chemical changes form the basis of a nervous impulse, and that these changes set free a certain amount of heat ; but these if they occur are too slight to be recognized satisfactorily by the means at present at our disposal. In fact, beyond the terminal results, such as a muscular contraction in the case of a nerve going to a muscle, or some affection of the central nervous system in the case of a nerve still in connection with its nervous centre, there is one event and one event only which we are able to recognize as the objective token of a nervous impulse, and that is the so-called negative variation of the nerve- current. For a piece of nerve removed from the body exhibits nearly the same electric phenomena as a piece of muscle. It has an equator which is electrically positive as compared to its two cut ends. In fact the diagram Fig. 12, and the description which it was used on p. 59 to illustrate, may be applied to nerve as well as CHAP. IL] THE CONTRACTILE TISSUES. 73 to muscle, except that the currents are in all cases much more feeble in the case of nerves than of muscles, and the special currents from the circumference to the centre of the transverse sections cannot well be shewn in a slender nerve; indeed it is doubtful if they exist at all. During the passage of a nervous impulse the ' natural nerve- \ current' undergoes a negative variation, just as the 'natural muscle- current' undergoes a negative variation during a contraction. There are however difficulties in the case of the nerve similar to those in the case of the muscle, concerning the pre-existence of any such 'natural' currents. It is maintained by many that a nerve in an absolutely natural condition is like a muscle, iso-electric ; hence we may say that in a nerve during the passage of a nervous impulse, as in a muscle during a muscular contraction, a ' current of action ' is developed. This ' current of action ' or ' negative variation ' may be shewn either by the galvanometer or by the rheoscopic frog. If the nerve of the 'muscle-nerve preparation' B (see p. 62) be placed in an appropriate manner on a thoroughly irritable nerve A (to which of course no muscle need be attached), i.e. touching say the equator and one end of the nerve, then single induction-shocks sent into the far end of A will cause single spasms in the muscle of B, while tetanization of A, i.e. rapidly repeated shocks sent into A, will cause tetanus of the muscle of B. That this current, whether it be regarded as an independent 4 current of action or as a negative variation of a ' pre-existing ' current, is an essential feature of a nervous impulse is shewn by the fact that the degree or intensity of the one varies with that of the other. They both travel too at the same rate. In describing the muscle-curve, and the method of measuring the muscular latent period, we have incidentally shewn (p. 47) how the velocity of the nervous impulse is measured also, and stated that the rate in the nerves of a frog is about 28 metres a second. Bernstein by means of a special and somewhat complicated apparatus finds that the current of action travels along an isolated piece of nerve at the same rate. He also finds that it, like the molecular change in a muscle preceding the contraction, and indeed like the contraction itself, passes over any given spot of the nerve in the form of a wave, rising rapidly to a maximum and then more gradually declining again. He has been able to measure tne length of the wave, and this he finds to be about 18 mm., taking *0007 sec. to pass over any one point. When an isolated piece of nerve is stimulated in the middle, the current of action is propagated equally well in both directions, and that whether the nerve be a chiefly sensory or a chiefly motor nerve, or indeed if it be a nerve-root composed exclusively of motor or of sensory fibres. Taking the current of action as the token of a nervous impulse, we infer from this that when a nerve-fibre is 74 CHANGES DURING A NERVOUS IMPULSE. [BOOK i. stimulated artificially at any part of its course, the nervous impulse set going travels in both directions. We used just now the phrase ' tetanization of a nerve/ meaning the application to a nerve of rapidly repeated shocks such as would produce tetanus in the muscle to which the nerve was attached, and we shall have frequent occasion to employ the phrase. It will however of course be understood that there is in the nerve as far as we know no summation of nervous impulses comparable to the summation of muscular contractions. The matter perhaps needs fuller investigation, but as far as we know at present, we may say that the series of shocks sent in at the far end of the nerve start a series of impulses; these travel down the nerve and reach the muscle as a series of distinct impulses; and the first changes in the muscle, the molecular latent-period changes, also form a series the members of which are distinct. It is not until these molecular changes become transformed into visible changes of form that any fusion or summation takes place. Putting together the facts contained in this and the preceding sections, the following may be taken as a brief approximate history of what takes place in a muscle and nerve when the latter is subjected to a single induction-shock. At the instant that the induced current passes into the nerve, changes occur, of whose nature we know nothing certain except that they cause a ' current |of action' or 'negative variation of the natural' nerve-current. These changes propagate themselves along the nerve in both directions as a nervous impulse in the form of a wave, having a wave-length of about 18 mm., and a velocity (in frog's nerve) of about 28 m. per sec. Passing down the nerve-fibres to the muscle, flowing along the branching and narrowing tracts, the wave at last breaks on the end-plates of the fibres of the muscle. Here it is transmuted into a muscle-impulse, with a shorter steeper wave, and a greatly diminished velocity (about 3m. per sec.). This muscle-impulse, of which we know hardly more than that it :is marked by a current of action, travels from each end-plate in both directions to the end of the fibre, where it appears to be lost, at all events we do not know what becomes of it. As it leaves the end plate it is followed by an explosive decomposition of material, leading to a discharge of carbonic acid, to the appearance of some substance or substances with an acid reaction, and probably of other unknown things, with a considerable development of heat. This explosive decomposition gives rise to the visible contraction- wave, which travels behind the invisible muscle-impulse at about the same rate, but with a vastly increased wave-length. The fibre, as the wave passes over it, swells and shortens, bringing its two ends nearer together, its molecules during the change of form arranging themselves in such a way that the extensibility of the fibre is increased. SEC. 3. THE NATURE OF THE CHANGES THROUGH WHICH AN ELECTRIC CURRENT IS ABLE TO GENE- RATE A NERVOUS IMPULSE. Action of the Constant Current. In the preceding account, the stimulus applied in order to give rise to a nervous impulse has always been supposed to be an induction shock, single or repeated. This choice of stimulus has been made on account of the almost momentary duration of the induced current. Had we used a current lasting for some consider- able time, the problems before us would have become more com- plex in consequence of our having to distinguish between the events taking place while the current was passing through the nerve from those which occurred at the moment when the current was thrown into the nerve or at the moment when it was shut off from the nerve. These complications do arise when instead of employing the induced current as a stimulus, we use a constant current, i.e. when we pass through the nerve (or muscle) a current direct from the battery without the intervention of any induction- coil. Before making the actual experiment, we might perhaps naturally suppose that the constant current would act as a stimulus throughout the whole time during which it was applied, that, so long as the current passed along the nerve, nervous impulses would be generated and thus the muscle thrown into something at all events like tetanus. And under certain conditions this does take place ; occasionally it happens that at the moment the current is thrown into the nerve, the muscle of the muscle- nerve preparation falls into a tetanus which is continued until the current is shut off. But such a result is exceptional. In the vast 76 ACTION OF THE CONSTANT CURRENT. [BOOK i. majority of cases what happens is as follows. At the moment that the circuit is made, the moment that the current is thrown into the nerve, a single spasm, a simple contraction, the so-called making contraction, is witnessed ; but after this has passed away the muscle remains absolutely quiescent in spite of the current continuing to pass through the nerve, and this quiescence is maintained until the circuit is broken, until the current is shut off from the nerve, when another simple contraction, the so- called breaking contraction, is observed. The mere passage of a constant current of uniform intensity through a nerve does not under ordinary circumstances act as a stimulus generating a nervous impulse ; such an impulse is only set up when the current either falls into or is shut off from the nerve. It is the entrance or the exit of the current, and not the continuance of the current, which is the stimulus. The quiescence of the nerve and muscle during the passage of the current is however dependent on the current remaining uniform in intensity or at least not being suddenly increased or diminished. Any sufficiently sudden and large increase or diminution of the intensity of the current, will act like the entrance or exit of a current, and by generating nervous impulses give rise to contractions. If the intensity of the current however be very slowly and gradually increased or diminished, a very wide range of intensity may be passed through without any contraction being seen. It is the sudden change from one condition to another, and not the condition itself, which causes the nervous impulse. In many cases, both a ' making ' and a ' breaking ' contraction, each a simple spasm, are observed, and this is perhaps the commonest event ; but when the current is very weak, and again when the current is very strong either the breaking or the making contraction may be absent, i.e. there may be a contraction only when the current is thrown into the nerve or only when it is shut off from the nerve. Under ordinary circumstances the contractions witnessed with the constant current either at the make or at the break, are of the nature of a ' simple ' contraction, but, as has already been said, the application of the current may give rise to a very pronounced tetanus. Such a tetanus is seen sometimes when the current is made, lasting during the application of the current, sometimes when the current is broken, lasting some time after the current has been wholly removed from the nerve. The former is spoken of as a ' making/ the latter as a ' breaking ' tetanus. But these excep- tional results of the constant current need not detain us now. The great interest attached to the action of the constant current lies in the fact, that during the passage of the current, in spite of the absence of all nervous impulses and therefore of all muscular contractions, the nerve is for the time both between and on each side of the electrodes profoundly modified in a most CHAP. IL] THE CONTRACTILE TISSUES. 77 peculiar manner. This modification, important both for the light it throws on the generation of nervous impulses and for its practical applications, is known under the name of electrotonus. Electrotonus. .The marked feature of the electrotonic con- dition is that the nerve though apparently quiescent is changed in respect to its irritability; and that in a different way in the neighbourhood of the two electrodes respectively. Suppose that on the nerve of a muscle-nerve preparation are placed two (non-polarizable) electrodes (Fig. 13, a, Ic) connected with a battery and arranged with a key so that a constant current can at pleasure be thrown into or shut off from the nerve. This constant current, whose effects we are about to study, may be called the f polarizing current.' Let a be the positive electrode or anode, and k the negative electrode or kathode, both placed at some distance from the muscle, and also with a certain interval between each other. At the point x let there be applied a pair of electrodes connected with an induction-machine. Let the muscle farther be connected with a lever, so that its contractions can be recorded, and their amount measured. Before the polarizing current is thrown into the nerve, let a single induction-shock of known intensity (a weak one being chosen, or at least not one which would cause in the muscle a maximum contraction) be thrown in at a;. A contraction of a certain amount will follow. B. FIG. 13. MUSCLE-NERVE PREPARATIONS, with the nerve exposed in A to a descending and in B to an ascending constant current. In each a is the anode, k the kathode of the constant current, x represents the spot where the induction-shocks used to test the irritability of the nerve are sent in. That contraction may be taken as a measure of the irritability of the nerve at the point x. Now let the polarizing current be thrown in, and let the direction of the current be a descending one, with the kathode or negative pole nearest the muscle, 78 ELECTROTONUS. [BOOK i. as in Fig. 13^1. If while the current is passing, the same induction-shock as before be sent through x, the contraction which results will be found to be greater than on the former occasion. If the polarizing current be shut off, and the point x after a short interval again tested with the same induction-shock, the contraction will be no longer greater, but of the same amount, or perhaps not so great, as at first. During the passage of the polarizing current, therefore, the irritability of the nerve at the point x has been temporarily increased, since the same shock applied to it causes a greater contraction during the presence than in the absence of the current. But this is only true so long as the polarizing current is a descending one, so long as the point x lies on the side of the kathode. On the other hand, if the polarizing current had been an ascending one, with the anode or positive pole nearest the muscle, as in Fig. 135, the irritability of the nerve at x would have been found to be diminished instead of increased by the polarizing current. That is to say, when a constant current is applied to a nerve, the irritability of the nerve between the polar- izing electrodes and the muscle is, during the passage of the current, increased when the kathode is nearest the muscle (and the polar- izing current descending) and diminished when the anode is nearest the muscle (and the polarizing current ascending). The same result, mutatis mutandis, and with some qualifications which we need not discuss, would be gained if x were placed not between the muscle and the polarizing current, but on the far side of the latter. Hence it may be stated generally that during the passage of a constant current through a nerve the irritability of the nerve is increased in the region of the kathode, and diminished in the region of the anode. The changes in the nerve which give rise to this increase of irritability in the region of the kathode are spoken of as katelectrotonus, and the nerve is said to be in a katelectrotonic condition. Similarly the changes in the region of the anode are spoken of as anelectrotonus, and the nerve is said to be in an anelectrotonic condition. It is also often usual to speak of the katelectrotonic increase, and anelectrotonic decrease of irritability. This law remains true whatever be the mode adopted for determining the irritability. The result holds good not only with a single induction-shock, but also with a tetanizing inter- rupted current, with chemical and with mechanical stimuli. It further appears to hold good not only in a dissected nerve-muscle preparation but also in the intact nerves of the living body. The increase and decrease of irritability are most marked in the immediate neighbourhood of the electrodes, but spread for a considerable distance in either direction in the extrapolar regions. The same modification is not confined to the extrapolar region, but exists also in the intrapolar region. In the intrapolar region there must be of course an indifferent point, where the katelectro- CHAP, ii.] THE CONTRACTILE TISSUES. 79 tonic increase merges into the anelectrotonic decrease, and where therefore the irritability is unchanged. When the polarizing current is a weak one, this indifferent point is nearer the anode than the kathode, but as the polarizing current increases in intensity, draws nearer and nearer the kathode (see Fig. 14). The amount of increase and decrease is dependent : (1) On the strength of the current, the stronger current up to a certain limit producing the greater effect. (2) On the irritability of the nerve, the more irritable, better conditioned nerve being the more affected by a current of the same intensity. In the experiments just described the increase or decrease of irritability is taken to mean that the same stimulus starts in the one case a larger or more powerful and in the other case a smaller or less energetic impulse ; but we have reason to think that the mere propagation or conduction of impulses started elsewhere is affected by the electrotonic condition. At all events anelectrotonus appears to offer an obstacle to the passage of a nervous impulse. These variations of irritability at the kathode and anode respec- tively must be the result of molecular changes, brought about by the action of the constant current. They are interesting theoreti- cally because they shew that the generation of a nervous impulse as the result of the making or breaking of a constant current is dependent on the change of a nerve from its normal condition into either katelectrotonus or anelectrotonus, or back again from one of these phases into its normal condition. And certain results as to the occurrence or absence of a contraction at the make or at the break, according as the current is strong or weak, ascending, or descending (results which need not detain us here but which have been formulated as the co-called "law of contraction") FIG. 14. DIAGRAM ILLUSTRATING THE VARIATIONS OF IRRITABILITY DURING ELECTRO- TONUS, WITH POLARIZING CURRENTS OF INCREASING INTENSITY (from Pfliiger). The anode is supposed to be placed at A, the kathode at B ; AB is consequently the intrapolar district. In each of the three curves, the portion of the curve below the base line represents diminished irritability, that above, increased irritability. 2/j represents the effect of a weak current; the indifferent point xl is near the anode A. In yv a stronger current, the indifferent point x^ is nearer the kathode B, the diminution of irritability in anelectrotonus and the increase in katelectro- tonus being greater than in yl ; the effect also spreads for a greater distance along the extrapolar regions in both directions. In */3 the same events are seen to be still more marked. 80 ELECT ROTONIG CURRENTS. [BOOK i. go far to shew that a nervous impulse is generated only when a nerve passes suddenly from a normal condition into the phase of katelectrotonus (making contraction) or returns from the phase of anelectrotonus to a normal condition (breaking contraction), in other words, when it passes suddenly from a phase of lower to a phase of higher irritability. The phenomena of electrotonus are also interesting practically in as much as they shew that in the constant current appropriately applied we have the means of changing at will the irritability of this or that nerve, decreasing it when we wish to lessen pain or spasm, increasing it when we wish to heighten sensibility or muscular action. For the increase or decrease is observed in the case of nervous impulses passing towards the central nervous system as well as in those passing to muscles. Electrotonic Currents. During the passage of a constant current through a nerve, variations in the electric currents of the nerve analogous in some respects to the variations of the irritability of the nerve may be witnessed. Thus if a constant current supplied by the battery P (Fig. 15) be applied to a piece of nerve by means of two non-polarizable electrodes p, p, the " currents of rest " obtainable from various points of the nerve will be different during the passage of the polarizing current from those which were manifest before or after the current was applied; and, moreover, the changes in the nerve-currents produced by the polariz- ing current will not be the same in the neighbourhood of the anode (p) as those in the neighbourhood of the kathode ( p'). Thus let G and H be two galvanometers so connected with the two ends of the nerve as to obtain good and clear evidence of the "currents of rest." Before the polarizing current is thrown into the nerve, the needle of H will occupy a position indicating the passage of a current of a certain intensity from h to h' through the galvanometer (from the positive longitudinal surface to the negative cut end of the nerve), the circuit being completed by a current in the nerve from h' to h, i.e. the current will flow in the direction of the arrow. Similarly the needle of G will by its deflection indicate the existence of a current flowing from g to g' through the galvanometer, and from g to g through the nerve, in the direction of the arrow. At the instant that the polarizing current is thrown into the nerve at pp'j the currents at gg', hhf will suffer a "current of action" correspond- ing to the nervous impulse, which, at the making of the polarizing current, passes in both directions along the nerve, and may cause a contraction in the attached muscle. The current of action is, as we have seen, of extremely short duration, it is over and gone in a small fraction of a second. It therefore must not be confounded with a permanent effect which, in the case we are dealing with, is observed in both galvanometers. This effect, which is dependent on the direction of the polarizing current, is as follows: Supposing that the polarizing current is flowing in the direction of the arrow in the figure, that is, passes in the nerve from the positive electrode or anode p to the negative electrode or kathode pft it is found that the current through the galvanometer G is increased, while that through H is diminished. We CHAP. IL] THE CONTRACTILE TISSUES. 81 may explain this result by saying that the polarizing current has caused the appearance in the nerve outside the electrodes of a new current, the 'electrotonic' current, having the same direction as itself, which adds to, or takes away from, the natural nerve-current or " current of rest " according as it is flowing in the same or in an opposite direction. .7 H FIG. 15. DIAGRAM ILLUSTRATING ELECTROTOXIC CURRENTS. P the polarizing battery, with k a key, p the anode, and p' the kathode. At the left end of the piece of nerve the natural current flows through the galvanometer G from g to g', in the direction of the arrows ; its direction therefore is the same as that of the polarizing current; consequently it appears increased, as indicated by the sign + . The current at the other end of the piece of nerve, from h to h', through the galvanometer H, flows in a contrary direction to the polarizing current ; it consequently appears to be diminished, as indicated by the sign — . N.B. For simplicity's sake, the polarizing current is here supposed to be thrown in at the middle of a piece of nerve, and the galvanometer placed at the two ends. Of course it will be understood that the former may be thrown in anywhere, and the latter connected with any two pairs of points which will give currents. The strength of the electrotonic current is dependent on the strength of the polarizing current, and on the length of the intrapolar region which is exposed to the polarizing current. When a strong polarizing current is used, the electromotive force of the electrotonic current may be much greater than that of the natural nerve-current. The strergth of the electrotonic current varies with the irritability, or vital condition of the nerve, being greater with the more irritable nerve; and a dead nerve will not manifest electrotonic currents. More- over, the propagation of the current is stopped by a ligature, or by crushing the nerve. F. 6 82 ELECTROTONIC CURRENTS. [BOOK i. We may speak of the conditions which give rise to this electrotonic current as a physical electrotonus analogous to that physiological electro- tonus which is made known by variations in irritability. The physical electrotonic current is probably due to the escape of the polarizing current along the nerve under the peculiar conditions of the living nerve; but we must not attempt to enter here into this disputed and difficult subject or into the allied question as to the exact con- nection between the physical and the physiological electrotonus, though there can be little doubt that the latter is dependent on the former. An induction-shock is a current of very short duration developed very suddenly and disappearing more gradually. Hence, when it falls into a nerve, the nerve undergoes a sudden transition from its normal condition to the katelectrotonic phase, and consequently a nervous impulse giving rise to a contraction is the result. The return from the anelectrotonic phase to the normal condition appears from a number of considerations to be less effective as a generator of nervous impulses than the change from the normal condition to the katelectrotonic phase. Hence in the induced current we have to deal with a ' making ' contraction only, the breaking contraction being absent. This is true whether the induced current be generated by the making or by the breaking of a con- stant current. The constant current applied directly to a muscle from which the purely nervous element has been eliminated by urari poisoning, has effects similar to and yet somewhat different from those which it has upon a nerve. The efficacy of the rise of katelectrotonus and the fall of anelectrotonus respectively in producing contraction is the same as in a nerve. In one respect the muscle is more striking, and offers a support of the hypothesis mentioned above. The making contraction may under favourable circumstances be seen to start from the kathode and the breaking contraction from the anode. Besides the make and break spasm a partial tetanus during the whole time of the passage of the current through a muscle is very often seen. Another marked difference between muscle and nerve is that in muscle the current must act for a much longer time upon the tissue before it can call forth a con- traction. This is what we might expect from the more sluggish nature of the muscular impulse-wave. Hence muscular tissue which has lost its nervous elements or does not possess them, is far less readily affected by the almost momentary induction-shocks than are nerves. - SEC. 4. THE MUSCLE-NERVE PREPARATION AS A MACHINE. The facts described in the foregoing sections shew that a muscle with its nerve may be justly regarded as a machine which, when stimulated, will do a certain amount of work. But the actual amount of work which a muscle-nerve preparation will do is found to depend on a large number of circumstances, and conse- quently to vary within very wide limits. These variations will be largely determined by the condition of the muscle and nerve in respect to their nutrition ; in other words, by the degree of irrita- bility manifested by the muscle or by the nerve or by both. But quite apart from the general influences affecting its nutrition and thus its irritability, a muscle-nerve preparation is affected as regards the amount of its work by a variety of other circumstances, which we may briefly consider here, reserving to a succeeding section the study of variations in irritability. The nature and mode of application of the stimulus as affecting the amount and character of the contraction. We have seen that a nervous impulse is a molecular disturbance travelling along the nerve in the form of a wave. We saw further that the velocity with which this wave travels is in the frog about 28 inches per sec., and in the mammal somewhat higher, but that it varies according to circumstances, being especially dependent on temperature. The wave-length, that is, the total length of nerve along which the disturbance is at any one instant taking place, from the point nearer the muscle which the disturbance has just reached, to the point farther from the muscle which the disturbance has just left, may we have seen be put down (in the frog) as 18 mm.; but possibly this too varies somewhat. The greatest and most important variations however are those of the energy of the nervous impulse, of the amount of disturbance which takes place in the nerve or in the nerve fibre as the wave of the nervous impulse passes over it ; this we might designate as the height of the wave. 6—2 84 THE MUSCLE-NERVE MACHINE. [BOOK i. Thus a weak stimulus gives rise to a small disturbance, that is a weak nervous impulse, and a strong stimulus gives rise to a large disturbance, that is a powerful nervous impulse. We are not in a position at present to speak definitely as to the occurrence of other differences in the characters of nervous impulses. As far as we know at present, nervous impulses what- ever their origin are alike in nature l ; the impulses generated, in a natural way, by the brain or spinal cord, or produced artificially by mechanical stimuli, as by cutting or pinching, or by thermal stimuli, as by touching the nerve with a red-hot wire, or by chemical stimuli, or by electrical stimuli, may differ in intensity, and in the rapidity with which they succeed each other, but, as far as we know at present, not otherwise. Thus a drop of acid placed on a nerve gives rise to tetanus in the muscle which differs from the tetanus produced by repeated induction shocks applied to the nerve, only so far as the tetanus is generally irregular, the individual nervous impulses generated by the acid forming an irregular series, not following each other at equal intervals and not being all of the same intensity, whereas the impulses generated by the 'interrupted current ' are generally of the same intensity and follow each other at equal intervals. So also we are led at present to believe that when muscles are thrown into action in a natural way in the living body by the agency of the spinal cord, what goes 011 in the nerve differs from what goes on in the same nerve when the interrupted current is brought to bear on it, only in so far as in the former case the impulses follow each other at a fixed rate (nineteen a second), whereas in the latter, the rate of repetition varies according to the rapidity with which in the induction-machine the shocks follow each other; the individual impulses as far as we know at present have the same characters in the two cases save only that they may differ in intensity. Supposing that the irritability of a nerve-muscle preparation remains for the period of the experiment fairly constant, care being taken to avoid the effects of exhaustion, and that the stimulus be applied to the same part of the nerve, we find that the intensity of the nervous impulse generated (as measured by the muscular contraction) varies up to a certain limit according to what we may call the strength of the stimulus. Thus taking a single induction shock as the most manageable stimulus, we find that if, before we begin, we slide the secondary coil (Fig. 1, sc.) a certain distance from primary coil pr. c., no visible effect at all follows upon the discharge of the induction shocks. The passage of the momentary weak current is either unable to produce any nervous impulse at all, or the weak nervous impulse to which it 1 It will be observed that we are speaking now exclusively of the nerve of a muscle-nerve preparation, i.e. of what we shall hereafter term a motor nerve. Whether sensory impulses differ essentially from motor impulses will be considered later on. CHAP, ii.] THE CONTRACTILE TISSUES. 85 gives rise is unable to stir the sluggish muscular substance to a visible contraction. As we slide the secondary coil towards the primary, sending in an induction shock at each new position, we find that at a certain distance between the secondary and primary coils, the muscle responds to each induction shock1 with a con- traction which makes itself visible by the slightest possible rise of the attached lever. This position of the coils, the battery remaining the same and other things being equal, marks the minimal stimulus giving rise to the minimal contraction. As the secondary coil is brought nearer to the primary, the contractions increase in height corresponding to the increase in the intensity of the stimulus. Very soon however an increase in the stimulus caused by continuing to slide the secondary coil over the primary fails to cause any increase in the contraction. This indicates that the maximal stimulus giving rise to the maximal contraction has been reached; though the shocks increase in intensity as the secondary coil is pushed further and further over the primary, the contractions remain of the same height, until fatigue lowers them. Sometimes however, after the contractions have for some time remained of the same height, in spite of the stimulus, at each fresh stimulation, being increased in strength, a point is reached at which, with a further increase in the strength of the stimulus, a new increase of contraction sets in; but we must not attempt to explain here this paradoxical super-maximal contraction as it is called. With single induction shocks then the muscular contraction, and by inference the nervous impulse, increases with an increase in the intensity of the stimulus, between the limits of the minimal and maximal stimuli; and this dependence of the nervous impulse and so of the contraction on the strength of the stimulus may be observed not only in electric but in all kinds of stimuli. It may here be remarked that in order for a stimulus to be effective, a certain abruptness in its action is necessary. Thus we have seen that the constant current when it is passing through a nerve with uniform intensity does not give rise to a nervous impulse and that it may be increased or diminished to almost any extent without generating nervous impulses, provided that the change be made gradually enough ; it is only wrhen there is a sudden change that the current becomes effective as a stimulus. The current which is induced in the secondary coil of an induction- machine at the breaking of the primary circuit, is more rapidly developed, and has a steeper rise than the current which appears when the primary circuit is made ; and accordingly we find that the breaking induction shock is more potent as a stimulus than the making shock. Similarly a sharp tap on a nerve will produce 1 In these experiments either the breaking or making shock must be used, not sometimes one and sometimes the other, for the two kinds of shock differ in efficiency, the breaking being the most potent. 86 THE MUSCLE-NERVE MACHINE. [Boom. a contraction, when a gradually increasing pressure will fail to do If so ; and in general the efficiency of a stimulus of any kind will II depend in part on the suddenness or abruptness of its action. A stimulus, in order that it may be effective, must have an action of a certain duration, the time necessary to produce an effect varying according to its strength and being different in nerve from what it is in muscle. It would appear that an electric current applied to a nerve must have a duration of at least about '0015 sec. to cause any contraction at all, and needs longer than this to produce its full effect. When the current is applied directly to a muscle, whose nervous elements are placed hors de combat by the action of urari, or by degeneration of the nerve-fibres this period of necessary duration seems to be still longer, and to be especially increased by deficient nutrition. And this may be offered as an explanation of the well-known clinical fact that in various cases of paralysis, muscles which have by degeneration of their nerves, lost their nervous supply, more readily respond to the break and make of the constant current than to induction shocks, the duration of the former as stimuli being much greater than that of the latter. In the case of electric stimuli, the strength of the contrac- tion, and by inference of the nervous impulse, depends on the manner in which the current flows into the nerve. Though the matter has been disputed, it appears that the current must pass along some appreciable length of nerve-fibre in order to produce an effect: a current which passes through a nerve in an absolutely transverse direction being powerless to generate impulses ; and further there is a connection between the efficiency of the current and the angle at which it falls into the nerve. It would also appear, at all events up to certain limits, and as a general rule, that the longer the piece of nerve through which the current passes, the greater is the effect of the stimulus. When two pairs of electrodes are placed on the nerve of a long and perfectly fresh and successful nerve-preparation, one near to the cut end, and the other nearer the muscle, it is found that the same stimulus produces a greater contraction when applied through the former pair of electrodes than through the latter. Two inter- pretations of this result are possible. Either the nerve at the part farther away from the muscle is more irritable, i.e. that the stimulus gives rise at the spot stimulated to a larger nervous impulse ; or the impulse started at the farther electrodes gathers strength, like an avalanche, in its progress to the muscle. The latter view has been strongly urged by Pfluger, and is generally known under the name of the 'avalanche theory'. Against it may be urged that as far as we know, the progress of the current of action along a nerve is marked by no such increase. It is probable that the larger contraction produced by stimulation of the portions of the nerve near the spinal cord is due to the CHAP, ii.] THE CONTRACTILE TISSUES. 87 stimulus setting free a larger impulse, i.e. to this part of the nerve being more irritable. It is possible that the irritability of a nerve may vary considerably at different points of its course. We have in a preceding section discussed at length the manner in which a stimulus repeated sufficiently rapidly produces a com- plete and uniform tetanus, during which the constituent single contractions cannot be recognized either by the appearance of the muscle itself or by any features in the curve which it may be made to describe, though the 'muscular sound' shews that the muscle is really in a state of vibration. If the frequency of the stimulus be reduced the tetanus becomes incomplete and a flickering of the muscle becomes obvious, and upon further reduction of the frequency the flickering gives place to a rhythmic series of single contractions. Since the height to which the lever is raised, i.e. the amount of total shortening resulting from any second contraction, is greater when that contraction starts from the summit of the preceding curve than when it starts from the decline, it is obvious that the amount of total contraction will up to a certain limit increase with the frequency of repetition of the stimulus. Thus a stimulus repeated rapidly will produce a tetanus, shortening the muscle and raising the weight to a greater extent than will the same stimulus less rapidly repeated. The exact frequency of repetition required to produce complete tetanus varies according to the condition of the muscle and is not the same for all muscles, being dependent on the rapidity with which the muscle executes each single contraction. In those animals which possess two kinds of skeletal muscles, red and pale, the red muscles (the single contractions of which are slow and long- drawn) are thrown into complete tetanus with a repetition of much less frequency than that required for the pale muscles. Thus, ten stimuli in a second are quite sufficient to throw the red muscles of the rabbit into complete tetanus, while the pale muscles require at least twenty stimuli in a second. When the stimulus is repeated more frequently than is required to bring about a complete tetanus the constituent contractions are still proportionately increased in frequency. This is shewn by the increased pitch of the muscular sound. How far the increase in the frequency of the constituent contractions can be carried by increasing the frequency of the stimulus is a question which presents considerable difficulties, and cannot be discussed here. The value of the muscle as a machine is also in part dependent on the Load. It might be imagined that a muscle, which, when loaded with a given weight, and stimulated by a current of a given intensity, had contracted to a certain extent, would only contract to half that extent when loaded with twice the weight and stimu- lated with the same stimulus. Such however is not the case; the height to which the weight is raised may be in the second instance 88 THE MUSCLE-NERVE MACHINE. [BOOK i. as great, or even greater, than in the first. That is to say, the resistance offered to the contraction actually augments the con- traction, the tension of the muscular fibre increases the facility with which the explosive changes resulting in a contraction take place. And it has been observed by Heidenhain that the degree of acid reaction, the amount of carbonic acid given off and the rise of temperature are greater in a muscle contracting against resistance than when the resistance is removed ; that is to say, the tension increases the metabolism. There is, of course, a limit to this favourable action of the resistance. As the load con- tinues to be increased, the height of the contraction is diminished, and at last a point is reached at which the muscle is unable (even when the stimulus chosen is the strongest possible) to lift the load at all. In a muscle viewed as a machine we have to deal not merely with the height of the contraction, that is with the amount of shortening, but with the work done. And this is measured as the height to which the load is raised multiplied into the weight of the load. Hence it is obvious from the foregoing observations that the work done must be largely dependent on the weight itself. Thus there is a certain weight of load, with which in any given muscle, stimulated by a given stimulus, the most work will be done. Since mere tension affects the changes going on in the muscular fibres, it is desirable in experiments in which muscles are loaded, that the weight should not bear upon the lever until the contraction actually begins. This is easily managed by interposing between the end of the muscle and the weight a lever with a support so arranged that, before contraction takes place, the weight only extends the muscle to the length natural to it during rest; but that the muscle directly it shortens at once begins to pull on the weight. The muscle is then said to be after-loaded1. The value of a muscle as a machine is further determined by the Size and Form of the Muscle. Since all known muscular fibres are much shorter than the wave-length of a contraction, it is obvious that the longer the fibre, the greater the height of the contraction with the same stimulus. Hence in a muscle of parallel fibres, the height to which the load is raised as the result of a given stimulus applied to its nerve, will depend on the length of the fibres, while the maximum weight of load capable of being lifted will depend .on the number of the fibres, since the load is distributed among them. Of two muscles therefore of equal length (and of the same quality) the most work will be done by that which has the greater sectional area; and of two muscles with equal sectional areas, the most work will be done by that which is the longer. If the two muscles are unequal both in length and sectional area, 1 This is perhaps the best equivalent of the German uberlastet. CHAP, ii.] THE CONTRACTILE TISSUES. 89 the work done will be the greater in the one which has the larger bulk, which contains the greater number of cubic units. In speaking therefore of the work which can be done by a muscle, we may use as a standard a cubic unit of bulk, or, the specific gravity of the muscle being the same, a unit of weight. Absolute power of a muscle. We have seen that with a given weight a stimulus (induction shock) may be chosen of such a strength that a contraction is only just visible. In such a case a very slight increase of the weight would prevent even that minimal contraction. Upon increasing the stimulus the minimal contraction would reappear and vanish again upon a further increase of the weight. Increasing the stimulus and weight in this way we should be able to find out the weight which, with a maximal stimulation, is just sufficient to prevent any visible con- traction from taking place, a very slight diminution of weight at once allowing a minimum contraction to make its appearance. Such a weight is taken as the measure of what is called the 'absolute power' of the muscle; and from what has been said in the previous paragraph, it is obvious that this will depend on the number of fibres in, or more correctly, on the sectional area of, the muscle. The absolute power of a square centimetre of a frog's muscle has been in this way estimated at about -2800 to 3000 grms.: of a square centimetre of human muscle at 6000 to 8000 grms. It may be worth while to mention in this connection the following interesting fact. If the weight be determined which will stop a contraction when applied directly the contraction begins, and also that which stops any further contraction when applied at a moment when the contraction is already partly accomplished, it will be found that the second weight is much less than the first. It appears, in fact, that the forces which cause the change in the form of the muscle are at their maximum at the beginning of the shortening, and thenceforwards decline until they become nothing when the short- ening is complete. ITie work done. We learn then from the foregoing paragraphs that the work done, i.e. the weight of the load multiplied into the height of the lift, will depend, not only on the activity of the nerve and muscle as determined by their own irritability, but also on the character and mode of application of the stimulus, on the kind of contraction (whether a single spasm, or a slowly repeated tetanus or a rapidly repeated tetanus) on the load itself, and on the size and form of the muscle. Taking the most favourable circum- stances, viz. a well nourished, lively preparation, a maximum stimulus causing a rapid tetanus and an appropriate load, we may determine the maximum work done by a given weight, say one gramme, of muscle. This in the case of the muscles of the frog has been estimated at about four gram-metres for one gramme of muscle. SEC. 5. THE CIRCUMSTANCES WHICH DETERMINE THE DEGREE OF IRRITABILITY OF MUSCLES AND NERVES. A muscle-nerve preparation, at the time that it is removed from the body, possesses a certain degree of irritability, it responds by a contraction of a certain amount to a stimulus of a certain strength, applied to the nerve or to the muscle. After a while, the exact period depending on a variety of circumstances, the same stimulus produces a smaller contraction, i.e. the irritability of the preparation has diminished. In other words, the muscle or nerve or both have become partially 'exhausted'; and the exhaustion subsequently increases, the same stimulus producing smaller contractions until at last all irritability is lost, no stimulus however strong producing any contraction whether applied to the nerve or directly to the muscle ; and eventually the muscle, as we have seen, becomes rigid. The progress of this exhaustion is more rapid in the nerves than in the muscles ; for some time after the nerve-trunk has ceased to respond to even the strongest stimulus, contractions may be obtained by applying the stimulus directly to the muscle. It is much more rapid in the warm-blooded than in the cold-blooded animals. The muscles and nerves of the former lose their irritability, when removed from the body, after a period varying according to circumstances from a few minutes to two or three hours; those of cold-blooded animals (or at least of an amphibian or a reptile) may under favourable conditions remain irritable for two, three, or even more days. The duration of irritability in warm-blooded animals may however be considerably prolonged by reducing the temperature of the body before death. CHAP, ii.] THE CONTRACTILE TISSUES. 91 If with some thin body a sharp blow be struck across a muscle which has entered into the later stages of exhaustion, a wheal lasting for several seconds is developed. This wheal appears to be a contraction wave limited to the part struck, and disappearing very slowly, without extending to the neighbouring muscular substance. It has been called an 'idio-muscular' contraction, because it may be brought out even when ordinarv stimuli have ceased to produce any effect. It may however be accompanied at its beginning by an ordinary contraction. It is readily produced in the living body on the pectoral and other muscles of persons suffering from phthisis and other exJiausting diseases. This natural exhaustion and diminution of irritability in muscles and nerves removed from the body may be modified both in the case of the muscle and of the nerve, by a variety of circum- stances. Similarly, while the nerve and muscle still remain in the body, the irritability of the one or of the other may be modified either in the way of increase or of decrease by various events. We have already seen (p. 78) how the constant current produces the variations in irritability known as katelectrotonus and anelec- trotonus. We have now to study the effect of more general influences, of which the most important are, severance from the central nervous system, and variations in temperature, in blood- supply, and in functional activity. The Effects of Severance from the Central Nervous System. •When a nerve, such for instance as the sciatic, is divided in situ, in the living body, there is first of all observed a slight increase of irritability, noticeable especially near the cut end ; but after a while the irritability diminishes, and gradually disappears. Both the slight initial increase and the subsequent decrease begin at the cut end and advance centrifugally towards the peripheral terminations. This centrifugal feature of the loss of irritability is often spoken of as the Bitter- Valli law. In a mammal it may be two or three days, in a frog, as many, or even more weeks, before irritability has disappeared from the nerve-trunk. It is maintained in the small (and especially in the intramuscular) branches for still longer periods. This centrifugal loss of irritability is the forerunner in the peripheral portion of the divided nerve of structural changes which proceed in a similar centrifugal manner. The medulla suffers changes similar to those seen in nerve-fibres after removal from the body. Its double contour and its characteristic indentations be- come more marked, it breaks up into small irregular fragments, or drops, a separation apparently taking place between its proteid and its fatty constituents. The latter are soon absorbed, but the former remain for a longer time within the sheath of Schwann, being in some cases scarcely, if at all, to be distinguished from the 92 VARIATIONS OF IRRITABILITY. [BOOK i. swollen axis-cylinder. Meanwhile the nuclei which occur, one in each segment of the nerve between each two nodes of Ranvier, divide and multiply rapidly. Lastly the axis-cylinder breaks up and disappears so that nothing remains of the original fibre but the sheath of Schwann enclosing a proteid mass with many nuclei. If no regeneration takes place these nuclei eventually disappear. In the central portion of the divided nerve similar changes may be traced as far only as the next node of Ranvier. Beyond this the nerve usually remains in a normal condition. Regeneration, when it occurs, is apparently carried out by the peripheral growth of the axis-cylinders of the intact central portion. When the cut ends of the nerve are close together the axis-cylinders growing out from the central portion run into and between the sheaths of Schwann of the peripheral portion ; but much uncertainty still exists as to the exact parts which the proliferated nuclei referred to above, the proteid remnants of the medulla, and the old axis-cylinders of the peripheral portion respectively play in giving rise to the new structures of the regenerated fibre. This degeneration may be observed to extend down to the very endings of the nerve in the muscle, including the end-plates, but does not at first affect the muscular substance itself. The muscle, though it has lost all its nervous elements, still remains irritable towards stimuli applied directly to itself: an additional proof of the existence of an independent muscular irritability. For some time the irritability of the muscle, as well towards stimuli applied directly to itself as towards those applied through the impaired nerve, seems to be diminished; but after a while a peculiar condition (to which we have already alluded on p. 86) sets in, in which the muscle is found to be not easily stimulated by single induction shocks but to respond readily to the make or break of a constant current. In fact it is said to become even more sensitive to the latter mode of stimulation than it was when its nerve was intact and functionally active. At the same time it also becomes more irritable towards direct mechanical stimuli, and very frequently fibrillar contractions, more or less rhythmic and apparently of spontaneous origin, though their causation is ob- scure, make their appearance. This phase of heightened sensitiveness of a muscle, especially to the constant current, appears to reach its maximum, in man at about the seventh week after nervous impulses, from injury to the nerves or nervous centre, have ceased to reach the muscle. If the muscle thus deprived of its nervous elements be left to itself its irritability however tested sooner or later diminishes, but if the muscle be periodically thrown into contractions by artificial stimulation with the constant current, the decline of irritability and attendant loss of nutritive power may be postponed for some considerable time. But as far as our experience goes at present CHAP, ii.] TUE CONTRACTILE TISSUES. 03 the artificial stimulation cannot fully replace the natural one and sooner or later the muscle like the nerve suffers degeneration, loses all irritability and ultimately becomes replaced by connective tissue. The Influence of Temperature. We have already seen that sudden heat applied to a limited part of a nerve or muscle, as when the nerve or muscle is touched with a hot wire, will act as a stimulus, and the same might be said of cold when sufficiently intense. It is however much more difficult to generate nervous or muscular impulses by ex- posing a whole nerve or muscle to a gradual rise of temperature. Thus according to most observers a nerve belonging to a muscle1 may be either cooled to 0° C. or below, or heated to 50° or even 100°C., without discharging any nervous impulses, as shewn by the absence of contraction in the attached muscle. The contractions moreover may be absent even when the heating has not been very gradual. A muscle may be cooled to 0° C. or below without any contrac- tion being caused ; but when it is heated to a limit, which in the case of frog's muscles is about 45°, of mammalian muscles about 50°, a sudden change takes place : the muscle falls, at the limiting temperature, into a rigor mortis, which is initiated by a forcible contraction or at least shortening. The rigor mortis thus brought about by heat is often spoken of as rigor caloris. Moderate warmth, ex. gr. in the frog an increase of temperature up to somewhat below 45° C., favours both muscular and nervous irritability. All the molecular processes are hastened and facili- tated : the contraction is for a given stimulus greater and more rapid, i.e. of shorter duration, and nervous impulses are generated more readily by slight stimuli. Owing to the quickening of the chemical changes, the supply of new material may prove insuffi- cient ; hence muscles and nerves removed from the body lose their irritability more rapidly at a high than at a low temperature. The gradual application of cold to a nerve, especially when the temperature is thus brought near to 0°, slackens all the molecular processes, so that the wave of nervous impulse is lessened and pro- longed, the velocity of its passage being much diminished, e.g. from 28 m. to 1 m. per sec. At about 0° the irritability of the nerve disappears altogether. When a muscle is exposed to similar cold, ex. gr. to a tempera- ture very little above zero, the contractions are remarkably pro- longed ; they are diminished in height at the same time, but not in proportion to the increase of their duration. Exposed to a temperature of zero or below, muscles soon lose their irritability, 1 The action of cold and heat on sensory nerves will be considered in the later portion of the woik. 94 VARIATIONS OF IRRITABILITY. [BOOK i. without however undergoing rigor mortis. After an exposure of not more than a few seconds to a temperature not much below zero, they may be restored, by gradual warmth, to an irritable con- dition, even though they may appear to have been frozen. When kept frozen however for some few minutes, or when exposed for a less time to temperatures of several degrees below zero, their irritability is permanently destroyed. When thawed, they enter into rigor mortis of a most pronounced character. The Influence of Blood-Supply. When a muscle still within the body is deprived by any means of its proper blood-supply, as when the blood-vessels going to it are ligatured, the same gradual loss of irritability and final appearance of rigor mortis are observed as in muscles removed from the body. Thus if the abdominal aorta be ligatured, the muscles of the lower limbs lose their irritability and finally become rigid. So also in systemic death, when the blood-supply to the muscles is cut off by the cessation of the circulation, loss of irritability ensues, and rigor mortis eventually follows. In a human corpse the muscles of the body enter into rigor mortis in a fixed order : first those of the jaw and neck, then those of the trunk, next those of the arms, and lastly those of the legs. The rapidity with which rigor mortis comes on after death varies considerably, being determined both by external circumstances and by the internal conditions of the body. Thus external warmth hastens and cold retards the onset. After great muscular exertion, as in hunted animals, and when death closes wasting diseases, rigor mortis in most cases comes on rapidly. As a general rule it may be said that the later it is in making its appearance, the more pronounced it is, and the longer it lasts ; but there are many exceptions, and when the state is recognized as being fundamentally due to a coagulation, it is easy to understand that the amount of rigidity, i.e. the amount of the coagulum, and the rapidity of the onset, i.e. the quickness with which coagulation takes place, may vary independently. The rapidity of onset after muscular exercise and wasting disease is apparently dependent on an increase of acid reaction, being produced under those circum- stances in the muscle, for this seems to be favourable to the coagu- lation of the muscle plasma. When rigor mortis has once become thoroughly established in a muscle through deprivation of blood, it cannot be removed by any subsequent supply of blood. Thus where the abdominal aorta has remained ligatured until the lower limbs have become completely rigid, untying the ligature will not restore the muscles to an irritable condition ; it simply hastens the decomposition of the dead tissues by supplying them with oxygen and, in the case of the mammal, with warmth also. A muscle however may acquire as a whole a certain amount of rigidity on account of some of the fibres becoming rigid, while the remainder, CHAP. Ji.] THE CONTRACTILE TISSUES. 95 though they have lost their irritability, have not yet advanced into rigor mortis. At such a juncture a renewal of the blood-stream may restore the irritability of those fibres which were not yet rigid, and thus appear to do away with rigor mortis ; yet it appears that in such cases the fibres which have actually become rigid never regain their irritability, but undergo degeneration. Mere loss of irritability, even though complete, if stopping short of the actual coagulation of the muscle-substance, may be with care removed. Thus if a stream of blood be sent artificially through the vessels of a separated (mammalian) muscle, the irrita- bility may be maintained for a very considerable time. On stopping the artificial circulation, the irritability diminishes and in time entirely disappears ; if however the stream be at once resumed, the irritability will be recovered. By regulating the flow, the irritability may be lowered and (up to a certain limit) raised at pleasure. From the epoch however of interference with the nor- mal blood-stream there is a gradual diminution in the responses to stimuli, and ultimately the muscle loses all its irritability and becomes rigid, however well the artificial circulation be kept up. This failure is probably in great part due to the blood sent through the tissue not being in a perfectly normal condition ; but we have at present very little information on this point. Indeed with respect to the quality of blood thus essential to the maintenance or restoration of irritability, our knowledge is definite with regard to one factor only, viz. the oxygen. If blood deprived of its oxygen be sent through a muscle removed from the body, irritability, so far from being maintained, seems rather to have its disappearance hastened. In fact, if venous blood continues to be driven through a muscle, the irritability of the muscle is lost even more rapidly than in the entire absence of blood. It would seem that venous blood is more injurious than none at all. If exhaustion be not carried too far, the muscle may however be revived by a proper supply of oxygenated blood. The influence of blood-supply cannot be so satisfactorily studied in the case of nerves as in the case of muscles ; there can however be little doubt that the effects are analogous. The Influence of Functional Activity. This too is more easily studied in the case of muscles than of nerves. When a muscle within the body is unused, it wastes ; when used it (within certain limits) grows. Both these facts shew that the nutrition of a muscle is favourably affected by its functional activity. Part of this may be an indirect effect of the increased blood-supply which occurs when a muscle contracts. When a nerve going to a muscle is stimulated, the blood-vessels of the muscle dilate. Hence at the time of the contraction more blood 96 VARIATIONS OF IRRITABILITY. [BOOK i. flows through the muscle, and this increased flow continues for some little while after the contraction of the muscle has ceased. But, apart from the blood-supply it is probable that the ex- haustion caused by a contraction is immediately followed by a reaction favourable to the nutrition of the muscle ; and this is a reason, possibly the chief reason, why a muscle is increased by use, that is to say, the loss of substance and energy caused by the contraction is subsequently more than made up for by increased metabolism during the following period of rest. Whether there be a third factor, whether muscles for in- stance are governed by so-called trophic nerves which affect their nutrition directly in some other way than by influencing either their blood-supply or their activity, must at present be left undecided. A muscle, even within the body, after prolonged action is fatigued, i.e. a stronger stimulus is required to produce the same contraction; in other words, its irritability may be lessened by functional activity. Whether functional activity therefore is in- jurious or beneficial depends on its amount in relation to the condition of the muscle. It may be here remarked that as a muscle becomes more and more fatigued, stimuli of short duration, such as induction shocks, sooner lose their efficacy than do stimuli of longer duration such as the break and make of the constant current. The sense of fatigue of which, after prolonged or unusual exertion, we are conscious in our own bodies, is probably of complex origin, and its nature, like that of the normal muscular sense of which we shall have to speak hereafter, is at present not thoroughly under- stood. It seems to be in the first place the result of changes in the muscles themselves, but is possibly also caused by changes in nervous apparatus concerned in muscular action, and especially in those parts of the central nervous system which are concerned in the production of voluntary impulses. In any case it cannot be taken as an adequate measure of the actual fatigue of the muscles; for a man who says he is absolutely exhausted may under excite- ment perform a very large amount of work with his already weary muscles. The will in fact rarely if ever calls forth the greatest contractions of which the muscles are capable. Absolute (temporary) exhaustion of the muscles, so that the strongest stimuli produce no contraction, may be produced even within the body by artificial stimulation; recovery takes place on rest. Out of the body absolute exhaustion takes place readily. Here also recovery may take place. Whether in any given case it does occur or not, is determined by the amount of contraction causing the exhaustion, and by the previous condition of the muscle. In all cases recovery is hastened by renewal (natural or artificial) of the blood-stream. The more rapidly the contractions follow each other, the less the interval between any two con- CHAP. IL] THE CONTRACTILE TISSUES. 97 tractions, the more rapid the exhaustion. A certain number of single induction-shocks repeated rapidly, say every second or oftener, bring about exhaustive loss of irritability more rapidly than the same number of shocks repeated less rapidly, for instance every 5 or 10 seconds. Hence tetanus is a ready means of pro- ducing exhaustion. In exhausted muscles the elasticity is much diminished ; the tired muscle returns less readily to its natural length than does the fresh one. The exhaustion due to contraction may be the result : — Either of the consumption of the store of really contractile material present in the muscle. Or of the accumulation in the tissue of the products of the act of contraction. Or of both of these causes. The restorative influence of rest may be explained by supposing that during the repose, either the internal changes of the tissue manufacture new explosive material out of the comparatively raw material already present in the fibres, or the directly hurtful pro- ducts of the act of contraction undergo changes by which they are converted into comparatively inert bodies. A stream of fresh blood may exert its restorative influence not only by quickening the above two events, but also by carrying off the immediate waste products while at the same time it brings new raw material. It is not known to what extent each of these parts is played. That the products of contraction are exhausting in their effects, is shewn by the facts that the injection of a solution of the muscle-extractives into the vessels of a muscle produces exhaustion and that exhausted muscles are recovered by the simple injection of inert saline solutions into their blood-vessels ; moreover lactic acid and indeed other acids injected into a muscle cause rapid exhaustion; and we may suppose that carbonic acid, with the other substances which after a contraction tend to give rise to an acid reaction, when generated too rapidly to be neutralized by the alkaline lymph in which the fibres are bathed, in part at least determine the exhaustion. But the matter has not yet been fully worked out. One important element brought by fresh blood is oxygen. This, as we have seen, is not necessary for the carrying out of the actual contraction, and yet is essential to the maintenance of irritability. It is probably of use as what may be called "intramolecular oxygen " in preparing the explosive material whose decomposition gives rise to the carbonic acid, and other products of contraction. F. SEC. 6. THE ENERGY OF MUSCLE AND NERVE, AND THE NATURE OF MUSCULAR AND NERVOUS ACTION. We may briefly recapitulate some of the chief results arrived at in the preceding pages as follows. A muscular contraction itself is essentially a translocation of molecules, a change of form not of bulk. We cannot say however anything definite as to the nature of this translocation or as to the way in which it is brought about. Though it would appear that the dim doubly refractive bands increase in bulk at the expense of the bright singly refractive bands, we cannot satis- factorily explain the connection between the striation of a muscular fibre and a muscular contraction. Nearly all rapidly contracting muscles are striated, and we must suppose that the striation is of some use ; but it is not essential to the carrying out of a contraction, for many muscles are not striated. But whatever be the exact way in which the translocation is effected, it is fundamentally the result of a chemical change, of an explosive decomposition of certain parts of the muscle-substance. The energy which is expended in the mechanical work done by the muscle has its source in the latent energy of the muscle-substance set free by that explosion. Concerning the nature of that ex- plosion we only know at present that it results in the production of carbonic acid and in an increase of the acid reaction, and that heat is set free as well as the specific muscular energy. There is a general parallelism between the extent of metabolism taking place and the amount of energy set free. The greater the development of carbonic acid, the larger is the contraction and the higher the temperature. It has not been possible hitherto to draw up a complete equa- tion between the latent energy of the material and the two forms of actual energy set free. The proportion of energy given out as heat to that taking on the form of work probably varies under different circumstances; and it would appear that on the whole a muscle would be no more economical than a steam-engine in respect to the conversion of chemical action into mechanical CHAP, ii.] THE CONTRACTILE TISSUES. 99 work, were it not that in warm-blooded animals the heat given out is not, as in the steam-engine, mere loss, but by keeping up the animal temperature serves many subsidiary purposes. It might be supposed that when in a contraction work is actually done, the increase of temperature is less than when the same contraction takes place without doing actual work, that is to say, that the mechanical work is done at the expense of energy which otherwise would go out as heat. Probable as this may seem it has not yet been experimentally verified. Of the exact nature of the chemical changes which underlie a muscular contraction we know very little, the most important fact being, that the contraction is not the outcome of a direct oxidation, but the splitting up or explosive decomposition of some complex substance. The muscle does consume oxygen, and the products of muscular metabolism are in the end products of oxidation, but the oxygen appears to be introduced not at the moment of explosion but at some earlier date. There is no evidence of nitrogenous products being given off as waste ; such nitrogenous crystalline bodies as are present in muscle, kreatin, &c., may be regarded rather as the wear-and-tear of the machine than as products of the material consumed in the work. Yet it is hardly consonant with what we know elsewhere, to suppose that the contraction of a muscular fibre has for its essence the decomposition of a non-nitrogenous substance ; and we may suppose that the explosion does involve some nitrogenous products, which however are re- tained within the tissue, and used up again. We may even go so far as to entertain with Hermann the view that a single complex substance, an hypothetical inogen, splits up partly into nitrogenous, partly into non-nitrogenous factors, the former, possibly of the nature of myosin, being rapidly built up again into new inogen, while the latter, such as the carbonic acid, are discharged at once from the muscle. But our knowledge of these matters is not yet ripe enough for the construction of an adequate and wholly satisfactory theory. It may be worth while to point out that during even the most complete repose muscle is undergoing chemi- cal changes, which, as far as we know, are the same in kind, and only differ in degree from those characteristic of a contraction. Thus carbonic acid is constantly being produced, as are probably other substances, all being got rid of as they form, just as they are got rid of in larger quantities during the repose which follows contraction. Supposing the existence of a substance which splits up into these various products, and which we may speak of as the true contractile material, it is evident that this material being thus constantly used up, must be as constantly repaired. Thus a stream of chemical substances may be conceived of as flowing through muscle, the raw material brought by the blood being gradually converted into true contractile stuff, the breaking-down again of which is- gentle and gradual so long as the muscle is at rest, but 7—2 100 MUSCULAR AND NERVOUS ACTION. [BOOK i. becomes excessive and violent when a contraction takes place. When rigor mortis sets in, the whole remaining contractile material is decomposed. While in muscle the chemical events are so prominent that we cannot help considering a muscular contraction to be essentially a chemical process, with electrical changes as attendant phenomena only, the case is different with nerves. Here the electrical pheno- mena completely overshadow the chemical. Our knowledge of the chemistry of nerves is at present of the scantiest, and the little we know as to the chemical changes of nervous substance is gained by the study of the central nervous organs rather than of the nerves. We find that the irritability of the former is closely dependent on an adequate supply of oxygen, and we may infer from this that in nervous as in muscular substance a metabolism, of in the main an oxidative character, is the real cause of the development of energy; and the axis-cylinder (which is probably the active element of a nerve-fibre, the medulla being useful for its nutrition and protec- tion only,) undoubtedly resembles in many of its chemical features the substance of a muscular fibre. But we have as yet no satis- factory experimental evidence that the passage of a nervous impulse along a nerve is the result, like the contraction of a muscular fibre, of chemical changes, and like it accompanied by an evolution of heat. On the other hand, the electric phenomena are so prominent that some have been tempted to regard a nervous impulse as essentially an electrical change. But it must be remembered that the actual energy set free in a nervous impulse is so to speak in- significant, so that chemical changes too slight to be recognized by the means at present at our disposal would amply suffice to provide all the energy set free. On the other hand, the rate of transmission of a nervous impulse, putting aside other features, is alone sufficient to prove that it is something quite different from an ordinary electric current. The curious disposition of the end-plates, and their remarkable analogy with the electric organs which ai e found in certain animals, has suggested the view that the passage of a nervous impulse from the nerve-fibre into the muscular substance is of the nature of an electric discharge. But these matters are too difficult and too abstruse to be discussed here. It may however be worth while to remind the reader that in every contraction of a muscular fibre, the actual change of form is preceded by invisible changes propagated all over the fibre and occupying the latent period, and that these changes resemble in their features the nervous impulse of which they are so to speak the continuation rather than the contraction of which they are the forerunners and to which they give rise. So that a muscle, even putting aside the visible terminations of the nerve, is funda- mentally a muscle and a nerve besides. SEC. 7. OTHER FORMS OF CONTRACTILE TISSUE. Unstriated Muscular Tissue. Our knowledge of the phenomena of these structures is very imperfect since (in vertebrates) they do not exist in isolated masses like the striated muscles, but occur as constituents of complex organs, such as the intestine, ureter, uterus, &c. They undergo rigor mortis : and what little informa- tion we do possess concerning their chemical and physical features leads us to believe that the processes which take place in them are fundamentally identical with those occurring in striated muscle, the two differing in degree rather than in kind. When stimulated, they contract. If a stimulus, mechanical or electrical, be applied to the intestine or ureter of a mammal, a circular contraction is seen to take place at the spot stimulated. The contraction, which is preceded by a very long latent period, lasts a very considerable time, in fact several seconds, after which relaxation slowly takes place. That is to say, over the circularly dispersed fibres of the intestine (or ureter) at the spot in question there has passed a con- traction-wave remarkable for its long latent period and for the slow- ness of its development. From the spot so directly stimulated, the contraction may pass as a wave (with a length of 1 cm. and a velocity of from 20 to 30 millimetres a second in the ureter), along the circular coat both upwards and downwards. The longitudinal fibres at the spot stimulated are also thrown into contractions of altogether similar character, and a wave of contraction may also travel longitudinally along the longitudinal coat both upwards and down wards. It is evident however that the wave of contraction of which we are now speaking is in one respect different from the wave of contraction treated of in dealing with striated muscle. In the latter case the contraction-wave is a simple wave propagated 102\ I $*\ ;;'; ?';*»\ jStjJ-TJED MUSCLE. [BOOK i. along the individual fibre ; in the case of the intestine or ureter, the wave is complex, being the sum of the contraction-waves of several fibres engaged in different phases and is propagated from fibre to fibre, both in the direction of the fibres, as when the whole circumference of the intestine is engaged in the contraction, or when the wave travels longitudinally along the longitudinal coat, and also in a direction at right angles to the axes of the fibres, as when the contraction-wave travels lengthways along the circular coat of the intestine, or when it passes across a breadth of the longitudinal coat. Moreover, it is obvious that the contraction- wave which passes along a single unstriated fibre differs from that passing along a striated fibre, in the very great length both of its latent period and of the duration of its contraction. Waves of contraction thus passing along the circular and longi- tudinal coats of the intestine constitute what is called peristaltic action. Like the skeletal muscles, whose nervous elements have been rendered functionally incapable (p. 86), unstriated muscles are much more sensitive to the making and breaking of a constant current than to induction-shocks. The unstriated muscles seem to be remarkably susceptible to the influences of temperature. Thus the unstriated muscles of the trachea are said not to contract at a temperature below 12°C., and are most active at a temperature above 21°C. So also the movements of the intestine cease at a temperature below 19°C. In striking contradistinction to what takes place in the striated muscles, automatic movements are exceedingly common in struc- tures built up of non-striated muscles ; these moreover exhibit a great tendency to rhythmic action. Thus the peristaltic action of the intestine and ureters, and the corresponding movements of the uterus, are at once rhythmic, and largely automatic. What share the nervous elements take in the automatism and the rhythm is uncertain. Cardiac Muscles. The most important features of this form of contractile tissue will be studied when we come to deal with the heart. It will be seen that they are intermediate between ordinary skeletal and non-striated muscles. Cilia. Ciliary movement consists in the rapid flexion (into a sickle or hook-form) of the cilium and its less rapid return to its previous straight form. The diminished velocity of the return leads to the force of the ciliary action being exerted in the same direction as the flexion. The cause of the flexion seems to be the contraction of the cilium, and that of the return, an elastic reaction. In the lower animals however many'varieties in the mode of move- ment of cilia may be observed. Various attempts to explain the movement by the presence of special mechanisms at the base of the cilia have hitherto failed. Some authors have attributed the movement to a' protoplasmic CHAP, ii.] CONTRACTILE TISSUES. 103 contraction of the cell itself, the cilium acting merely as a minute elastic rod ; and some such view as this is supported by the fact that no movement has ever been observed in an isolated cilium. It is difficult however to understand how the peculiar sickle-like flexion of the cilium can be brought about unless the contractile material is continued up into the cilium itself; and the tail of a spermatozoon, which is practically a single cilium, may contract even when separated from the head. Ciliary movement appears therefore to differ from ordinary muscular contraction chiefly in the size of the apparatus concerned. The movement is rapid: thus Engelmann has estimated that in the frog the flexions are repeated at least twelve times in a second. The movement in fact is too rapid to be visible; it can only be seen at a time when exhaustion and coming death have begun to retard the action; Engelmann found that he was first able to count them when their rapidity declined to eight in a second. In the vertebrate animal, cilia are, as far as we know, wholly independent of the nervous system, and their movement is pro- bably ceaseless. In such animals however as Infusoria, Hydrozoa, &c. the movements in a ciliary tract may often be seen to stop and go on again, to be now fast now slow, according to the needs of the economy, and, as it almost seems, according to the will of the creature ; indeed in some of these animals the ciliary move- ments are clearly under the influence of the nervous system. Observations with galvanic currents, constant and interrupted, have not led to any satisfactory results, and, as far as we know at present, ciliary action is most affected by changes of temperature and chemical media. Moderate heat quickens the movements, but a rise of temperature beyond a certain limit (about 40°C. in the case of the pharyngeal membrane of the frog) becomes injurious ; cold retards. Very dilute alkalis are favourable, acids are injurious. An excess of carbonic acid or an absence of oxygen diminishes or arrests the movements, either temporarily or permanently, according to the length of the exposure. Chloroform or ether in slight doses diminishes or suspends the action temporarily, in excess kills and disorganises the cells. Migrating Cells. We have already (p. 35) urged the view that an amoeboid movement of a white corpuscle is essentially a form of contraction. All the circumstances which affect muscular contraction, heat, absence or presence of oxygen and carbonic acid, &c., also affect protoplasmic movements. The white corpuscles, like muscular fibres, suffer rigor mortis, in which state they become spherical. CHAPTER III. THE FUNDAMENTAL PROPERTIES OF NERVOUS TISSUES. IN its simplest, and probably earliest form, a nerve is nothing more than a thin strand of irritable protoplasm, forming the means of FIG. 16. DIAGRAM TO ILLUSTRATE THE SIMPLEST FORMS OP A NERVOUS SYSTEM. A. An ectoderm cell e.c., with its muscular process m.p., as in Hydra. B. The ectoderm cell e.c. is connected with the muscle cell m.c. by means of the primary motor nerve m.n. C. The differentiated sensitive cell s.c. is connected by means of the sensory nerve s.n. with the central cell c.c. , which is again connected by means of the motor nerve m.n. with the muscle cell m.c. CHAP, in] PBOPKRTIRS OF NERVOUS TISSUES. 105 vital communication between a sensitive ectodermic cell exposed to extrinsic accidents, and a muscular, highly contractile cell (or a muscular process of the same cell) buried at some distance from the surface of the body, and thus less susceptible to external influences. (Fig. 16, A, B.) If in Hydra, we imagine the junction of the ectodermic muscular process with the body of its cell to be drawn out into a thin thread (as is said to be the case in some other Hydrozoa), we should have just such a primary nerve. Since there would be no need for such a means of communication to be contractile and capable of itself changing in form, but on the other hand an ad- vantage in its remaining immobile, and in its dimensions being reduced as much as possible consistent with the maintenance of irritability, the primary nerve would in the process of development lose the property of contractility in proportion as it became more irritable, i.e. more apt in the propagation of the waves of disturb- ance arising in the ectodermic cell. We have already seen that automatism, i.e. the power of initiat- ing disturbances or vital impulses, independent of any immediate disturbing event or stimulus from without, is one of the fundamen- tal properties of protoplasm. In simpler but less exact language, such a mass of protoplasm as an amoeba, though susceptible in the highest degree to influences from without, 'has a will of its own;' it executes movements which cannot be explained by reference to any changes in surrounding circumstances at the time being. A hydra has also a will of its own ; and seeing that all the constituent cells (beyond the distinction into ectoderm and endoderm) are alike, we have no reason for thinking that the will resides in one cell more than in another, but are led to infer that the protoplasm of each of the cells (of the ectoderm at least) is automatic, the will of the individual being the co-ordinated wills of the component cells. In both Hydra and Amceba the processes concerned in automatic or spontaneous impulses, though in origin independent of, are subject to and largely modified by, influences proceeding from without. Indeed the great value of automatic processes in a living body depends on the automatism being affected by external influences, and on the simple effects of stimulation being profoundly modified by automatic action. The next step of development beyond Hydra, is evidently to differentiate the single (ectodermic) cell into two cells, of which one, by division of labour, confines itself chiefly to the simple de- velopment of impulses as the result of stimulation, leaving to the other the task of automatic action, and the more complex trans- formation of the impulses generated in itself. The latter, which we may call the eminently automatic cell (though much of the work which it has to do is of the kind we shall presently speak of as reflex action), will naturally be withdrawn from the surface of the body, while the other, which we may call the eminently sensitive cell, will still retain its superficial position, so that it may most 106 SENSORY AND MOTOR NERVES. [BOOK i. X readily be affected by all changes in the world without, Fig. 16 C. And just as a primary motor nerve arises as a retained thread of communication between a sensitive cell and its muscular process, so a primary sensory nerve may be conceived of as arising as a thread of communication between an eminently sensitive cell and its twin the eminently automatic or central cell. By this arrange- ment the sensitive cell, relieved of the heavy burden of spontaneous action, is enabled to devote itself with greater vigour to the re- ception of external influences ; while the automatic cell, no longer hampered by the physical necessities of being which are imposed on the superficial cell, exposed as this is to every wind and wave, but secure in its internal retreat, is able with similar increased energy, to devote itself either to the production of spontaneous impulses, or to profoundly modifying the impulses which it receives from the sensitive cell. Naturally the muscular process or muscu- lar fibre would on the splitting of the original single cell remain in connection with the more eminently automatic. We thus arrive at that triple fundamental arrangement of a nervous system, in its simplest form, viz. a sensitive cell on the surface of the body connected by means of a sensory nerve with the internal automatic central nervous cell, which in turn is connected by means of a motor nerve with the muscular fibre-cell. We have already seen that the physiology of the motor nerve cannot without inconvenience be separated from that of the mus- cular fibre. In the same way the physiology of the sensory nerve cannot well be separated from those modifications of superficial sensitive cells which constitute the organs of sense. We may add that the special physiology of the central nervous cells can only profitably be studied in connection with the sensory organs. In the present chapter, therefore, we purpose to confine ourselves to the consideration of the simplest and most general properties of the central nervous cells. These are arranged in the vertebrate body in two great systems : the cerebro-spinal axis, and the various ganglia scattered over the body ; we shall deal with such properties only as are more or less common to the two systems. We may premise that as far as our knowledge at present goes, the processes which are concerned in the propagation of nervous impulses along a sensory nerve-trunk are identical with those which take place in a motor nerve-trunk. The phenomena of the natural nerve current, of the currents of action during the passage of an impulse and of electrotons (and these facts mark out, as we have seen, the limits of our information on this matter,) are exactly the same, whether the piece of nerve- trunk experimented on be a mixed nerve-trunk, or an almost purely motor, or an almost purely sensory nerve-trunk, or an an- terior or posterior nerve-root, or the special sensory nerve of a particular sense, such as the optic nerve. In both sensory and motor nerves the changes accompanying a nervous impulse are transmitted equally well in both directions. CHAP, in.] PROPERTIES OF NERVOUS TISSUES. 107 We seem justified in concluding that the events which occur in a sensory nerve when it is an instrument of sensation, differ from those which take place in a motor nerve when that is an instru- ment of movement, only so far as the sensory impulses are gener- ated by particular processes which bear the stamp of the sensory cell in which they originated, while the motor impulses are gener- ated by particular processes which bear the stamp of the central nervous cells in which they in turn originated. All sensory im- pulses appear to be tetanic iri nature, i. e. to be composed of a series of constituent simple impulses ; and it is probable that while the motor impulses which proceed from the central nervous system to the muscles are composed of simple impulses repeated with the same rapidity, and thus giving rise to the same muscular note (p. 52), the sensory impulses which proceed from the periph- eral sense organs to the central nervous system vary exceedingly as to the way in which their constituent simple impulses are com- bined. It is indeed possible that the complex sensory impulses which give rise, for instance, to sight and touch respectively, may differ only in the wave-length, so to speak, of their constituent simple impulses, much in the same way as red light differs from blue light. In the scheme sketched out above, the same central nervous cell is supposed to be engaged at once, both in originating auto- matic actions and in modifying sensory impulses (i.e. impulses proceeding from the superficial sensitive cells) previous to these being passed on to the muscular fibre. It is evident that, where two or more central nervous cells occur together, a further differen- tiation would be of advantage : a differentiation into cells which, though still susceptible of being influenced from without, should be more especially restricted to automatic action, and into cells which should forego their automatism for the sake of being more efficient in modifying sensory impulses, with a view of transmuting them into motor impulses, and so of giving rise to appropriate move- ments. We thus gain the fundamental and primary differentiation of the work of a central nervous system into automatic and into reflex operations. These are very clearly manifested by the brain and spinal cord, and probably also, though this is less certain, by the sporadic ganglia. Automatic Actions. In the vertebrate animal the highest form of automatism, individual volition, with which conscious intelli- fence is associated, is a function of certain parts of the brain, 'here are evidences of the existence in the brain of other forms of automatism. All these will be considered in detail hereafter. In the spinal cord separated from the brain by section of the medulla oblongata, it becomes difficult to draw a line between purely automatic and reflex actions. Thus, when we come to deal with respiration, we shall see that while there can be no doubt that 108 AUTOMATIC ACTIONS. [BOOK i. the muscular respiratory apparatus is kept at work by impulses proceeding, in a rhythmic manner, from a group of nerve-cells, or respiratory nervous centre, in the medulla oblongata it is an open question whether those impulses, whose generation is certainly modified by centripetal impulses passing to the centre along various nerves, are absolutely automatic: i.e. whether they can continue to make their appearance when no influences whatever from without are brought to bear upon the centre. Similar doubts hover round other automatic functions of the spinal cord. We shall see hereafter reasons for speaking of the existence in the medulla oblongata of a vaso-motor centre, that is of a group of nerve-cells, whence impulses habitually proceed along the so- called vaso-motor nerves to the muscular coats of the small arteries, and keep these vessels in a state of semi-contraction or tone. Here too it is doubtful whether these motor or efferent impulses can be generated in the absence of all sensory or afferent impulses. The posterior lymphatic hearts of the frog are connected by the small tenth pair of spinal nerves with the grey matter of the termination of the spinal cord, in such a manner that destruction of that part of the spinal cord or section of the tenth nerves apparently puts an end to the rhythmic pulsations of the lymphatic hearts. Here it would seem as if rhythmic impulses were automatically generated in the lower end of the cord, and proceeded along the efferent nerves to the hearts, thus determining their rhythmic pulsations. But if it be true, as asserted, that the rhythmic pulsations, though arrested for a time by severance of the nerves, or destruction of the lower end of the cord, are after a while resumed, then these too, can be no longer counted among the automatic phenomena of the cord. And so in other instances which we shall meet with in the course of this book. The existence of automatism, then, even of this comparatively simple character, is at least doubtful. That all higher automatism comparable at least to that of the cerebral hemi- spheres is absent, may be regarded as certain. In the sporadic ganglia the evidence of automatic action seems more clear, and yet is by no means absolutely decisive. The beat of the heart is a typical automatic action : and, since the heart will continue to beat for some time when isolated from the rest of the body (that of a cold-blooded animal continuing to beat for hours, or even days), its automatism must lie in its own structures. When, however, we come to discuss the beat of the heart in detail, we shall find that it is still an open question whether the automa- tism is confined to the ganglia (either of the sinus venosus, auricles, or auriculo-ventricular boundary), or shared in by the muscular tissue : whether, in fact, the automatism is a muscular automatism like that of a ciliated cell, or the automatism of a differentiated nerve-ceil. And yet the heart is the case where the automatism of the ganglia seems clearest. The peristaltic contractions of the alimentary canal are auto- CHAP. IIL] AUTOMATIC ACTIONS. 109 matic movements ; T,re cannot speak of them as being simply excited by the presence of food in the canal, any more than we can say that the beat of the heart is caused by the presence of blood in its cavities. When absent they may be set agoing, and when present may be stopped without any change in the contents of the canal. They may, of course, be influenced by the contents, just as the beat of the heart is, influenced by the quantity of blood in its cavities. Throughout the intestines are found the nerve plexus of Auerbach and that of Meissner ; to each or both of these the automatism of the peristaltic movements has been referred. Yet in the ureter, whose peristaltic waves of contraction closely resemble that of the intes- tine, automatism is evident in the middle third of its length even when completely isolated; in which region (in the rabbit at least), according to Engelmann, ganglia, and indeed nerve-cells, are entirely absent. Thus, while in the spinal cord there is doubt whether purely automatic, as stringently distinguished from reflex, actions take place, in the case of the sporadic ganglia the uncertainty is whether the clearly automatic movements of the organs with which the ganglia are associated are due to the nerve-cells of the ganglia, or to the muscular tissue itself. Reflex Actions. The spinal cord offers the best and most numerous examples of reflex action. In fact, reflex action may be said to be, par excellence, the function of the spinal cord ; and the grey matter of the spinal cord may be broadly considered as a multitude of reflex centres. We have here to consider the cord merely in its general aspects ; and must postpone the special con- sideration of the particular forms of reflex action which it exhibits, as they come before us in various connections, or until we have to deal with it as part of the great central nervous machinery. In its simplest form a reflex action is as follows. All the ma- chinery it demands is (a) a sentient surface (external or internal), connected by (6) a sensory, or — to adopt the more general and better term — afferent nerve, with (c) a central nerve-cell or group of connected nerve-cells, which is in relation by means of (d) a motor, or efferent, nerve, or nerves, with (e) a muscle, or muscles, or some other irritable tissue-elements, capable of responding by some change in their condition, to the advent of efferent impulses. The afferent impulses started in a, passing along 6, reach the centre c, are there transmuted into efferent impulses, which, passing along d, finally reach e, and there produce a cognisable effect. The essence of a reflex action consists in the transmutation, by means of the irritable protoplasm of a nerve-cell, of afferent into efferent impulses. As an approach to a knowledge of the nature of that transmutation, we jnay lay down the following propositions. The number, intensity, character and distribution of the efferent impulses are determined chiefly by the events which take place in the 110 REFLEX ACTIONS. [Boon i. protoplasm of the reflex centre. It is not that the afferent impulse is simply reflected in the nerve-cell, and so becomes with but little change an efferent impulse. On the contrary, an afferent impulse passing along a single sensory fibre may give rise to efferent im- pulses passing along many motor nerves, and call forth the most complex movements. An instance of this disproportion of the afferent and efferent impulses is seen in the case where the contact with the glottis of a foreign body so insignificant as a hair causes a violent fit of coughing. Under such circumstances a slight contact with the mucous membrane, such as could not possibly give rise to anything more than few and feeble impulses, may cause the discharge of so many efferent impulses along so many motor nerves, that not only all the respiratory muscles, but almost all the muscles of the body, are brought into action. Similar though less striking instances of how incommensurate are afferent and efferent impulses may be seen in most reflex actions. In fact, the afferent impulse when it reaches the protoplasm of the nerve produces there a series of changes, of explosive disturbances, which, except that the nerve-cell does not in any way change its form, may be likened to the explosive changes in a muscle on the arrival of an impulse along its motor nerve1. The changes in a nerve-cell during reflex action, we might say during any form of activity, far more closely resemble the changes during a muscular contraction than those which accompany the passage along a nerve of either an afferent or efferent impulse. The simple passage along a nerve is accompanied by little expenditure of energy ; it neither gains nor loses force to any great extent as it progresses. The transmutation in a nerve- cell is most probably (though the direct proofs are perhaps wanting) accompanied by a large expenditure of energy, and a simple nervous impulse in suffering the transmutation in a central nervous organ may accumulate in intensity to a very remarkable extent, as in the case of strychnia poisoning. £^ The nature of the efferent impulses is, however, determined also ' by the nature of the afferent impulses. The nerve-centre remaining in the same condition, the stronger or more numerous impulses will give rise to the more forcible or more comprehensive movements. Thus if the flank of a brainless frog be very lightly touched, the only reflex movement which is visible is a slight twitching of the muscles lying immediately underneath the spot of skin stimulated. If the stimulus be increased, the movements will spread to the hind-leg of the same side, which frequently will execute a movement calculated to push or wipe away the stimulus. By forcibly pinching the same spot of skin, or otherwise increasing the stimulus, the resulting movements may be led to embrace the fore-leg of the same side, then the opposite side, and finally, almost all the muscles of the body. In other words, the disturbance 1 The question as to how far these processes in the central cells are connected with the development of consciousness is here purposely passed over. CHAP, in ] REFLEX ACTIONS. Ill set going in the central nerve-cells, confined when the stimulus is slight to a few nerve-cells and to a few nerve-fibres, overflows, so to speak, when the stimulus is increased, on to a number of adjoining and (we must conclude) connected cells, and thus throws impulses into a larger and larger number of efferent nerves. Certain relations may be observed between the sentient spot stimulated and the resulting movement. In the simplest cases of reflex action this relation is merely of such a kind that the muscles thrown into action are those governed by a motor nerve which is the fellow of the sensory nerve, the stimulation of which calls forth the movement. In the more complex reflex actions of the brainless frog, and in other cases, the relation is of such a kind that the resulting movement bears an adaptation to the stimulus : the foot is with- drawn from the stimulus, or the movement is calculated to push or wipe away the stimulus. In other words, a certain purpose is evident in the reflex action. Thus in all cases, except perhaps the very simplest, the move- ments called forth by a reflex action are exceedingly complex, com- pared with those which result from the direct stimulation of a motor trunk. When the peripheral stump of a divided sciatic nerve is stimulated with the interrupted current, the muscles of the leg are at once thrown into tetanus, continue in the same rigid condition during the passage of the current, and relax immediately on the current being shut off. When the same current is applied for a second only, to the skin of the flank of a brainless frog, the leg is drawn up and the foot rapidly swept over the spot irritated, as if to wipe away the irritation ; but this movement is a complex one, requiring the contraction of particular muscles in a definite sequence, with a carefully adjusted proportion between the amounts of contraction of the individual muscles. And this complex move- ment, this balanced and arranged series of contractions, may be repeated more than once as the result of a single stimulation of the skin. When a deep breath is caused by a dash of cold water, the same co-ordinated and carefully arranged series of contractions is also seen to result, as part of a reflex action, from a simple stimulus. And many more examples might be given. In such cases as these, part of the complexity may be due to the fact that the stimulus is applied to terminal sensory organs and not directly to a nerve-trunk. As we shall see in speaking of the senses, the impulses which are generated by the application of a stimulus to a sensory organ are more complex than those which result from the direct stimulation of a sensory nerve-trunk. Never- theless, reflex actions of great if not of equal complexity may be induced by stimuli applied directly to a nerve-trunk. We are therefore obliged to conclude that in a reflex action, the processes which are originated in the central nerve-cells by the arrival of even simple impulses along afferent nerves may be highly complex; and that it is the constitution and condition of the nerve-cells which 112 GANGLIA. [BOOK i. determine the complexity and character of the movements which are affected. In other words, the central nerve-cells concerned in reflex actions are to be regarded as constituting a sort of molecular machinery, the character of the resulting movements being deter- mined by the nature of the machinery set going and its condition at the time being, the character and amount of the afferent impulses determining exactly what parts of and how far the central machinery is thrown into action. Actions of Sporadic Ganglia. Seeing that in the spinal cord the nerve-cells undoubtedly are the central structures concerned in the production of reflex action, it is only natural to infer that the nerve-cells of the sporadic ganglia possess similar functions. Yet the evidence of this is at present of very limited extent. With regard to the ganglia on the posterior roots of the spinal nerves, all the evidence goes to shew that these possess no power whatever of reflex action. Of the larger ganglia visible to the naked eye, such as the ciliary, otic, &c., we have indications of reflex action in one only, viz. the submaxillary, and these indications are, as we shall see in treating of the salivary glands, disputed. We have no exact proof that the ganglia of the sympathetic chain, or of the larger sympathetic plexuses, are capable of executing reflex actions. In fact, in searching for reflex actions in ganglia, we are reduced to the small microscopic groups of cells buried in the midst of the tissues to which they belong, such as the ganglia of the heart, of the intestine, the bladder, &c. When a quiescent frog's heart is stimulated by touching its surface, a beat takes place. This beat is, as we shall see, a complex, co-ordinated move- ment, very similar to a reflex action brought about by means of the spinal cord; and in its production it is probable that the cardiac ganglia are in some way concerned. When a quiescent intestine is touched or otherwise stimulated, peristaltic action is set up. Here again the ganglia present in the intestinal walls may be supposed to play a part ; but this movement is much more simple than the beat of the heart, and as regards it, and more especially as regards the similar peristaltic action of the ureter, it becomes difficult to distinguish between a movement governed by ganglia, and one produced by direct stimulation of the muscular fibres. We have seen that the great distinction between a reflex action and a movement caused by direct stimulation of a nerve or of a muscle lies in the greater complexity of the former ; and we may readily imagine, that by continued simplification of the central nervous machinery, the two might in the end become so much alike as to be almost indistinguishable. In the vertebrate animal then the chief seat of reflex action is the spinal cord and brain. We say 'and brain' because, as we shall see later on, the brain, in addition to its automatism, is as busy a field of reflex action as the spinal cord. CHAP, in.] PROPERTIES OF NERVOUS TISSUES. 113 Inhibition. In speaking of reflex action, we took it for granted that the spinal cord was, at the moment of the arrival of the afferent impulses at the central nerve-cells, in a quiescent state ; that the nerve-cells themselves were not engaged in any auto- matic action. We were justified in doing so, because as far as the muscles generally of the body are concerned, the spinal cord is in a brainless frog perfectly quiescent; an afferent impulse reaching an ordinary nerve-cell of the spinal cord does not find it preoccupied in discharging efferent impulses to the muscles with which by means of nerve-fibres it is connected. But what happens when afferent impulses reach a nerve-cell or a group of nerve-cells already engaged in automatic action ? We have already referred to an automatic respiratory centre in the medulla oblongata. We may here premise, what we shall shew more in detail hereafter, that the pneumogastric nerve is peculiarly associated as an afferent nerve with this respiratory centre. Now if the central end of the divided pneumogastric be stimulated at the time when the respiratory centre is engaged in its accustomed rhythmic action, sending out complex co- ordinated impulses of inspiration (and of expiration) at regular intervals, one of two things may happen, the choice of events being determined by circumstances which need not be considered here. The most striking event, and the one which interests us now, is that the respiratory rhythm is slowed or stopped altogether. That is to say, afferent impulses which, under ordinary con- ditions, would, on reaching a quiescent nervous centre, give rise to movement, may, under certain conditions, when brought to bear on an already active automatic nervous centre, check or stop movement by interfering with the production of efferent impulses in that centre. This stopping or checking an already present action is spoken of as an ' inhibition ; ' and the effect of the pneumogastric in this way on the respiratory centre is spoken of as ' the inhibitory action of the pneumogastric on the respiratory centre.' The other event is that the respiratory rhythm is accelerated. We shall hereafter discuss the explanation of the two events. We may however state that according to one view the pneumo- gastric contains among its afferent fibres two sets, which are either of a different nature from each other, or are so differently connected with the respiratory centre, that impulses arriving along one stop, while those arriving along the other quicken, the action of that centre. Hence, the one set are called ' inhibitory,' the other ' ac- celerating' or 'augmenting' fibres. But we are concerned at present only with the fact that the stimulation of a nerve may produce either inhibitory or augmentative effects. Similarly the vaso-motor centre in the medulla may, by im- pulses arriving along various afferent tracts, be inhibited, during jr. 8 114 INHIBITION. [BooK i. CHAP. in. which the muscular walls of various arteries are relaxed ; or augmented, whereby the tonic contraction of various arteries is increased. The most striking instance of inhibition is offered by the heart. If when the heart is beating well and regularly, the pneumogastric be divided, and the peripheral portion be stimulated even for a very short time with an interrupted current, the heart is immediately brought to a standstill. Its beats are arrested, it lies perfectly flaccid and motionless, and it is not till after some little time that it recommences its beat. Here again it is usually said that the pneumogastric contains efferent cardio-inhibitory fibres, impulses passing along which from the medulla stop the automatic actions of the cardiac ganglia; the respiratory inhibitory fibres of the same nerve are afferent, i.e. impulses pass along them up to the medulla. Though inhibition is most clearly seen in the case of automatic actions, other actions may be similarly inhibited. Thus, as we shall see later on, the reflex actions of the spinal cord may, by appropriate means, be inhibited. To sum up, then, the most fundamental properties of nervous tissues. Nerve-fibres are concerned in the propagation only, not in the origination or transformation, of nervous impulses. As far as is at present known, impulses are propagated in the same manner along both sensory and motor nerves. Sensory impulses differ from motor impulses inasmuch as the former are generated in sensory organs and pass up to the central nervous cells, while the latter pass from the central nervous cells to the muscles or to some other peripheral organs. The operations of the nerve-cells are either automatic or reflex. In both an automatic and a reflex action, the diversity and the co-ordination of the impulses are determined by the condition of the nerve-cells. During the passage of an impulse along a nerve- fibre, there is no augmentation of energy ; in passing through a nerve-cell, the augmentation may be, and generally is, most con- siderable. When afferent impulses reach a centre already in action, the activity of that centre may, according to circumstances, be either depressed or exalted, may be ' inhibited ' or ' augmented.' CHAPTEE IV. THE VASCULAR MECHANISM. IN order that the blood may be a satisfactory medium of com- munication between all the tissues of the body, two things are necessary. In the first place, there must be through all parts of the body a flow of blood, of a certain rapidity and general con- stancy. In the second place, this flow must be susceptible of both general and local modifications. In order that any tissue or organ may readily adapt itself to changes of circumstances (action, repose, &c.), it is of advantage that the quantity of blood passing to it should be not absolutely constant, but capable of variation. In order that the material equilibrium of the body may be main- tained as exactly as possible, it is desirable that the loading of the blood with substances proceeding from the unwonted activity of any one tissue, should be accompanied by a greater flow of blood through some excretory or metabolic tissue by which these substances may be removed. Similarly it is of advantage to the body that the general flow of blood should in some circum- stances be more energetic, and in others less so, than normal. The first of these conditions is dependent on the mechanical and physical properties of the vascular mechanism ; and the problems connected with it are almost exclusively mechanical or physical problems. The second of these conditions depends on the intervention of the nervous system ; and the problems con- nected with it are essentially physiological problems. 8—2 116 PHYSICAL PHENOMENA OF CIRCULATION. [BOOK i, I. THE PHYSICAL PHENOMENA OF THE CIRCULATION. The apparatus concerned in the Maintenance of the Normal Flow is composed of the following factors : 1. The heart, beating rhythmically by virtue of its contractility and intrinsic mechanisms, and at each beat discharging a certain quantity of blood into the aorta. [For simplicity's sake we omit for the present the pulmonary circulation.] 2. The arteries, highly elastic throughout, with a circular mus- cular element increasing in relative importance as the arteries diminish in size. It must not be forgotten that the muscular element is also elastic. When an artery divides, the united sectional area of the branches is, as a rule, larger than the sectional area of the stem. Thus the collective capacity of the arteries is continually (and rapidly) increasing from the heart towards the capillaries. If all the arterial branches were fused together, they would form a funnel, with its apex at the aorta. The united sectional area of the capillaries has been calculated by Vierordt to amount to several (eight ?) hundred times that of the aorta. 3. The capillaries, channels of exceedingly small but variable size. Their walls are elastic (as shewn by their behaviour during the passage of blood-corpuscles through them), exceedingly thin and permeable. They are permeable both in the sense of allowing fluids to pass through them by osmosis, and also in the sense of allowing white and red corpuscles to traverse them. The small arteries and veins, which gradually pass into and from the capil- laries properly so called, are similarly permeable, the more so, the smaller they are. 4. The veins, less elastic than the arteries (the difference beiog especially marked when both sets of vessels become distended) and with a very variable muscular element. The united sectional area of the veins diminishes from the capillaries to the heart, thus resem- bling the arteries ; but the united sectional area of the venae cavae at their junction with the right auricle is greater than that of the aorta at its origin. (The proportion is nearly two to one.) The total capacity of the veins is similarly much greater than that of the arteries. The veins alone can hold the total mass of blood which in life is distributed over both arteries and veins. Indeed nearly the whole blood is capable of being received by what is merely a part of the venous system, viz. the vena portaa and its branches. Such veins as are for various reasons liable to a reflux of blood from the heart towards the capillaries are provided with valves. SEC. 1. MAIN GENEBAL FACTS OF THE CIRCULATION. 1. The Capillary Circulation. If the web of a frog's foot be examined with a microscope, the blood, as judged of by the movements of the corpuscles, is seen to be passing in a continuous stream from the small arteries through the capillaries to the veins. The velocity is greater in the arteries than in the veins, and greater in both than in the capillaries. In the arteries faint pulsations, synchronous with the heart's beat, are occasionally visible ; and not unfrequently varia- tions in velocity and in the distribution of the blood, due to causes which will be hereafter discussed, are witnessed from time to time. The flow through the smaller capillaries is very variable. Sometimes the corpuscles are seen passing through the channel in single file with great regularity; at other times, they may be few and far between. Sometimes the corpuscle may remain stationary at the entrance into a capillary, the channel itself being for some little distance entirely free from corpuscles. Any one of these conditions readily passes into another ; and, especially with a somewhat feeble circulation, instances of all of them may be seen in the same field of the microscope. It is only when the vessels of the web are unusually full of blood that all the capillaries can be seen equally filled with corpuscles. The long oval red corpuscle moves with its long axis parallel to the stream, frequently rotating on its long axis and sometimes on its short axis. The flexibility and elasticity of a corpuscle are well seen when it is being driven into a 118 THE CAPILLARY CIRCULATION. [BOOK i. capillary narrower than itself, or when it becomes temporarily lodged at the angle between two diverging channels. The small mam- malian corpuscles rotate largely as they are driven along. In the web of the frog's foot the average velocity with which the corpuscles move may be put down as about half a millimetre in a second. In the human retina, the velocity of the capillary flow has, by indirect methods, been estimated at "75 mm. per sec. The movement of the blood in the capillaries is very slow, compared with that in the arteries or even in the veins. In the larger capillaries, and especially in the small arteries and veins which permit the passage of several corpuscles abreast, it is observed that the red corpuscles run in the middle of the channel, forming a coloured core, between which and the sides of the vessel all round is a layer, which has been called the ' inert layer,' or better the 'plasmatic layer,' containing no red corpuscles. This division into a plasmatic layer and an axial stream is due to the fact that in any stream passing through a closed channel the friction is greatest at the immediate sides, and diminishes towards the axis. The corpuscles pass where the friction is least, in the axis. A quite similar axial core is seen when any fine particles are driven with a sufficient velocity in a stream of fluid through a narrow tube. As the velocity is diminished the axial core becomes less marked and disappears. In the plasmatic layer, especially in that of the veins, are frequently seen white corpuscles, sometimes clinging to the sides of the vessel, sometimes rolling slowly along, and in general moving irregularly, and often in jerks. The greater the velocity of the flow of blood, the fewer the white corpuscles in the plasmatic layer, and with a very rapid flow they, as well as the red corpuscles, may be all confined to the axial stream. The presence of the white corpuscles in the plasmatic layer has been attributed to their being specifically lighter than the red corpuscles, it being affirmed that when fine particles of two kinds, one lighter than the other, are driven through a narrow tube, the heavier particles flow in the axis and the lighter in the more peripheral portions of the stream. This however has been disputed, and the phenomenon explained by the white corpuscles being dis- tinctly more adhesive than the red, as is seen by the manner in which they become fixed to the glass slide and cover-slip when a drop of blood is mounted for microscopical examination. By reason of this adhesiveness which possibly may vary with the varying nutritive conditions of the corpuscles and of the blood- vessels, the white corpuscles, it is urged, become temporarily attached to the walls of the vessel, and consequently appear in the plasmatic layer. The resistance to the flow of blood thus caused by the friction generated in so many minute passages, is one of the most important physical facts in the circulation. In the large arteries the friction is small; it increases as they divide, and receives a very great CHAP, iv.] THE VASCULAR MECHANISM. 119 120 THE FLOW IN THE ARTERIES. [BOOK i. FIG. 17. APPARATUS FOR INVESTIGATING BLOOD-PRESSURE. At the upper right-hand corner, is seen, on an enlarged scale, the carotid artery, clamped by the forceps bd, with the vagus nerve v lying by its side. The artery has been ligatured at V and the glass cannula c has been introduced into the artery between the ligature I' and the forceps bd, and secured in position by the ligature I. The shrunken artery on the distal side of the cannula is seen at ca'. p.b. is a box containing a bottle holding a saturated solution of sodium car- bonate or a solution of sodium bicarbonate of sp. gr. 1083, and capable of being raised or lowered at pleasure. The solution flows by the tube p.t. regulated by the clamp c" into the tube t. A syringe, with a stop-cock, may be substituted for the bottle, and attached at c". This indeed is in many respects a more convenient plan. The tube t is connected with the leaden tube i, and the stopcock c with the mano- meter, of which ra is the descending and ra' the ascending limb, and s the support. The mercury in the ascending limb bears on its surface the float fl, a long rod attached to which is fitted with the pen p, writing on the recording surface r. The clamp cl. at the end of the tube t has an arrangement shewn on a larger scale at the right hand upper corner. The descending tube m of the manometer, and the tube t being completely filled along its whole length with fluid to the exclusion of all air, the cannula c is filled with fluid, slipped into the open end of the thick- walled india-rubber tube i, until it meets the tube t (whose position within the india-rubber tube is shewn by the dotted lines), and is then securely fixed in this position by the clamp cl. The stopcocks c and c" are now opened, and the pressure-bottle raised or fluid driven in by the syringe until the mercury hi the manometer is raised to the required height. The clamp c" is then closed and the forceps bd removed from the artery. The pressure of the blood in the carotid ca. is in consequence brought to bear through t upon the mercury in the manometer. addition in the minute arteries and capillaries. We may speak of it therefore as the 'peripheral friction5 and the resistance which it offers as the 'peripheral resistance.' It need perhaps hardly be said that this peripheral friction not only opposes the flow of blood through the capillaries themselves, but, working backwards along the whole arterial system, has to be met by the heart at each systole of the ventricle. It is well known that when any portion of the skin is pressed upon, it becomes pale and bloodless; this is due to the pressure driving the blood out of the capillaries and minute vessels and preventing any fresh blood entering into them. By carefully investigating the amount of pressure necessary to prevent the blood entering the capillaries and minute arteries of the web of the frog's foot, or of the skin beneath the nail in man or elsewhere, the internal pressure which the blood is exercising on the walls of the capillaries and minute arteries and veins may be approximately determined. In the frog's web this has been found to be equal to about 7 or 11 mm. mercury. 2. The Flow in the Arteries. When an artery is severed, the flow from the proximal section is not equable, but comes in jets, which correspond to the heart- CHAP, iv.] THE VASCULAR MECHANISM. 121 beats, though the flow does not cease between the jets. The blood is ejected with considerable force; thus, in Dr Stephen Hales' experiments, when the crural artery of a mare was severed, the jet, even after much loss of blood, rose to the height of two feet. The larger the artery and the nearer to the heart, the greater the force with which the blood issues, and the more marked the intermittence of the flow. The flow from the distal section may be very slight, or may take place with considerable force and marked intermittence, according to the amount of collateral communication. Arterial pressure. If a mercury (or other) manometer, Fig. 17m, m, be connected with a large artery, e.g. the carotid, in such a way that while the blood is allowed to flow uninterruptedly along the artery, there is free communication between the interior of the artery and the proximal (descending) limb of the manometer, the following facts are observed. Immediately that communication is established between the interior of the artery and the manometer, blood rushes from the former into the latter, driving some of the mercury from the de- scending limb into the ascending limb, and thus causing the level of the mercury in the ascending limb to rise rapidly. This rise is marked by jerks corresponding with the heart-beats. Having reached a certain level, the mercury ceases to rise any more. It does not, however, remain absolutely at rest, but undergoes oscilla- tions ; it keeps rising and falling. Each rise, which is very slight compared with the total height to which the mercury has risen, has the same rhythm as the systole of the ventricle. Similarly, each fall corresponds with the diastole. If a float, swimming on the top of the mercury in the ascending limb of the manometer, and bearing a brush or other marker, be brought to bear on a travelling surface, some such tracing as that represented in Fig. 18 will be described. Each of the smaller FIG. 18. TRACING OF ARTERIAL PRESSURE WITH A MERCURY MANOMETER. The smaller curves p p are the pulse-curves. The space from r to r embraces a respiratory undulation. The tracing is taken from a dog, and the irregularities visible in it are those frequently met with in this animaL curves (p, p) corresponds to a heart-beat, the rise corresponding to the systole and the fall to the diastole of the ventricle. The larger undulations (r, r) in the tracing, which are respiratory in origin, 122 ARTERIAL PRESSURE, [BOOK i. will be discussed hereafter. This observation teaches us that the blood, as it is passing along the carotid artery, is capable of support- ing a column of mercury of a certain height (measured by the difference of level between the mercury in the descending limb, and that in the ascending limb, of the manometer), when the mercury is placed in direct communication with the side of the stream of blood. In other words, the blood, as it passes through the artery, exerts a lateral pressure on the sides of the artery, equal to so many millimeters of mercury. In this lateral pressure we have further to distinguish between the slighter oscillations corre- sponding with the heart-beats, and a mean pressure above and below which the oscillations range. A similar mean pressure with similar oscillations is found, when any artery of the body is examined in the same way. In all arteries the blood exerts a certain pressure on the walls of the vessels which contain it. This is generally spoken of as arterial pressure or arterial tension, and the pressure in the aorta of any animal is usually spoken of as its blood- pressure. Description Of Experiment. The carotid, or other vessel, is laid bare, clamped in two places and divided between the clamps. Into the cut ends is inserted a hollow |— piece of the same bore as the artery, the cross portion forming the continuation of the artery. The other portion is connected by means of a non-elastic flexible tube with the descending limb of the manometer. In order to avoid loss of blood, fluid is in- jected into the flexible tube until the mercury in the manometer stands a very little below what may be beforehand guessed at as the probable mean pressure. The fluid chosen is a saturated solution of sodium car- bonate or a solution of sodium bicarbonate of sp. gr. 1083, with a view to hinder the coagulation of the blood in the tube. When the clamps are removed from the artery the blood rushes through the cross of the f— piece. Some passes into the side limb of the {— piece and continues to do so until the mean pressure is quite reached. Thenceforward there is no more escape ; but the pressure continues in the interior of the |— piece, is transmitted along the connecting tube to the manometer, and the mercury continues to stand at a height indicative of the mean pressure with oscillations corresponding to the heart's beats. Practically the use of the |— piece is found inconvenient. Accordingly the general custom is to ligature the artery, to place a clamp on the vessel on the proximal side of the ligature, and to introduce a straight cannula, Fig. 17 c, connected with the manometer, into the artery between the ligature and the clamp, and to secure it in that position. In this case, on loosing the clamp, the whole column of blood in the artery is brought to bear on the manometer, and the tracings taken illustrate the lateral pressure not of the artery in which the cannula has been placed, hut of the vessel (aorta &c. as the case may be) of which it is itself a branch. Tracings of the movements of the column of mercury in the mano- meter may be taken either on a smoked surface of a revolving cylinder (Fig. 1), or by means of a brush and ink on a continuous roll of paper, as iii the more complex kymograph (Fig. 19). CHAP, iv.] THE VASCULAR MECHANISM. 123 In such a mercury manometer, the inertia of the mercury obscures many of the features of the minor curves caused by the heart-beats. When therefore these, rather than variations in the mean pressure, are being studied, other methods have to be adopted. The average pressure of the blood in the same body is greatest in the largest arteries, and diminishes as the arteries get less ; but the fall is a very gradual one until the smallest arteries are reached, in which it becomes very rapid. In the carotid of the horse, the mean arterial pressure varies from 150 to 200 mm. of mercury ; of the dog from 100 to 175 ; of the rabbit from 50 to 90. In the carotid of man it probably amounts to 150 or 200. FIG. 19. LARGE KYMOGRAPH WITH CONTINUOUS ROLL OF PAPER. The clock-work machinery, some of the details of which are seen, unrolls the paper from the roll C, carries it smoothly over the cylinder B, and then winds it up into the roll A. Two electromagnetic markers are seen in the position in which they record their movements on the paper as it - travels over B. The manometer, or any other recording instrument used, can be fixed either in the notch immediately in front of B or in any other position that may be desired. Since in all arteries the blood is pressing on the arterial walls with some considerable force, all the arteries must be in a state of permanent distension, so long as blood is flowing through them from the heart. When the blood-current is cut off, as by a ligature, this expansion or distension disappears. Not only is there a permanent expansion corresponding to the mean pressure, but just as the mercury in the manometer rises above the level of mean pressure at each systole of the heart, and 124 THE VELOCITY OF THE FLOW. [BOOK i. falls below it at each diastole, so at any spot in the artery there is for each heart-beat a temporary expansion succeeded by temporary contraction, the diameter of the artery in its temporary expansions and contractions oscillating, in correspondence with the oscillations of the manometer, beyond and within the diameter of permanent expansion. These temporary expansions constitute what is called the pulse, and will be discussed more fully hereafter. The velocity of the flow. When even a small artery is severed a considerable quantity of blood escapes from the proximal cut end in a very short space of time. That is to say, the blood moves in the arteries from the heart to the capillaries, with a very con- siderable velocity. By various methods, this velocity of the blood- current has been measured at different parts of the arterial system; the results, owing to imperfections in the methods employed, cannot be regarded as satisfactorily exact, but may be accepted as approxi- mately true. The velocity of the arterial stream is greatest in the largest arteries, and diminishes from the heart to the capillaries, pari passu with the increase of the width of the bed, i.e. with the increase of the united sectional area. Methods. The Hsemadromometer of Volkmann. An artery, e.g. a carotid, is clamped in two places, and divided between the clamps. Two cannulse, of a bore as nearly equal as possible to that of the artery, or of a known bore, are inserted in the two ends. The two cannulse are con- nected by means of two stop-cocks, which work together, with the two ends of a long glass tube, bent in the shape of a U, and filled with normal saline solution, or with a coloured innocuous fluid. The clamps on the artery being released, a turn of the stop-cocks permits the blood to enter the proximal end of the long U tube, along which it courses, driving the fluid out into the artery through the distal end. Attached to the tube is a graduated scale, by means of which the velocity with which the blood flows along the tube may be read off. Even supposing the cannulss to be of the same bore as the artery, it is evident that the conditions of the flow through the tube are such as will only admit of the result thus gained being considered as an approximative estimation of the real velocity in the artery itself. The Rheometer (Stromuhr) of Ludwig. This consists of two glass bulbs A and 2i, Fig. 20, communicating above with each other and with the common tube C by which they can be filled. Their lower ends are fixed in the metal disc Z>, which can be made to rotate, through two right angles, round the lower disc E. In the upper disc are two holes a and b continuous with A and B respectively, and in the lower disc are two similar holes a' and b', similarly continuous with the tubes H and G. Hence, in the position of the discs shewn in the figure, the tube G is continuous through the two discs with the bulb A and the tube H with the bulb B. On turning the disc D through two right angles the tube G becomes continuous with B instead of A, and the tube-ZT with .4 instead of B. There is a further arrangement, omitted from the figure for the sake of simplicity, by which when the disc D is turned through one CHAP. iv.J THE VASCULAR MECHANISM. 125 instead of two right angles from either of the above positions, G becomes directly continuous with H, both being completely shut off from the bulbs. FlG. 20. DIAGRAMMATIC REPRESENTATION OF LUDWIG'S SlEOMTJHR. The ends of the tubes H and G are made to fit exactly into two cannulae inserted into the two cut ends of the artery about to be experi- mented upon, and having a bore as nearly equal as possible to that of the artery. The method of experimenting is as follows. The disc D, being placed in the intermediate position, so that a and b are both cut off from a and b', the bulb A is filled with pure olive oil up to the mark a?, and the bulb B, the rest of A, and the junction C, with defibrinated blood; and C is then clamped. The tubes H and G are also filled with de- fibrinated blood, and G is inserted into the cannula of the central, H into that of the peripheral, end of the artery. On removing the clamps from the artery the blood flows through G to ff, and so back into the artery. The observation now begins by turning the disc D into the position shewn in the figure ; the blood then flows into A, driving the oil there contained out before it into the bulb B, in the direction of the arrow, the defibrinated blood previously present in B passing by H into the artery, and so into the system. At the moment that the blood is seen to rise to the mark cc, the disc D is with all possible rapidity turned through two right angles; and thus -the bulb B, now largely filled with oil, placed in communication with G. The blood-stream now drives the oil back into A, and the new blood in A through H into the artery. As soon as the oil has wholly returned to its original position, the disc is again turned round, and A once more placed in communication with G, and the oil once more driven from A to B. And this is repeated several times, indeed generally until the clotting of the blood or the admixture of the oil with the blood puts an end to the experiment. Thus the flow of blood is used to fill alternately with blood or oil the space of the bulb A, whose cavity as far as the mark x has been exactly measured; hence if the number of times in any given time the disc D has to be turned round be known, the number of times A has been filled is also known, and thus the quantity of blood which has passed in that time through the 126 MEASUREMENTS OF VELOCITY OF FLOW. [BOOK r. cannula connected with the tube G is directly measured. For instance, supposing that the quantity held by the bulb A when filled up to the mark x is 5 c.c., and supposing that from the moment of allowing the first 5 c.c. of blood to begin to enter the tube to the moment when the escape of the last 5 c.c. from the artery into the tube was complete, 100 seconds had elapsed, during which time 5 c.c. had been received 10 times into the tube from the artery (all but the last 5 c.c. being returned into the distal portion of the artery), obviously '5 c.c. of blood had flowed from the proximal section of the artery in one second. Hence supposing that the diameter of the cannula (and of the artery, they being the same) were 2 mm., with a sectional area therefore of 3'H square mm., an outflow through the section of -o c.c. or 500 c.mm. in a second would give (£JJ), a velocity of about 159 mm. in a second. The Hsematachometer of Vierordt is constructed on the principle of measuring the velocity of the current by observing the amount of devia- tion undergone by a pendulum, the free end of which hangs loosely in the stream. A square or rectangular chamber, one side of which is of glass and marked with a graduated scale in the form of an arc of a circle, is connected by means of two short tubes with the two cut ends of an artery; the blood consequently flows from the proximal (central) portion of the artery through the chamber into the distal portion of the artery. Within the chamber and suspended from its roof is a short pendulum, which when the blood-stream is cut off from the chamber hangs motionless in a vertical position, but when the blood is allowed to flow through the chamber, is driven by the force of the current out of its position of rest. The pendulum is so placed that a marker attached to its free end travels close to the inner surface of the glass side along the arc of the graduated side. Hence the amount of deviation from a vertical position may easily be read off on the scale from the outside. The graduation of the scale having been carried out by experimenting with streams of known velocity, the velocity can at once be calculated from the amount of deviation. An instrument based on the same principle has been invented by Chauveau and improved by Lortet. In this the part which corresponds to the pendulum in Vierordt's instrument is prolonged outside the chamber, and thus the portion within the chamber is made to form the short arm of a lever, the fulcrum of which is at the point where the wall of the chamber is traversed and the long arm of which projects outside. A somewhat wide tube, the wall of which is at one point composed of an india-rubber membrane, is introduced between the two cut ends of an artery. A long light lever pierces the india-rubber membrane. The short expanded arm of this lever projecting within the tube is moved on its fulcrum in the india-rubber ring by the current of blood passing through the tube, the greater the velocity of the current, the larger being the excursion of the lever. The movements of the short arm give rise to corresponding movements in the opposite direction of the long arm outside the tube, and these, by means of a marker attached to the end of the long arm, may be directly inscribed on a recording surface. This instrument is very well adapted for observing changes in the velocity of the flow. In determining actual velocities, for which purpose it has to be experimentally graduated, it is not so useful. CHAP, iv.] THE VASCULAR MECHANISM. 127 In the horse, Volkmann found the velocity of the stream to be in the carotid artery about 300 mm., in the maxillary artery 165 mm., and in the metatarsal artery 56 mm. in the second. Chauveau determined the velocity in the carotid of the horse to vary from 520 to 150 mm. per sec. at each beat of the heart, flow- ing at the former rate during the height of each pulse-expansion, and at the latter in the interval between each two beats. Ludwig and Dogiel found the velocity in the dog and in the rabbit to vary within very wide limits, not only in different arteries, but in the same artery under different circumstances. Thus while in the carotid of the rabbit it may be said to vary from 100 to 200 mm. per sec., and in the carotid of the dog from 200 to 500 mm. per sec., both these limits were frequently passed. 3. The Flow in the Veins. When a vein is severed, the flow from the distal cut end (i.e. the end nearest the capillaries) is continuous, the blood is ejected with comparatively little force, and with no great velocity. When a vein is connected with a manometer, the lateral pressure is found to be very small ; it is greater in the veins farther from the heart than in those nearer the heart,. In the former it is much less than that of the small arteries, and in the latter amounts only to a few millimetres of mercury. Indeed in the immediate neigh- bourhood of the heart the pressure may (during the inspiratory movement) become negative, i.e. when the manometer is brought into connection with the interior of the vein, the mercury in the distal limb falls, instead of, as in the case of an artery, rising. In the case of most veins, under ordinary circumstances the mercury of a manometer connected with a vein does not shew any of those pulse -oscillations which are so striking in the arteries. As a general rule the pulse is seen on the arterial side only of the j J^ capillaries, though in special cases, under conditions which we shall study presently, it may make its way through the capillaries from the arteries to the small veins ; and it is probable that in general a slight impulse does make its way right through the capil- laries, but so feeble that it cannot be recognised by ordinary in- struments save in special cases. Moreover, in the great veins near the heart, under certain circumstances at all events, the movements of that organ may make themselves felt as a so-called 'venous pulse' transmitted in a backward direction along the veins from the heart. But these exceptional instances and these recurrent oscillations do not invalidate the truth of the general statement that the pulse is absent from the veins. The exact determination of venous pressure is attended with great experimental difficulties, and our knowledge in 128 THE FLOW IN THE VEINS. [BOOK i. this direction is very incomplete ; but in all probability the pressure in a vein varies within much wider limits than does the pressure in the corresponding artery. In the small veins the velocity of the current, measured in the same way as in the case of the arteries, is very slight. It increases • 'in the larger veins, corresponding to the diminution of the area of 'the bed' ; it is about 200 mm. per sec. in the jugular vein of the dog. Thus the flow in the veins presents strong contrasts with that in the arteries. In the arteries, even in the smallest branches, there is a considerable mean pressure. In the veins, even in the small veins where it is largest, the mean pressure is very slight. In other words, there is always a difference of pressure tending to make the blood flow continuously from the arteries into the veins. \^^A pulse is present in the arteries, but, with certain exceptions, absent in the veins. The velocity of the stream of blood in the tjj arteries is considerable ; in the small veins it is much less, but it increases in the larger trunks; for in both arteries and veins it corresponds with the area of the bed, diminishing in the former from the heart to the capillaries, and increasing in the latter from the capillaries to the heart. Hydraulic Principles of the Circulation. All the above phenomena are the simple results of an intermit- tent force (like that of the systole of the ventricle) working in a closed circuit of branching elastic tubes, so arranged that while the individual tubes first diminish (from the heart to the capillaries) and then increase (from the capillaries to the heart), the area of the bed first increases and then diminishes, the tubes together thus forming two cones placed base to base at the capillaries, with their apices converging to the heart. To this it must be added that the friction in the small arteries and capillaries, at the junction of the bases of the cones, offers a very great resistance to the flow of the blood through them. It is this peripheral resistance (in the minute arteries and capillaries, for the resistance offered by the friction in the larger vessels may, when compared with this, be practically neglected), reacting through the elastic walls of the arteries upon the intermittent force of the heart, which gives the circulation of the blood its peculiar features. Circumstances determining the character of the flow. When fluid is driven by an intermittent force, as by a pump, through a perfectly rigid tube (or system of tubes), there escapes at each stroke of the pump from the distal end of the system just as much fluid as enters it at the proximal end. The escape moreover takes place at the same time as the entrance, since the time taken up by CHAP, iv.] THE VASCULAR MECHANISM. 129 the transmission of the shock is so small, that it may be neglected. This result remains the same when any resistance to the now is introduced into the system. The force of the pump remaining the same, the introduction of the resistance undoubtedly lessens the quantity issuing at the distal end at each stroke, but it does so simply by lessening the quantity entering at the proximal end; the income and outgo remain equal to each other, and occur at almost the same time. And what is true of the two ends, is also true of any part of the course of the system, so far, at all events, as the following proposition is concerned, that in a system of rigid tubes, either with or without an intercalated resistance, the flow caused by an intermittent force is, in every part of the tubes, intermittent synchronously with that force. In a system of elastic tubes in which there is little resistance to the progress of the fluid, the flow caused by an intermittent force is also intermittent. The outgo being nearly as easy as the income, the elasticity of the walls of the tubes is scarcely at all called into play. These behave practically like rigid tubes. When, however, sufficient resistance is introduced into any part of the course, the fluid, being unable to pass by the resistance as rapidly as it enters the system from the pump, tends to accumulate on the proximal side of the resistance. This it is able to do by expanding the elastic walls of the tubes. At each stroke of the pump a certain quantity of fluid enters the system at the proximal end. Of this only a fraction can pass through the resistance during the stroke. At the moment when the stroke ceases, the rest still remains 011 the proximal side of the resistance, the elastic tubes having expanded to receive it. During the interval between this and the next stroke, the distended elastic tubes, striving to return to their natural undistended condition, press on this extra quantity of fluid which they contain and tend to drive it past the resistance. Thus in the rigid system (and in the elastic system without resistance) there issues, from the distal end of the system, at each stroke, just as much fluid as enters it at the proximal end, while between the strokes there is perfect quiet. In the elastic system with resistance, on the contrary, the quantity which passes the resistance is only a fraction of that which enters the system from the pump, the remainder or a portion of the remainder continuing to pass during the interval between the strokes. In the former case, the system is no fuller at the end of the stroke than at the beginning; in the latter case there is an accumulation of fluid between the pump and the resistance, and a corresponding dis- tension of that part of the system, at the close of each stroke — an accumulation and distension, however, which go on diminishing until the next stroke comes. The amount of fluid thus remaining after the stroke will depend on the amount of resistance in relation to the force of the stroke, and on the distensibility of the tubes ; and the amount which passes the resistance before the next stroke F. 130 INTERMITTENT FLOW. [BOOK T. will depend on the degree of elastic reaction of which the tubes are capable. Thus, if the resistance be very considerable in relation to the force of the stroke, and the tubes very distensible, only a small portion of the fluid will pass the resistance, the greater part remaining lodged between the pump and the re- sistance. If the elastic reaction be great, a large portion of this will be passed on through the resistance before the next stroke comes. In other words, the greater the resistance (in relation to the force of the stroke), and the more the elastic force is brought into play, the less intermittent, the more nearly continuous, will be the flow on the far side of the resistance. If the first stroke be succeeded by a second stroke before its quantity of fluid has all passed by the resistance, there will be an additional accumulation of fluid on the near side of the resistance, an additional distension of the tubes, an additional strain on their elastic powers, and, in consequence, the flow between this second stroke and the third will be even more marked than that between the first and the second, though all three strokes were of the same force, the addition being due to the extra amount of elastic force called into play. In fact, it is evident that, if there be a sufficient store of elastic power to fall back upon, by continually repeating the strokes a state of things will be at last arrived at, in which the elastic force, called into play by the continually increasing dis- tension of the tubes on the near side of the resistance, will be sufficient to drive through the resistance, between each two strokes, just as much fluid as enters the near end of the system at each stroke. In other words, the elastic reaction of the walls of the tubes will have converted the intermittent into a continuous flow. The flow on the far side of the resistance is in this case not the direct result of the strokes of the pump. All the force of the pump is spent, first in getting up, and afterwards in keeping up, the over-distension of the tubes on the near side of the resistance ; the cause of the continuous flow lies in the over-distension of the tubes which leads them to empty of themselves into the far side of the resistance, at such a rate, that they discharge through the resistance during a stroke and in the succeeding interval just as much as they receive from the pump by the stroke itself. This is exactly what takes place in the vascular system. The friction in the minute arteries and capillaries presents a considerable resistance to the flow of blood through them into the small veins. In consequence of this resistance, the force of the heart's beat is spent in maintaining the whole of the arterial system in a state of over-distension, as indicated by the arterial pressure. The over- distended arterial system is, by the agency of its elastic walls, con- tinually emptying itself by overflowing through the capillaries into the venous system, overflowing at such a rate, that just as much blood passes from the arteries to the veins during each systole and its succeeding diastole as enters the aorta at each systole. CHAP, iv.] THE VASCULAR MECHANISM. 131 I It cannot be too much insisted upon that the whole arterial system is over-distended. This is what is meant by the higlr arterial pressure. On the other hand, the veins are much less distended. This is shewn by the low venous pressure. The dis- tended arteries are continually striving to pass their surplus in a continuous stream through the capillaries into the veins, so as to bring both venous and arterial pressure to the same level. As continually the heart by its beat is keeping the arteries distended, and thus maintaining the difference between the arterial and venous pressure, and thus preserving the steady capillary stream. When the heart ceases to beat, the arteries do succeed in emptying their surplus into the veins, and when the pressure on both sides of the capillaries is thus equalized, the flow through the capillaries ceases. In the facts just discussed, it makes no essential difference whether the outflow on the far side of the resistance be an open one, or whether, as is the case in the vascular system, the fluid be returned to the pump, provided only that the resistance offered to that return be sufficiently small. We shall see, in speaking of the heart, that, so far from there being any resistance to the flow of blood from the great veins into the auricle, the flow is favoured by a variety of circumstances. We have seen moreover that, besides the very sudden decrease in the immediate neighbourhood of the capillaries, there is in passing along the whole vascular system from the aorta to the venae cavse a gradual fall of pressure. A little consideration shews that this must be the case. After what has been said it is obvious that the movement of the blood may be compared to that of a body of fluid, driven by pressure from the ventricle through the vessels to its outflow in the auricle. Were the pressure a continuous one, and were there no peripheral resistance, there would be a gradual fall of pressure, from the part farthest from the outfall, viz. the aorta, to the part nearest the outfall, viz. the venaa cavae. The introduction of the peripheral resistance and its attendant phenomena gives rise to the feature of a very sudden and marked fall in the capillary region, but leaves untouched the gradual character of the fall in the rest of the course, from the aorta to the minute arteries, and from the minute veins to the venae cavae. To recapitulate : there are three chief factors in the mechanics of the circulation, (1) the force and frequency of the heart-beat, (2) the peripheral resistance, (3) the elasticity of the arterial walls. These three factors, in order to produce a normal circulation, must be in a certain relation to each other. A disturbance of these relations brings about abnormal conditions. Thus, if the peripheral resistance be reduced beyond certain limits, while the force and frequency of the heart remain the same, so much blood passes through the capillaries at each stroke of the heart that there is not sufficient left behind to distend the arteries, and bring their 9—2 132 VARIATIONS IN VELOCITY. [BOOK i. elasticity into play. In this case the intermittence of the arterial flow is continued on into the veins. An instance of this is seen in the experiments on the sub-maxillary gland, where sometimes the resistance offered by the minute arteries of the gland is so much lowered, that the pulse is carried right through the capillaries, and the blood in the veins of the gland pulsates1. A like result occurs when, the peripheral resistance remaining the same, the frequency of the heart's beat is lowered. Thus the beats may be so infrequent that the whole quantity sent on by a stroke has time to escape before the next stroke comes. Lastly, if, while the heart's beat and the peripheral resistance remain the same, the arterial walls become more rigid, the arteries will be unable to expand sufficiently to retain the surplus of each stroke or to exert sufficient elastic reaction to carry forward the stream between the strokes ; land in consequence more or less intermittence will become manifest. Circumstances determining the velocity of the flow. We have seen that the velocity of the blood-stream diminishes from the aorta to the capillaries, and increases from the capillaries to the great veins. Thus in the dog the velocity in the great arteries may be stated at from 300 to 500 mm., in the capillaries at less than 1 mm. ('5 to *75 mm.), and in the large veins at about 200 mm. in a sec. In fact, the greater part of the time of the circuit is taken up in the capillary region. An iron salt, injected into the jugular vein of one side of the neck of a horse, makes its appear- ance in the blood of the jugular vein of the other side in about 30 seconds. Bering's mean result in the horse was 27'G sees. In the dog Vierordt found it to be 15*2 sees.; in the rabbit 7 sees. Without laying too much stress on this experiment, it may be taken as a fair indication of the time in which the whole circuit may be completed. It takes about the same time to pass through about 20 mm. of capillaries. Hence, if any corpuscle had in its circuit to pass through 10 mm. of capillaries, half the whole time of its journey would be spent in the narrow channels of the .capillaries. Since, however, the average length of a capillary is about '5 mm., about one second is spent in the capillaries. In- asmuch as the purposes served by the blood are chiefly carried out in the capillaries, it is obviously of advantage that its stay in them I should be prolonged. The local differences in the velocity of the stream are directly dependent on the area of the 'bed.' When a fluid is driven by a uniform pressure through a narrow tube with an enlarge- ment in the middle, the velocity of the stream diminishes in the enlargement, but increases again when the tube once more narrows. So a river slackens speed in a ' broad' but rushes on 1 See Book i. cap. i. sec. 2, on the Secretion of the Digestive Juices. CHAP, iv.] THE VASCULAR MECHANISM. 133 rapidly again when the banks close in. Exactly in the same way the velocity of the blood-stream slackens from the aorta to the capillaries corresponding with the increased total bed, but hurries on again as the numerous veins are gathered into the smaller bed of the venae cavse. The loss of velocity in the capillaries, as com- ' pared with the arteries, is not due to there being so much more ; friction in the narrow channels of the former than in the wide j canals of the latter. For the peripheral resistance caused by the j friction in the capillaries and small arteries is an obstacle not only to the flow of blood through these small vessels where the resist- ance is actually generated, but also to the escape of the blood from the large into the small arteries, and indeed from the heart intoi the large arteries. It exerts its influence along the whole arterial* tract. And it is obvious that if it were this peripheral resistance which checked the flow in the capillaries, there could be no re- [ covery of velocity along the venous tract. The rapidity of the flow in arteries, capillaries, and veins, is in each case determined by the total sectional area of the channels. There is, however, a loss of velocity on the whole course. At each stroke as much blood enters the right auricle as issues from the left ventricle ; but the sectional area of the venae cavae is greater than that of the aorta, so that even if the auricle were tilled in exactly the same time as the ventricle is emptied, the blood must pass more rapidly through the narrow aorta than through the broad venae cava?, in order that the same quantity of blood should pass each in the same time. The diastole of the auricle, however, is distinctly longer than the systole of the ventricle; the time during which the auricle is being filled is greater than that during which the ventricle is being emptied, and hence the velocity of the venous flow into the auricle must be still \ less than that of the arterial blood in the commencing aorta. The temporary variations of the velocity of the stream in any given' channel, and these we have already (p. 127) seen to be very considerable in the case of the arteries at least, are dependent on a variety of circumstances. In a tube of constant calibre, the velo- city with which fluid flows from one point to another, for instance from the point a to the point 6, will be in main dependent on the difference between the pressures existing at a and b. The lower the pressure at b as compared with a the greater the rapidity with which the fluid flows from a to 6. And temporary variations of pressures form undoubtedly the main cause of the temporary varia- tions observable in the velocity of the arterial flow. Thus with each systole of the ventricle there is an increase of velocity in the whole arterial flow followed by a diminution during the diastole. So also if the peripheral resistance in the minute arteries into which a larger artery divides be suddenly lowered (by the action of vaso-motor nerves, in a manner which we shall presently discuss), without the calibre of the larger artery itself being changed, the pressure on the distal (peripheral) side of the artery may be much 134 VARIATIONS IN VELOCITY. [BOOK i. diminished, while the pressure on the proximal (cardiac) side re- mains at first .unaltered ; and this would necessarily cause an increase in the rapidity of the stream through that artery. But, as we shall see later on, from the complications of the vascular machinery such problems as these become very intricate; and the results of observations on variations in arterial velocity are not altogether intelligible. It has been suggested that varying conditions of the blood, by affecting the amount of adhesion between the blood and the walls of the vessels, may be an important factor in determining the variations in the velocity of the stream. SEC. 2. THE HEART. The heart is a pump, the motive power of which is supplied by the contraction of its muscular fibres. Its action consequently presents problems which are partly mechanical, and partly vital. Regarded as a pump, its effects are determined by the frequency of the beats, by the force of each beat, by the character of each beat — whether, for instance, slow and lingering, or sudden and sharp — and by the quantity of fluid ejected at each beat. Hence, with a given frequency, force, and character of beat, and a given quantity ejected at each beat, the problems which have to be dealt with are for the most part mechanical. The vital problems are chiefly con- nected with the causes which determine the frequency, force, and character of the beat. The quantity ejected at each beat is governed more by the state of the rest of the body, than by that of the heart itself. TJie Phenomena of the Normal Beat. The visible movements. When the chest of a mammal is opened and artificial respiration kept up, a complete beat of the whole heart, or cardiac cycle, may be observed to take place. as follows. The great veins, inferior and superior vense cavse and pulmonary- veins, are seen, while full of blood, to contract in the neighbourhood of the heart : the contraction runs in a peristaltic wave towards the auricles, increasing in intensity as it goes. Arrived at the auricles, which are then full of blood, the wave suddenly spreads, at a rate too rapid to be fairly judged by the eye, over the whole of those organs, which accordingly contract with a sudden sharp systole. In the systole, the walls of the auricles press towards the auriculc- 136 MOVEMENTS OF THE HEART. [BOOK i. ventricular orifices, and the auricular appendages are drawn inwards, becoming smaller and paler. During the auricular systole, the ven- tricles may be seen to become more and more turgid. Then follows, as it were immediately, the ventricular systole, during which the ventricles become more conical. Held between the fingers they are felt to become tense and hard. As the systole progresses, the aorta and pulmonary arteries expand and elongate, and the heart twists slightly on its long axis, moving from the left and behind towards the front and right so that more of the left ventricle becomes dis- played. As the systole gives way to the succeeding pause or diastole, the ventricles resume their previous form, the aorta and pulmonary artery contract and shorten, the heart turns back to- wards the left, and thus the cycle is completed. A more exact determination of the changes in the form and position of the heart during a beat is attended with considerable difficulties. The following experiment has been made with the view of studying these changes without opening the chest and thus without depriving the heart of its natural supports. If, in the un- opened chest of a rabbit or dog, three needles be inserted through the chest-wall so that their points are plunged into the substance of the ventricle, one (B) at the base, close to the auricles, another (A) through the apex, and a third (M) at about the middle of the ventricle, all three needles will be observed to move at each beat of the heart. The head of B will move suddenly upwards, shewing that the point of the needle plunged in the ventricle moves down- wards, whereas A will only quiver, and move neither distinctly up- wards nor downwards. M will move upwards (and therefore its point downwards), but not to the same extent as B. The nearer to B, M is, the more it moves : the nearer to A, the less. After the death of the animal, the needles, if properly inserted at first, perpendicular to the chest, will be found with all their heads directed downwards, indicating that the whole ventricle has been drawn up by the contraction of the empty aorta and pulmonary artery. The behaviour of the needles during the beat has been in- terpreted as follows. At the systole the whole heart is thrust downward by the elongation of the aorta and pulmonary artery. The needle A at the apex however does not move its place, because this downward movement is compensated by an upward movement due to a shortening, during systole, of the longitudinal diameter of the ventricle. The base in which the needle B is plunged, moves downwards and drawrs closer to A, i.e. to the apex, partly by the downward thrust from the elongation of the great arteries and partly from the shortening of the ventricle itself. Naturally the behaviour of the needle M is intermediate in character, its downward movement being the more conspicuous the nearer it is to B. The experiment then is taken to prove that during the systole the ventricle shortens in its CHAP, iv.] THE VASCULAR MECHANISM. 137 longitudinal diameter, but that the apex remains stationary on account of the compensating downward thrust of the whole ventricle. It has been urged however that this method is untrust- worthy, and that similar movements of needles thus placed might be produced by the twisting of the heart on its long axis, com- bined with an approximation of the heart to the chest-wall. And different conclusions have been arrived at by taking plaster of Paris models on the one hand of a dog's heart, which, while having ceased beating but not yet become rigid, has been filled with blood at a moderate pressure, and on the other hand of a heart of the same size in which a condition simulating systolic contraction has been brought about by immersing the empty heart in a saturated solution of potassium bichromate at 50° C. The former is taken to represent the diastolic and the latter the systolic form of the heart; and the results are checked by measurements taken between marks placed on various points of the surface of the heart as well as by sections of a heart filled with blood and hardened in a cold solu- tion of potassium bichromate and of one emptied and hardened in the same solution warmed to 50°. A comparison of the two hearts in these different conditions tends to shew that while both the right-to-left and antero-posterior diameters are diminished during systole, especially in the plane of the ostia venosa (whereby the auriculo-ventricular orifices become narrowed) the longitudinal diameter, at all events of the left ventricle, is not lessened, the distance between the apex and the auriculo-ventricular groove remaining unchanged. The right ventricle, the change of form of which is complicated, does shorten to a certain extent, and there is during systole a downward movement of the con us arteriosus upon the plane of the ventricular base (which possibly may explain the movement of the needle B in the above mentioned experiment) so that the distance between the apex and the upper border of the conus is less during systole than during diastole. This method also confirms the view that the left ventricle in systole turns on its long axis, towards the right, the movement increasing from the base downwards so that the groove between the two ventricles forms a closer spiral than during diastole. Objections may be brought against this method also, and it seems impossible to explain the movements of a lever placed upon the heart unless we admit that during systole, the antero-posterior diameter, of the middle portion of the ventricle at least is increased instead of lessened. We may however probably go so far as to conclude that as far as the ventricles are concerned the chief change during systole is one from a roughly hemispherical to a more conical form, effected without any marked diminution of the distance between the apex and the ventricular base. Cardiac Impulse. If the hand be placed on the chest, a shock or impulse will be felt at each beat, and on examination 138 CARDIAC IMPULSE. [BOOK i. this impulse, 'cardiac impulse,' will be found to be synchronous with the systole of the ventricle. In man, the cardiac impulse may be most distinctly felt in the fifth costal interspace, about an inch below and a little to the median side of the left nipple. The same impulse may be felt in an animal by making an incision through the diaphragm from the abdomen, and placing the finger between the chest-wall and the apex. It then can be distinctly recognized as the result of the hardening of the ventricle during the systole. And the impulse which is felt on the outside of the chest is the same hardening of the stationary portion of the ventricle in contact with the chest-wall, transmitted through the chest-wall to the finger. In its flaccid state, during diastole, the apex is (in a standing position at least) at this point in contact with the chest- wall, lying between it and the tolerably resistant diaphragm. During the systole, while being brought even closer to the chest- wall, by the movement to the front and to the right of which we have already spoken, it suddenly grows tense and hard. The ventricles, in executing their systole, have to contract against resistance. They have to produce within their cavities, tensions greater than those in the aorta and pulmonary arteries, respectively. This is, in fact, the object of the systole. Hence, during the swift systole, the ventricular portion of the heart becomes suddenly tense, just as a bladder full of fluid would become tense and hard when forcibly squeezed. The sudden onset of this hardness gives an impulse or shock both to the chest-wall and to the diaphragm, which may be felt readily both on the chest- wall, and also through the diaphragm when the abdomen is opened, and the finger inserted. If the modification of the sphygmograph (see section on Pulse), called the cardiograph, be placed on the spot where the impulse is felt most strongly, the lever is seen to be raised during the systole of the ventricles, and to fall again as the systole passes away, very much as if it were placed on the heart directly. A tracing may thus be obtained, of which we shall have to speak more 'fully immediately. If the button of the lever be placed, not on the exact spot of the impulse, but at a little distance from it, the lever will be depressed during the systole. While at the spot of impulse itself the contact of the ventricle is increased during systole, away from the -spot the ventricle retires from the chest-wall (by the diminution of its right-to-left diameter), and hence, by the mediastinal attachments of the peri- cardium, draws the chest-wall after it. Endo-cardiac events. In order to study more fully the changes going on in the heart during the cardiac cycle, it becomes necessary to know something of what is taking place in the interior of the cavities of the heart. Chauveau and Marey, by introducing into the right auricle and ventricle respectively of the horse, through the jugular vein, small elastic bags, each communicating with a CHAP, iv.] THE VASCULAR MECHANISM. 339 recording tambour, were enabled to take simultaneous tracings of changes occurring in the two cavities. These results are embodied in Fig. 21, of which the upper curve is a tracing taken TC V FlG. 21. SIMULTANEOUS TRACINGS FROM THE INTERIOR OF THE RIGHT AURICLE, FROM THE INTERIOR OF THE RIGHT VENTRICLE, AND OF THE CARDIAC IMPULSE, IN THE HORSE. (AFTER CHAUVEAU AND MARF.Y.) To be read from left to right1. The upper curve represents changes taking place within the auricle, the middle curve changes within the ventricle. The lower curve represents the variations of pressure transmitted to a lever outside the chest and constituting the cardiac impulse. A complete cardiac cycle, beginning at the close of the ventricular systole, is comprised between the thick vertical lines I and II. The thin vertical lines represent tenths of a second. The explanation of the letters is given in the text. from the auricle, the middle curve a similar tracing taken from the ventricle, while the lower curve is a cardiographic tracing of the cardiac impulse. All these curves were taken simultaneously on the same recording surface. Method. A tube of appropriate curvature is furnished with two small elastic bags, one at the extreme end and the other at such a distance that when the former is within the cavity of the ventricle the latter is in the cavity of the auricle ; such an instrument is spoken of as a ' cardiac sound.' Each bag (Fig. 22 A) or 'ampulla' communicates by a separate air-tight tube with an air-tight tambour (Fig. 22 B) on which a lever rests so that any pressure on either bag is communicated to the cavity of its respective tambour, the lever of which is raised in 1 It must be remembered that the curves in the diagram are intended merely to illustrate the changes occurring at different times in the same chamber, or to shew what changes in the one chamber are coincident in point of time with changes in the other. They in no way indicate the amount of pressure exerted in the auricle as compared with that in the ventricle. 140 ENDO-CARDIAC EVENTS. [BOOK i. proportion. The writing points of all three levers are brought to bear on the same recording surface exactly underneath each other. The tube is carefully introduced through the right jugular vein into the right side of the heart until the lower (ventricular) bag is fairly in the FIG. 22. MAREY'S TAMBOUR, WITH CARDIAC SOUND. A. A simple cardiac sound such as may be used for exploration of the left ventricle. The portion a of the ampulla at the end is of thin india-rubber, stretched over an open framework with metallic supports above and below. The long tube b serves to introduce it into the cavity which it is desired to explore. B. The Tambour. The metal chamber ra is covered in an air-tight manner with the india-rubber c, bearing a thin metal plate ra' to which is attached the lever Z moving on the hinge h. The whole tambour can be placed by means of the clamp cl at any height on the upright s'. The india-rubber tube t serves to connect the interior of the tambour either with the cavity of the ampulla of A or with any other cavity. Supposing that the tube t were connected with b, any pressure exerted on a would cause the roof of the tambour to rise and the point of the lever would be pro- portionately raised. cavity of the right ventricle, and consequently the upper (auricular) bag in the cavity of the right auricle. Changes of pressure on either ampulla then cause movements of the corresponding lever. When the pressure, for instance, on the ampulla in the auricle is increased, the auricular lever is raised and describes on the recording surface an ascending curve ; when the pressure is taken off the curve descends ; and so also with the ventricle. The ' sound ' may in a similar manner be readily introduced through the carotid artery into the left ventricle and the changes taking place in that chamber also explored; these are found to be very similar to those of the right ventricle. We may employ these curves as giving a general and useful view of the sequence of events in the interior of the heart; but we must bear in mind exactly what they mean. The tracings given CHAP, iv.] THE VASCULAR MECHANISM. 141 by the auricular and ventricular levers really represent variations in the pressure exerted on the respective ampullse, and so far are instructive; but they must not be taken as representing variations in the pressure exerted on the blood in' the several cavities. For we can easily conceive that, in the systole of the ventricle for instance, the contraction of the muscular walls might continue after all the blood contained in the ventricle had been driven out. In such a case the ventricle would continue to press upon the ampulla, and this continued pressure would be transmitted to the lever, and indicated on the curve; but we should be in error in interpreting this part of the curve as meaning that the ventricle was still continuing to exert pressure on the blood as yet remain- ing in its cavity. With this caution, and with the remark that the tracing of the cardiac impulse is very unlike the usual cardio- graphic tracings taken from man, we may use the curves to deduce the following conclusions. A complete cardiac cycle is comprised between the vertical lines I and II. The recording surface was travelling at such a rate that the intervals between any two of the thin vertical lines corresponds to one-tenth of a second. Hence in this case (the heart being that of a horse) the whole cardiac cycle occupied about f§ths of a second. Any point in the cycle might of course be taken as its commencement. In the figure, the cycle is supposed to begin shortly after the end of the ventricular systole, and the beginning of the diastole. On examining the three curves we see, at a, a steady rise of the auricular, accompanied by similar gradual ascents of the ventricular and also of the cardiograph lever. These may be interpreted as indicating that the blood is pouring from the great veins into the auricle, increasing the pressure there, and at the same time passing on into the ventricle, increasing the internal pressure there as well, a, and also by distending the ventricle, causing it to press somewhat on the chest-wall and thus to raise the cardiograph lever, a . This continues for about -j^ths of a second, and is then followed by the sudden rise of auricular pressure b due to the auricular systole, followed by a sudden fall as the blood escapes into the ventricle and the systole ceases. The sudden entrance of blood into the ventricle causes a sudden increase of the pressure in the ventricle as indicated by the ventricular lever b', and a sudden increase in the pressure on the chest-wall b". The auricular systole is followed immediately by the sudden strong ventricular systole c', the lever rising very abruptly. Owing to the presence of the tricuspid valves, the pressure exerted by the ventricular systole is kept off the auricle almost altogether; but the chest-wall, as shewn by the tracing at c", feels the sudden increase of the pressure of the ventricle against it. The most important points concerning this rise of ventricular pressure are that it is sudden in its onset and also rapid in its decline, and 142 THE MECHANISM OF THE VALVES. [BOOK i. that it lasts for a comparatively long time; in the figure this part of the curve embraces more than four-tenths of a second. These [features, the sudden rise, the long duration, and the rapid fall of the pressure exerted by the ventricle are seen in all tracings of the ventricles engaged in a cardiac beat whatever be the method employed. They mean of course that the muscular contractions which constitute the ventricular systole come on suddenly, that they last altogether a considerable time, and that relaxation is also rapid. With the end of the ventricular systole the cycle represented in figure ends, and a new cycle begins, repeating the same changes. The meaning of the features on the curves marked e and d, &c., as well as a more complete discussion of the changes thus briefly described, we must defer till we have spoken of The Mechanism of the Valves. The auriculo-ventricular valves present no difficulty. As the blood is being driven by the auricular systole into the ventricle, a reflux current is probably set up, by which the blood, passing along the sides of the ventricle, gets between them and the flaps of the valve (whether tricuspid or mitral). As the pressure of the auricular systole diminishes, the same reflux current floats the flaps up, until at or immediately after the close of the systole they meet, and thus the orifice is at once and firmly closed, at the very beginning of the ventricular beat. The increasing intraventricular pressure serves only to render the valve more and more tense, and in consequence more secure, the chordae tendineae (the slackening of which through the change of form of the ventricle is probably obviated by a regulative contraction of the papillary muscles) at the same time preventing the valve from being inverted -or even bulging into the auricle, and indeed, according to some observers, keeping the valvular sheet actually convex to the ventricular cavity, by which means the complete emptying of the ventricle is more fully effected. Since the same papillary muscle is in many cases connected by chordae with the adjacent edges of two flaps, its contraction also serves to keep these flaps in more complete apposition. Moreover the extreme borders of the valves, outside the attachments of the chordae, are excessively thin, so that when the valve is closed, these thin portions are pressed flat together back to back ; hence while the tougher central parts of the valves bear the force of the ventricular systole, the opposed thin membranous edges, pressed together by the blood, more completely secure the closure of the orifice. CHAP, iv.] THE VASCULAR MECHANISM. 143 The semilunar valves are, during the ventricular systole, pressed outwards towards but not close to the arterial walls, reflex currents probably keeping them in an intermediate position, their orifice forming an equilateral triangle with curved sides ; they thus offer little obstacle to the escape of blood from the cavities of the ventricles. The ventricle propels the blood with great force and rapidity into the aorta and the whole contents are speedily ejected. Now, when in a closed channel a rapid current suddenly ceases, a negative pressure makes its appearance in the rear of the fluid, and sets up a reflux current. So when the last portions of blood leave the ventricle a negative pressure makes its appearance behind them in the ventricle, and leads to a reflux current from the aorta towards the ventricle. This alone would tend to bring the valves together; but in all probability it is not till a short (variable) time afterwards, that upon the commencing diastolic relaxation of the ventricle, the elastic rebound of the arterial walls completely fills and renders tense the pockets, causing their free margins to come into close and firm contact, and thus entirely blocking the way. The corpora Arantii meet in the centre, and the thin membranous festoons or lunulse are brought into exact apposi- tion. As in the tricuspid valves, so here, while the pressure of the blood is borne by the tougher bodies of the several valves, each two thin adjacent lunulsfi, pressed together by the blood acting on both sides of them, are kept in complete contact, without any strain being put upon them; in this way the orifice is closed in a most efficient manner. The ingenious view put forward by Briicke that during the ven- tricular systole, the flaps are pressed back flat against the arterial walls, and in the case of the aorta completely cover up the orifices of the coronary arteries, so that the flow of blood from the aorta into the coronary arteries can take place only during the ventricular diastole or at the very beginning of the systole, and not at all during the systole itself, has been disproved. The Sounds of the Heart. When the ear is applied to the chest, either directly or by means of a stethoscope, two sounds are heard, the first a com- paratively long dull booming sound, the second a short sharp budden one. Between the first and second sounds, the interval of time is very short, too short to be measurable, but between the second and the succeeding first sound there is a distinct pause. The sounds have been likened to the pronunciation of the syllables, lubb, dup, so that the cardiac cycle, as far as the sounds are concerned, might be represented by : — lubb, dup, pause. 144 THE SOUNDS OF THE HEART. [BOOK i. The second short sharp sound presents no difficulties. It is coincident in point of time with the closure of the semilunar valves, and is heard to the best advantage over the second right costal cartilage close to its junction with the sternum, i. e. at the point where the aortic arch comes nearest to the surface. Its characters are such as would belong to a sound generated by the sudden tension of valves like the semilunar valves. It is obscured and altered, replaced by ' murmurs ' when the semilunar valves are affected by disease, the alteration being most manifest to the ear at the above-mentioned spot when the aortic valves are affected. When the aortic valves are hooked up by means of a wire intro- duced down the arteries, the second sound is obliterated and replaced by a murmur. These facts prove that the second sound is due to the sudden tension of the aortic (and pulmonary) semi- lunar valves. The first sound, longer, duller, and of a more 'booming' character than the second, heard with greatest distinctness at the spot where the cardiac impulse is felt, presents many difficulties in the way of a complete explanation. It is heard distinctly when the chest-walls are removed. The cardiac impulse therefore can have little or nothing to do with it. In point of time, and in the position in which it may be heard to the greatest advantage (at the spot of the cardiac impulse where the ventricles come nearest to the surface), it corresponds to the closure of the auriculo-ven- tricular valves. In point of character it is not such a sound as one would expect from the vibration of membranous structures, but has, on the contrary, many of the characters of a muscular sound. In favour of its being a valvular sound, may be urged the fact that it is obscured, altered, replaced by murmurs, when the tricuspid or mitral valves are diseased ; and according to some authors clamp- ing the great veins so as to shut off the blood supply stops the sound though the beat continues. The first argument may be met by the consideration that a murmur though itself undoubtedly of valvular origin, might largely or completely hide a sound occurring at the same time as the closure of the valves but due to other causes ; and the second is directly contradicted by an experiment of Ludwig and Dogiel. These observers tied in succession, in the order of the flow of blood, the great veins and arteries of the heart of a dog so as to completely deprive the heart of blood, and listened to the heart both within the body and after removal. For the short time that the heart continued to beat, the first sound was heard, feeble but with its main characters recognisable. From this they inferred that the sound was of muscular origin. But there is a great difficulty in regarding the sound as a muscular one, for a muscular sound is the result of a tetanic contraction, the height of the note produced varying with the rate of re- petition of the simple contractions which go to make up the CHAP, iv.] THE VASCULAR MECHANISM. 145 tetanus. A simple contraction or spasm cannot possibly produce a sound having the characters of the first cardiac sound. And the evidence, though perhaps not conclusive, goes to shew that the beat of the heart is a slow long-continued single spasm, intermediate between the contraction of an ordinary striated and that of an unstriated muscle, and not a tetanic contraction. We cannot, it is true, now rely in support of this view on the fact that when the nerve of a rheoscopic muscle-nerve preparation is placed on the beating ventricle, each beat is followed by a single spasm of the muscle, and not by a tetanus ; for we now know that many forms of tetanus (e. g. those caused by the constant current, by strychnia, and probably all natural voluntary contractions) give rise, in a rheoscopic muscle-nerve preparation, to a single initial spasm and not to a tetanus. But the general features of the beat, its long latent period and the gradation of the ventricular systole through the auricular systole into the rhythmic contractions of the un- striated fibres of the walls of the great veins, render it difficult to suppose that the beat is really a tetanus. Moreover the long duration of the ventricular systole is readily explained by the wave of contraction passing in a complicated peristaltic manner over the different fibres in succession. But if the beat be a simple contraction, it cannot give rise to a muscular sound, unless we suppose that this sequence of simple contractions over various parts of the ventricle in succession is adequate to produce such a sound. This, however, does not seem very satisfactory. On the other hand, if we reject the distinctly muscular origin of the sound, we are almost driven to suppose that the abrupt systole is able even in the absence of blood to produce such a sudden tension of the valves, and of the ventricular walls, as to give rise to a note. On such a view, the sound ought to vary in character according as the ventricle is more or less filled, being low and booming when it is full, and high and sharp when the contents are scanty. And such is said to be the case. But the matter does not at present seem ripe for any dogmatic statement. In the normal state of things, the beats of the two ventricles are so far synchronous with each other that practically only one first sound and one second sound is heard. It sometimes happens however that the synchronism fails to such an extent and the closure of the pulmonary and aortic valves respectively are sepa- rated by such an interval as to give the second sound a double character. 10 146 SPECIAL CARDIAC PHASES. [BOOK i. On the relative duration and special characters of the Cardiac events. We may now return to a more detailed study of what is taking place in the heart during a beat. We have already spoken of the conclusions which may be drawn from Chauveau and Marey's curves, and have incidentally (p. 138) referred to the cardiograph. Various forms of cardiograph have been used to record the cardiac impulse. In some the pressure of the impulse as in the sphygmograph is transmitted directly to a lever which writes upon FIG. 23. CARDIOGRAPHIC TRACING OF CARDIAC IMPULSE IN MAN (from Landois). An entire beat occurs between a and /. The auricular systole is marked by b, the end of the ventricular relaxation by/. At c, the highest point of the curve, the blood begins to be propelled from the ventricle, d and e are considered by some to indicate the closure of the aortic and semilunar valves respectively, see text. Five cardiac beats are represented ; the convex curve which their base line forms is due to the respiratory movements. a travelling surface. In others the impulse is, by means of an ivory button, brought to bear on an air-chamber, connected by a tube with a tambour as in Fig. 22 ; the pressure of the cardiac impulse compresses the air in the air-chamber, and through this the air in the chamber of the tambour by which the lever is raised. In such delicate and complicated movements as those of the heart however, the use of long tubes filled with air is liable to introduce various errors. A cardiographic tracing of ordinary characters is given in Fig. 23. Curves of the variations in internal pressure may be obtained by passing a tube connected with a mercurial manometer (as in the investigation of arterial pressure, p. 122) into the right ventricle through the jugular vein or into the left ventricle through the carotid artery. But this method, though useful for the purpose of investigating generally the pressure exerted by the cardiac walls, is, by reason of the inertia of the mercury, unsuitable for detecting rapid and small changes. CHAP, iv.] THE VASCULAR MECHANISM. 147 Tracings of the movements of the ventricles themselves, corre- sponding to the cardiac impulse and so to a certain extent to the variations of internal pressure, may also be taken directly by bringing a light lever to bear on the outside of the ventricles, the chest having been previously opened and artificial respiration kept up. A curve1 taken by this method is shewn in Fig. 24. FIG. 24. Normal heart curve shewing changes in the antero-posterior diameter of the ventricle obtained from the cat by a light recording lever moved by a button which pressed gently on the anterior surface of the ventricle. The time curve gives 50 double vibrations per sec. and lines have been drawn to shew the duration of the different phases of the ventricular movement, a to 6 corresponds to the distension of the ventricle including the auricular systole, the wave-like rise during this period being due to the increase in the diameter of the ventricle resulting from the entrance into it of the contents of the auricle. The period from 6 to c corresponds to the time from the commencement of the ventricular contraction to the moment when the organ has completed its change in shape from a flattened to a more rounded form. The highest part of the curve corresponds also in time with the opening of the semilunar valves as well as the firm closure of the auriculo-ventrlcular valves. The duration of this 1 The majority of cardiograph ic, sphygmographic and other tracings shew certain points which can be understood at a glance, but many characteristics can only be learned by "measuring out the curve" as it is termed. This is done as follows. Every tracing ought to bear on it an abscissa line, marked by a point which remains motionless while the recording surface is travelling. Moreover, either before or after taking a curve, while the paper or recording surface is at rest, the point of the lever should be always moved up and down so as to describe a segment of a circle of which the axis of the lever is the centre. The tracing thus prepared, when it has to be measured, is pinned out on aboard, and, by means of a pair of compasses, the distance between whose points has previously been made equal to the distance between the axis and the point of the lever used in making the experiment, the centre of the circle of which the curved lines previously made as directed are segments is found and marked on the paper. Through this centre, which of course corresponds to the position of the axis of the lever, a horizontal line is drawn parallel to the abscissa line. Keeping one of the compass points on this line, segments of circles are drawn in succession through various points of the curve, the distance between the points of the compass being fixed, but the centre of the circle described being shifted backwards and forwards along the horizontal line. The points where these segments cut the horizontal line are marked upon it, and the distances between them measured as, for example, in Fig. 29, p. 166. If the curve of a tuning-fork, the point of whose recording style was carefully placed on the same vertical line as the point of the lever, be also present, the segments of circles may be continued until they cut this, and the time corresponding to distances between them (as, for instance, in Fig. 24 the intervals between a, 6, c, d,) thus directly measured off. 10—2 148 SPECIAL CARDIAC PHASES. [BOOK i. .period in this ease is only about 3-50ths of a sec. The period from c to d is that during which the ventricle having grasped its contents is emptying its cavity and remaining contracted. It can be seen that only during the first half of this period is there any marked descent of the lever point ; in other words the antero-posterior diameter does not continue to diminish during the whole period of the systole, indicating that little or no blood was thrown out during the second half of this period, the ventricle remaining simply contracted after having emptied its cavity. The period from d to a is that during which the ventricular muscle is relaxing. Here, as is frequently the case, there is no period of pause between the close of the relaxation of the ventricle and the commencement of the succeeding distension. The tracing gives no evidence as to the time of closure of the semilunar valves. The chief interest and the chief difficulties are attached to the* f systole of the ventricles. In order to understand this, the most important of the cardiac events, it must be borne in mind that, as we have already seen, the pressure of the blood in the aorta is always considerable. This pressure closes and keeps closed the semilunar valves ; and it is not till the pressure in the ventricle becomes greater than the pressure in the aorta that these valves open to allow of the escape of the ventricular contents. The blood therefore does not begin to pass from the left ventricle into the aorta until some time, and that a variable time, after the commence- ment of the systole of the ventricle ; and the same may be said of the right ventricle and pulmonary artery, it being understood that the arterial pressure on the right side is less than on the left. In Fig. 24 the ventricular lever reaches its maximum c at once, gradually declining afterwards till the more sudden fall begins, and we may suppose that the escape of blood from the ventricle begins at the moment when the maximum is attained; and this view is confirmed by carefully comparing a tracing of the expansion of an artery with the cardiac tracing. It is quite possible however to conceive that owing to circumstances, such as an increasing con- traction of the ventricular fibres or deficient expansion of the arteries, the pressure might continue to increase even after blood was escaping from the cavity of the ventricle. And indeed in some curves, the ventricular lever after the first sudden leap continues to rise gradually and does not reach the maximum point until afterwards. In such cases the summit of the first rise must be taken as marking the beginning of the flow from the ventricle. By the sudden systole the blood is ejected with considerable force and rapidity from the ventricle, and as the ventricle becomes empty a negative pressure, as we have seen, makes its appearance behind the column of blood which leaves the cavity and leads to the closure of the semilunar valves. Much dispute has taken place as to the exact condition of the ventricle at the moment of closure of the semilunar valves. The slight rise e in Chauveau and Marey's curves (Fig. 21) in the ventricular curve, seen also in the auricle at e and in the cardiac impulse at e", and which has been taken to indicate the shutting of the semilunar valves, appears quite at the close of the descent of the ventricular lever. This would mean that at the moment of the closure of the valves the ventricle CHAP, iv.] THE VASCULAR MECHANISM. 149 had not only completed its contraction but was far advanced in relaxation. Such a view is not only cb priori improbable but is directly contradicted by the fact that when we compare a tracing obtained by placing a lever directly on the heart or indeed a tracing of the cardiac impulse with a pulse tracing, that is a tracing of the expansion of an artery, we find that the ventricle continues con- tracted after its contents have entirely left the cavity. That is to say, the actual flow of blood takes place only during the middle portion of the time during which the muscular fibres of the ven- tricle are contracting and engaged in carrying on the systole. During the first part, pressure is being got up, during the second the blood is being propelled, during the third the ventricle continues to remain empty and contracted. By this means the complete emptying of the ventricle is effectually secured. And others have urged that the closure of the semilunar valves, being entirely due to the reflux spoken of above, follows close upon the emptying of the ventricle ; in other words that it takes place while the ven- tricle is still contracted. It is very difficult to point out indications on the ventricular curve which indubitably correspond to this event. In tracings of the cardiac impulse, and in tracings taken by a lever placed directly on the heart, a notch, followed by a rise, is some- times observed in that part of the curve which intervenes between the first large rise and the final sudden fall ; and this secondary rise has been taken to indicate the closure of the semilunar valves ; but, if this be the case, the time during which the ventricle remains contracted after the closure of the valves forms a very con- siderable fraction of the whole period of the systole; and this presents difficulties. Sometimes two such notches and peaks are seen, and the occurrence of the two has been attributed to a want of synchronism in the closure of the pulmonary and aortic semilunar valves, the latter closing some little time before the former. But it is by no means clear that these notches and peaks are thus due to the closure of the valves; they may possibly have another origin, they are not always present, and the attempt to fix the time of the closure of the semilunar valves by them cannot be regarded as satisfactory. On the other hand, the second sound of the heart is undoubtedly due to the complete closure and sudden tension of the semilunar valves ; and not only is this second sound separated from the first sound by a distinctly appreciable interval (from which we may infer either that the systole of the ventricle ceases before the complete closure and sudden tension of the semilunar valves or that the first sound does not last so long as the systole itself and is therefore not a muscular sound) but the time elapsing between the beginning of the first sound and the second sound is, as we shall see, remarkably constant. Now we have reason to believe that the quantity of blood expelled at any one beat, and hence the time taken up in its escape, does vary very considerably ; whereas the duration of the actual systole is probably much more constant. 150 ENDO-CARDIAC 2>RESSUPE. [BOOK i. Hence we may infer, and the conclusion may be supported by other arguments, that at the actual closure of the semilunar valves, giving rise to the second sound, the ventricle has just finished its systole and is beginning to relax. If this view be correct the time of the closure of the valves is not indicated on the cardiographic tracing by any special mark, but coincides with the commencement of the more sudden and final fall of the lever as at d in Fig. 24. Marey thought that the oscillations seen at d' in his curves and obvious in the auricle and cardiac impulse as well, were due to oscillations of the auriculo-ventricular valve, but in that case they would be inverted in the auricular curve; whereas they are not. It is difficult to say what gives rise to them. We may repeat that many of the details of these curves vary considerably even with the same method of investigation and when the same apparatus is employed. In all probability the character and sequence of the events are modified by various circumstances, such as the rate and rapidity of the beat, the quantity of blood flowing into the heart, and the pressure obtaining in the arteries. Amount of Pressure. Although the instrument of Chauveau and Marey may be experimentally graduated and has been used to measure the amount of pressure in the several cavities of the heart, it is, as we have said, open to objections. Better results may be gained by passing through the jugular vein into the right auricle and thence into the right ventricle, or through the carotid artery into the left ventricle, a tube open at the end introduced into the heart and connected at the other end with a manometer. Varia- tions of pressure in the cardiac cavities are thus transmitted di- rectly to the mercury column of the manometer in the same way as those of an artery when arterial pressure is measured. The inertia of the mercury column however prevents an exact response to the rapid movements of the heart, and obscures the results ; though by using maximum and minimum manometers, the maximum and minimum pressures of the several cavities may be determined. The principle of the maximum manometer, Fig. 25, consists in the introduction into the tube leading from the heart to the mercury column, of a (modified cup-and-ball) valve, opening, like the aortic semilunar valves, easily from the heart, but closing firmly when fluid attempts to return to the heart. By reversing the direction of the valve, the manometer is converted from a maximum into a minimum instrument. When an ordinary manometer is connected with a ven- tricular cavity, the movements of the mercury do not follow exactly the rapid variations of pressure of the cavity, and the height of the column fails to indicate both the highest and the lowest pressures. In this way in the dog a maximum pressure has been observed in the left ventricle of about 140 mm. (mercury), in the right ventricle of about 60 mm. and in the right auricle of about 20 mm. CHAP, iv.] THE VASCULAR MECHANISM. 151 Marey had previously, by means of his own instrument, determined the pressure in the horse to be in the left ventricle about 150mm., in the right ventricle only about 30 mm., while that of the right auricle he estimated at not more than a few mm. FIG. 25. THE MAXIMUM MANOMETER OF GOLTZ AND GAULE. At e a connection is made with the tube leading to the heart. When the screw clamp k is closed, the valve v comes into action, and the instrument, in the position of the valve shewn in the figure, is a maximum manometer. By reversing the direction of v it is converted into a minimum manometer. When k is opened, the variations of pressure are conveyed along a, and the instrument then acts like an ordinary manometer. It is interesting to observe that the minimum pressure may fall below that of the atmosphere : thus in the left ventricle (of the dog) a minimum pressure varying from — 52 to — 20 mm. may be reached, the minimum of the right ventricle being from — 17 to — 16 mm., and of the right auricle from — 12 to — 7 mm.1 Part of this diminution of pressure in the cardiac cavities may be due, as will be explained in a later part of this work, to the aspiration of the thorax in the respiratory movements. But even when the thorax is opened, and artificial respiration kept up, under which circumstances no such aspiration takes place, the pressure in the left ventricle may still sink as low as — 24 mm. The minimum ma- nometer, which shews most distinctly the existence of this negative pressure, obviously gives no information as to the exact phase of the beat in which it occurs ; and there is some difference of opinion as to the exact time at which it takes place. Goltz and Gaule, to 1 These numbers are to be considered merely as instances which have been observed, and not as averages drawn from a large number of cases. 152 DURATION OF THE CARDIAC PHASES. [Boon i. "whom we are indebted for the maximum and minimum manometer, believed that the negative pressure appeared at the beginning of the diastole and indeed that it was caused by the expansion of the ventricle. Were this the case, the ventricle might be regarded not only as a force pump driving blood into the arteries, but also as a suction pump drawing blood from the auricles and great veins. Others however find great difficulties in supposing that the ventricular walls can, either by virtue of the elasticity of their fibres, or by the contraction of special dilating fibres, or by becoming suddenly injected with blood through the coronary arteries, actually expand so as to exert any such suction power. And they maintain that the negative pressure seen in the ventricle is merely that same negative pressure due to the sudden emptying of the ventricle which we have already described as serving to close the semilunar valves. When the minimum manometer is used, the lowest limit of negative pressure is not reached until after several beats, indicating that its duration in any single beat must be very brief. The negative pressure due simply to the cessation of the flow is in fact almost immediately made away with by the ventricular walls, in their continued contraction coming into com- plete contact ; it passes off therefore before any blood can enter into the ventricle from the auricle, and hence can exert no suction power. Admitting this, however, it is still open for us to suppose that after this negative pressure has passed away, a second negative pressure is caused by the expansion of the ventricle in diastole ; and that this, though also brief, does exert a suction power. And indeed the view that the ventricle in expanding can produce such a negative pressure is one which cannot as yet be regarded as definitely disproved. The duration of the several phases. The time-measurements given in Fig. 21 afford a general idea of the relative duration of the several events in the slowly beating heart of the horse. Thus it is obvious that the longest phase (viz. about •£$ sec.) is that occurring between the end of the ventricular systole at e to the beginning of the auricular systole at b ; this is often spoken of as the diastole, or as the " passive interval," since during this time both auricles and ventricles are in diastole. The next longest phase is the systole of the ventricles (viz. rather more than yL- sec.), and the shortest (viz. rather less than T% sec.) is the systole of the auricles. When we desire to arrive at more complete measurements, we are obliged to make use of calculations based on various data; and these give only approximate results. Naturally the most interest is attached to the duration of events in the human heart. The datum which perhaps has been most largely used is the interval between the beginning of the first and the occurrence of the second sound. This may be determined with approximative correctness, and according to Bonders varies from '301 to '327 sec., CHAP, iv.] THE VASCULAR MECHANISM. 153 occupying from 40 to 46 p. c. of the whole period; and being fairly constant for different rates of heart-beat. The observer, listening to the sounds of the heart, made a signal at each event on a recording surface, the difference in time between the marks being measured by means of the vibrations of a tuning fork recorded on the same surface. By practice it was found possible to reduce the errors of observation within very small limits. Now whatever be the exact causation of the first sound, it is undoubtedly coincident with the systole of the ventricles, though possibly the actual commencement of its becoming audible may be slightly behind the actual beginning of the muscular con- tractions. Similarly the occurrence of the second sound due to the closure of the semilunar valves may, as we have seen, be taken to mark the close of the ventricular systole. And thus the interval between the beginning of the first and the occurrence of the second sound has been regarded as indicating approximatively the duration of the ventricular systole, i.e. the period during which the ventri- cular fibres are contracting. If however we accept the view that the ventricle still remains contracted for a brief period after the valves are shut, then the second sound does not mark the end of the systole, and the duration of the systole is rather longer than the *3 sec. given above. The propulsion of the blood into the aorta leads to an expansion of the aorta walls, known as the pulse, which we shall study more fully immediately. This pulse travels, as we shall see, along the arteries at a certain rate : it is later at arterial points more distant from the heart than at points nearer the heart. "We can calculate with approximative correctness the time it takes for the expansion to travel from the aortic valves to the radial artery at the wrist, for example. Now when we record, as we may do on the same recording surface, the exact moment at which the first sound begins, or at which the lever of the cardiograph begins to rise in the ventricular systole, and also the exact moment at which the expansion of the corresponding pulse at the wrist begins, and measure the interval of time between them, we find that the interval is greater than is required for the expansion of the pulse-wave to travel from the heart to the wrist. The difference gives the measure of the time during which the ventricle by its contraction is getting up an adequate pressure upon its contents, and during which, as yet, blood has not escaped from the ventricular cavity and begun to ex- pand the aorta : the measure in fact of what we called, a little while ago, the first period of the ventricular systole. This may also be estimated by directly measuring the time taken up by the upstroke of the cardiographic tracing, and has been said to be on an average about '085 sec. These measurements however are approximative only and there can be no doubt that the time varies very largely, being dependent on the quantity of blood in the ventricle, on the blood-pressure in the aorta and on the condition of the heart. 154 DURATION OF THE CARDIAC PHASES. [BoOK T- During the expansion of the artery and probably for some little time beyond, viz. up to the occurrence of what in speaking of the pulse-wave we shall callthe dicrotic notch, blood is being propelled from the ventricle. By measuring this time or by deductions from the curve of the cardiac impulse, it has been concluded that the time during which blood is escaping from the ventricle or the duration of the second phase of the ventricular systole, amounts to about O'l sec. Deducting these two periods from the total period of 0'3 sec., there would be left a period of O'l 15 sec., marking the third phase of the systole, during which the ventricle, though empty, is con- tinuing its contractions. Upon the view however that the closure of the valves does not mark the end of the systole, this phase must be taken as still longer. In a heart beating 72 times a minute, which may be taken as the normal rate, each entire cardiac cycle would last about 0'8 sec., and taking 0'3 sec. as the duration of the systole, the deduction of this would leave 0'5 sec. for the whole diastole of the ventricle including its relaxation. At the close of this period, there occurs the systole of the auricles, the exact duration of which it is difficult to determine, it being hard to say when it really begins, but which perhaps may be taken as lasting on an average O'l sec. The systole of the ventricle follows so immediately upon that of the auricles, that practically no interval exists between the two events. We may sum up therefore the details of the duration of the more important phases of the cardiac cycle in the following tabular form. sees. sees. Systole of ventricular previous to ~\ opening of semilunar valves . 0'085 Escape of blood into aorta . . O'lOO !- Continued contraction of the emptied ventricle . . . O'lloj Total systole of the ventricle . . 0'3 Diastole of both auricle and ven- 1 tricle or "passive interval" . 0'400 j> Systole of auricle . . . O'lOO J Sum of above two, making the diastole of ventricle or "pause" between second and first sound . 0'5 Total Cardiac Cycle . . . .; (^8 Or selecting only the important facts out of the -£$ sec. occupying the whole canfiac cycle, -^ sec. or possibly rather more are taken up by the systole, and T% sec. or possibly rather less by the diastole of the ventricle. The following diagram may be useful as giving in a graphic form a general idea of the sequence and duration of the several CHAP, iv.] THE VASCULAR MECHANISM. 155 cardiac events. It will be understood of course that the diagram is intended to shew merely the general relations of the several events and not to represent exact measurements. Fio. 26. DIAGRAMMATIC KEPBESENTATION OF THE MOVEMENTS AND SOUNDS OP TUB HEART DURING A CARDIAC PERIOD. (After Dr SHARPET.) We may repeat that the details given above are at the best approximative only, and, we may add, to a certain extent hypo- thetical. We have given them at such length not on account of their intrinsic importance, or because they are trustworthy data for further calculations, but because the study of them may help the reader in forming a more vivid image in his mind of what is taking place in the heart during a beat. Moreover it must be remembered that the figures quoted are those belonging to what may be considered a normal rate of heart beat. The rate how- ever at which the heart beats varies, as we shall see, under the influence of circumstances, within very wide limits. With regard to the duration of the several phases at different rates of heart beat, the most important fact is perhaps that the pause varies much more than does the systole of the ventricles. A quickly beating heart differs from a slowly beating heart by reason of the pause being shortened, much more than by each systole being of less duration. We may briefly recapitulate the main facts connected with the passage of blood through the heart as follows. The right auricle during its diastole, by the relaxation of its muscular fibres, and by the fact that all pressure from the ventricle is removed by the tension of the tricuspid valves, offers but little resistance to the ingress of blood from the veins. On the other hand, the blood in the trunks, of both the superior and inferior vena cava, is under a pressure, which diminishing towards the heart and becoming within 156 DURATION OF THE CARDIAC PHASES. [BOOK i. the thorax actually negative (as we shall see in speaking of respirations), remains higher than the pressure obtaining in the interior of the auricle; the blood in consequence flows into the empty auricle, its progress in the case of the superior vena cava being assisted by gravity. At each inspiration, this flow is favoured by the increased negative pressure in the heart and great vessels caused by the respiratory movements. Before this flow has gone on very long, the diastole of the ventricle begins, its cavity dilates, the flaps of the tricuspid valve fall back, and blood for some little time flows in an unbroken stream from the venae cavse into the ventricle. In a short time, however, probably before much blood has had time to enter the ventricle, the auricle is full, and forth- with its sharp sadden systole takes place. Partly by reason of the onward pressure in the veins, which increases rapidly from the heart towards the capillaries, partly from the presence of valves in the venous trunks and at the mouth of the inferior vena cava, but still more from the fact that the systole begins at the great veins themselves and spreads thence over the auricle, the force of the auricular contraction is spent in driving the blood, not back into the veins, but into the ventricle, where the pressure is still ex- ceedingly low. Whether there is any backward flow at all into the great veins or whether by the progressive character of the systole the flow of blood continues, so to speak, to follow up the systole without break so that the stream from the veins into the auricle is really continuous, is at present doubtful ; though a slight positive wave of pressure- synchronous with the auricular systole, travelling backward along the great veins has been observed at least in cases where the heart is beating vigorously. The ventricle thus being filled by the auricular systole, the play of the tricuspid valves described above comes into action, the auricular systole is followed by that of the ventricle and the pressure within the ventricle, cut off from the auricle by the tricuspid valves, is brought to bear entirely on the conus arteriosus and the pulmonary semilunar valves. As soon as by the rapidly increasing shortening of the ventricular fibres the pressure within the ventricle becomes greater than that in the pulmonary artery, the semilunar valves open and the still continuing systole discharges the contents of the ventricle into that vessel. As the ventricle thus rapidly and forcibly empties itself, a transient negative pressure makes its appearance in the rear of the ejected column of blood. This in return leads to a reflux of blood towards the ventricle. The first act of this reflux however is, as we have seen, to close the semilunar valves, and even if it be urged that the exit of the ventricular contents does not always end with sufficient abruptness to cause a negative pressure adequate to produce this result, the elastic rebound of the arteries, upon their receiving no fresh blood, has the same effect of closing the semilunar valves, and thus of shutting off the blood in the over- CHAP, iv.] THE VASCULAR MECHANISM. 157 distended arteries from the emptied ventricle. Coincidently with this closure, the systole as we have seen probably ends and relaxation begins ; then once more the cavity of the ventricle be- comes unfolded and finally distended by the influx of blood from the auricle. During the whole of this time the left side has with still greater energy been executing the same manoeuvre. At the same time that the vense cavas are filling the right auricle, the pulmonary veins are filling the left auricle. At the same time that the right auricle is contracting, the left auricle is contracting too. The systole of the left ventricle is synchronous with that of the right ventricle, but executed with greater force ; and the flow of blood is guided on the left side by the mitral and aortic valves in the same way that it is on the right by the tricuspid valves and those of the pulmonary artery. The Work done. We can measure with approximative exactness the intraven- tricular pressure, the length of each systole, and the number of times the systole is repeated in a given period, but perhaps the most important factor of all in the determination of the work of the vascular mechanism, the quantity ejected from the ventricle into the aorta at each systole, cannot be accurately determined ; we are obliged to fall back on calculations having many sources of error. The mean result of these calculations gives about 180 grms. (6 oz.) as the quantity of blood which is driven from each ventricle at each systole in a full-grown man of average size and weight. It is evident that exactly the same quantity must issue at a beat from each ventricle ; for if the right ventricle at each beat gave out rather less than the left, after a certain number of beats the whole of the blood would be gathered in the systemic circu- lation. Similarly, if the left ventricle gave out less than the right, all the blood would soon be crowded into the lungs. The fact that the pressure in the right ventricle is so much less than that in the left (probably 30 or 40 mm. as compared with 200 mm. of mercury), is due, not to differences in the quantity of blood in the cavities, but to the fact that the peripheral resistance which has to be overcome in the lungs is so much less than that in the rest of the body. Various methods have been adopted for calculating the average amount of blood ejected at each ventricular systole. It has been calculated from the capacity of the recently removed and as yet not rigid ventricle, filled with blood under a pressure equal to the calculated average pressure in the ventricle. This method of course presupposes 158 THE WORK DONE BY THE II E ART. [BOOK i. that the whole contents of the ventricle are ejected at each systole. Yolkmann measured the sectional area of the aorta, and taking an average velocity of the blood in the aorta (a very uncertain datum), calculated the quantity of blood which must pass through the sectional area in a given time. The number of beats in that time then gavo him the quantity flowing through the area, and consequently ejected from the heart, at each beat. The mean of many experiments on different animals came out '0025 p. c. of the body weight, which in. a man of 75 kilos would be 187*5 grms. Yierordt measured the mean velocity and the sectional area in the carotid, and thence, from a measurement of the sectional area of the aorta, and from a calculation of the blood's mean velocity in it, based on the supposition that the mean velocity in an artery was inversely as its sectional area, arrived at the quantity flowing through the aortic sectional area in a given time, and thus at the quantity passing at each beat. Both these calculations are vitiated by the fact that the variations of velocity in the aorta are so great, that any mean has really but little positive value. Pick by means of calculations based partly on the data gained by observing the increase of the volume of the whole arm at each cardiac systole, arrived at results much less than either of the above. In one case he estimated the quantity ejected from the heart at each beat at 53 grm., and in a second case at 77 grm. It must be remembered that though it is of advantage to speak of an average quantity ejected at each stroke, it is more than probable that that quantity may vary within very wide limits. Taking, however, 180 grms. as the quantity, in man, ejected at each stroke at a pressure of 250 mm.1 of mercury, which is equiva- lent to 3'21 metres of blood, this means that the left ventricle is capable at its systole of lifting 180 grms. 3'21 m. high, i.e. it does 578 gram-metres of work at each beat. Supposing the heart to beat 72 times a minute, this would give for the day's work of the left ventricle, nearly 60,000 kilogram-metres ; calculating the work of the right ventricle at one-fourth that of the left, the work of the whole heart would amount to 75,000 kilogram-metres, which is just about the amount of work done in the ascent of Snowdon by a tolerably heavy man. A calculation of more practical value is the following. Taking the quantity of blood as •£$ of the body weight, the blood of a man weighing 75 kilos would be about 5,760 grms. If 180 grms. left the ventricle at each beat, a quantity equivalent to the whole blood would pass through the heart in 32 beats, i.e. in less than half a minute. 1 A high estimate is purposely taken here. CHAP, iv.] THE VASCULAR MECHANISM. 159 Variations in the Heart's beat. These are for the most part in reality vital phenomena, i.e. brought about by events depending on changes in the vital properties of some or other of the tissues of the body. It will be convenient, however, briefly to review them here, though the discussion of their causation must be deferred to its appropriate place. The frequency of the heart, i.e. the number of beats in any given time, may vary. The average rate of the human pulse or heart-beat is 72 a minute. It is quicker in children than in adults, but quickens again a little in advanced age. It is quicker in the adult female than in the adult male, in persons of short stature than in tall people. It is increased by exertion, and thus is quicker in a standing than in a sitting, and in a sitting than in a lying posture. It is quickened by meals, and while varying thus from time to time during the day, is on the whole quicker in the evening than in early morning. It is said to be on the whole quicker in summer than in winter. Even independently of muscular exertion it seems to be quickened by great altitudes. It is profoundly influenced by mental conditions. The length of the systole may vary, indeed we have reason to think that it does vary considerably, though as a general and broad rule it may be stated that a frequent differs from an infrequent pulse chiefly by the length of the diastole. Donders found the length of the systole as measured by the interval between the first and second sounds to be for ordinary pulses remarkably constant in different persons, varying not more than from '327 to '301 sec., and being therefore relatively to the whole cardiac period less in slow than in quick pulses. • The force of the beat may vary ; the ventricular systole may be weak or strong. When the rate of beat is suddenly increased there is a tendency for the individual beats to be diminished in force, and on the other hand to be increased in force when the rate is diminished. But there is no necessary connection between rate and strength ; both a frequent and an infrequent pulse may be either weak or strong. The character of the beat may vary; the systole may be sudden and sharp, rapidly reaching a maximum and rapidly declining, or slow and lengthened, reaching its maximum only after some time and declining very gradually; the latter being the slow pulse (pulsus tardus) as distinguished from the infrequent pulse (pulsus rams). The pulse is also sometimes spoken of as being slapping, and sometimes as heaving. But, as we shall see immediately, the features of the pulse are dependent not only on the heart beat but also on the condition of the arteries. 160 VARIATIONS IN THE HEARTS BEAT. [BOOK I. The rhythm may be intermittent or irregular. Thus in an intermittent pulse, a beat may be so to speak dropped : the hiatus occurring either regularly or irregularly. In an irregular rhythm succeeding beats may differ in length, force; or character. SEC. 3. THE When the finger is placed on an artery, such as the radial, an intermittent pressure on the finger, coming and going with the beat of the heart, is felt. When a light lever such as that of the sphygmograph is placed on the artery, the lever is raised at each beat, falling between. The pressure on the finger, and the raising of the lever, are expressions of the expansion of the elastic artery, of the temporary additional distension which the artery undergoes at each systole of the ventricle. This intermittent expansion is called the pulse; it corresponds to the intermittent outflow of blood from a severed artery, being present in the arteries only, and except under particular circumstances, absent from the veins and capillaries. The expansion is frequently visible to the eye, and in some cases, as where an artery has a bend, may cause a certain amount of locomotion of the vessel. All the more important phenomena of the pulse may be witnessed on an artificial scheme. If two levers be placed on the arterial tubes of an artificial1 scheme, one near to the pump, and the other near to the peripheral resistance, with a considerable length of tubing between them, and both levers be made to write on a recording surface, one im- mediately below the other, so that their curves can be more easily compared, the following facts may be observed, when the pump is set to work regularly. 1 By this is simply meant a system of tubes, along which fluid can be driven by a pump worked at regular intervals. In the course of the tubes a (variable) resistance is introduced in imitation of the peripheral resistance. The tubes on the proximal side of the resistance consequently represent arteries; those on the distal side, veins. F. 11 162 THE PULSE. [BOOK 1. With each stroke of the pump, each lever (Fig. 27, L and II.) rises to a maximum, la, 2a, and then falls again, thus describing a curve, — the pulse-curve. This shews that the expansion of the 1 '• — 5ov\AAAAAAAAAAAAAAA/ FIG. 27. Pulse-curves described by a series of sphygmographic levers placed at intervals of 20 cm. from each other along an elastic tube into which fluid is forced by the sudden stroke of a pump. The pulse- wave is travelling from left to right, as indicated by the arrows over the primary (a) and secondary (b, c) pulse- waves. The dotted vertical lines drawn from the summit of the several primary waves to the tuning-fork curve below, each complete vibration of which occupies ^sec., allow the time to be measured which is taken up by the wave in passing along 20 cm. of the tubing. The waves a are waves reflected from the closed distal end of the tubing ; this is indicated by the direction of the arrows. It will be observed that in the more distant lever VI. the reflected wave, having but a slight distance to travel, becomes fused with the primary wave. (From Marey.) tubing passes the point on which the lever rests in the form of a wave. At one moment the lever is quiet: the tube beneath it is simply distended to the normal permanent amount indicative CHAP, iv.] THE VASCULAR MECHANISM. 163 of the mean arterial pressure; at the next moment the pulse expansion reaches the lever, and the lever begins to rise, and continues to do so until the top of the wave reaches it, after which it falls again until it is once more at rest, the wave having completely passed by. The rise of each lever is somewhat sudden, but the fall is more gradual, and is generally marked with some irregularities. The suddenness of the rise is due to the suddenness with which the sharp stroke of the pump expands the tube; the fall is more gradual because the elastic reaction of the walls, whereby the tube returns to its former condition after the expanding power of the pump has ceased, is gradual in its action. 2. The size and form of each curve depend in part on the amount of pressure exerted by the levers on the tube. If the levers only just touch the tube in its expanded state, the rise in each will be insignificant. If on the other hand they be pressed down too firmly, the tube beneath will not be able to expand as it otherwise would, and the rise of the levers will be proportion- ately diminished. There is a certain pressure, depending on the expansive power of the tubing, at which the tracings are best marked. 3. If the points of the two levers be placed exactly one under the other on the recording surface, it is obvious that, the levers being alike except for their position on the tube, any difference in time between the movements of the two levers will be shewn by an interval between the beginnings of the curves they describe, if the recording surface be made to travel sufficiently rapidly. If the movements of the two levers be thus compared, it will be seen that the far lever (Fig. 27, II.) commences later than the near one (Fig. 27, 1.), the farther apart the two levers are, the greater is the interval in time between their curves. Compare the series I. to VI. (Fig. 27). This means that the wave of expansion, the pulse-wave, takes some time to travel along the tube. By exact measurement it would similarly be found that the rise of the near lever began some fraction of a second after the stroke of the pump. The velocity with which the pulse-wave travels depends chiefly on the amount of rigidity possessed by the tubing. The more extensible (with corresponding elastic reaction) the tube, the slower is the wave ; the more rigid the tube becomes, the faster the wave travels. The width of the tube is of much less influence, though ac- cording to some observers the wave travels more slowly in the wider tubes. The rate at which the normal pulse- wave travels in the human body has been variously estimated at from 10 to 5 metres per second. In all probability the lower estimate is the more correct one ; but it must be remembered that in all probability the rate varies very considerably under different conditions. According to all observers the velocity of the wave in passing from the groin to 11—2 164 THE PULSE. [BOOK i. the foot is greater than that in passing from the axilla to the wrist (6 m. against 5 m.). This is probably due to the fact that the femoral artery with its branches is more rigid than the axil- lary. So also in the arteries of children, the wave travels more slowly than in the more rigid arteries of the adult ; and the velocity appears to be increased by circumstances which heighten and decreased by those which lessen the mean arterial pressure, since with increasing or diminishing pressure the arterial walls become more or less rigid. 4. When two curves taken at different distances from the pump are compared with each other, the far curve will be found to be shallower, with a less sudden rise, and with a more rounded summit than the near curve : compare 5a with la, Fig. 27. In other words, the pulse-wave as it travels onward becomes diminished and flattened out. If a series of levers, otherwise alike, were placed at intervals on a piece of tubing sufficiently long to convert the intermittent stream into a continuous flow, the pulse-wave might be observed to gradually flatten out and grow less until it ceased to be visible. Care must be taken not to confound the progression of the pulse-wave with the progression of the fluid itself. The pulse- wave travels over the moving blood somewhat as a rapidly moving natural wave travels along a sluggishly flowing river, the velocity of the pulse-wave being 9 metres per sec., while that of the current of blood is not more than half a metre per sec. even in the large arteries, and diminishes rapidly in the smaller ones. Taking the duration of the pulse-wave, that is the time taken by any point in the arterial tract, in expanding and returning to its former calibre, so low as -^ of a second, it is evident that the pulse-wave started by any one systole, even if it travels so slowly as 5 m. per sec., will before it is completed have reached a point y^ of 5m. = 2 in. distant from the ventricle. But even in the tallest man the tips of the toes are not 2 m. distant from the heart. In other words, the length of the pulse-wave is much greater than the whole length of the arterial system, so that the beginning of each wave has become lost in the small arteries and capillaries some time before the end of it has finally passed away from the beginning of the aorta. The general causation of the pulse may then be summed up somewhat as follows. The systole of the ventricle drives a quantity of blood into the already full aorta. The sudden injection of this quantity of blood expands the portion of the aorta next to the heart, and thus gives rise to the sudden up-stroke of the pulse-curve. The rapidity of the flow from the ventricle being greatest at its beginning, the maximum of expansion is soon reached, and the aortic walls, even while for a short time blood is still, with diminishing rapidity, issuing from the ventricle, tend by virtue of their elasticity to return to their former calibre. This CHAP, iv.] THE VASCULAR MECHANISM. 165 return continues after the flow has ceased, and the aortic valves soon becoming closed, the elastic force thus brought into play serves to drive the blood onward. The elastic recoil being slower than the initial expansion, the down-stroke of the pulse-curve is more gradual than the up-stroke. Of this portion of the aorta, which actually receives the blood ejected from the heart, the part immediately adjacent to the semilunar valves begins to expand first, and the ex- pansion travels thence on to the end of this portion. In the same way it travels on from this portion through all the succeeding portions of the arterial system. For the total expansion required to make room for the new quantity of blood cannot be provided by that portion alone of the aorta into which the blood is actually received ; it is supplied by the whole arterial system : the old quantity of blood which is replaced by the new in this first portion has to find room for itself in the rest of the arterial space. As the expansion travels onward, however, the increase of pressure which each portion transmits to the succeeding portion will be less than that which it received from the preceding portion. For the whole increase of pressure due to the systole of the ventricle has to be distributed over the whole of the arterial system, and a fraction of it must therefore be left behind at each stage of its progress ; that is to say, the expansion is continually growing less, as the pulse travels from the heart to the capillaries ; hence the diminished height of the pulse-curve in the more distant arteries, and its disappearance in the capillaries. Secondary Waves and Dicrotism. In nearly all pulse tracings, the curve of the expansion and contraction of the artery is broken A/VVWl/WWWWV FlG. 28. PULSE-TBACING FEOM CAROTID ARTERY OF HEALTHY MAN1 (from Moens). x, commencement of expansion of the artery. A, summit of the first rise. C , dicrotic secondary wave. B, predicrotic secondary wave, p notch preceding this. D, succeeding secondary wave. The curve above is that of a tuning-fork with ten double vibrations in a second. 1 It will be understood that in the case of this and the succeeding sphygmo- graphic tracings (for the latter I am indebted to Dr Galabin and Dr Roy) comparisons between the several curves can only be made in a limited manner and with precautions, since the tracings are taken with different amplifications, pressures, &c. — and are some from man, others from animals. They are introduced simply to illustrate points treated of successively in the text. 166 THE PULSE. [BOOK L by two, three, or several smaller elevations and depressions: secondary waves are imposed upon the fundamental wave. In the sphygmographic tracing from the carotid and radial reproduced in Figs. 28 and 29 and in many of the other tracings given, these secondary elevations are marked as B, C, D. When one such FIG. 29. PULSE-CURVE FROM RADIAL OP MAN. Taken with extra vascular pressure of 70 mm. mercury. The vertical curved line L, gives the tracing which the recording lever made when the blackened paper was motionless. The horizontal line forms the abscissa of the tracing. The curved interrupted lines shew the distance from one another in time of the chief phases of the pulse wave, x = commencement and A close of expansion of artery, p, predi- crotic notch, d, dicrotic notch. C, dicrotic crest. D, post-dicrotic crest. /, the post-dicrotic notch. secondary elevation only is conspicuous, so that the pulse-curve presents two notable crests only, the primary crest and the second- ary one, the pulse is said to be "dicrotic"; when two secondary crests are prominent, the pulse is often called "tricrotic," where FIG. 30. ANACROTIC PULSE-TRACING FROM THE CAROTID OF RABBIT. several "polycrotic." As a general rule, the secondary elevations appear only on the descending limb of the whole wave as in most of the curves given, and the curve is then spoken of as "katacrotic." Sometimes, however, the first elevation or crest is not the highest but CHAP, iv.] THE VASCULAR MECHANISM. 167 appears on the ascending portion of the main curve as in Fig. 30 and Fig. 33 : such a curve is spoken of as "anacrotic." Of these secondary elevations, the most frequent, conspicuous and important is the one which appears some way down on the descending limb and is marked C on most of the curves. It is more or less distinctly visible on all sphygmographic tracings and may be seen in sphygmograms of the aorta as well as of other arteries. Sometimes it is so slight as to be hardly discernible; at other times it may be so marked as to give rise to a really double pulse (Fig. 31), i.e. a pulse which can be felt as double by the finger ; hence it has been called the dicrotic elevation or the dicrotic wave, the notch preceding the elevation being spoken of as the "dicrotic FlG. 31. TWO GBADES OF MARKED DICBOTISM IN RADIAL PULSE OF MAN. (Typhoid Fever.) notch." Neither it nor any other secondary elevations can be recog- nised in the tracings of blood-pressure taken with a manometer. This may be explained by the fact that the movements of the mercury column are too sluggish to reproduce these finer variations; but dicrotism is also conspicuous by its absence in the tracings given by more delicately responsive instruments. Moreover, when the normal pulse is felt by the finger, most persons find themselves unable to detect any dicrotism. Hence some have been led to FlG. 32. NOBMAL PULSE-CURVE IN THE AORTA FROM THE DOG. maintain that this and the other secondary elevations do not really exist in the normal pulse. But it seems difficult to maintain this view in face of the experiment of Landois, in which the tracing obtained by allowing the blood to spirt directly from an opened small artery, such as the dorsalis pedis, upon a recording surface, shewed in an unmistakeable manner the existence of the dicrotic wave. 168 THE PULSE. [BOOK i. Less constant and conspicuous than the dicrotic wave but yet appearing in most sphygmograms is an elevation which appears higher up on the descending limb of the main wave; it is marked B on some of the curves and is frequently called the predicrotic FIG. 33. ANAGBOTIC SPHTGMOGBAPH TRACING FROM THE ASCENDING AORTA (Aneurism). wave ; it may become very prominent. Sometimes other secondary waves are seen following the dicrotic wave as at D in Fig. 28; but these are very inconstant and usually even when present incon- spicuous. When tracings are taken from several arteries or from the same artery under different conditions of the body, these secondary waves are found to vary very considerably, giving rise to many characteristic forms of pulse-curve. Moreover in the same artery, FlG. 34. PULSE-TRACING FROM THE DORSALIS PEDIS. and with the same instrument, the form and even the special features of the curve vary according to the amount of pressure (expressed either in ounces or in mm. of mercury) with which the lever is pressed upon the artery. Figs. 35, 36 shew a series of changes thus brought about by varying the pressure of the lever ; and Fig. 37 shews the effect of this extra vascular pressure on the form of a fully dicrotic pulse. This effect of pressure in fact varies according to the condition of the vascular system. "Were we able with certainty to trace back the several features of the curves to their respective causes, an adequate examination of sphygmographic tracings would undoubtedly disclose much valuable information concerning the condition of the body pre- senting them. Unfortunately the problem of the origin of these secondary waves is a most difficult and complex one ; so much so that the detailed interpretation of a sphygmographic tracing is still in most cases extremely uncertain. CHAP, iv.] THE VASCULAR MECHANISM. 169 Various causes have been suggested as bringing about the secondary waves, and much discussion has arisen especially con- cerning the dicrotic wave. When the tube of the artificial scheme bearing two levers is blocked just beyond the far lever, the primary wave is seen to be accompanied by a second wave, which at the far lever is seen close to, and often fused into, the primary wave Fra. 35. INFLUENCE OF CHANGES IN THE PRESSURE APPLIED TO THE EXTERIOR OF THE VESSEL ON THE FORM OF THE CURVE. a, From the Art. radialis of healthy man of 27 years of age with an extra arterial pressure equal in a to 70 mm., in a' to 50mm., in a" to 30 mm. mercury. (Fig. 27, VI. a'), but at the near lever is at some distance from it (Fig. 27, I. a), being the farther from it, the longer the interval between the lever and the block in the tube. The second wave is evidently the primary wave reflected at the block and travelling backwards towards the pump. It thus of course passes the far lever before the near one. And it has been argued that the dicrotic wave of the pulse is really such a reflected wave, started either at the minute arteries and capillaries, or at the points of bifurcation of the larger arteries, and travelling backwards to the aorta. But if this were the case the distance between the primary crest and the dicrotic crest ought to be less in arteries more distant from the heart than in those nearer, just as in the artificial scheme the reflected wave is fused with a primary 170 THE PULSE. [BOOK i. wave near the block, but becomes more and more separated from it, the farther back we trace it. Now this is not the case with the dicrotic wave. Careful measurements shew that the distance between the primary and dicrotic crests is either greater FlO. 36. NOBMAL PULSE-CURVE FBOM CAEOTID OF BABBIT J shewing influence on height and form of curve of changes in the extra vascular pressure which was in a 20 mm., in 6 30 mm., in c 40 mm., and d 50 mm. of mer- cury. or certainly not less in the smaller or more distant arteries than in the larger or nearer ones. This feature indeed proves that the dicrotic wave cannot be in any way a retrograde wave. Again, the more rapidly the primary wave is obliterated or at least diminished on its way to the periphery the less conspicuous should be the dicrotic wave. Hence increased extensibility and increased elastic reaction of the arterial walls which tend to use up rapidly the primary wave, should also lessen the dicrotic wave. But as a matter of fact these conditions are favourable to the prominence of CHAP, iv.] THE VASCULAR MECHANISM. 171 the dicrotic wave. Besides the multitudinous peripheral division would render one large peripherically reflected wave impossible. But in addition to reflected waves, other waves which may be called "waves of oscillation," make their appearance when a fluid is driven through a system of tubes, by means of an intermittent force. And different origins have been assigned to secondary waves of this description. FIG. 37. DICROTIC PULSE-CURVE DUE TO LOSS OF BLOOD. From carotid of rabbit with, extra-vascular pressures in a of 50 mm., & of 40 mm. c of 20 mm., and d of 10mm. of mercury. Thus when the rapid flow of a fluid along a tube is suddenly checked at a point of its course the inertia of the fluid will carry the column of fluid still forwards so as to leave behind it a diminution of pressure. This diminution will appear on a graphic record of the pressure as a depression or notch ; and will be followed by a secondary rise as a reflux of fluid takes place towards the point where the pressure has become diminished. Both the depression and the secondary rise will travel as a wave along the tube, being frequently followed by other smaller waves of similar character and similar origin. Waves thus originating have been appealed to as explaining the secondary waves of the pulse-curve. Thus at the moment when the ventricle, having emptied itself, ceases to throw any more blood into the aorta, the blood which was last ejected being carried forward by its inertia gives rise to a diminution of pressure in the ventricle and at the root of the aorta. The aortic walls forthwith contract upon this diminished pressure, and a reflux of blood towards the semilunar valves takes place, leading to the appearance of a depression or notch in the pulse-curve, which is propagated forwards along the aorta. This reflux closes the semi- lunar valves and at the same time leads to a recovery of pressure 172 THE PULSE. [BOOK i. which similarly appears on the pulse-curve as an elevation succeed- ing the notch. Then again it has been argued that in any section of the arterial tract, the inertia of the walls and of the contained blood, in each expansion of the section, carries them on in their movement of expansion some little time after the actual expanding force has ceased to act. This leads to a falling back or contraction, which again by reason of the same inertia overshoots its mark, and thus through a series of oscillations, of which the first is the most conspicuous, the artery settles down to its normal calibre before the next expansion reaches it. The extent of such oscillations is determined, not only by the character of the walls but by the specific gravity of the contained fluid. In the artificial scheme with the same elastic tubing the secondary waves thus caused are much greater with mercury than with water, and disappear almost wholly when air is employed. Such waves of oscillation may be supposed to be generated in different degrees, in each and every section of the arterial tract ; the waves due to a cessation of the flow are on the contrary generated at the point where the inter- mittence is effected, and may be seen in rigid as well as in elastic tubes ; but these latter waves also are profoundly modified by the nature of the walls of the tubes along which they are transmitted. Lastly, it has been maintained that these secondary waves are of active not passive origin; that is, that they are caused by a rapid muscular contraction of the arterial walls following up so to speak the arterial beat. We have dwelt at so great a length on these secondary waves of the pulse-curve because of the importance attached to them in clinical medicine ; but it would be hardly profitable to enter more fully into the discussion of these several contending views. As an instance of the difficulty of the subject and the insufficiency of our knowledge, we may point out that observers are not yet agreed as to which part of the curve corresponds to the closure of the semilunar valves. Thus some maintain that this event corresponds to and indeed is indicated by the dicrotic wave, the dicrotic notch representing the reflux towards the ventricle, and the dicrotic elevation a new forward movement reflected from the closed valves. But under this view, though it seems the more probable, the predicrotic wave presents a difficulty; and indeed others maintain that the moment of closure of the semilunar valves is indicated by this the predicrotic, and not by the dicrotic wave. Until this and other points are finally settled, all interpretations of modifications of the pulse-curve must remain uncertain and un- satisfactory. The following facts however may be borne in mind as not only of practical importance, but as necessary data for any judgments concerning the pulse-curve. CHAP, iv.] THE VASCULAR MECHANISM. 173 1. Whatever the origin of the dicrotic wave, its features may be modified by changes taking place in the peripheral (arterial) districts without any alteration in the central (cardiac) events. Thus dicrotism may become conspicuous in one artery while re- maining indistinct in others. 2. The prominence of the dicrotic wave, though favoured by a sudden strong ventricular systole, is especially assisted by a diminution of blood-pressure. Thus it is a marked characteristic of the pulse in many cases of fever (Fig. 31) where blood-pressure , is low. So also it may be brought on at once in an artery in which it was previously insignificant by sudden lowering of the blood- pressure as is shewn in Fig. 38. It may similarly be induced by FIG. 38. TRACING FBOM RADIAL IN MAN ; shewing change in form of pulse-curve accompanying a sudden fall in the blood- pressure. The pulse, at first not markedly dicrotic, rapidly becomes so, and then passes on into the condition known as hyperdicrotism, where the dicrotic notch reaches a level lower than that from which the primary rise started. section of the vaso-motor nerves belonging to the branches of the artery; this, as we shall presently see, diminishes the peripheral resistance, through an expansion of the minute arteries, and so leads to a lowering of the blood-pressure in the main arteries. The prominence of the dicrotic wave is further dependent on the amount of extensibility and elastic reaction of the arterial walls. Hence the dicrotic wave is not well marked in arteries which have become rigid by disease or old age. We may add that an anacrotic pulse, in which a crest followed by a notch is visible on the ascending portion of the curve, before the maximum of expansion is reached, though it may sometimes be produced temporarily in healthy persons, is generally associated with diseased conditions, usually such in which the arteries are abnor- mally rigid. It has been interpreted as due to the pressure in the aorta rising even after the first rapid rush from the ventricle. Under 174 THE PULSE. [BOOK i. normal conditions, as we have already seen, the maximum expansion is soon reached, but in cases where the arterial walls are unusually rigid and the heart at the same time not abnormally weak, the ventricle may continue to empty itself against a resistance which increases rapidly with the amount of blood passing into the aorta, so that in spite of the diminishing rapidity with which the blood is leaving the ventricle the insufficient distensibility of the vessels causes the pressure in their interior to continue to rise until nearly the end of the outflow from the heart. An anacrotic pulse also frequently accompanies hypertrophy and dilation of the left ventricle. The pulse then is the expression of two sets of conditions : one pertaining to the heart, and the other to the arterial system. The arterial conditions remaining the same, the characters of the pulse may be modified by changes taking place in the beat of the heart ; and again, the beat of the heart remaining the same, the pulse may be modified by changes taking place in the arterial walls. Hence the diagnostic use of the pulse-characters. It must however be remembered that arterial changes may be accompanied by com- pensating cardiac changes, to such an extent, that the same features of the pulse may obtain under totally diverse conditions, provided that these conditions affect both factors in compensating directions. Venous Pulse. Under certain circumstances the pulse may be carried on from the arteries through the capillaries into the veins. Thus when the salivary gland is actively secreting, the blood may issue from the gland through the veins in a rapid pulsating stream. The nervous events which give rise to the secretion of saliva, lead at the same time, by the agency of vaso-motor nerves, of which we shall presently speak, to a dilation of the small arteries of the gland. This dilation of the small arteries diminishes the peripheral resist- ance by allowing more blood to pass through them with less friction; in consequence the elasticity of the arterial walls is brought into play to a less extent than before, and this may in certain cases go so far, that as in the case of the artificial apparatus, where the elastic tubing has an open end (see p. 129), not enough elasticity is brought into action to convert the intermittent arterial flow into a con- tinuous one. A similar venous pulse is also sometimes seen in other organs. Careful tracings of the great veins in the neighbourhood of the heart shew elevations and depressions, which appear due to the variations of intracardiac pressure, and which may perhaps be spoken of as constituting a "venous pulse"; but at present they need further elucidation. In cases of insufficiency of the tricuspid valves, the systole of the ventricle makes itself felt in the great veins; and a distension travelling backwards from the heart be- CHAP, iv.] THE VASCULAR MECHANISM. 175 comes very visible in the veins of the neck. This is sometimes spoken of as a venous pulse. Variations of pressure in the great veins due to the respiratory movements are also sometimes spoken of as a venous pulse ; the nature of these variations will be explained in treating of respi- ration. II. THE VITAL PHENOMENA OF THE CIRCULATION. So far the facts with which we have had to deal, with the ex- ception of the heart's beat itself, have been simply physical facts. All the essential phenomena which we have studied may be re- produced on a dead model. Such an unvarying mechanical vascular system would however be useless to a living body whose actions were at all complicated. The prominent feature of a living mechanism is the power of adapting itself to changes in its in- ternal and external circumstances. In such a system as we have sketched above there would be but scanty power of adaptation. The well-constructed machine might work with beautiful regu- larity; but its regularity would be its destruction. The same quantity of blood would always flow in the same steady stream through each and every tissue and organ, irrespective of local and general wants. The brain and the stomach, whether at work and needing much, or at rest and needing little, would receive their ration of blood, allotted with a pernicious monotony. Just the same amount of blood would pass through the skin on the hottest as on the coldest day. The canon of the life of every part for the whole period of its existence would be furnished by the inborn diameter of its blood-vessels, and by the unvarying motive power of the heart. Such a rigid system however does not exist in actual living beings. The vascular mechanism in all animals which possess one is capable of local and general modifications, adapting it to local and general changes of circumstances. These modifications fall into two great classes : 1. Changes in the heart's beat. These, being central, have of course a general effect. 2. Changes in the peripheral resistance, due to variations in the calibre of the minute arteries, brought about by the agency of their contractile muscular coats. These changes may be either local or general. CHAP, iv.] THE VASCULAR MECHANISM. 177 To these may be added as subsidiary modifying events : 3. Changes in the peripheral resistance of the capillaries due to alterations in the adhesiveness of the capillary walls or to other influences arising out of the as yet obscure relations existing between the blood within and the tissue without the thin per- meable capillary walls, and depending on the vital conditions of the one or of the other. Such changes causing an increase of peri- pheral resistance are seen to a marked degree in the pathological condition known as stasis. 4. Changes in the quantity of blood in circulation. The two first and chief classes of events (and probably the third) are directly under the dominion of the nervous system. It is by means of the nervous system that the heart's beat and the calibre of the minute arteries are brought into relation with each other, and with almost every part of the body. It is by means of the nervous system acting either on the heart, or on the small arteries, or on both, that a change of circumstances affecting either the whole or a part of the body is met by compensating or regulative changes in the flow of blood. It is by means of the nervous system that an organ has a more full supply of blood when at work than when at rest, that the stream of blood through the skin rises and ebbs with the rise and fall of the temperature of the air, that the work of the heart is tempered to meet the strain of overfull arteries, and that the arterial gates open and shut as the force of the central pump waxes and wanes. Each of these vital factors of the circulation must therefore be considered in connection with those parts of the nervous system which are concerned in its action. F. 12 SEC. 4. CHANGES IN THE BEAT OF THE HEART. We have already discussed the more purely mechanical pheno- mena of the heart. We have therefore in the present section only to inquire into the nature and working of the mechanism (chiefly at least nervous) by which the beat of the heart is maintained, varied, and regulated. In studying closely the phenomena of the beat of the heart it becomes necessary to obtain a graphic record of various movements. 1. In the frog or other cold-blooded animal, a light lever may be placed directly on the ventricle (or on an auricle,