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The Molecular Properties and Evolution of Excitable Cells PDF

260 Pages·1967·3.672 MB·English
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INTERNATIONAL SERIES OF MONOGRAPHS IN PURE AND APPLIED BIOLOGY Division: ZOOLOGY GENERAL EDITOR: G.A.KERKUT VOLUME 35 THE MOLECULAR PROPERTIES AND EVOLUTION OF EXCITABLE CELLS The Molecular Properties and Evolution of Excitable Cells BY C. J. DUNCAN Department of Zoology, the University of Durham, Durham P E R G A M ON PRESS OXFORD · LONDON · EDINBURGH · NEW YORK TORONTO · SYDNEY · PARIS · BRAUNSCHWEIG Pergamon Press Ltd., Headington Hill Hall, Oxford 4 & 5 Fitzroy Square, London W.l Pergamon Press (Scotland) Ltd., 2 & 3 Teviot Place, Edinburgh 1 Pergamon Press Inc., 44-01 21st Street, Long Island City, New York 11101 Pergamon of Canada, Ltd., 6 Adelaide Street East, Toronto, Ontario Pergamon Press (Aust.) Pty. Ltd., 20-22 Margaret Street, Sydney, N.S.W. Pergamon Press S.A.R.L., 24 rue des Écoles, Paris 5 e Vieweg & Sohn GmbH, Burgplatz 1, Braunschweig Copyright © 1967 Pergamon Press Ltd. First edition 1967 Library of Congress Catalog Card No. 66-29718 2797/67 FOR My Mother My. Father and My Wife PREFACE OVER the past 5 years I have been interested in the manner in which excitable cells such as nerves, muscles and sense organs operate. I was therefore pleased when Dr. G. A. Kerkut suggested that I should present these ideas in book form with the accent on the theoretical aspects of the subject. My main aim has been to present a concrete hypothesis, and for this reason much of the experimental evidence is presented in sum- mary form, although in certain instances further amplification can be found in the figure legends. I have redrawn many of the figures used, and the following jour- nals, societies and publishers gave their permission to reproduce material: Academic Press (Arch. Biochem. Biophys.), Acta Physio- logica Scandinavica, American Physiological Society, Animal Be- haviour, Annual Reviews Inc., Elsevier Publishing Company (Bio- chim. Biophys. Acta, 3, p. 503, Fig. 4), Japanese Journal of Physio- logy, Journal of Biological Chemistry, Journal of Physiology, Nature, New York Academy of Sciences, the Rockefeller Institute Press (J. gen. Physiol.), the Royal Society, the Society for Experimental Biology, the Wistar Institute of Anatomy and Biology (J. cell. comp. Physiol.), and Yale University Press. I am most grateful to my friends (especially those at Liverpool, where these ideas were first formulated) who have given generously of their time and have helped me in many ways. In particular it is a pleasure to thank Professor D. Barker, Dr. K. Bowler, Dr. G.A. Kerkut, Professor R. J.Pumphrey, F.R.S., Dr. D. V. Roberts and Dr. C.L.Smith. However, the responsibility for the errors and shortcomings is mine alone. I should like to thank Mrs. R. Bullen and Miss L. Rocks, who helped me with much of the typing of the final manuscript, and I am grateful to my wife who not only typed a great deal of the first draft but also helped in the many tasks associated with checking and preparing the manuscript for press. xi CHAPTER 1 INTRODUCTION THE purpose of this monograph is to present evidence and to deve- lop a hypothesis concerning the evolution and properties of ex- citable cells. Such a story is essentially concerned with the proper- ties of the bounding membrane of such cells and with its complex permeability system, upon which the process of excitation depends. As a review it is not comprehensive, because neurophysiologists are fortunate in having many detailed accounts of axonal and synaptic transmission, and in particular two recent monographs by A.L. Hodgkin {The Conduction of the Nervous Impulse, 1964) and J.C.Eccles {The Physiology of Synapses, 1964) give a summary of current thinking in these fields. Apart from a brief paragraph of introduction where necessary, I shall not attempt to duplicate their approach; the reader is referred to the extensive bibliographies which these books contain. Rather, I shall take the phenomena described by Hodgkin and Eccles as a starting point and try to present a hypothesis concerning the events which underlie them, assembling evidence from the results of a range of experimental techniques and disciplines. Again, it would be almost impossible to cover all the relevant literature in the fields of electron microscopy, histochemistry, biochemistry, physiology, pharmacology and mole- cular biology, and I have relied on quoting reviews where possible or selecting what seems to me to be suitable experimental evidence to support each hypothesis. The result is not an exhaustive review, but a monograph with a strong personal flavour, in which I shall try to suggest the ways in which excitable cells operate. The primary aim will be one of unification, a presentation of uniform concepts from the wealth of data available from active fields of research. It will be suggested that excitable cells could have evolved from a primitive condition which is illustrated in such simple animals as Amoeba, the hypothesis presented in this monograph having been developed from some preliminary ideas concerning the properties 1 2 MOLECULAR PROPERTIES AND EVOLUTION of excitable cells which have been given in previous papers (Duncan, 1963a, 1964a, 1965). The complex process of nervous conduction is, of course, as- sociated with the subtle ionic permeability properties of the nerve membrane, their transient transformation during the passage of the action potential and the maintenance of the differential ionic con- centration across the nerve membrane by the action of the active cation pump. In this review, therefore, we shall consider evidence concerning the nature of the system which controls the passive ionic permeability of the membrane of the excitable cell and suggest how it may have originated, evolved and differentiated. The membrane theory of conduction along the nerve fibre may be stated briefly as follows. The membrane is assumed to be more permeable to potassium than to sodium ions in the resting condi- tion. If the membrane were permeable to potassium ions only, the potential difference across it would approach the maximum value predicted by the Nernst equation : [K]o VK = — · l0g Γ e [K] t [Na] 0 Γ [Na] t INTRODUCTION 3 would be + 55 mV for a squid giant axon, giving a theoretical total potential change of 130 mV. Again, recorded values for the positive overshoot fall below the predicted maximum, indicating that the membrane is not completely selective for sodium. FIG. 1.1. Diagram to illustrate the membrane theory of axonal conduc- tion. The potentials across the membrane of the squid axon are shown under conditions of excitation and rest, together with their approximate derivation from the Nernst equation. Propagation of the action potential is achieved by a flow of cur- rent in a local circuit between the active area and the resting region of the nerve membrane immediately ahead. The current flow reduces the membrane potential in the inactive region, and this depolariza- tion in turn causes a rise in sodium permeability there (see Chap- ter 10). Experimental evidence suggests that an active cation pump is also present in the membrane and serves to drive out ions against their concentration gradient, the ions having been accumulated either during nerve activity or by membrane leakage. There is good evidence (Chapter 4) that a membrane adenosine triophosphatase (ATPase) enzyme system is concerned with such transport and that it is dependent on metabolism and a supply of ATP (see review, Hodg- kin, 1964). 4 MOLECULAR PROPERTIES AND EVOLUTION 1. THE ORGANIZATION OF EXCITABLE CELLS Grundfest (1957, 1959a, b, 1961) has elaborated on the early ideas of Parker (1919) and has produced a hypothesis for the evo- lution and organization of excitable cells. Parker (1919) suggested that the nervous system of the Metazoa evolved from a cell which was a primitive receptor-effector. Such a cell is found in sponges; it is sensitive to stimuli and is able to respond by appropriate ac- tivity. The receptor and effector components became separated in space, and specialized for their separate functions during the evolu- tion of the Metazoa. Connection between the two was maintained by the development of an axonal component in the receptor, and distinct neuronal cells with integrative functions were subsequently evolved. Input Conductile component Output component Γ1" component Ί Graded, Specific localized de- Graded stimuli or secretion ' hyperpolarization Excitation Depolarizing . Inhibition t All-sopri-kneost hing Hyperpolarizing FIG. 1.2. Scheme suggested by Grundfest (1957, 1959a, b, 1961) for the organization of excitable cells. There are three components of action, namely input, conduction and output (upper part of figure). The lower part of the figure illustrates the types of potential changes which are re- corded and also indicates that the secretion of the output may have either a depolarizing (excitatory) or hyperpolarizing (inhibitory) action. Grundfest (1957, 1959a) has shown, however, that although such evolutionary specialization has taken place, each excitable cell has retained its dual role of receptor and effector and has, therefore, three components of action, namely input, conductile and output portions. Grundfest's scheme is summarized in Fig. 1.2. (i) The input component is not electrically excitable, but responds INTRODUCTION 5 to specific stimuli and is chemosensitive (see Chapter 7). Thus, an input area may be a sensory ending, sensitive to certain stimulus energies, or a postsynaptic membrane which is excited by its trans- mitter chemical. All input components, therefore, act as transducers, converting the stimulus energy into a localized, non-propagated, electrical response. The stimulus may have either an excitatory or an inhibitory effect, producing either a depolarization or a hyper- polarization respectively. The essential features of these localized changes in resting potential are that they are maintained and graded, and appropriate depolarization is able to initiate a train of spike potentials in the conducting portion of the excitable cell. (ii) The conductile component has the converse properties. It is not chemosensitive, but responds to electrical stimulation. As stated above, the sodium-permeability properties of the axon are sensitive to depolarization. The electrical response of the conductile cell, far from being graded, is the all-or-none spike potential. A definite threshold intensity is required to stimulate the axon, but above this level, and with other factors constant, the size and shape of the spike potential is independent of the intensity of the stimulus. Unlike the potentials recorded at input components, the spike potentials are propagated (see above). (iii) The output component. The arrival of the spike potentials at the effector-output component initiates secretory activity and the liberation of the chemical transmitter which is then able to act upon the input component of the next excitable cell in the neuronal chain. It is Grundfest's hypothesis that all excitable cells can be fitted within this generalized scheme. Some confusion exists in the terminology that has been proposed for the localized potentials developed at input components. In this review, the terminology proposed by Davis (1961) for sense organs will be followed (Pringle, 1962) and is shown in simplified form in Fig. 1.3. Not all features shown in the diagram are present in all sense organs (e.g. accessory structures). The generator potential is defined as that potential which triggers the all-or-none response of the initial segment of the sensory neuron, whilst the receptor poten- tial is defined in terms of the response of the sense organ to the action of the external energy. There may be no specialized receptor cell, the response being developed in the sensory neuron or, alter- natively, there may be no synapse with a chemical mediator, the potential in the receptor cell stimulating the initial segment directly EMP 2

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