ON THE INTERNAL FORM AND STRUCTURE OF THE CELL
In the early days of the cell-theory, more than seventy years ago,
Goodsir was wont to speak of cells as “centres of growth” or “centres
of nutrition,” and to consider them as essentially “centres of force.”
He looked forward to a time when the forces connected with the cell
should be particularly investigated: when, that is to say, minute
anatomy should be studied in its dynamical aspect. “When this branch of
enquiry,” he says “shall have been opened up, we shall expect to have
a science of organic forces, having direct relation to anatomy, the
science of organic forms[198].” And likewise, long afterwards, Giard
contemplated a science of _morphodynamique_,—but still looked upon it
as forming so guarded and hidden a “territoire scientifique, que la
plupart des naturalistes de nos jours ne le verront que comme Moïse vit
la terre promise, seulement de loin et sans pouvoir y entrer[199].”
To the external forms of cells, and to the forces which produce and
modify these forms, we shall pay attention in a later chapter. But
there are forms and configurations of matter within the cell, which
also deserve to be studied with due regard to the forces, known or
unknown, of whose resultant they are the visible expression.
In the long interval since Goodsir’s day, the visible structure, the
conformation and configuration, of the cell, has been studied far
more abundantly than the purely dynamic problems that are associated
therewith. The overwhelming progress of microscopic observation has
multiplied our knowledge of cellular and intracellular structure;
and to the multitude of visible structures it {157} has been often
easier to attribute virtues than to ascribe intelligible functions or
modes of action. But here and there nevertheless, throughout the whole
literature of the subject, we find recognition of the inevitable fact
that dynamical problems lie behind the morphological problems of the
cell.
Bütschli pointed out forty years ago, with emphatic clearness, the
failure of morphological methods, and the need for physical methods, if
we were to penetrate deeper into the essential nature of the cell[200].
And such men as Loeb and Whitman, Driesch and Roux, and not a few
besides, have pursued the same train of thought and similar methods of
enquiry.
Whitman[201], for instance, puts the case in a nutshell when, in
speaking of the so-called “caryokinetic” phenomena of nuclear division,
he reminds us that the leading idea in the term “_caryokinesis_” is
_motion_,—“motion viewed as an exponent of forces residing in, or
acting upon, the nucleus. It regards the nucleus as a _seat of energy,
which displays itself in phenomena of motion_[202].”
In short it would seem evident that, except in relation to a dynamical
investigation, the mere study of cell structure has but little value
of its own. That a given cell, an ovum for instance, contains this
or that visible substance or structure, germinal vesicle or germinal
spot, chromatin or achromatin, chromosomes or centrosomes, obviously
gives no explanation of the _activities_ of the cell. And in all such
hypotheses as that of “pangenesis,” in all the theories which attribute
specific properties to micellae, {158} idioplasts, ids, or other
constituent particles of protoplasm or of the cell, we are apt to fall
into the error of attributing to _matter_ what is due to _energy_ and
is manifested in force: or, more strictly speaking, of attributing to
material particles individually what is due to the energy of their
collocation.
The tendency is a very natural one, as knowledge of structure
increases, to ascribe particular virtues to the material structures
themselves, and the error is one into which the disciple is likely to
fall, but of which we need not suspect the master-mind. The dynamical
aspect of the case was in all probability kept well in view by those
who, like Goodsir himself, first attacked the problem of the cell and
originated our conceptions of its nature and functions.
But if we speak, as Weismann and others speak, of an “hereditary
_substance_,” a substance which is split off from the parent-body, and
which hands on to the new generation the characteristics of the old,
we can only justify our mode of speech by the assumption that that
particular portion of matter is the essential vehicle of a particular
charge or distribution of energy, in which is involved the capability
of producing motion, or of doing “work.”
For, as Newton said, to tell us that a thing “is endowed with an occult
specific quality, by which it acts and produces manifest effects, is
to tell us nothing; but to derive two or three general principles of
motion[203] from phenomena would be a very great step in philosophy,
though the causes of these principles were not yet discovered.” The
_things_ which we see in the cell are less important than the _actions_
which we recognise in the cell; and these latter we must especially
scrutinize, in the hope of discovering how far they may be attributed
to the simple and well-known physical forces, and how far they be
relevant or irrelevant to the phenomena which we associate with, and
deem essential to, the manifestation of _life_. It may be that in this
way we shall in time draw nigh to the recognition of a specific and
ultimate residuum. {159}
And lacking, as we still do lack, direct knowledge of the actual forces
inherent in the cell, we may yet learn something of their distribution,
if not also of their nature, from the outward and inward configuration
of the cell, and from the changes taking place in this configuration;
that is to say from the movements of matter, the kinetic phenomena,
which the forces in action set up.
The fact that the germ-cell develops into a very complex structure,
is no absolute proof that the cell itself is structurally a very
complicated mechanism: nor yet, though this is somewhat less obvious,
is it sufficient to prove that the forces at work, or latent, within it
are especially numerous and complex. If we blow into a bowl of soapsuds
and raise a great mass of many-hued and variously shaped bubbles, if we
explode a rocket and watch the regular and beautiful configuration of
its falling streamers, if we consider the wonders of a limestone cavern
which a filtering stream has filled with stalactites, we soon perceive
that in all these cases we have begun with an initial system of very
slight complexity, whose structure in no way foreshadowed the result,
and whose comparatively simple intrinsic forces only play their part by
complex interaction with the equally simple forces of the surrounding
medium. In an earlier age, men sought for the visible embryo, even for
the _homunculus_, within the reproductive cells; and to this day, we
scrutinize these cells for visible structure, unable to free ourselves
from that old doctrine of “pre-formation[204].”
Moreover, the microscope seemed to substantiate the idea (which we may
trace back to Leibniz[205] and to Hobbes[206]), that there is no limit
to the mechanical complexity which we may postulate in an organism, and
no limit, therefore, to the hypotheses which we may rest thereon.
But no microscopical examination of a stick of sealing-wax, no study
of the material of which it is composed, can enlighten {160} us as to
its electrical manifestations or properties. Matter of itself has no
power to do, to make, or to become: it is in energy that all these
potentialities reside, energy invisibly associated with the material
system, and in interaction with the energies of the surrounding
universe.
That “function presupposes structure” has been declared an accepted
axiom of biology. Who it was that so formulated the aphorism I do
not know; but as regards the structure of the cell it harks back to
Brücke, with whose demand for a mechanism, or organisation, within the
cell histologists have ever since been attempting to comply[207]. But
unless we mean to include thereby invisible, and merely chemical or
molecular, structure, we come at once on dangerous ground. For we have
seen, in a former chapter, that some minute “organisms” are already
known of such all but infinitesimal magnitudes that everything which
the morphologist is accustomed to conceive as “structure” has become
physically impossible; and moreover recent research tends generally
to reduce, rather than to extend, our conceptions of the visible
structure necessarily inherent in living protoplasm. The microscopic
structure which, in the last resort or in the simplest cases, it
seems to shew, is that of a more or less viscous colloid, or rather
mixture of colloids, and nothing more. Now, as Clerk Maxwell puts it,
in discussing this very problem, “one material system can differ from
another only in the configuration and motion which it has at a given
instant[208].” If we cannot assume differences in structure, we must
assume differences in _motion_, that is to say, in _energy_. And if we
cannot do this, then indeed we are thrown back upon modes of reasoning
unauthorised in physical science, and shall find ourselves constrained
to assume, or to “admit, that the properties of a germ are not those of
a purely material system.” {161}
But we are by no means necessarily in this dilemma. For though we
come perilously near to it when we contemplate the lowest orders of
magnitude to which life has been attributed, yet in the case of the
ordinary cell, or ordinary egg or germ which is going to develop into
a complex organism, if we have no reason to assume or to believe that
it comprises an intricate “mechanism,” we may be quite sure, both on
direct and indirect evidence, that, like the powder in our rocket, it
is very heterogeneous in its structure. It is a mixture of substances
of various kinds, more or less fluid, more or less mobile, influenced
in various ways by chemical, electrical, osmotic, and other forces, and
in their admixture separated by a multitude of surfaces, or boundaries,
at which these, or certain of these forces are made manifest.
Indeed, such an arrangement as this is already enough to constitute a
“mechanism”; for we must be very careful not to let our physical or
physiological concept of mechanism be narrowed to an interpretation
of the term derived from the delicate and complicated contrivances
of human skill. From the physical point of view, we understand by a
“mechanism” whatsoever checks or controls, and guides into determinate
paths, the workings of energy; in other words, whatsoever leads in the
degradation of energy to its manifestation in some determinate form
of _work_, at a stage short of that ultimate degradation which lapses
in uniformly diffused heat. This, as Warburg has well explained, is
the general effect or function of the physiological machine, and in
particular of that part of it which we call “cell-structure[209].”
The normal muscle-cell is something which turns energy, derived from
oxidation, into work; it is a mechanism which arrests and utilises the
chemical energy of oxidation in its downward course; but the same cell
when injured or disintegrated, loses its “usefulness,” and sets free a
greatly increased proportion of its energy in the form of heat.
But very great and wonderful things are done after this manner by means
of a mechanism (whether natural or artificial) of extreme simplicity.
A pool of water, by virtue of its surface, {162} is an admirable
mechanism for the making of waves; with a lump of ice in it, it becomes
an efficient and self-contained mechanism for the making of currents.
The great cosmic mechanisms are stupendous in their simplicity; and, in
point of fact, every great or little aggregate of heterogeneous matter
(not identical in “phase”) involves, _ipso facto_, the essentials of a
mechanism. Even a non-living colloid, from its intrinsic heterogeneity,
is in this sense a mechanism, and one in which energy is manifested in
the movement and ceaseless rearrangement of the constituent particles.
For this reason Graham (if I remember rightly) speaks somewhere or
other of the colloid state as “the dynamic state of matter”; or in the
same philosopher’s phrase (of which Mr Hardy[210] has lately reminded
us), it possesses “_energia_[211].”
Let us turn then to consider, briefly and diagrammatically, the
structure of the cell, a fertilised germ-cell or ovum for instance,
not in any vain attempt to correlate this structure with the structure
or properties of the resulting and yet distant organism; but merely
to see how far, by the study of its form and its changing internal
configuration, we may throw light on certain forces which are for the
time being at work within it.
We may say at once that we can scarcely hope to learn more of these
forces, in the first instance, than a few facts regarding their
direction and magnitude; the nature and specific identity of the force
or forces is a very different matter. This latter problem is likely to
be very difficult of elucidation, for the reason, among others, that
very different forces are often very much alike in their outward and
visible manifestations. So it has come to pass that we have a multitude
of discordant hypotheses as to the nature of the forces acting within
the cell, and producing, in cell division, the “caryokinetic” figures
of which we are about to speak. One student may, like Rhumbler, choose
to account for them by an hypothesis of mechanical traction, acting
on a reticular web of protoplasm[212]; another, like Leduc, may shew
us how in {163} many of their most striking features they may be
admirably simulated by the diffusion of salts in a colloid medium;
others again, like Gallardo[213] and Hartog, and Rhumbler (in his
earlier papers)[214], insist on their resemblance to the phenomena of
electricity and magnetism[215]; while Hartog believes that the force
in question is only analogous to these, and has a specific identity of
its own[216]. All these conflicting views are of secondary importance,
so long as we seek only to account for certain _configurations_ which
reveal the direction, rather than the nature, of a force. One and
the same system of lines of force may appear in a field of magnetic
or of electrical energy, of the osmotic energy of diffusion, of the
gravitational energy of a flowing stream. In short, we may expect to
learn something of the pure or abstract dynamics, long before we can
deal with the special physics of the cell. For indeed (as Maillard
has suggested), just as uniform expansion about a single centre, to
whatsoever physical cause it may be due will lead to the configuration
of a sphere, so will any two centres or foci of potential (of
whatsoever kind) lead to the configurations with which Faraday made us
familiar under the name of “lines of force[217]”; and this is as much
as to say that the phenomenon, {164} though physical in the concrete,
is in the abstract purely mathematical, and in its very essence is
neither more nor less than _a property of three-dimensional space_.
But as a matter of fact, in this instance, that is to say in trying
to explain the leading phenomena of the caryokinetic division of the
cell, we shall soon perceive that any explanation which is based, like
Rhumbler’s, on mere mechanical traction, is obviously inadequate, and
we shall find ourselves limited to the hypothesis of some polarised and
polarising force, such as we deal with, for instance, in the phenomena
of magnetism or electricity.
Let us speak first of the cell itself, as it appears in a state of
rest, and let us proceed afterwards to study the more active phenomena
which accompany its division.
――――――――――
Our typical cell is a spherical body; that is to say, the uniform
surface-tension at its boundary is balanced by the outward resistance
of uniform forces within. But at times the surface-tension may be a
fluctuating quantity, as when it produces the rhythmical contractions
or “Ransom’s waves” on the surface of a trout’s egg; or again, while
the egg is in contact with other bodies, the surface-tension may be
locally unequal and variable, giving rise to an amoeboid figure, as in
the egg of Hydra[218].
Within the ovum is a nucleus or germinal vesicle, also spherical, and
consisting as a rule of portions of “chromatin,” aggregated together
within a more fluid drop. The fact has often been commented upon that,
in cells generally, there is no correlation of _form_ (though there
apparently is of _size_) between the nucleus and the “cytoplasm,” or
main body of the cell. So Whitman[219] remarks that “except during
the process of division the nucleus seldom departs from its typical
spherical form. It divides and sub-divides, ever returning to the same
round or oval form .... How different with the cell. It preserves the
spherical form as rarely as the nucleus departs from it. Variation
in form marks the beginning and the end of every important chapter
in its {165} history.” On simple dynamical grounds, the contrast is
easily explained. So long as the fluid substance of the nucleus is
qualitatively different from, and incapable of mixing with, the fluid
or semi-fluid protoplasm which surrounds it, we shall expect it to
be, as it almost always is, of spherical form. For, on the one hand,
it is bounded by a liquid film, whose surface-tension is uniform; and
on the other, it is immersed in a medium which transmits on all sides
a uniform fluid pressure[220]. For a similar reason the contractile
vacuole of a Protozoon is spherical in form: it is just a “drop”
of fluid, bounded by a uniform surface-tension and through whose
boundary-film diffusion is taking place. But here, owning to the small
difference between the fluid constituting, and that surrounding, the
drop, the surface-tension equilibrium is unstable; it is apt to vanish,
and the rounded outline of the drop, like a burst bubble, disappears
in a moment[221]. The case of the spherical nucleus is closely akin
to the spherical form of the yolk within the bird’s egg[222]. But if
the substance of the cell acquire a greater solidity, as for instance
in a muscle {166} cell, or by reason of mucous accumulations in an
epithelium cell, then the laws of fluid pressure no longer apply, the
external pressure on the nucleus tends to become unsymmetrical, and
its shape is modified accordingly. “Amoeboid” movements may be set
up in the nucleus by anything which disturbs the symmetry of its own
surface-tension. And the cases, as in many Rhizopods, where “nuclear
material” is scattered in small portions throughout the cell instead
of being aggregated in a single nucleus, are probably capable of very
simple explanation by supposing that the “phase difference” (as the
chemists say) between the nuclear and the protoplasmic substance is
comparatively slight, and the surface-tension which tends to keep them
separate is correspondingly small[223].
It has been shewn that ordinary nuclei, isolated in a living or fresh
state, easily flow together; and this fact is enough to suggest that
they are aggregations of a particular substance rather than bodies
deserving the name of particular organs. It is by reason of the same
tendency to confluence or aggregation of particles that the ordinary
nucleus is itself formed, until the imposition of a new force leads to
its disruption.
Apart from that invisible or ultra-microscopic heterogeneity which
is inseparable from our notion of a “colloid,” there is a visible
heterogeneity of structure within both the nucleus and the outer
protoplasm. The former, for instance, contains a rounded nucleolus
or “germinal spot,” certain conspicuous granules or strands of the
peculiar substance called chromatin, and a coarse meshwork of a
protoplasmic material known as “linin” or achromatin; the outer
protoplasm, or cytoplasm, is generally believed to consist throughout
of a sponge-work, or rather alveolar meshwork, of more and less fluid
substances; and lastly, there are generally to be detected one or more
very minute bodies, usually in the cytoplasm, sometimes within the
nucleus, known as the centrosome or centrosomes.
The morphologist is accustomed to speak of a “polarity” of {167}
the cell, meaning thereby a symmetry of visible structure about a
particular axis. For instance, whenever we can recognise in a cell
both a nucleus and a centrosome, we may consider a line drawn through
the two as the morphological axis of polarity; in an epithelium cell,
it is obvious that the cell is morphologically symmetrical about a
median axis passing from its free surface to its attached base. Again,
by an extension of the term “polarity,” as is customary in dynamics,
we may have a “radial” polarity, between centre and periphery; and
lastly, we may have several apparently independent centres of polarity
within the single cell. Only in cells of quite irregular, or amoeboid
form, do we fail to recognise a definite and symmetrical “polarity.”
The _morphological_ “polarity” is accompanied by, and is but the
outward expression (or part of it) of a true _dynamical_ polarity, or
distribution of forces; and the “lines of force” are rendered visible
by concatenation of particles of matter, such as come under the
influence of the forces in action.
When the lines of force stream inwards from the periphery towards
a point in the interior of the cell, the particles susceptible of
attraction either crowd towards the surface of the cell, or, when
retarded by friction, are seen forming lines or “fibrillae” which
radiate outwards from the centre and constitute a so-called “aster.” In
the cells of columnar or ciliated epithelium, where the sides of the
cell are symmetrically disposed to their neighbours but the free and
attached surfaces are very diverse from one another in their external
relations, it is these latter surfaces which constitute the opposite
poles; and in accordance with the parallel lines of force so set up,
we very frequently see parallel lines of granules which have ranged
themselves perpendicularly to the free surface of the cell (cf. fig.
97).
A simple manifestation of “polarity” may be well illustrated by the
phenomenon of diffusion, where we may conceive, and may automatically
reproduce, a “field of force,” with its poles and visible lines of
equipotential, very much as in Faraday’s conception of the field of
force of a magnetic system. Thus, in one of Leduc’s experiments[224],
if we spread a layer of salt solution over a level {168} plate of
glass, and let fall into the middle of it a drop of indian ink, or
of blood, we shall find the coloured particles travelling outwards
from the central “pole of concentration” along the lines of diffusive
force, and so mapping out for us a “monopolar field” of diffusion: and
if we set two such drops side by side, their lines of diffusion will
oppose, and repel, one another. Or, instead of the uniform layer of
salt solution, we may place at a little distance from one another a
grain of salt and a drop of blood, representing two opposite poles:
and so obtain a picture of a “bipolar field” of diffusion. In either
case, we obtain results closely analogous to the “morphological,”
but really _dynamical_, polarity of the organic cell. But in all
probability, the dynamical polarity, or asymmetry of the cell is a very
complicated phenomenon: for the obvious reason that, in any system,
one asymmetry will tend to beget another. A chemical asymmetry will
induce an inequality of surface-tension, which will lead directly to a
modification of form; the chemical asymmetry may in turn be due to a
process of electrolysis in a polarised electrical field; and again the
chemical heterogeneity may be intensified into a chemical “polarity,”
by the tendency of certain substances to seek a locus of greater or
less surface-energy. We need not attempt to grapple with a subject
so complicated, and leading to so many problems which lie beyond the
sphere of interest of the morphologist. But yet the morphologist, in
his study of the cell, cannot quite evade these important issues; and
we shall return to them again when we have dealt somewhat with the form
of the cell, and have taken account of some of the simpler phenomena of
surface-tension.
――――――――――
We are now ready, and in some measure prepared, to study the numerous
and complex phenomena which usually accompany the division of the cell,
for instance of the fertilised egg.
Division of the cell is essentially accompanied, and preceded, by a
change from radial or monopolar to a definitely bipolar polarity.
In the hitherto quiescent, or apparently quiescent cell, we perceive
certain movements, which correspond precisely to what must accompany
and result from a “polarisation” of forces within the {169} cell:
of forces which, whatever may be their specific nature, at least are
capable of polarisation, and of producing consequent attraction or
repulsion between charged particles of matter. The opposing forces
which were distributed in equilibrium throughout the substance of
the cell become focussed at two “centrosomes,” which may or may
not be already distinguished as visible portions of matter; in the
egg, one of these is always near to, and the other remote from, the
“animal pole” of the egg, which pole is visibly as well as chemically
different from the other, and is the region in which the more rapid and
conspicuous developmental changes will presently begin. Between the two
centrosomes, a spindle-shaped
[Illustration: Fig. 41. Caryokinetic figure in a dividing cell (or
blastomere) of the Trout’s egg. (After Prenant, from a preparation by
Prof. P. Bouin.)]
figure appears, whose striking resemblance to the lines of force made
visible by iron-filings between the poles of a magnet, was at once
recognised by Hermann Fol, when in 1873 he witnessed for the first time
the phenomenon in question. On the farther side of the centrosomes are
seen star-like figures, or “asters,” in which we can without difficulty
recognise the broken lines of force which run externally to those
stronger lines which lie nearer to the polar axis and which constitute
the “spindle.” The lines of force are rendered visible or “material,”
just as in the experiment of the iron-filings, by the fact that, in the
heterogeneous substance of the cell, certain portions of matter are
more “permeable” to the acting force than the rest, become themselves
polarised after the {170} fashion of a magnetic or “paramagnetic”
body, arrange themselves in an orderly way between the two poles of
the field of force, cling to one another as it were in threads[225],
and are only prevented by the friction of the surrounding medium from
approaching and congregating around the adjacent poles.
As the field of force strengthens, the more will the lines of force
be drawn in towards the interpolar axis, and the less evident will
be those remoter lines which constitute the terminal, or extrapolar,
asters: a clear space, free from materialised lines of force, may
thus tend to be set up on either side of the spindle, the so-called
“Bütschli space” of the histologists[226]. On the other hand, the
lines of force constituting the spindle will be less concentrated if
they find a path of less resistance at the periphery of the cell: as
happens, in our experiment of the iron-filings, when we encircle the
field of force with an iron ring. On this principle, the differences
observed between cells in which the spindle is well developed and the
asters small, and others in which the spindle is weak and the asters
enormously developed, can be easily explained by variations in the
potential of the field, the large, conspicuous asters being probably
correlated with a marked permeability of the surface of the cell.
The visible field of force, though often called the “nuclear spindle,”
is formed outside of, but usually near to, the nucleus. Let us look
a little more closely into the structure of this body, and into the
changes which it presently undergoes.
Within its spherical outline (Fig. 42), it contains an “alveolar”
{171} meshwork (often described, from its appearance in optical
section, as a “reticulum”), consisting of more solid substances, with
more fluid matter filling up the interalveolar meshes. This phenomenon
is nothing else than what we call in ordinary language, a “froth” or
a “foam.” It is a surface-tension phenomenon, due to the interacting
surface-tensions of two intermixed fluids, not very different in
density, as they strive to separate. Of precisely the same kind (as
Bütschli was the first to shew) are the minute alveolar networks which
are to be discerned in the cytoplasm of the cell[227], and which we
now know to be not inherent in the nature of protoplasm, or of living
matter in general, but to be due to various causes, natural as well as
artificial. The microscopic honeycomb structure of cast metal under
various conditions of cooling, even on a grand scale the columnar
structure of basaltic rock, is an example of the same surface-tension
phenomenon. {172}
[Illustration: Fig. 42.]
[Illustration: Fig. 43.]
But here we touch the brink of a subject so important that we must not
pass it by without a word, and yet so contentious that we must not
enter into its details. The question involved is simply whether the
great mass of recorded observations and accepted beliefs with regard
to the visible structure of protoplasm and of the cell constitute a
fair picture of the actual _living cell_, or be based on appearances
which are incident to death itself and to the artificial treatment
which the microscopist is accustomed to apply. The great bulk of
histological work is done by methods which involve the sudden killing
of the cell or organism by strong reagents, the assumption being that
death is so rapid that the visible phenomena exhibited during life
are retained or “fixed” in our preparations. While this assumption
is reasonable and justified as regards the general outward form of
small organisms or of individual cells, enough has been done of late
years to shew that the case is totally different in the case of
the minute internal networks, granules, etc., which represent the
alleged _structure_ of protoplasm. For, as Hardy puts it, “It is
notorious that the various fixing reagents are coagulants of organic
colloids, and that they produce precipitates which have a certain
figure or structure, ... and that the figure varies, other things
being equal, according to the reagent used.” So it comes to pass that
some writers[228] have altogether denied the existence in the living
cell-protoplasm of a network or alveolar “foam”; others[229] have
cast doubts on the main tenets of recent histology regarding nuclear
structure; and Hardy, discussing the structure of certain gland-cells,
declares that “there is no evidence that the structure discoverable in
the cell-substance of these cells after fixation has any counterpart
in the cell when living.” “A large part of it” he goes on to say “is
an artefact. The profound difference in the minute structure of a
secretory cell of a mucous gland according to the reagent which is
used to fix it would, it seems to me, almost suffice to establish this
statement in the absence of other evidence.”
Nevertheless, histological study proceeds, especially on the part of
the morphologists, with but little change in theory or in method,
in spite of these and many other warnings. That certain visible
structures, nucleus, vacuoles, “attraction-spheres” or centrosomes,
etc., are actually present in the living cell, we know for certain;
and to this class belong the great majority of structures (including
the nuclear “spindle” itself) with which we are at present concerned.
That many other alleged structures are artificial has also been placed
beyond a doubt; but where to draw the dividing line we often do not
know[230]. {173}
The following is a brief epitome of the visible changes undergone by a
typical cell, leading up to the act of segmentation, and constituting
the phenomenon of mitosis or caryokinetic division. In the egg of a
sea-urchin, we see with almost diagrammatic completeness what is set
forth here[231].
[Illustration: Fig. 44.]
[Illustration: Fig. 45.]
1. The chromatin, which to begin with was distributed in granules on
the otherwise achromatic reticulum (Fig. 42), concentrates to form a
skein or _spireme_, which may be a continuous thread from the first
(Figs. 43, 44), or from the first segmented. In any case it divides
transversely sooner or later into a number of _chromosomes_ (Fig. 45),
which as a rule have the shape of little rods, straight or curved,
often bent into a V, but which may also be ovoid, or round, or even
annular. Certain deeply staining masses, the nucleoli, which may be
present in the resting nucleus, do not take part in the process of
chromosome formation; they are either cast out of the nucleus and are
dissolved in the cytoplasm, or fade away _in situ_.
2. Meanwhile, the deeply staining granule (here extra-nuclear), known
as the _centrosome_, has divided in two. The two resulting granules
travel to opposite poles of the nucleus, and {174} there each becomes
surrounded by a system of radiating lines, the _asters_; immediately
around the centrosome is a clear space, the _centrosphere_ (Figs.
43–45). Between the two centrosomes with their asters stretches a
bundle of achromatic fibres, the _spindle_.
3. The surface-film bounding the nucleus has broken down, the definite
nuclear boundaries are lost, and the spindle now stretches through the
nuclear material, in which lie the chromosomes (Figs. 45, 46). These
chromosomes now arrange themselves midway between the poles of the
spindle, where they form what is called the _equatorial plate_ (Fig.
47).
[Illustration: Fig. 46.]
[Illustration: Fig. 47.]
4. Each chromosome splits longitudinally into two: usually at this
stage,—but it is to be noticed that the splitting may have taken place
so early as the spireme stage (Fig. 48).
5. The halves of the split chromosomes now separate from one another,
and travel in opposite directions towards the two poles (Fig. 49). As
they move, it becomes apparent that the spindle consists of a median
bundle of “fibres,” the central spindle, running from pole to pole, and
a more superficial sheath of “mantle-fibres,” to which the chromosomes
seem to be attached, and by which they seem to be drawn towards the
asters.
6. The daughter chromosomes, arranged now in two groups, become closely
crowded in a mass near the centre of each aster {175} (Fig. 50).
They fuse together and form once more an alveolar reticulum and may
occasionally at this stage form another spireme.
[Illustration: Fig. 48.]
[Illustration: Fig. 49.]
A boundary or surface wall is now developed round each reconstructed
nuclear mass, and the spindle-fibres disappear (Fig. 51). The
centrosome remains, as a rule, outside the nucleus.
[Illustration: Fig. 50.]
[Illustration: Fig. 51.]
7. On the central spindle, in the position of the equatorial plate,
there has appeared during the migration of the chromosomes, a
“cell-plate” of deeply staining thickenings (Figs. 50, 51). This is
more conspicuous in plant-cells. {176}
8. A constriction has meanwhile appeared in the cytoplasm, and the
cell divides through the equatorial plane. In plant-cells the line
of this division is foreshadowed by the “cell-plate,” which extends
from the spindle across the entire cell, and splits into two layers,
between which appears the membrane by which the daughter cells are
cleft asunder. In animal cells the cell-plate does not attain such
dimensions, and no cell-wall is formed.
――――――――――
The whole, or very nearly the whole of these nuclear phenomena may be
brought into relation with that polarisation of forces, in the cell as
a whole, whose field is made manifest by the “spindle” and “asters” of
which we have already spoken: certain particular phenomena, directly
attributable to surface-tension and diffusion, taking place in more or
less obvious and inevitable dependence upon the polar system†.
† The reference numbers in the following account refer to the
paragraphs and figures of the preceding summary of visible nuclear
phenomena.
At the same time, in attempting to explain the phenomena, we cannot say
too clearly, or too often, that all that we are meanwhile justified
in doing is to try to shew that such and such actions lie _within
the range_ of known physical actions and phenomena, or that known
physical phenomena produce effects similar to them. We want to feel
sure that the whole phenomenon is not _sui generis_, but is somehow or
other capable of being referred to dynamical laws, and to the general
principles of physical science. But when we speak of some particular
force or mode of action, using it as an illustrative hypothesis, we
must stop far short of the implication that this or that force is
necessarily the very one which is actually at work within the living
cell; and certainly we need not attempt the formidable task of trying
to reconcile, or to choose between, the various hypotheses which have
already been enunciated, or the several assumptions on which they
depend.
――――――――――
Any region of space within which action is manifested is a field of
force; and a simple example is a bipolar field, in which the action is
symmetrical with reference to the line joining two points, or poles,
and also with reference to the “equatorial” plane equidistant from
both. We have such a “field of force” in {177} the neighbourhood of
the centrosome of the ripe cell or ovum, when it is about to divide;
and by the time the centrosome has divided, the field is definitely a
bipolar one.
The _quality_ of a medium filling the field of force may be uniform,
or it may vary from point to point. In particular, it may depend upon
the magnitude of the field; and the quality of one medium may differ
from that of another. Such variation of quality, within one medium, or
from one medium to another, is capable of diagrammatic representation
by a variation of the direction or the strength of the field (other
conditions being the same) from the state manifested in some uniform
medium taken as a standard. The medium is said to be _permeable_ to the
force, in greater or less degree than the standard medium, according as
the variation of the density of the lines of force from the standard
case, under otherwise identical conditions, is in excess or defect. _A
body placed in the medium will tend to move towards regions of greater
or less force according as its permeability is greater or less than
that of the surrounding medium_[232]. In the common experiment of
placing iron-filings between the two poles of a magnetic field, the
filings have a very high permeability; and not only do they themselves
become polarised so as to attract one another, but they tend to be
attracted from the weaker to the stronger parts of the field, and as
we have seen, were it not for friction or some other resistance, they
would soon gather together around the nearest pole. But if we repeat
the same experiment with such a metal as bismuth, which is very little
permeable to the magnetic force, then the conditions are reversed, and
the particles, being repelled from the stronger to the weaker parts
of the field, tend to take up their position as far from the poles as
possible. The particles have become polarised, but in a sense opposite
to that of the surrounding, or adjacent, field.
Now, in the field of force whose opposite poles are marked by {178}
the centrosomes the nucleus appears to act as a more or less permeable
body, as a body more permeable than the surrounding medium, that is to
say the “cytoplasm” of the cell. It is accordingly attracted by, and
drawn into, the field of force, and tries, as it were, to set itself
between the poles and as far as possible from both of them. In other
words, the centrosome-foci will be apparently drawn over its surface,
until the nucleus as a whole is involved within the field of force,
which is visibly marked out by the “spindle” (par. 3, Figs. 44, 45).
If the field of force be electrical, or act in a fashion analogous to
an electrical field, the charged nucleus will have its surface-tensions
diminished[233]: with the double result that the inner alveolar
meshwork will be broken up (par. 1), and that the spherical boundary
of the whole nucleus will disappear (par. 2). The break-up of the
alveoli (by thinning and rupture of their partition walls) leads to the
formation of a net, and the further break-up of the net may lead to the
unravelling of a thread or “spireme” (Figs. 43, 44).
Here there comes into play a fundamental principle which, in so far
as we require to understand it, can be explained in simple words.
The effect (and we might even say the _object_) of drawing the more
permeable body in between the poles, is to obtain an “easier path” by
which the lines of force may travel; but it is obvious that a longer
route through the more permeable body may at length be found less
advantageous than a shorter route through the less permeable medium.
That is to say, the more permeable body will only tend to be drawn in
to the field of force until a point is reached where (so to speak)
the way _round_ and the way _through_ are equally advantageous. We
should accordingly expect that (on our hypothesis) there would be
found cases in which the nucleus was wholly, and others in which it
was only partially, and in greater or less degree, drawn in to the
field between the centrosomes. This is precisely what is found to
occur in actual fact. Figs. 44 and 45 represent two so-called “types,”
of a phase which follows that represented in Fig. 43. According to
the usual descriptions (and in particular to Professor {179} E. B.
Wilson’s[234]), we are told that, in such a case as Fig. 44, the
“primary spindle” disappears and the centrosomes diverge to opposite
poles of the nucleus; such a condition being found in many plant-cells,
and in the cleavage-stages of many eggs. In Fig. 45, on the other hand,
the primary spindle persists, and subsequently comes to form the main
or “central” spindle; while at the same time we see the fading away
of the nuclear membrane, the breaking up of the spireme into separate
chromosomes, and an ingrowth into the nuclear area of the “astral
rays,”—all as in Fig. 46, which represents the next succeeding phase
of Fig. 45. This condition, of Fig. 46, occurs in a variety of cases;
it is well seen in the epidermal cells of the salamander, and is also
on the whole characteristic of the mode of formation of the “polar
bodies.” It is clear and obvious that the two “types” correspond to
mere differences of degree, and are such as would naturally be brought
about by differences in the relative permeabilities of the nuclear
mass and of the surrounding cytoplasm, or even by differences in the
magnitude of the former body.
But now an important change takes place, or rather an important
difference appears; for, whereas the nucleus as a whole tended to
be drawn in to the _stronger_ parts of the field, when it comes to
break up we find, on the contrary, that its contained spireme-thread
or separate chromosomes tend to be repelled to the _weaker_ parts.
Whatever this difference may be due to,—whether, for instance, to
actual differences of permeability, or possibly to differences in
“surface-charge,”—the fact is that the chromatin substance now
_behaves_ after the fashion of a “diamagnetic” body, and is repelled
from the stronger to the weaker parts of the field. In other words,
its particles, lying in the inter-polar field, tend to travel towards
the equatorial plane thereof (Figs. 47, 48), and further tend to
move outwards towards the periphery of that plane, towards what the
histologist calls the “mantle-fibres,” or outermost of the lines of
force of which the spindle is made up (par. 5, Fig. 47). And if this
comparatively non-permeable chromatin substance come to consist of
separate portions, more or less elongated in form, these portions, or
separate “chromosomes,” will adjust themselves longitudinally, {180}
in a peripheral equatorial circle (Figs. 48, 49). This is precisely
what actually takes place. Moreover, before the breaking up of the
nucleus, long before the chromatin material has broken up into separate
chromosomes, and at the very time when it is being fashioned into a
“spireme,” this body already lies in a polar field, and must already
have a tendency to set itself in the equatorial plane thereof. But
the long, continuous spireme thread is unable, so long as the nucleus
retains its spherical boundary wall, to adjust itself in a simple
equatorial annulus; in striving to do so, it must tend to coil and
“kink” itself, and in so doing (if all this be so), it must tend to
assume the characteristic convolutions of the “spireme.”
[Illustration: Fig. 52. Chromosomes, undergoing splitting and
separation. (After Hatschek and Flemming, diagrammatised.)]
After the spireme has broken up into separate chromosomes, these
particles come into a position of temporary, and unstable, equilibrium
near the periphery of the equatorial plane, and here they tend to place
themselves in a symmetrical arrangement (Fig. 52). The particles are
rounded, linear, sometimes annular, similar in form and size to one
another; and lying as they do in a fluid, and subject to a symmetrical
system of forces, it is not surprising that they arrange themselves
in a symmetrical manner, the precise arrangement depending on the
form of the particles themselves. This symmetry may perhaps be due,
as has already been suggested, to induced electrical charges. In
discussing Brauer’s observations on the splitting of the chromatic
filament, and the symmetrical arrangement of the separate granules, in
_Ascaris megalocephala_, Lillie[235] {181} remarks: “This behaviour
is strongly suggestive of the division of a colloidal particle under
the influence of its surface electrical charge, and of the effects
of mutual repulsion in keeping the products of division apart.” It
is also probable that surface-tensions between the particles and the
surrounding protoplasm would bring about an identical result, and
would sufficiently account for the obvious, and at first sight, very
curious, symmetry. We know that if we float a couple of matches in
water they tend to approach one another, till they lie close together,
side by side; and, if we lay upon a smooth wet plate four matches, half
broken across, a precisely similar attraction brings the four matches
together in the form of a symmetrical cross. Whether one of these,
or some other, be the actual explanation of the phenomenon, it is at
least plain that by some physical cause, some mutual and symmetrical
attraction or repulsion of the particles, we must seek to account for
the curious symmetry of these so-called “tetrads.” The remarkable
_annular_ chromosomes, shewn in Fig. 53, can also be easily imitated
by means of loops of thread upon a soapy film when the film within the
annulus is broken or its tension reduced.
[Illustration: Fig. 53. Annular chromosomes, formed in the
spermatogenesis of the Mole-cricket. (From Wilson, after Vom Rath.)]
――――――――――
So far as we have now gone, there is no great difficulty in pointing to
simple and familiar phenomena of a field of force which are similar,
or comparable, to the phenomena which we witness within the cell. But
among these latter phenomena there are others for which it is not
so easy to suggest, in accordance with known laws, a simple mode of
physical causation. It is not at once obvious how, in any simple system
of symmetrical forces, {182} the chromosomes, which had at first been
apparently repelled from the poles towards the equatorial plane, should
then be split asunder, and should presently be attracted in opposite
directions, some to one pole and some to the other. Remembering that it
is not our purpose to _assert_ that some one particular mode of action
is at work, but merely to shew that there do exist physical forces, or
distributions of force, which are capable of producing the required
result, I give the following suggestive hypothesis, which I owe to my
colleague Professor W. Peddie.
As we have begun by supposing that the nuclear, or chromosomal
matter differs in _permeability_ from the medium, that is to say the
cytoplasm, in which it lies, let us now make the further assumption
that its permeability is variable, and depends upon the _strength of
the field_.
[Illustration: Fig. 54.]
In Fig. 54, we have a field of force (representing our cell),
consisting of a homogeneous medium, and including two opposite poles:
lines of force are indicated by full lines, and _loci of constant
magnitude of force_ are shewn by dotted lines.
Let us now consider a body whose permeability (µ) depends on the
strength of the field _F_. At two field-strengths, such as _F_{a}_,
_F_{b}_, let the permeability of the body be equal to that of the
{183} medium, and let the curved line in Fig. 55 represent generally
its permeability at other field-strengths; and let the outer and
inner dotted curves in Fig. 54 represent respectively the loci of the
field-strengths _F_{b}_ and _F_{a}_. The body if it be placed in the
medium within either branch of the inner curve, or outside the outer
curve, will tend to move into the neighbourhood of the adjacent pole.
If it be placed in the region intermediate to the two dotted curves, it
will tend to move towards regions of weaker field-strength.
[Illustration: Fig. 55.]
The locus _F_{b}_ is therefore a locus of stable position, towards
which the body tends to move; the locus _F_{a}_ is a locus of unstable
position, from which it tends to move. If the body were placed across
_F_{a}_, it might be torn asunder into two portions, the split
coinciding with the locus _F_{a}_.
Suppose a number of such bodies to be scattered throughout the medium.
Let at first the regions _F_{a}_ and _F_{b}_ be entirely outside the
space where the bodies are situated: and, in making this supposition we
may, if we please, suppose that the loci which we are calling _F_{a}_
and _F_{b}_ are meanwhile situated somewhat farther from the axis than
in our figure, that (for instance) _F_{a}_ is situated where we have
drawn _F_{b}_, and that _F_{b}_ is still further out. The bodies then
tend towards the poles; but the tendency may be very small if, in Fig.
55, the curve and its intersecting straight line do not diverge very
far from one another beyond _F_{a}_; in other {184} words, if, when
situated in this region, the permeability of the bodies is not very
much in excess of that of the medium.
Let the poles now tend to separate farther and farther from one
another, the strength of each pole remaining unaltered; in other words,
let the centrosome-foci recede from one another, as they actually
do, drawing out the spindle-threads between them. The loci _F_{a}_,
_F_{b}_, will close in to nearer relative distances from the poles. In
doing so, when the locus _F_{a}_ crosses one of the bodies, the body
may be torn asunder; if the body be of elongated shape, and be crossed
at more points than one, the forces at work will tend to exaggerate its
foldings, and the tendency to rupture is greatest when _F_{a}_ is in
some median position (Fig. 56).
[Illustration: Fig. 56.]
When the locus _F_{a}_ has passed entirely over the body, the body
tends to move towards regions of weaker force; but when, in turn, the
locus _F_{b}_ has crossed it, then the body again moves towards regions
of stronger force, that is to say, towards the nearest pole. And, in
thus moving towards the pole, it will do so, as appears actually to be
the case in the dividing cell, along the course of the outer lines of
force, the so-called “mantle-fibres” of the histologist[236].
Such considerations as these give general results, easily open to
modification in detail by a change of any of the arbitrary postulates
which have been made for the sake of simplicity. Doubtless there are
many other assumptions which would more or less meet the case; for
instance, that of Ida H. Hyde that, {185} during the active phase
of the chromatin molecule (during which it decomposes and sets free
nucleic acid) it carries a charge opposite to that which it bears
during its resting, or alkaline phase; and that it would accordingly
move towards different poles under the influence of a current,
wandering with its negative charge in an alkaline fluid during its
acid phase to the anode, and to the kathode during its alkaline phase.
A whole field of speculation is opened up when we begin to consider
the cell not merely as a polarised electrical field, but also as an
electrolytic field, full of wandering ions. Indeed it is high time we
reminded ourselves that we have perhaps been dealing too much with
ordinary physical analogies: and that our whole field of force within
the cell is of an order of magnitude where these grosser analogies may
fail to serve us, and might even play us false, or lead us astray.
But our sole object meanwhile, as I have said more than once, is
to demonstrate, by such illustrations as these, that, whatever be
the actual and as yet unknown _modus operandi_, there are physical
conditions and distributions of force which _could_ produce just such
phenomena of movement as we see taking place within the living cell.
This, and no more, is precisely what Descartes is said to have claimed
for his description of the human body as a “mechanism[237].”
――――――――――
The foregoing account is based on the provisional assumption that
the phenomena of caryokinesis are analogous to, if not identical
with those of a bipolar electrical field; and this comparison, in my
opinion, offers without doubt the best available series of analogies.
But we must on no account omit to mention the fact that some of
Leduc’s diffusion-experiments offer very remarkable analogies to
the diagrammatic phenomena of caryokinesis, as shewn in the annexed
figure[238]. Here we have two identical (not opposite) poles of osmotic
concentration, formed by placing a drop of indian ink in salt water,
and then on either side of this central drop, a hypertonic drop of
salt solution more lightly coloured. On either side the pigment of the
central drop has been drawn towards the focus nearest to it; but in
the middle line, the pigment {186} is drawn in opposite directions by
equal forces, and so tends to remain undisturbed, in the form of an
“equatorial plate.”
Nor should we omit to take account (however briefly and inadequately)
of a novel and elegant hypothesis put forward by A. B. Lamb. This
hypothesis makes use of a theorem of Bjerknes, to the effect that
synchronously vibrating or pulsating bodies in a liquid field attract
or repel one another according as their oscillations are identical
or opposite in phase. Under such circumstances, true currents, or
hydrodynamic lines of force, are produced, identical in form with the
lines of force of a magnetic field; and other particles floating,
though not necessarily pulsating, in the liquid field, tend to be
attracted or repelled by the pulsating bodies according as they are
lighter or heavier than the surrounding fluid. Moreover (and this is
the most remarkable point of all), the lines of force set up by the
_oppositely_ pulsating bodies are the same as those which are produced
by _opposite_ magnetic poles: though in the former case repulsion, and
in the latter case attraction, takes place between the two poles[239].
[Illustration: Fig. 57. Artificial caryokinesis (after Leduc), for
comparison with Fig. 41, p. 169.]
――――――――――
But to return to our general discussion.
While it can scarcely be too often repeated that our enquiry is not
directed towards the solution of physiological problems, save {187}
only in so far as they are inseparable from the problems presented by
the visible configurations of form and structure, and while we try, as
far as possible, to evade the difficult question of what particular
forces are at work when the mere visible forms produced are such as
to leave this an open question, yet in this particular case we have
been drawn into the use of electrical analogies, and we are bound to
justify, if possible, our resort to this particular mode of physical
action. There is an important paper by R. S. Lillie, on the “Electrical
Convection of certain Free Cells and Nuclei[240],” which, while I
cannot quote it in direct support of the suggestions which I have made,
yet gives just the evidence we need in order to shew that electrical
forces act upon the constituents of the cell, and that their action
discriminates between the two species of colloids represented by the
cytoplasm and the nuclear chromatin. And the difference is such that,
in the presence of an electrical current, the cell substance and the
nuclei (including sperm-cells) tend to migrate, the former on the whole
with the positive, the latter with the negative stream: a difference
of electrical potential being thus indicated between the particle
and the surrounding medium, just as in the case of minute suspended
particles of various kinds in various feebly conducing media[241]. And
the electrical difference is doubtless greatest, in the case of the
cell constituents, just at the period of mitosis: when the chromatin
is invariably in its most deeply staining, most strongly acid, and
therefore, presumably, in its most electrically negative phase. In
short, {188} Lillie comes easily to the conclusion that “electrical
theories of mitosis are entitled to more careful consideration than
they have hitherto received.”
Among other investigations, all leading towards the same general
conclusion, namely that differences of electric potential play a
great part in the phenomenon of cell division, I would mention a very
noteworthy paper by Ida H. Hyde[242], in which the writer shews (among
other important observations) that not only is there a measurable
difference of potential between the animal and vegetative poles of
a fertilised egg (_Fundulus_, toad, turtle, etc.), but that this
difference is not constant, but fluctuates, or actually reverses
its direction, periodically, at epochs coinciding with successive
acts of segmentation or other important phases in the development of
the egg[243]; just as other physical rhythms, for instance in the
production of CO_{2}, had already been shewn to do. Hence we shall be
by no means surprised to find that the “materialised” lines of force,
which in the earlier stages form the convergent curves of the spindle,
are replaced in the later phases of caryokinesis by divergent curves,
indicating that the two foci, which are marked out within the field by
the divided and reconstituted nuclei, are now alike in their polarity
(Figs. 58, 59).
It is certain, to my mind, that these observations of Miss Hyde’s, and
of Lillie’s, taken together with those of many writers on the behaviour
of colloid particles generally in their relation to an electrical
field, have a close bearing upon the physiological side of our problem,
the full discussion of which lies outside our present field.
――――――――――
The break-up of the nucleus, already referred to and ascribed to
a diminution of its surface-tension, is accompanied by certain
diffusion phenomena which are sometimes visible to the eye; and we
are reminded of Lord Kelvin’s view that diffusion is implicitly {189}
associated with surface-tension changes, of which the first step is a
minute puckering of the surface-skin, a sort of interdigitation with
the surrounding medium. For instance, Schewiakoff has observed in
_Euglypha_[244] that, just before the break-up of the nucleus, a system
of rays appears, concentred about it, but having nothing to do with the
polar asters: and during the existence of this striation, the nucleus
enlarges very considerably, evidently by imbibition of fluid from the
surrounding protoplasm. In short, diffusion is at work, hand in hand
with, and as it were in opposition to, the surface-tensions which
define the nucleus. By diffusion, hand in hand with surface-tension,
the alveoli of the nuclear meshwork are formed, enlarged, and finally
ruptured: diffusion sets up the movements which give rise to the
appearance of rays, or striae, around the nucleus: and through
increasing diffusion, and weakening surface-tension, the rounded
outline of the nucleus finally disappears. {190}
[Illustration: Fig. 58. Final stage in the first segmentation of the
egg of Cerebratulus. (From Prenant, after Coe.)[245]]
[Illustration: Fig. 59. Diagram of field of force with two similar
poles.]
As we study these manifold phenomena, in the individual cases of
particular plants and animals, we recognise a close identity of type,
coupled with almost endless variation of specific detail; and in
particular, the order of succession in which certain of the phenomena
occur is variable and irregular. The precise order of the phenomena,
the time of longitudinal and of transverse fission of the chromatin
thread, of the break-up of the nuclear wall, and so forth, will
depend upon various minor contingencies and “interferences.” And it
is worthy of particular note that these variations, in the order of
events and in other subordinate details, while doubtless attributable
to specific physical conditions, would seem to be without any obvious
classificatory value or other biological significance[246].
――――――――――
As regards the actual mechanical division of the cell into two halves,
we shall see presently that, in certain cases, such as that of a
long cylindrical filament, surface-tension, and what is known as the
principle of “minimal area,” go a long way to explain the mechanical
process of division; and in all cells whatsoever, the process of
division must somehow be explained as the result of a conflict between
surface-tension and its opposing forces. But in such a case as our
spherical cell, it is not very easy to see what physical cause is at
work to disturb its equilibrium and its integrity.
The fact that, when actual division of the cell takes place, it does
so at right angles to the polar axis and precisely in the direction of
the equatorial plane, would lead us to suspect that the new surface
formed in the equatorial plane sets up an annular tension, directed
inwards, where it meets the outer surface layer of the cell itself. But
at this point, the problem becomes more complicated. Before we could
hope to comprehend it, we should have not only to enquire into the
potential distribution at the surface of the cell in relation to that
which we have seen to exist in its interior, but we should probably
also have to take account of the differences of potential which the
material arrangements along the lines of force must themselves tend
to produce. Only {191} thus could we approach a comprehension of the
balance of forces which cohesion, friction, capillarity and electrical
distribution combine to set up.
The manner in which we regard the phenomenon would seem to turn, in
great measure, upon whether or no we are justified in assuming that,
in the liquid surface-film of a minute spherical cell, local, and
symmetrically localised, differences of surface-tension are likely
to occur. If not, then changes in the conformation of the cell
such as lead immediately to its division must be ascribed not to
local changes in its surface-tension, but rather to direct changes
in internal pressure, or to mechanical forces due to an induced
surface-distribution of electrical potential.
It has seemed otherwise to many writers, and we have a number of
theories of cell division which are all based directly on inequalities
or asymmetry of surface-tension. For instance, Bütschli suggested,
some forty years ago[247], that cell division is brought about by an
increase of surface-tension in the equatorial region of the cell.
This explanation, however, can scarcely hold; for it would seem that
such an increase of surface-tension in the equatorial plane would
lead to the cell becoming flattened out into a disc, with a sharply
curved equatorial edge, and to a streaming of material towards the
equator. In 1895, Loeb shewed that the streaming went on from the
equator towards the divided nuclei, and he supposed that the violence
of these streaming movements brought about actual division of the
cell: a hypothesis which was adopted by many other physiologists[248].
This streaming movement would suggest, as Robertson has pointed out,
a _diminution_ of surface-tension in the region of the equator. Now
Quincke has shewn that the formation of soaps at the surface of an
oil-droplet results in a diminution of the surface-tension of the
latter; and that if the saponification be local, that part of the
surface tends to spread. By laying a thread moistened with a dilute
solution of caustic alkali, or even merely smeared with soap, across
a drop of oil, Robertson has further shewn that the drop at once
divides into two: the edges of the drop, that is to say the ends of
the {192} diameter across which the thread lies, recede from the
thread, so forming a notch at each end of the diameter, while violent
streaming motions are set up at the surface, away from the thread in
the direction of the two opposite poles. Robertson[249] suggests,
accordingly, that the division of the cell is actually brought about by
a lowering of the equatorial surface-tension, and that this in turn is
due to a chemical action, such as a liberation of cholin, or of soaps
of cholin, through the splitting of lecithin in nuclear synthesis.
But purely chemical changes are not of necessity the fundamental
cause of alteration in the surface-tension of the egg, for the action
of electrolytes on surface-tension is now well known and easily
demonstrated. So, according to other views than those with which we
have been dealing, electrical charges are sufficient in themselves
to account for alterations of surface-tension; while these in turn
account for that protoplasmic streaming which, as so many investigators
agree, initiates the segmentation of the egg[250]. A great part of our
difficulty arises from the fact that in such a case as this the various
phenomena are so entangled and apparently concurrent that it is hard
to say which initiates another, and to which this or that secondary
phenomenon may be considered due. Of recent years the phenomenon of
_adsorption_ has been adduced (as we have already briefly said) in
order to account for many of the events and appearances which are
associated with the asymmetry, and lead towards the division, of the
cell. But our short discussion of this phenomenon may be reserved for
another chapter.
However, we are not directly concerned here with the phenomena of
segmentation or cell division in themselves, except only in so far as
visible changes of form are capable of easy and obvious correlation
with the play of force. The very fact of “development” indicates that,
while it lasts, the equilibrium of the egg is never complete[251].
And we may simply conclude the {193} matter by saying that, if you
have caryokinetic figures developing inside the cell, that of itself
indicates that the dynamic system and the localised forces arising
from it are in continual alteration; and, consequently, changes in the
outward configuration of the system are bound to take place.
――――――――――
As regards the phenomena of fertilisation,—of the union of the
spermatozoon with the “pronucleus” of the egg,—we might study these
also in illustration, up to a certain point, of the polarised forces
which are manifestly at work. But we shall merely take, as a single
illustration, the paths of the male and female pronuclei, as they
travel to their ultimate meeting place.
The spermatozoon, when within a very short distance of the egg-cell,
is attracted by it. Of the nature of this attractive force we have no
certain knowledge, though we would seem to have a pregnant hint in
Loeb’s discovery that, in the neighbourhood of other substances, such
even as a fragment, or bead, of glass, the spermatozoon undergoes a
similar attraction. But, whatever the force may be, it is one acting
normally to the surface of the ovum, and accordingly, after entry, the
sperm-nucleus points straight towards the centre of the egg; from the
fact that other spermatozoa, subsequent to the first, fail to effect
an entry, we may safely conclude that an immediate consequence of the
entry of the spermatozoon is an increase in the surface-tension of the
egg[252]. Somewhere or other, near or far away, within the egg, lies
its own nuclear body, the so-called female pronucleus, and we find
after a while that this has fused with the head of the spermatozoon
(or male pronucleus), and that the body resulting from their fusion
has come to occupy the centre of the egg. This _must_ be due (as
Whitman pointed out long ago) to a force of attraction acting between
the two bodies, and another force acting upon one or other or both in
the direction of the centre of the cell. Did we know the magnitude
of these several forces, it would be a very easy task to calculate
the precise path which the two pronuclei would follow, leading to
conjugation and the central {194} position. As we do not know the
magnitude, but only the direction, of these forces we can only make a
general statement: (1) the paths of both moving bodies will lie wholly
within a plane triangle drawn between the two bodies and the centre
of the cell; (2) unless the two bodies happen to lie, to begin with,
precisely on a diameter of the cell, their paths until they meet one
another will be curved paths, the convexity of the curve being towards
the straight line joining the two bodies; (3) the two bodies will meet
a little before they reach the centre; and, having met and fused,
will travel on to reach the centre in a straight line. The actual
study and observation of the path followed is not very easy, owing to
the fact that what we usually see is not the path itself, but only a
_projection_ of the path upon the plane of the microscope; but the
curved path is particularly well seen in the frog’s egg, where the path
of the spermatozoon is marked by a little streak of brown pigment, and
the fact of the meeting of the pronuclei before reaching the centre has
been repeatedly seen by many observers.
The problem is nothing else than a particular case of the famous
problem of three bodies, which has so occupied the astronomers; and
it is obvious that the foregoing brief description is very far from
including all possible cases. Many of these are particularly described
in the works of Fol, Roux, Whitman and others[253].
――――――――――
The intracellular phenomena of which we have now spoken have assumed
immense importance in biological literature and discussion during
the last forty years; but it is open to us to doubt whether they
will be found in the end to possess more than a remote and secondary
biological significance. Most, if not all of them, would seem to
follow immediately and inevitably from very simple assumptions as to
the physical constitution of the cell, and from an extremely simple
distribution of polarised forces within it. We have already seen that
how a thing grows, and what it grows into, is a dynamic and not a
merely material problem; so far as the material substance is concerned,
it is so only by reason {195} of the chemical, electrical or other
forces which are associated with it. But there is another consideration
which would lead us to suspect that many features in the structure and
configuration of the cell are of very secondary biological importance;
and that is, the great variation to which these phenomena are subject
in similar or closely related organisms, and the apparent impossibility
of correlating them with the peculiarities of the organism as a whole.
“Comparative study has shewn that almost every detail of the processes
(of mitosis) described above is subject to variation in different
forms of cells[254].” A multitude of cells divide to the accompaniment
of caryokinetic phenomena; but others do so without any visible
caryokinesis at all. Sometimes the polarised field of force is within,
sometimes it is adjacent to, and at other times it lies remote from the
nucleus. The distribution of potential is very often symmetrical and
bipolar, as in the case described; but a less symmetrical distribution
often occurs, with the result that we have, for a time at least,
numerous centres of force, instead of the two main correlated poles:
this is the simple explanation of the numerous stellate figures, or
“Strahlungen,” which have been described in certain eggs, such as
those of _Chaetopterus_. In one and the same species of worm (_Ascaris
megalocephala_), one group or two groups of chromosomes may be present.
And remarkably constant, in general, as the number of chromosomes in
any one species undoubtedly is, yet we must not forget that, in plants
and animals alike, the whole range of observed numbers is but a small
one; for (as regards the germ-nuclei) few organisms have less than six
chromosomes, and fewer still have more than sixteen[255]. In closely
related animals, such as various species of Copepods, and even in the
same species of worm or insect, the form of the chromosomes, and their
arrangement in relation to the nuclear spindle, have been found to
differ in the various ways alluded to above. In short, there seem to be
strong grounds for believing that these and many similar phenomena are
in no way specifically related to the particular organism in which they
have {196} been observed, and are not even specially and indisputably
connected with the organism as such. They include such manifestations
of the physical forces, in their various permutations and combinations,
as may also be witnessed, under appropriate conditions, in non-living
things.
When we attempt to separate our purely morphological or “purely
embryological” studies from physiological and physical investigations,
we tend _ipso facto_ to regard each particular structure and
configuration as an attribute, or a particular “character,” of this or
that particular organism. From this assumption we are apt to go on to
the drawing of new conclusions or the framing of new theories as to the
ancestral history, the classificatory position, the natural affinities
of the several organisms: in fact, to apply our embryological knowledge
mainly, and at times exclusively, to the study of _phylogeny_.
When we find, as we are not long of finding, that our phylogenetic
hypotheses, as drawn from embryology, become complex and unwieldy, we
are nevertheless reluctant to admit that the whole method, with its
fundamental postulates, is at fault. And yet nothing short of this
would seem to be the case, in regard to the earlier phases at least
of embryonic development. All the evidence at hand goes, as it seems
to me, to shew that embryological data, prior to and even long after
the epoch of segmentation, are essentially a subject for physiological
and physical investigation and have but the very slightest link with
the problems of systematic or zoological classification. Comparative
embryology has its own facts to classify, and its own methods and
principles of classification. Thus we may classify eggs according to
the presence or absence, the paucity or abundance, of their associated
food-yolk, the chromosomes according to their form and their number,
the segmentation according to its various “types,” radial, bilateral,
spiral, and so forth. But we have little right to expect, and in
point of fact we shall very seldom and (as it were) only accidentally
find, that these embryological categories coincide with the lines of
“natural” or “phylogenetic” classification which have been arrived at
by the systematic zoologist.
――――――――――
The cell, which Goodsir spoke of as a “centre of force,” is in {197}
reality a “sphere of action” of certain more or less localised
forces; and of these, surface-tension is the particular force which
is especially responsible for giving to the cell its outline and its
morphological individuality. The partially segmented differs from the
totally segmented egg, the unicellular Infusorian from the minute
multicellular Turbellarian, in the intensity and the range of those
surface-tensions which in the one case succeed and in the other fail to
form a visible separation between the “cells.” Adam Sedgwick used to
call attention to the fact that very often, even in eggs that appear
to be totally segmented, it is yet impossible to discover an actual
separation or cleavage, through and through between the cells which
on the surface of the egg are so clearly delimited; so far and no
farther have the physical forces effectuated a visible “cleavage.” The
vacuolation of the protoplasm in _Actinophrys_ or _Actinosphaerium_
is due to localised surface-tensions, quite irrespective of the
multinuclear nature of the latter organism. In short, the boundary
walls due to surface-tension may be present or may be absent with or
without the delimination of the other specific fields of force which
are usually correlated with these boundaries and with the independent
individuality of the cells. What we may safely admit, however, is
that one effect of these circumscribed fields of force is usually
such a separation or segregation of the protoplasmic constituents,
the more fluid from the less fluid and so forth, as to give a field
where surface-tension may do its work and bring a visible boundary
into being. When the formation of a “surface” is once effected, its
physical condition, or phase, will be bound to differ notably from that
of the interior of the cell, and under appropriate chemical conditions
the formation of an actual cell-wall, cellulose or other, is easily
intelligible. To this subject we shall return again, in another chapter.
From the moment that we enter on a dynamical conception of the cell,
we perceive that the old debates were in vain as to what visible
portions of the cell were active or passive, living or non-living.
For the manifestations of force can only be due to the _interaction_
of the various parts, to the transference of energy from one to
another. Certain properties may be manifested, certain functions may
be carried on, by the protoplasm apart {198} from the nucleus; but
the interaction of the two is necessary, that other and more important
properties or functions may be manifested. We know, for instance, that
portions of an Infusorian are incapable of regenerating lost parts
in the absence of a nucleus, while nucleated pieces soon regain the
specific form of the organism: and we are told that reproduction by
fission cannot be _initiated_, though apparently all its later steps
can be carried on, independently of nuclear action. Nor, as Verworn
pointed out, can the nucleus possibly be regarded as the “sole vehicle
of inheritance,” since only in the conjunction of cell and nucleus do
we find the essentials of cell-life. “Kern und Protoplasma sind nur
_vereint_ lebensfähig,” as Nussbaum said. Indeed we may, with E. B.
Wilson, go further, and say that “the terms ‘nucleus’ and ‘cell-body’
should probably be regarded as only topographical expressions denoting
two differentiated areas in a common structural basis.”
Endless discussion has taken place regarding the centrosome, some
holding that it is a specific and essential structure, a permanent
corpuscle derived from a similar pre-existing corpuscle, a “fertilising
element” in the spermatozoon, a special “organ of cell-division,”
a material “dynamic centre” of the cell (as Van Beneden and Boveri
call it); while on the other hand, it is pointed out that many cells
live and multiply without any visible centrosomes, that a centrosome
may disappear and be created anew, and even that under artificial
conditions abnormal chemical stimuli may lead to the formation of
new centrosomes. We may safely take it that the centrosome, or the
“attraction sphere,” is essentially a “centre of force,” and that this
dynamic centre may or may not be constituted by (but will be very apt
to produce) a concrete and visible concentration of matter.
It is far from correct to say, as is often done, that the cell-wall,
or cell-membrane, belongs “to the passive products of protoplasm
rather than to the living cell itself”; or to say that in the animal
cell, the cell-wall, because it is “slightly developed,” is relatively
unimportant compared with the important role which it assumes in
plants. On the contrary, it is quite certain that, whether visibly
differentiated into a semi-permeable membrane, or merely constituted by
a liquid film, the surface of the cell is the seat of {199} important
forces, capillary and electrical, which play an essential part in
the dynamics of the cell. Even in the thickened, largely solidified
cellulose wall of the plant-cell, apart from the mechanical resistances
which it affords, the osmotic forces developed in connection with it
are of essential importance.
But if the cell acts, after this fashion, as a whole, each part
interacting of necessity with the rest, the same is certainly true of
the entire multicellular organism: as Schwann said of old, in very
precise and adequate words, “the whole organism subsists only by means
of the _reciprocal action_ of the single elementary parts[256].”
As Wilson says again, “the physiological autonomy of the individual
cell falls into the background ... and the apparently composite
character which the multicellular organism may exhibit is owing to
a secondary distribution of its energies among local centres of
action[257].”
It is here that the homology breaks down which is so often drawn, and
overdrawn, between the unicellular organism and the individual cell of
the metazoon[258].
Whitman, Adam Sedgwick[259], and others have lost no opportunity of
warning us against a too literal acceptation of the cell-theory,
against the view that the multicellular organism is a colony (or,
as Haeckel called it (in the case of the plant), a “republic”) of
independent units of life[260]. As Goethe said long ago, “Das
lebendige ist zwar in Elemente {200} zerlegt, aber man kann es aus
diesen nicht wieder zusammenstellen und beleben;” the dictum of the
_Cellularpathologie_ being just the opposite, “Jedes Thier erscheint
als eine Summe vitaler Einheiten, von denen _jede den vollen Charakter
des Lebens an sich trägt_.”
Hofmeister and Sachs have taught us that in the plant the growth of
the mass, the growth of the organ, is the primary fact, that “cell
formation is a phenomenon very general in organic life, but still only
of secondary significance.” “Comparative embryology” says Whitman,
“reminds us at every turn that the organism dominates cell-formation,
using for the same purpose one, several, or many cells, massing its
material and directing its movements and shaping its organs, as if
cells did not exist[261].” So Rauber declared that, in the whole world
of organisms, “das Ganze liefert die Theile, nicht die Theile das
Ganze: letzteres setzt die Theile zusammen, nicht diese jenes[262].”
And on the botanical side De Bary has summed up the matter in an
aphorism, “Die Pflanze bildet Zellen, nicht die Zelle bildet Pflanzen.”
Discussed almost wholly from the concrete, or morphological point
of view, the question has for the most part been made to turn on
whether actual protoplasmic continuity can be demonstrated between
one cell and another, whether the organism be an actual reticulum, or
syncytium. But from the dynamical point of view the question is much
simpler. We then deal not with material continuity, not with little
bridges of connecting protoplasm, but with a continuity of forces, a
comprehensive field of force, which runs through and through the entire
organism and is by no means restricted in its passage to a protoplasmic
continuum. And such a continuous field of force, somehow shaping the
whole organism, independently of the number, magnitude and form of the
individual cells, which enter, like a froth, into its fabric, seems to
me certainly and obviously to exist. As Whitman says, “the fact that
physiological unity is not broken by cell-boundaries is confirmed in so
many ways that it must be accepted as one of the fundamental truths of
biology[263].”
{201}