*Some Remarks on the Importance of Surface Tension in
Morphogenesis.*--There are a few purely physical phenomena which have
a special importance in organic morphology, all of them connected
with capillarity or surface tension. Soap-lather is a very familiar
thing to all of you: you know that the soap-solution is arranged here
in very thin planes separated by spaces containing air: it was first
proved by Berthold[31] that the arrangement of cells in organic tissues
follows the same type as does the arrangement of the single bubbles of
a soap-lather, and Bütschli[32] added to this the discovery that the
minute structure of the protoplasm itself is that of a foam also. Of
course it is not one fluid and one gas which make up the constituents
of the structure in the organisms, as is the case in the well-known
inorganic foams, but two fluids, which do not mix with one another. One
general law holds for all arrangements of this kind: the so-called law
of least surfaces, expressed by the words that the sum of all surfaces
existing is a minimum; and it again is a consequence of this law, if
discussed mathematically, that four lines will always meet in one point
and three planes in one line. This feature, together with a certain law
about the relation of the angles meeting in one line to the size of the
bubbles, is realised most clearly in many structures of organic tissues,
and makes it highly probable, at least in some cases, that capillarity
is at work here. In other cases, as for instance in many plants, a kind
of outside pressure, the so-called tissue tension, may account for the
arrangement in surfaces *minimae areae*. Cleavage stages are perhaps
the very best type in which our physical law is expressed: and here
it may be said to have quite a simple application whenever all of the
blastomeres are of the same physical kind, whilst some complications
appear in germs with a specialised organisation and, therefore,
with differences in the protoplasm of their single blastomeres. In
such instances we may say that the physical law holds as far as the
conditions of the system permit, these conditions ordinarily consisting
in a sort of non-homogeneity of the surfaces.
[31] *Studien über Protoplasmamechanik*, Leipzig, 1886.
[32] *Unters. üb. mikroskopische Schäume und das Protoplasma*, Leipzig,
1892.
It seems, from the researches of Dreyer,[33] that the formation of
organic skeletons may also be governed by the physically conditioned
arrangement of protoplasmatic or cellular elements, and some phenomena
of migration and rearrangement among cleavage cells, as described by
Roux, probably also belong here.
[33] *Jena. Zeitschr.* 26, 1892.
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