Still more curious are the phenomena exhibited when the formative forces
of the liquid are partly disturbed by putting in contact with the
liquid's surface some rigid body. If we immerse, for example, the wire
framework of a cube in our mass of oil, the oil will everywhere stick to
the wire framework. If the quantity of oil is exactly sufficient we
shall obtain an oil cube with perfectly smooth walls. If there is too
much or too little oil, the walls of the cube will bulge out or cave in.
In this manner we can produce all kinds of geometrical figures of oil,
for example, a three-sided pyramid, a cylinder (by bringing the oil
between two wire rings), and so on. Interesting is the change of form
that occurs when we gradually suck out the oil by means of a glass tube
from the cube or pyramid. The wire holds the oil fast. The figure grows
smaller and smaller, until it is at last quite thin. Ultimately it
consists simply of a number of thin, smooth plates of oil, which extend
from the edges of the cube to the centre, where they meet in a small
drop. The same is true of the pyramid.
[Illustration: Fig. 2.]
The idea now suggests itself that liquid figures as thin as this, and
possessing, therefore, so slight a weight, cannot be crushed or deformed
by their weight; just as a small, soft ball of clay is not affected in
this respect by its weight. This being the case, we no longer need our
mixture of alcohol and water for the production of figures, but can
construct them in the open air. And Plateau, in fact, found that these
thin figures, or at least very similar ones, could be produced in the
air, by dipping the wire nets described in a solution of soap and water
and quickly drawing them out again. The experiment is not difficult. The
figure is formed of itself. The preceding drawing represents to the eye
the forms obtained with cubical and pyramidal nets. In the cube, thin,
smooth films of soap-suds proceed from the edges to a small, quadratic
film in the centre. In the pyramid, a film proceeds from each edge to
the centre.
These figures are so beautiful that they hardly admit of appropriate
description. Their great regularity and geometrical exactness evokes
surprise from all who see them for the first time. Unfortunately, they
are of only short duration. They burst, on the drying of the solution in
the air, but only after exhibiting to us the most brilliant play of
colors, such as is often seen in soap-bubbles. Partly their beauty of
form and partly our desire to examine them more minutely induces us to
conceive of methods of endowing them with permanent form. This is very
simply done.[2] Instead of dipping the wire nets in solutions of soap,
we dip them in pure melted colophonium (resin). When drawn out the
figure at once forms and solidifies by contact with the air.
Public-domain text, read in full here on John Shaqi.
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