Liquid Drops and Globules, Their Formation and Movements: Three lectures delivered to popular audiencesDarling, Charles R. (Charles Robert)
Science
Liquid Drops and Globules, Their Formation and Movements: Three lectures delivered to popular audiences
Darling, Charles R. (Charles Robert)
Drops; Liquids; Surface tension
*The Centrifugoscope.*—I have here a toy, which we may suitably call the
centrifugoscope, which shows in a simple way the formation of spheres of
liquid in a medium of practically equal density. It consists of a large
glass bulb attached to a stem, about three-quarters full of water, the
remaining quarter being occupied by orthotoluidine. This liquid, being
slightly denser than water at the temperature of the room, rests on the
bottom of the bulb. When I hold the stem horizontally, and rotate
it—suddenly at first, and steadily afterwards—a number of fragments are
detached from the orthotoluidine, which immediately become spherical,
and rotate near the outer side of the bulb. The main mass of the red
liquid rises to the centre of the bulb, and rotates on its axis (Fig.
7), and we thus get an imitation of the solar system, with the planets
of various sizes revolving round the central mass; and even the
asteroids are represented by the numerous tiny spheres which are always
torn off from the main body of liquid along with the larger ones. When
the rotation ceases, the detached spheres sink, and after a short time
join the parent mass of orthotoluidine. We can therefore take this
simple apparatus at any time, and use it to show that a mass of liquid,
possessing a free surface all round, and unaffected by gravity,
automatically becomes a sphere. After all, this is only what we should
expect of an elastic skin filled with a free-flowing medium.
*Effect of Temperature on Sphere of Orthotoluidine.*—I will now return
to the large sphere formed under water in the flat-sided vessel, and
direct your attention to an experiment which teaches an important
lesson. By placing a little ice on the top of the water, we are enabled
to cool the contents of the vessel, and we soon notice that the
red-coloured sphere becomes flattened on the top and below, and sinks a
short distance into the saline layer. Evidently the cooling action,
which has affected both liquids, has caused the orthotoluidine to become
denser than water. I now surround the vessel with warm water, and allow
the contents gradually to attain a temperature higher than 75° F. You
observe that the flattened drop changes in shape until it is again
spherical; and as the heating is continued elongates in a vertical
direction, and then rises to the surface, being now less dense than
water. So sensitive are these temperature effects that a difference of 1
degree on either side of 75° F. causes a perceptible departure from the
spherical shape in the case of a large drop. It therefore follows that
orthotoluidine may be either heavier or lighter than water, according to
temperature, and this fact admits of a simple explanation.
Orthotoluidine expands more than water on heating, and contracts more on
cooling. The effect of expansion is to decrease the density, and of
contraction to increase it; hence the reason why warm air rises through
cold air, and vice versa. Now if orthotoluidine and water, which are
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