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
*Movements of Aniline Globules on a Water Surface.*—If we allow a small
quantity of aniline to run on to the surface of water, it forms itself
into a number of floating globules. I now project on the screen a water
surface on which a little aniline has been poured, and we are thus
enabled to watch the movements which occur. All the globules appear to
be twitching or shuddering; and if you observe closely you will notice
the surface of each globule stretching and recoiling alternately. The
recoil is accompanied by the projection of tiny globules from the rim,
which becomes scalloped when the globule is stretched. The small
globules thrown off appear to be formed from the protuberances at the
edge (Fig. 36), and after leaving the main globule they spread out over
the surface, or dissolve. This process continues for a long time,
gradually diminishing in vigour, until small stationary globules are
left floating on the surface, which is now covered with a skin of
aniline. This action is in striking contrast to the tranquil formation
of floating globules of oil, and calls for some special comment.
Let us recall again the three forces at work at the edge of a floating
globule (Fig. 35). The surface tension of the water, acting
horizontally, tends to stretch the globule, and is successful
momentarily in overcoming the opposing tensions, each of which pulls at
an angle to the surface. Enlargement of the upper surface of the
globule, however, reduces the angles at which the tensions B and C act,
and in consequence their effective strength is increased. The spreading
of the aniline over the water surface diminishes the pull A, which B and
C combined now overcome, and hence the surface of the globule shrinks
again. For some unexplained reason both the stretching and recoil of the
globule occur suddenly, there being an interval of repose between each,
and these jerky movements result in small portions of the rim being
detached, each of which forms a separate small globule. The aniline
which spreads over the surface of the water dissolves, and the water
tension A, which had been enfeebled by the presence of the aniline skin,
recovers its former strength, and again stretches the globule; and so
the whole process is repeated. When the surface of the water becomes
permanently covered with a skin, which occurs when the top layer is
saturated with aniline, the globule remains at rest, and has such a
shape that the tensions B and C act at angles which enable them just to
balance the weakened pull of A. Why the edge of the globule becomes
indented during the movements, and why these movements are spasmodic
instead of gradual, has not been clearly made out. It is interesting to
recall that a spheroid of liquid on a hot plate also possesses a
scalloped edge, and it may be that the two phenomena have something in
common.
[Illustration: __Fig._ 37.—Orthotoluidine globules on a water surface._]
Public-domain text, read in full here on John Shaqi.
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