I have proved, frictional slip between two portions
of liquid in contact is inconsistent with stability.
There is a further condition, upon which I cannot
enter into detail just now, but which may be understood
in a general way when I say that it is a condition
of either uniform or of increasing molecular rotation
from the surface inward, analogous to the condition
that the density of a liquid, resting for example
under the influence of gravity, must either be uniform
or must be greater below than above for stability
of equilibrium. All that I have said in favor
of the model vortex gas composed of perforated solids
with fluid circulations through them holds without
modification for the purely hydro-kinetic model, composed
of either Helmholtz cored vortex rings or of coreless
vortices, and we are now troubled with no such difficulty
as that of the impacts between solids. Whether,
however, when the vortex theory of gases is thoroughly
worked out, it will or will not be found to fail in
a manner analogous to the failure which I have already
pointed out in connection with the kinetic theory
of gases composed of little elastic solid molecules,
I cannot at present undertake to speak with certainty.
It seems to me most probable that the vortex theory
cannot fail in any such way, because all I have been
able to find out hitherto regarding the vibration
of vortices,[2] whether cored or coreless, does not
seem to imply the liability of translational or impulsive
energies of the individual vortices becoming lost
in energy of smaller and smaller vibrations.
[Footnote 1: Investigations respecting coreless
vortices will be found in a paper by the author, “Vibrations
of a Columnar Vortex,” Proc. R.S.E.,
March 1, 1880; and a paper by Hicks, recently read
before the Royal Society.]
[Footnote 2: See papers by the author “On
Vortex Motion.” Trans. R.S.E.
April, 1867, and “Vortex Statics,” Proc.
R.S.E. December, 1875; also a paper by J.J.
Thomson, B.A., “On the Vibrations of a Vortex
Ring,” Trans. R.S. December,
1881, and his valuable book on “Vortex Motion.”]
As a step toward kinetic theory of matter, it is certainly
most interesting to remark that in the quasi-elasticity,
elasticity looking like that of an India-rubber band,
which we see in a vibrating smoke-ring launched from
an elliptic aperture, or in two smoke-rings which
were circular, but which have become deformed from
circularity by mutual collision, we have in reality
a virtual elasticity in matter devoid of elasticity,
and even devoid of rigidity, the virtual elasticity
being due to motion, and generated by the generation
of motion.
* * * *
*
APPLICATION OF ELECTRICITY TO TRAMWAYS.
By M. HOLROYD SMITH.
Last year, when I had the pleasure of reading a paper
before you on my new system of electric tramways,
I ventured to express the hope that before twelve
months had passed, “to be able to report progress,”
and I am happy to say that notwithstanding the wearisome
delay and time lost in fruitless negotiations, and
the hundred and one difficulties within and without
that have beset me, I am able to appear before you
again and tell you of advance.