Keely and His Discoveries: Aerial NavigationMoore, Bloomfield H., Mrs.
Religion
Keely and His Discoveries: Aerial Navigation
Moore, Bloomfield H., Mrs.
Keely motor; Keely, John Ernest Worrell, 1827-1898
I assume that sound, like odour, is a real substance of unknown
and wonderful tenuity, emanating from a body where it has been
induced by percussion, and throwing out absolute corpuscles of
matter--inter-atomic particles--with a velocity of 1120 feet per
second, in vacuo 20,000. The substance which is thus disseminated is a
part and parcel of the mass agitated, and if kept under this agitation
continuously would, in the course of a certain cycle of time, become
thoroughly absorbed by the atmosphere; or, more truly, would pass
through the atmosphere to an elevated point of tenuity corresponding
to the condition of subdivision that governs its liberation from its
parent body. The sounds from vibratory forks, set so as to produce
etheric chords, while disseminating their compound tones permeate most
thoroughly all substances that come under the range of their atomic
bombardment. The clapping of a bell in vacuo liberates these atoms
with the same velocity and volume as one in the open air; and were
the agitation of the bell kept up continuously for a few millions of
centuries, it would thoroughly return to its primitive element. If
the chamber were hermetically sealed, and strong enough, the vacuous
volume surrounding the bell would be brought to a pressure of many
thousands of pounds to the square inch, by the tenuous substance
evolved. In my estimation, sound truly defined is the disturbance
of atomic equilibrium, rupturing actual atomic corpuscles; and the
substance thus liberated must certainly be a certain order of etheric
flow. Under these conditions is it unreasonable to suppose that, if
this flow were kept up, and the body thus robbed of its element, it
would in time disappear entirely? All bodies are formed primitively
from this high tenuous ether, animal, vegetable and mineral, and
they only return to their high gaseous condition when brought under
a state of differential equilibrium.
Public-domain text, read in full here on John Shaqi.
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