Hawkins Electrical Guide v. 01 (of 10): Questions, Answers, & Illustrations, A progressive course of study for engineers, electricians, students and those desiring to acquire a working knowledge of electricity and its applicationsHawkins, N. (Nehemiah)
Science
Hawkins Electrical Guide v. 01 (of 10): Questions, Answers, & Illustrations, A progressive course of study for engineers, electricians, students and those desiring to acquire a working knowledge of electricity and its applications
Hawkins, N. (Nehemiah)
Electrical engineering -- Handbooks, manuals, etc.
[Illustration: FIGS. 26 to 29.--Explanation of Faraday’s ice pail
experiment. For simplicity the electroscope, insulating stand and silk
thread have been omitted. Only the three principal conductors K, P, and
the earth E are shown. In fig. 26 the ball K is sufficiently close to P to
act inductively on it; six lines are shown as falling on P, and the other
six as passing to E by different paths. Corresponding to the six lines
falling on P from K, six others pass to E from the lower surfaces. In fig.
27 where K is just entering the pail, two lines only pass from K to E
through the dielectric; the remaining ten fall on P, and ten others
starting from the distant parts of P pass to E. In fig. 28, K is so far
within P that none of its lines can reach E through the dielectric; they
all fall on P and from the outside of P an equal number start and pass
through the dielectric to E. It is evident that in this position K can be
moved about within P, without affecting the outside distribution in the
slightest, and that even when K touches P as shown in fig. 29, and when,
therefore, all lines between them disappear, the lines in the dielectric
outside remain just as they are in fig. 28. K is now completely
discharged, since lines no longer emanate from it, hence it can be removed
by the silk cord without disturbing the electrification of P. If K be
again charged and introduced into P it will be again discharged, for the
fact that P is already charged will have no effect on the final result,
provided when K touches P it is well _under cover_.]
Since the electricity thus yielded by the electrophorus is not obtained at
the expense of any part of the original charge, it is a matter of some
interest to inquire whence is the source from which the energy of this
apparently unlimited supply is drawn; for it cannot be called into
existence without the expenditure of some other form of energy. The fact
is, _more work is done in lifting the cover when it is charged_ with the
positive electricity than when it is not charged; for when charged, there
is the force of the electric attraction to be overcome as well as the
force of gravity; this excess force is the real origin of the energy
stored up in the separate charges.
[Illustration: FIGS. 30 and 31.--The Leyden jar and discharger. Its
discovery is attributed to the attempt of Musschenbrock and his pupil
Cuneus to collect the supposed electric “fluid” in a bottle half filled
with water. The bottle was held in the hand and was provided with a nail
to lead the “fluid” down through the cork to the water from the electric
machine. The invention of the Leyden jar is also claimed by Kleist, Bishop
of Pomerania.]
Public-domain text, read in full here on John Shaqi.
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