The Study of Elementary Electricity and Magnetism by Experiment: Containing Two Hundred Experiments Performed with Simple, Home-made Apparatus — John Shaqi
The Study of Elementary Electricity and Magnetism by Experiment: Containing Two Hundred Experiments Performed with Simple, Home-made ApparatusSt. John, Thomas M. (Thomas Matthew)
Science
The Study of Elementary Electricity and Magnetism by Experiment: Containing Two Hundred Experiments Performed with Simple, Home-made Apparatus
(B) Touch the charged T B with the finger, watching C T.
_Part 2._ (C) Bring the re-charged E C near the neutral T B,
and parallel to its end surface; but keep them at least an inch
apart, so that a spark cannot pass. Watch C T.
(D) Withdraw E C, and try to explain the action of C T.
_=159. Electric Polarization; Theory of Induction.=_ This experiment
should remind the student of Exp. 24, in magnetism, in which a piece of
soft iron was magnetized by the inductive action of a magnet. The soft
iron was in a magnetic field; it became polarized. Is it possible that
the box, T B, was polarized, being in the electric field of E C?
We know, by the action of C T (Fig. 42), that the top end of T B was
charged while E C was in place. The charge was not conducted.
You know, from previous experiments, that + and - electrifications rush
together whenever possible. Why can we not suppose that a neutral body,
like the box at the start, contains an equal amount of both kinds, and
that these different electrifications have already rushed together?
If you imagine a small army of positive soldiers struggling, "man to
man," with the same number of equally strong negative soldiers, you can
readily see that one-half of them can hold the other half from running
away. A body remains neutral, then, according to this idea, as long as
it has an equal quantity of the two opposite kinds of electrification.
(See Theories, § 145, 146.)
As soon as the positively charged E C was brought near T B, it
destroyed the neutrality of T B, by pulling at its - electrification,
and by pushing back its + electrification to the top end and into C
T. We say that the charged E C produced a separation of the combined
electrifications of T B by _induction_, and not by contact. As soon as
the inductive action of E C was removed, T B became neutral again.
[Illustration: Figs. 43-44.]
=160. Note.= Figs. 43 and 44 may aid the student. In Fig. 43, T B
is supposed to be neutral. The "double sign" means that the + and -
electrifications are united; and, as there are an equal number of both
kinds, none are left free to tell the tale. Fig. 44 shows what happens
when the + E C is near.
What would happen if we could cut into T B at the middle with an
insulated knife while it is polarized by E C?
=EXPERIMENT 76. To learn how to charge a body by induction.=
_Apparatus._ Fig. 42, same as in Exp. 75.
=161. Directions.= (A) Bring the charged E C within an inch of
the bottom of T B, and as soon as C T is repelled, showing that
T B is polarized (Exp. 75), touch T B with your finger; then
remove your finger while you still hold E C in place.
(B) Withdraw E C and its inductive action. Explain the motions
of C T during the experiment. Is it still repelled by T B after
E C is removed?
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