On the various forces of nature and their relations to each otherFaraday, Michael
Science
On the various forces of nature and their relations to each other
Faraday, Michael
Physics
But now we come to another fact. I will take this piece of shell-lac
and make it attractive by friction; and remember that whenever we get
an attraction of gravity, chemical affinity, adhesion, or electricity
(as in this case), the body which attracts is attracted also; and just
as much as that ball was attracted by the shell-lac, the shell-lac
was attracted by the ball. Now, I will suspend this piece of excited
shell-lac in a little paper stirrup, in this way (fig. 33), in order
to make it move easily, and I will take another piece of shell-lac,
and after rubbing it with flannel, will bring them near together. You
will think that they ought to attract each other; but now what happens?
It does not attract; on the contrary, it very strongly _repels_, and
I can thus drive it round to any extent. These, therefore, repel each
other, although they are so strongly attractive--repel each other to
the extent of driving this heavy piece of shell-lac round and round
in this way. But if I excite this piece of shell-lac, as before, and
take this piece of glass and rub it with silk, and then bring them
near, what think you will happen? [The Lecturer held the excited glass
near the excited shell-lac, when they attracted each other strongly.]
You see, therefore, what a difference there is between these two
attractions,--they are actually two _kinds_ of attraction concerned in
this case, quite different to anything we have met with before; but the
_force_ is the same. We have here, then, a double attraction--a dual
attraction or force--one attracting, and the other repelling.
Again, to shew you another experiment which will help to make this
clear to you. Suppose I set up this rough indicator again [the excited
shell-lac suspended in the stirrup]--it is rough, but delicate enough
for my purpose; and suppose I take this other piece of shell-lac, and
take away the power, which I can do by drawing it gently through the
hand; and suppose I take a piece of flannel (fig. 34), which I have
shaped into a cap for it and made dry. I will put this shell-lac into
the flannel, and here comes out a very beautiful result. I will rub
this shell-lac and the flannel together (which I can do by twisting the
shell-lac round), and leave them in contact; and then, if I ask, by
bringing them nearer our indicator, what is the attractive force?--it
is nothing! But if I take them apart, and then ask what will they do
when they are separated--why, the shell-lac is strongly repelled, as it
was before, but the cap is strongly attractive; and yet if I bring them
both together again, there is no attraction--it has all disappeared
[the experiment was repeated]. Those two bodies, therefore, still
contain this attractive power: when they were parted, it was evident to
your senses that they had it, though they do not attract when they are
together.
[Illustration: Fig. 34.]
[Illustration: Fig. 35.]
Public-domain text, read in full here on John Shaqi.
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