Fragments of Science: A Series of Detached Essays, Addresses, and Reviews. V. 1-2Tyndall, John
Science
Fragments of Science: A Series of Detached Essays, Addresses, and Reviews. V. 1-2
Tyndall, John
Chemistry; Physics; Science
With the view of stamping the thing more firmly on your minds, I will
make use of a strong and vivid image. In optics, red and green are
called complementary colours; their mixture produces white. Now I ask
you to imagine each of these colours to possess a self-repulsive
power; that red repels red, that green repels green; but that red
attracts green and green attracts red, the attraction of the
dissimilar colours being equal to the repulsion of the similar ones.
Imagine the two colours mixed so as to produce white, and suppose two
strips of wood painted with this white-; what will be their action
upon each other? Suspend one of them freely as we suspended our
darning-needle, and bring the other near it; what will occur? The red
component of the strip you hold in your hand will repel the red
component of your suspended strip; but then it will attract the green,
and, the forces being equal, they neutralise each other. In fact, the
least reflection shows you that the strips will be as indifferent to
each other as two unmagnetised darning-needles would be under the same
circumstances.
But suppose, instead of mixing the colours, we painted one half of
each strip from centre to end red, and the other half green, it is
perfectly manifest that the two strips would now behave towards each
other exactly as our two magnetised darning-needles--the red end would
repel the red and attract the green, the green would repel the green
and attract the red; so that, assuming two colours thus related to
each other, we could by their mixture produce the neutrality of an
unmagnetised body, while by their separation we could produce the
duality of action of magnetised bodies.
But you have already anticipated a defect in my conception; for if we
break one of our strips of wood in the middle we have one half
entirely red, and the other entirely green, and with these it would be
impossible to imitate the action of our broken magnet. How, then,
must we modify our conception? We must evidently suppose _each
molecule of the wood_ painted green on one face and red on the opposite
one. The resultant action of all the atoms would then exactly
resemble the action of a magnet. Here also, if the two opposite
colours of each atom could be caused to mix so as to produce white, we
should have, as before, perfect neutrality.
Public-domain text, read in full here on John Shaqi.
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