Waves and ripples in water, air, and æther : $b Being a course of Christmas lectures delivered at the Royal Institution of Great BritainFleming, J. A. (John Ambrose), Sir
Science
Waves and ripples in water, air, and æther : $b Being a course of Christmas lectures delivered at the Royal Institution of Great Britain
Fleming, J. A. (John Ambrose), Sir
Electric waves; Sound; Waves
I have it in my power to show you a still more remarkable experiment in
electric refraction. It is found that dry ice is very transparent to
these electric rays, but if the ice is wetted on the surface, then, as
you have already learnt, the film of moisture is opaque. We have had
constructed for the purposes of this lecture a prism of ice by freezing
water in a properly shaped zinc box. This prism is now being arranged
between the radiator and the receiver, and its surfaces must next be
dried carefully with dusters and white blotting paper to remove every
trace of moisture. When this is done we find we can repeat with the ice
prism the same experiment performed just now with the paraffin prism,
and we can refract the electric ray. If you will recall to your memory
the statements which were made in connection with the refraction of
rays of sound and waves of water, you will remember that it was pointed
out that the refraction of a ray of sound and the bending of a train
of water waves was due to the passage of the waves in the air or in
the water from a region where they were moving quickly to a region in
which they were compelled to move more slowly; and it was furthermore
shown that this bending must take place whenever a plain wave of any
kind passes in an oblique direction from one region to another region
where it undergoes an alteration in velocity. In other words, it was
shown that the bending or refraction of the direction of motion of a
wave, whether in air or water, is a proof that there is a difference
in its velocity in the two places bounded by the surface at which the
refraction takes place. If this bending takes place in such fashion
that the ray is bent towards the perpendicular line drawn to the
bounding surface, which is the same thing as saying if the line of
the wave is bent so as to make a less angle with the bounding surface
after it has passed from one region to the other, then it shows that
the wave-motion travels more slowly after it has passed the bounding
surface than before.
If we now return to the consideration of the electric experiment
with the prism of paraffin or ice, we shall find that this, properly
interpreted, gives us a proof that the electric radiation travels
more slowly in paraffin wax or ice than it does in air, and the ratio
between its velocity in air or in empty space and its velocity in any
non-conductor is called the _electric index of refraction_ for that
non-conductor. This index can be determined by making two measurements.
First, that of the refracting angle of the prism; and secondly, that of
the deviation of the ray.[26] I have made these two experiments for the
prisms of paraffin and ice in my laboratory, and I find the electric
refractive index of paraffin to be 1·64, and the electric refractive
index of ice to be 1·83.
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