Scientific American Supplement, No. 467, December 13, 1884 — John Shaqi
Scientific American Supplement, No. 467, December 13, 1884Various
Science
Scientific American Supplement, No. 467, December 13, 1884
Various
Science -- Periodicals
When the spectrum is very carefully produced, far more perfectly than
Newton knew how to show it, we have a homogeneous spectrum. It must
be noticed that Newton did not understand what we call a homogeneous
spectrum; he did not produce it, and does not point out in his writings
the conditions for producing it. With an exceedingly fine line of light
we can bring it out as in sunlight, like this upper picture, red,
orange, yellow, green, blue, indigo, and violet according to Newton's
nomenclature. Newton never used a narrow beam of light, and so could
not have had a homogeneous spectrum.
This is a diagram painted on glass and showing the colors as we know
them. It would take two or three hours if I were to explain the
subject of spectrum analysis to-night. We must tear ourselves away
from it. I will just read out to you the wave lengths corresponding
to the different positions in the sun's spectrum of certain dark
lines commonly called "Fraunhofer's lines." I will take as a unit the
one-hundred-thousandth of a centimeter. A centimeter is 0.4 of an
inch; it is a rather small half an inch. I take the thousandth of a
centimeter and the hundred of that as a unit. At the red end of the
spectrum the light in the neighborhood of that black line A has for its
wave length 7.6; B has 6.87; D has 5.89; the "frequency" for A is 3.9
times 100 million million; the frequency of D light is 5.1 times 100
million million per second.
Now, what force is concerned in those vibrations as compared with
sound at the rate of 400 vibrations per second? Suppose for a moment
the same matter was to move to and fro through the same range but
400 million million times per second. The force required is as the
square of the number expressing the frequency. Double frequency would
require quadruple force for the vibration of the same body. Suppose I
vibrate my hand again, as I did before. If I move it once per second, a
moderate force is required; for it to vibrate ten times per second, 100
times as much force is required; for 400 vibrations per second, 160,000
times as much force.
If I move my hand once per second through a space of a quarter of
an inch; a very small force is required; it would require very
considerable force to move it ten times a second, even through so small
a range; but think of the force required to move a tuning fork 400
times a second; compare that with the force required for a motion of
400 million million times a second. If the mass moved is the same, and
the range of motion is the same, then the force would be one million
million million million times as great as the force required to move
the prongs of the tuning fork. It is as easy to understand that number
as any number like 2, 3, or 4.
Public-domain text, read in full here on John Shaqi.
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