Scientific American Supplement, No. 633, February 18, 1888Various
Science
Scientific American Supplement, No. 633, February 18, 1888
Various
Science -- Periodicals
A man who could thus arouse popular enthusiasm for science a century and
a half ago must have been a remarkable genius. Trusted students of
Linnaeus were sent on botanical exploring expeditions throughout the
world. The high renown in which Linnaeus was held was shown in the
significant title, almost universally bestowed upon him, of "The Flower
King."--_Western Druggist._
* * * * *
ON A METHOD OF MAKING THE WAVE LENGTH OF SODIUM LIGHT THE ACTUAL AND
PRACTICAL STANDARD OF LENGTH.
BY ALBERT A. MICHELSON AND EDWARD W. MORLEY.
The first actual attempt to make the wave length of sodium light a
standard of length was made by Peirce.[1] This method involves two
distinct measurements: first, that of the angular displacement of the
image of a slit by a diffraction grating, and, second, that of the
distance between the lines of the grating. Both of these are subject to
errors due to changes of temperature and to instrumental errors. The
results of this work have not as yet been published; but it is not
probable that the degree of accuracy attained is much greater than one
part in fifty or a hundred thousand. More recently, Mr. Bell, of the
Johns Hopkins University, using Rowland's gratings, has made a
determination of the length of the wave of sodium light which is claimed
to be accurate to one two hundred thousandth part[2]. If this claim is
justified, it is probably very near the limit of accuracy of which the
method admits. A short time before this, another method was proposed by
Mace de Lepinay.[3] This consists in the calculation of the number of
wave lengths between two surfaces of a cube of quartz. Besides the
spectroscopic observations of Talbot's fringes, the method involves the
measurement of the index of refraction and of the density of quartz, and
it is not surprising that the degree of accuracy attained was only one
in fifty thousand.
[Footnote 1: Nature, xx, 99, 1879; this Journal, III, xviii, 51, 1879.]
[Footnote 2: On the absolute wave lengths of light, this Journal,
III, xxxiii, 167, 1887.]
[Footnote 3: Comptes Rendus, cii, 1153, 1886; Journal, de Phys.,
II, v, 411, 1886.]
Several years ago, a method suggested itself which seemed likely to
furnish results much more accurate than either of the foregoing, and
some preliminary experiments made in June have confirmed the
anticipation. The apparatus for observing the interference phenomena is
the same as that used in the experiments on the relative motion of the
earth and the luminiferous ether.
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