The Chautauquan, Vol. 03, December 1882: A Monthly Magazine Devoted to the Promotion of True Culture.; Organ of the Chautauqua Literary and Scientific CircleChautauqua Literary and Scientific Circle
Religion
The Chautauquan, Vol. 03, December 1882: A Monthly Magazine Devoted to the Promotion of True Culture.; Organ of the Chautauqua Literary and Scientific Circle
Chautauqua Literary and Scientific Circle
Chautauqua Institution -- Periodicals; Chautauqua Literary and Scientific Circle -- Periodicals
Among the most ingenious of these is (or rather was, for I think it
is no longer maintained even by its eminent author), Prof. Tyndall’s
theory of a comet’s tail as an actinic cloud, generated by the
passage of the solar rays through exceedingly tenuous matter after
those rays had been in part deprived of their heating power, during
their passage through the comet’s head. According to this theory the
actinic cloud can not be formed under the heating rays, but so soon
as the actinic rays fall on the tenuous matter alone, the cloud is
formed,—so that all round the region in which would be the comet’s
shadow, there is no luminous cloud, while along that region the cloud
exists. The rapidity with which light travels would of course make
this explanation absolutely perfect in explaining cometic tails lying
always exactly in a straight line directed from the sun, or with their
axis so situated. But unfortunately this exceedingly rapid formation of
the tail (a tail of ninety million miles in length would be formed in
about eight minutes) is more than observation requires or can explain.
Prof. Tyndall made a slight oversight in dealing with this part of his
theory. Noticing that the actinic cloud, as he called it, is not formed
instantly, but after a delay of a few seconds, in his experiments, he
reasoned as though it would follow from this that the formation of
the actinic cloud behind a comet’s head in space might be a process
extending its action in distance from the head at a rate considerably
less than that at which light travels, yet still fast enough to account
for the exceedingly rapid formation of the tail of Newton’s comet,
and of other similar tails. But a little consideration will show that
the few seconds following the fall of light on the vapors dealt with
by Tyndall, before the luminous cloud appeared, would produce no such
effect as he imagined. The rate of formation of the tail would still
be that at which light travels. Imagine the head at A, for the sake of
argument, and the sun’s light after reaching A, passing on to B, C, D,
E, etc., to Z, a distance say of one hundred million miles, in nine
minutes:
A ... B ... C ... D ... E ... ... Z.
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