The Story of the HeavensBall, Robert S. (Robert Stawell)
History
The Story of the Heavens
Ball, Robert S. (Robert Stawell)
Astronomy
It is possible to submit some of the questions involved to the test of
calculation, and it can be shown that the repulsive force adequate to
produce the straight tail of Type I. need only be about twelve times as
large as the attraction of gravitation. Tails of the second type could
be produced by a repulsive force which was about equal to gravitation,
while tails of the third type would only require a repulsive force about
one-quarter the power of gravitation.[33] The chief repulsive force
known in nature is derived from electricity, and it has naturally been
surmised that the phenomena of comets' tails are due to the electric
condition of the sun and of the comet. It would be premature to assert
that the electric character of the comet's tail has been absolutely
demonstrated; all that can be said is that, as it seems to account for
the observed facts, it would be undesirable to introduce some mere
hypothetical repulsive force. It must be remembered that on quite other
grounds it is known that the sun is the seat of electric phenomena.
As the comet gradually recedes from the sun the repulsive force becomes
weaker, and accordingly we find that the tail of the comet declines. If
the comet be a periodic one, the same series of changes may take place
at its next return to perihelion. A new tail is formed, which also
gradually disappears as the comet regains the depths of space. If we may
employ the analogy of terrestrial vapours to guide us in our reasoning,
then it would seem that, as the comet retreats, its tail would condense
into myriads of small particles. Over these small particles the law of
gravitation would resume its undivided sway, no longer obscured by the
superior efficiency of the repulsion. The mass of the comet is, however,
so extremely small that it would not be able to recall these particles
by the mere force of attraction. It follows that, as the comet at each
perihelion passage makes a tail, it must on each occasion expend a
corresponding quantity of tail-making material. Let us suppose that the
comet was endowed in the beginning with a certain capital of those
particular materials which are adapted for the production of tails. Each
perihelion passage witnesses the formation of a tail, and the
expenditure of a corresponding amount of the capital. It is obvious that
this operation cannot go on indefinitely. In the case of the great
majority of comets the visits to perihelion are so extremely rare that
the consequences of the extravagance are not very apparent; but to those
periodic comets which have short periods and make frequent returns, the
consequences are precisely what might have been anticipated: the
tail-making capital has been gradually squandered, and thus at length we
have the spectacle of a comet without any tail at all. We can even
conceive that a comet may in this manner be completely dissipated, and
we shall see in the next chapter how this fate seems to have overtaken
Biela's periodic comet.
Public-domain text, read in full here on John Shaqi.
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