A Popular History of Astronomy During the Nineteenth Century: Fourth EditionClerke, Agnes M. (Agnes Mary)
History
A Popular History of Astronomy During the Nineteenth Century: Fourth Edition
Clerke, Agnes M. (Agnes Mary)
Astronomy -- History -- 19th century
There are, however, grave difficulties in identifying the two kinds of
phenomena. One (already mentioned) is the total absence of the regular
swirling motion--in a direction contrary to that of the hands of a watch
north of the solar equator, in the opposite sense south of it--which
should impress itself upon every lineament of a sun-spot if the cause
assigned were a primary producing, and not merely (as it possibly may
be) a secondary determining one. The other, pointed out by Young,[467]
is that the cause is inadequate to the effect. The difference of
movement, or _relative drift_, supposed to occasion such prodigious
disturbances, amounts, at the utmost, for two portions of the
photosphere 123 miles apart, to about five yards a minute. Thus the
friction of contiguous sections must be quite insignificant.
A view better justified by observation was urged by Secchi in and after
the year 1872, and was presented in an improved form by Professor Young
in his excellent little book on _The Sun_, published in 1882.[468] Spots
are manifestly associated with violent eruptive action, giving rise to
the faculæ and prominences which usually garnish their borders. It is
accordingly contended that upon the withdrawal of matter from below by
the flinging up of a prominence must ensue a sinking-in of the surface,
into which the partially cooled erupted vapours rush and settle,
producing just the kind of darkening by increased absorption told of by
the spectroscope. Round the edges of the cavity the rupture of the
photospheric shell will form lines of weakness provocative of further
eruptions, which will, in their turn, deepen and enlarge the cavity. The
phenomenon thus tends to perpetuate itself, until equilibrium is at last
restored by internal processes. A sun-spot might then be described as an
inverted terrestrial volcano, in which the outbursts of heated matter
take place on the borders instead of at the centre of the crater, while
the cooled products gather in the centre instead of at the borders.
But on the earth, the solid crust forcibly represses the steam gathering
beneath until it has accumulated strength for an explosion, while there
is no such restraining power that we know of in the sun. Zöllner,
indeed, adapted his theory of the solar constitution to the special
purpose of procuring it; yet with very partial success, since almost
every new fact has proved adverse to his assumptions. Volcanic action is
essentially spasmodic. It implies habitual constraint varied by
temporary outbreaks, inconceivable in a gaseous globe, such as we
believe the sun to be.
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