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
The extreme internal mobility betrayed by Carrington's and Spörer's
observations led to the inference that the matter composing the sun was
mainly or wholly gaseous. This had already been suggested by Father
Secchi[435] a year earlier, and by Sir John Herschel in April,
1864;[436] but it first obtained general currency through Faye's more
elaborate presentation. A physical basis was afforded for the view by
Cagniard de la Tour's experiments in 1822,[437] proving that, under
conditions of great heat and pressure, the vaporous state was compatible
with a very considerable density. The position was strengthened when
Andrews showed, in 1869,[438] that above a fixed limit of temperature,
varying for different bodies, true liquefaction is impossible, even
though the pressure be so tremendous as to retain the gas within the
same space that enclosed the liquid. The opinion that the mass of the
sun is gaseous now commands a very general assent; although the gaseity
admitted is of such a nature as to afford the consistence rather of
honey or pitch than of the aeriform fluids with which we are familiar.
On another important point the course of subsequent thought was
powerfully influenced by Faye's conclusions in 1865. Arago somewhat
hastily inferred from experiments with the polariscope the wholly
gaseous nature of the visible disc of the sun. Kirchhoff, on the
contrary, believed (erroneously, as we now know) that the brilliant
continuous spectrum derived from it proved it to be a white-hot solid or
liquid. Herschel and Secchi[439] indicated a cloud-like structure as
that which would best harmonise the whole of the evidence at command.
The novelty introduced by Faye consisted in regarding the photosphere no
longer "as a defined surface, in the mathematical sense, but as a limit
to which, in the general fluid mass, ascending currents carry the
physical or chemical phenomena of incandescence."[440] Uprushing floods
of mixed vapours with strong affinities--say of calcium or sodium and
oxygen--at last attain a region cool enough to permit their combination;
a fine dust of solid or liquid compound particles (of lime or soda, for
example) there collects into the photospheric clouds, and descending by
its own weight in torrents of incandescent rain, is dissociated by the
fierce heat below, and replaced by ascending and combining currents of
similar constitution.
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