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<p>place at which the combined conditions of pressure and temperature will be first reached? If so, liquefaction, commencing at the centre, will spread
thence to the periphery; and, in virtue of the law that solids have higher melting points under pressure than when hi, it may be that solidification
will similarly, at a later stage, begin at the centre and progress outwards: eventually producing, in that case, a state such as Sir William
Thomson alleges exists in the Earth. But now suppose that instead of such a spheroid, we hiume one of, say, twenty or thirty times the mhi; what will
then happen? Notwithstanding convection-currents, the temperature at the centre must always be higher than elsewhere; and in the process of cooling
the “critical point” of temperature will sooner be reached in the outer parts. Though the requisite pressure will not exist near the surface, there
is evidently, in a large spheroid, a depth below the surface at which the pressure will be great enough, if the temperature is sufficiently low.
Hence<i>it is inferable that somewhere between centre and surface in the supposed larger spheroid,</i>there will arise that state described by Prof.
Andrews, in which “flickering striæ” of liquid float in gaseous matter of equal density. And it may be inferred that gradually, as the process goes
on, these striæ will become more abundant while the gaseous interspaces diminish; until, eventually, the liquid becomes continuous. Thus there will
result a molten shell containing a gaseous nucleus equally dense with itself at their surface of contact and more dense at the centre—a molten </p>
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<p align="center" style="font: 11px;">shell which will slowly thicken by additions to both exterior and interior. That a solid crust will eventually form on this molten shell may be
reasonably concluded. To the demurrer that solidification cannot commence at the surface, because the solids formed would sink, there are two
replies. The first is that various metals expand while solidifying, and therefore would float. The second is that since the envelope of the
supposed spheroid would consist of the gases and non-metallic elements, compounds of these with the metals and with one another would continually
accumulate on the molten shell; and the crust, consisting of oxides, chlorides, sulphurets, and the rest, having much less specific gravity than </p>
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<p>the molten shell, would be readily supported by it. Clearly a planet thus constituted would be in an unstable state. Always it
would remain liable to a catastrophe resulting from change in its gaseous nucleus. If, under some condition of pressure and temperature eventually
reached, the components of this suddenly entered into one of those proto-chemical combinations forming a new element, there might result an
explosion capable of shattering the entire planet, and propelling its fragments in all directions with high velocities. If the hypothetical
planet between Jupiter and Mars was intermediate in size as in position, it would apparently fulfil the conditions under which such a catastrophe might </p>
<BR><span style="font-family: Helvetica, Arial, sans-serif; font-size: 10px;"></span>
<p align="center" style="font: 16px;">occur. Note IV. The argument set forth in the foregoing note, is in part designed to introduce a question which seems to require re-consideration—the origin
of the minor planets or planetoids. The hypothesis of Olbers, as propounded by him, implied that the disruption of the hiumed planet between mars and
Jupiter had taken place at no very remote period in the past; and this implication was shown to be inadmissible by the discovery that there exists .</p>
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