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Experimental investigation of the spirit manifestations, [electronic ...

Experimental investigation of the spirit manifestations, [electronic ...

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376 OF MATTER, MIND, AND SriRIT.called for. It lias, for some years, occurred to nic, that <strong>the</strong> Newtoniandoctrine <strong>of</strong> radiation might be associated with that <strong>of</strong> undulation.1830. The fact that radiant heat could be collected by a mirror so as toraise <strong>the</strong> temperature <strong>of</strong> bodies placed in <strong>the</strong> focus, and that this processcould take place in vacuo, as ascertained by Sir Humphrey Davy, had beenadduced as unquestionable evidence <strong>of</strong> <strong>the</strong> materiality <strong>of</strong> caloric,<strong>the</strong> supposedfluid cause <strong>of</strong> heat. But as <strong>the</strong> cold proceeding from a snowball orany cold body could be collected by <strong>the</strong> same process, it was urged bysome chemists that <strong>the</strong> evidence <strong>of</strong> <strong>the</strong> materiality <strong>of</strong> <strong>the</strong> cause <strong>of</strong> coldmust also be admitted.Prevost met this argument by suggesting that nobody in nature is absolutely cold. Every body, however refrigerated, isnot so cold as to be incapable <strong>of</strong> greater refrigeration. Hence all bodiesbeing absolutely above <strong>the</strong> zero <strong>of</strong> nature, are throwing <strong>of</strong>f rays to eacho<strong>the</strong>r, and where <strong>the</strong>re is equality <strong>of</strong> temperature, <strong>the</strong>y do not cause anychange in <strong>the</strong>ir relative temperatures. The rays thrown <strong>of</strong>f by A are compensatedby those which it receives from B, and vice versa. But if Athrows <strong>of</strong>f to B more than B reciprocates, <strong>the</strong> temperature <strong>of</strong> A must falluntil an equilibrium is attained. Thus, A being <strong>the</strong> mirror and B <strong>the</strong>snowball, <strong>the</strong> mirror is refrigerated, and causes a greater radiation fromany body situated about its focus. This explanation was generally received,but to me, <strong>the</strong> following rationale, which I advanced, appearedpreferable :1831. I assumed caloric to exist throughout <strong>the</strong> sublunary creation, as<strong>the</strong> luminiferous e<strong>the</strong>r is assumed to be diffused throughout all space by<strong>the</strong> undulationists ; <strong>the</strong> diffusion arising from <strong>the</strong> reciprocal repulsion <strong>of</strong>its particles being similar to that which had been supposed to cause <strong>the</strong>diffusion <strong>of</strong> caloric. There is <strong>the</strong> greatest analogy between this diffusionand that which is known to exist in <strong>the</strong> case <strong>of</strong> gases. The process is <strong>the</strong>same, whe<strong>the</strong>r <strong>the</strong> gas be dense like chlorine, or thirty-six times as rare,as in <strong>the</strong> instance <strong>of</strong> hydrogen, and in <strong>the</strong> luminiferous e<strong>the</strong>r resembles<strong>the</strong> process by which hydrogen is rarilied, or might be rendered more rare,were <strong>the</strong> pressure <strong>of</strong> <strong>the</strong> atmosphere removed.1832. It is known that in any gas or gaseous mixture like that which webrea<strong>the</strong>, if a deficit <strong>of</strong> pressure be caused in any spot, <strong>the</strong> gaseous particleswill quickly move toward it, in order to restore <strong>the</strong> equilibrium <strong>of</strong>pressure, and that if, on <strong>the</strong> o<strong>the</strong>r hand, any augmentation <strong>of</strong> pressure beproduced at any spot, <strong>the</strong> gas will move outward to restore <strong>the</strong> equilibrium.1833. The particles being symmetrically arranged in lines, a row <strong>of</strong>particles may be conceived to lie between every two remote points. If wesuppose any number <strong>of</strong> points in <strong>the</strong> focal body, and a correspondingnumber in <strong>the</strong> surface <strong>of</strong> <strong>the</strong> mirror, it may be conceived that <strong>the</strong> interveninge<strong>the</strong>real or calorific particles will move in rows one way or <strong>the</strong> o<strong>the</strong>r,as <strong>the</strong> pressure in <strong>the</strong> focal space may become greater or less. Thus aneffect is brought about, equivalent to that which <strong>the</strong> Newtonian idea <strong>of</strong>

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