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

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APPENDIX. 455<strong>the</strong> poles <strong>of</strong> tho disturbing; apparatus^ neutralize each o<strong>the</strong>r intermediately.8np])0sin^j; <strong>the</strong> ponderable as ^vell as <strong>the</strong> inipondtirable matter in a perfectconductor to be susceptible <strong>of</strong> <strong>the</strong> polar arrangement, <strong>of</strong> which an electriiiedstate is thus represented to consist, non-conductors to be insusceptible<strong>of</strong> such polar derangement; imperfect conductors may have a constitutionintermediate between metals and electrics.71. "When an electrical discharge is made through any space devoid <strong>of</strong>air or o<strong>the</strong>r matter, it must <strong>the</strong>n find its way solely by <strong>the</strong> polarization <strong>of</strong><strong>the</strong> rare imponderable matter existing <strong>the</strong>rein ; and consequently its corruscationsshould be proporlionably more diffuse, which is actually foundto be true ; but when gaseous ethcrco-ponderable atoms intervene, as inwire, <strong>the</strong>y enable competent waves to exist within a narrower channel andto attain a greater intensity.72. I consider all bodies as insulators which cause discharges through<strong>the</strong>m to be more difficult than through a vacuum, and which, by <strong>the</strong>irinterposition within a circuit, can prevent that propagation <strong>of</strong> <strong>the</strong> oppositelypolarizing undulations which would o<strong>the</strong>rwise ensue. This furnishesa good mean <strong>of</strong> discrimination between insulators and conductors, <strong>the</strong>criterion being that a discharge ensues more readily as <strong>the</strong>re is more <strong>of</strong><strong>the</strong> one and less <strong>of</strong> <strong>the</strong> o<strong>the</strong>r in <strong>the</strong> way : that <strong>the</strong> one leads <strong>the</strong> waveswhere <strong>the</strong>y would not go, <strong>the</strong> o<strong>the</strong>r impedes <strong>the</strong>ir going where <strong>the</strong>y wouldproceed. Both in <strong>the</strong> case <strong>of</strong> disruptive discharge through air, producinga spark, or <strong>of</strong> a deflagrating discharge through wire, causing itsexplosion,<strong>the</strong>re is a dispersion <strong>of</strong> intervening ponderable particles ; and yet <strong>the</strong>re isthis manifest discordancj^, that in one case <strong>the</strong> undulatory process <strong>of</strong> transferis assisted, in <strong>the</strong> o<strong>the</strong>r resisted. The waves follow <strong>the</strong> metallic filamentwith intense attraction, while <strong>the</strong>y strive to get out <strong>of</strong> <strong>the</strong> way <strong>of</strong> thoseformed by <strong>the</strong> aeriform matter, as if repelled. Hence <strong>the</strong> term disruptive,from cUrumpo, to break through, was happily employed by Farraday todesignate spark discharges.73. The zigzag form <strong>of</strong> <strong>the</strong> disruptive spark shows that <strong>the</strong>re is a tendencyin <strong>the</strong> aeriform particles to turn <strong>the</strong> waves out <strong>of</strong> that straightcourse, which, if unresisted or facilitated, <strong>the</strong>y would naturally pursue.On <strong>the</strong> one hand, <strong>the</strong> aerial filaments being unsuitable for <strong>the</strong> conveyance<strong>of</strong> <strong>the</strong> electric waves, <strong>the</strong>se are forced by <strong>the</strong>m out <strong>of</strong> <strong>the</strong> normal pathfirst in one direction, <strong>the</strong>n in ano<strong>the</strong>r; while, on <strong>the</strong> o<strong>the</strong>r hand, <strong>the</strong> finestmetallic filament furnishes a channel for <strong>the</strong> electric waves, so favourablethat this channel is pursued, although <strong>the</strong> consequent polarization <strong>of</strong> <strong>the</strong>conducting particles be so intense as to make <strong>the</strong>m fly asunder with explosiveviolence. Even when a bell-wire has been dissipated by lightning, ithas been found to facilitate and determine <strong>the</strong> path <strong>of</strong> <strong>the</strong> discharge.74. The various forms <strong>of</strong> <strong>the</strong> electric spark, resulting from varying <strong>the</strong>gas through which it may be made to pass, agreeably to <strong>the</strong> researches <strong>of</strong>Farraday, is explained by <strong>the</strong> supposition that <strong>the</strong> peculiarities <strong>of</strong> <strong>the</strong> sparkis partially <strong>the</strong> consequence <strong>of</strong> <strong>the</strong> polarizability <strong>of</strong> <strong>the</strong> gaseous atomsthrough which <strong>the</strong> discharge is made, and varies, accordingly, in its appearance.

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