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

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APPENDIX. 439Ohjcctions to <strong>the</strong> Theories severally <strong>of</strong> Frnnldinj Dufai/j and Ampere,with an effort to cjphiiii Eleetrieal Phenomena, hij Sfatieal or Undnlatori/P<strong>of</strong>arir.ation.* Bij llohert JTare, M.D., Emeritus Pr<strong>of</strong>essor <strong>of</strong>Chanisfry in <strong>the</strong> University <strong>of</strong> Pennsylvania.1. Tt appears, from <strong>the</strong> experiments <strong>of</strong> Whcatstone, that <strong>the</strong> discharge<strong>of</strong> a Leydcn jar, by means <strong>of</strong> a copper wire, takes place witliin a lime sosmall, that were <strong>the</strong> transfer <strong>of</strong> a iluid from <strong>the</strong> positive to <strong>the</strong> negativesurface requisite for its accomi3lishment, a current having a velocity exceedingtwo hundred thousand miles in a second would be necessary.2. The only causes for <strong>the</strong> velocity <strong>of</strong> an electric current, according toFranklin, are <strong>the</strong> repulsion between <strong>the</strong> particles <strong>of</strong> <strong>the</strong> electric fluid <strong>of</strong>which it has been assumed to consist, and <strong>the</strong> attraction between those particlesand o<strong>the</strong>r matter. These forces are alleged to concur in distributing<strong>the</strong> supposed fluid throughout space, whe<strong>the</strong>r o<strong>the</strong>rwise void, or partiallyoccupied by conducting solids or fluids. Hence, when between two ormore spaces, surfaces, or conducting masses, <strong>the</strong>re is an unequal distribution<strong>of</strong> <strong>the</strong> electric fluid, <strong>the</strong> equilibrium is restored whenever a communicationis opened by means <strong>of</strong> a sufficiently conducting medium. Agreeablyto this view <strong>of</strong> <strong>the</strong> subject, <strong>the</strong>re seems to be a resemblance between <strong>the</strong>supposed eftbrt <strong>of</strong> <strong>the</strong> electrical fluid to attain a state <strong>of</strong> equable diffusion,and that which would exist in <strong>the</strong> case <strong>of</strong> a gas confined in adjoining receivers,so as to be more dense within one than within <strong>the</strong> o<strong>the</strong>r; for,however <strong>the</strong> subtilty <strong>of</strong> <strong>the</strong> supposed electric fluid may exceed that <strong>of</strong> anygas, <strong>the</strong>re seems to be an analogy as respects <strong>the</strong> processes <strong>of</strong> diflusionwhich must prevail. But on opening a communication between cavitiesin which any aeriform fluid exists, in different degrees <strong>of</strong> condensation,<strong>the</strong> density must lessen in one cavity and augment in <strong>the</strong> o<strong>the</strong>r, with arapidity which must diminish gradually, and become evanescent with <strong>the</strong>difference <strong>of</strong> pressure by which it is induced. Far from taking place inan analogous manner, electrical discharges are effected with an extremesuddenness, <strong>the</strong> whole <strong>of</strong> <strong>the</strong> redundancy being discharged at once, ina mode more like <strong>the</strong> flight <strong>of</strong> a bullet, projected with infinite velocity,than that <strong>of</strong> a jet gradually varying in celerity from a maximum to aminimum.3. So far, in fact, is an electrical discharge from displaying <strong>the</strong> featureswhich belong to <strong>the</strong> reaction <strong>of</strong> a condensed elastic fluid, that agreeably to<strong>the</strong> observations <strong>of</strong> our distinguished countryman Henry, <strong>the</strong> result is morelike <strong>the</strong> vibrations <strong>of</strong> a spring, which, in striving to regain its normal position,goes beyond it. The first discharge between <strong>the</strong> surfaces <strong>of</strong> aLeyden jar is not productive <strong>of</strong> a perfect cc^uilibrium. The transfer <strong>of</strong>•••According to Farraday's researches and general experience, we have reason to believethat all particles <strong>of</strong> matter are endowed with one or <strong>the</strong> o<strong>the</strong>r <strong>of</strong> two species <strong>of</strong> polarity.This word polarity conveys <strong>the</strong> idea that two terminations in each particle are respectivelyendowed with forces which are analogous, hut contrary in <strong>the</strong>ir nature; so that <strong>of</strong> any twohomogeneous particles, <strong>the</strong> similar poles repel each o<strong>the</strong>r, while <strong>the</strong> dissimilar attract;likewise, when freely suspended, <strong>the</strong>y take a certain position relatively to each o<strong>the</strong>r, andon due proximity-, <strong>the</strong> opposite polar forces, counteracting each o<strong>the</strong>r, appear to be extinct.When deranged from this natural state <strong>of</strong> reciprocal neutralization, <strong>the</strong>ir liberated polesreact with <strong>the</strong> particles <strong>of</strong> adjacent bodies, or those in <strong>the</strong> surrounding medium. Under<strong>the</strong>se circumstances, any body Avhich may be constituted <strong>of</strong> <strong>the</strong> particles thus reacting issaid to be polarized, or in a state <strong>of</strong> polarization.Statical implies stationary; undulatory, wave-like.

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