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

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440 APPENDIX.different polarities goes beyond <strong>the</strong> point <strong>of</strong> reciprocal neutralization, producinga state, to a small extent, <strong>the</strong> opposite <strong>of</strong> that at first existing; andhence a refluent discharge ensues, opposite in direction to <strong>the</strong> primary one.But even this does not produce an equilibrium, so that a third efllbrt ismade. These alternate discharges were detected by means <strong>of</strong> <strong>the</strong> magnetismimparted to needles exposed in coils <strong>of</strong> copper wire.*4. Supposing one or more rows <strong>of</strong> electrical particles, forming such afilament <strong>of</strong> electricity as must occupy <strong>the</strong> space within a wire <strong>of</strong> greatlength, to be made <strong>the</strong> medium <strong>of</strong> discharge to a Lcyden jar; agreeablyto <strong>the</strong> hypo<strong>the</strong>sis <strong>of</strong> one fluid, <strong>the</strong> electrical filament must be attracted atone end <strong>of</strong> <strong>the</strong> wire and repelled at <strong>the</strong> o<strong>the</strong>r, as soon as its terminationsare brought into due communication with <strong>the</strong> coatings <strong>of</strong> <strong>the</strong> jar. Yet<strong>the</strong> influence <strong>of</strong> <strong>the</strong> oppositely-charged surfaces <strong>of</strong> <strong>the</strong> jar cannot be conceivedto extend to those portions <strong>of</strong> <strong>the</strong> electricity which are remote from<strong>the</strong> points <strong>of</strong> contact, until <strong>the</strong>y be reached by a succession <strong>of</strong> vibrations.Hence, it is inconceivable that every particle in <strong>the</strong> filament <strong>of</strong> electricmatter can be made at <strong>the</strong> same time to move, so as to constitute a currenthaving <strong>the</strong> necessary velocity and volume to transfer, instantaneously, <strong>the</strong>electricity requisite to constitute a charge. Even <strong>the</strong> transmission <strong>of</strong> <strong>the</strong>impulses, in such an infinitesimal <strong>of</strong> time, seems to be inconceivable.5. In reply to <strong>the</strong>se objections, it has been urged by <strong>the</strong> Frankliniansthat a conductor being replete with electricity, as soon as this fluid shouldbe removed at one end, it ought to move at <strong>the</strong> o<strong>the</strong>r. This might be true<strong>of</strong> a fluid if incompressible, but could not hold good were it elastic. Abell wire moves at both ends when pulled only at one ; but this would notensue were a cord <strong>of</strong> gum-elastic substituted for <strong>the</strong> wire.6. But if <strong>the</strong> flow <strong>of</strong> one fluid, with <strong>the</strong> enormous velocity inferred, bedifficult to conceive, still more must it be incomprehensible that two fluidscan rush with similar celerity, from each surface <strong>of</strong> <strong>the</strong> jar, in oppositedirections, through <strong>the</strong> narrow channel afi'orded by a wire; especially as<strong>the</strong>y are alleged to exercise an intense affinity; so that it is only by aseries <strong>of</strong> decompositions and recompositions that <strong>the</strong>y can pass each o<strong>the</strong>r.7. That agreeably to <strong>the</strong> <strong>the</strong>ory <strong>of</strong> Bufiiy, equivalent portions <strong>of</strong> <strong>the</strong>resinous and vitreous fluids must exchange places during an electrical discharge,will appear evident from <strong>the</strong> following considerations : One surfacebeing redundant with vitreous and deficient commensuratcly <strong>of</strong> resinouselectricity, and <strong>the</strong> o<strong>the</strong>r redundant with <strong>the</strong> resinous and deficient <strong>of</strong> <strong>the</strong>vitreous fluid, it is inevitable that, to restore <strong>the</strong> equilibrium, <strong>the</strong>re mustbe a simultaneous transfer <strong>of</strong> each redundancy to <strong>the</strong> surfaces wherein <strong>the</strong>reis a deficiency <strong>of</strong> it to be supplied. If, after decomposing a large portion<strong>of</strong> <strong>the</strong> neutral compound previously existing on <strong>the</strong> surface <strong>of</strong> <strong>the</strong> jar, andtransferring <strong>the</strong> ingredients severall}^ in opposite directions, so as to causeeach to exist in excess upon <strong>the</strong> surface assigned to it, should <strong>the</strong> redundancies,thus originated, be neutralized by meeting in <strong>the</strong> discharging rod,nei<strong>the</strong>r surface could recover its quota <strong>of</strong> <strong>the</strong> electrical ingredient <strong>of</strong> whichit must have been deprived agreeably to <strong>the</strong> premises.8. This calls to mind <strong>the</strong> fact that no evidence has been adduced <strong>of</strong> <strong>the</strong>existence <strong>of</strong> any tertiinn quid, arising from <strong>the</strong> union <strong>of</strong> <strong>the</strong> supposedelectricities, founded on any property displayed by <strong>the</strong>ir resulting combinationin <strong>the</strong> neutral state. It must, if it exist, constitute an anomalous* Communicated to <strong>the</strong> American Philosophical Society.

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