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

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

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382 OF MATTER, MIND, AND SPIRIT.manner <strong>of</strong> atoms or particles which are endowed with polarity, so thatwhen <strong>the</strong> opposite poles are in proximity, <strong>the</strong>re is neutralization : repulsion,and disturbance, when similar poles are approximated. This being premised,<strong>the</strong> allegation may be intelligible, that when bodies are electrified,<strong>the</strong> poles <strong>of</strong> <strong>the</strong> component atoms or particles are conceived to be derangedfrom <strong>the</strong>ir natural position <strong>of</strong> reciprocal neutralization, so that <strong>the</strong>y reactwith exterior bodies, disturbing <strong>the</strong> poles <strong>of</strong> <strong>the</strong>ir constituent particles,and thus electrifying <strong>the</strong>m by induction.1864. This abnormal state <strong>of</strong> disturbance, is conceived to be producedon glass or resin, or any electric, when duly subjected to friction.1865. Thus when in an electric machine a vitreous surface is rubbedby a lea<strong>the</strong>r cushion, <strong>the</strong> particles both <strong>of</strong> <strong>the</strong> lea<strong>the</strong>r and glass surfaces arederanfrcd from <strong>the</strong>ir natural state <strong>of</strong> reciprocalneutralization, and present<strong>the</strong>ir poles in an active state, and <strong>the</strong> glass surface, moving through <strong>the</strong>e<strong>the</strong>real medium, (812) polarizes it as it passes, <strong>the</strong> e<strong>the</strong>r resuming itsnormal state till <strong>the</strong> e<strong>the</strong>real atmosphere over <strong>the</strong> conductor is reached.that it imparts durable polarity ; <strong>the</strong> metallic superficies <strong>of</strong> <strong>the</strong> conductortaking <strong>the</strong> opposite state, so that <strong>the</strong> charge is retained until <strong>the</strong> glass goesto and returns from <strong>the</strong> cushion, with a far<strong>the</strong>r supply <strong>of</strong> polarity.1866. The charges <strong>of</strong> polarization received by <strong>the</strong> plates at each succeedingrevolution <strong>of</strong> <strong>the</strong> plate or cylinder, is divided with <strong>the</strong> e<strong>the</strong>realatmosphere over <strong>the</strong> conductor, and this process is reiterated till <strong>the</strong> frictionalpower has accomplished its maximum effect. Then <strong>the</strong> conductoris said to be charged positively, according to <strong>the</strong> <strong>the</strong>ory <strong>of</strong> one fluid, andvitreously, according to that <strong>of</strong> Dufay, or <strong>the</strong> <strong>the</strong>ory <strong>of</strong> two fluids.ToMeanwhile,if <strong>the</strong> cushion communicates duly with an insulated conductor, aprocess perfectly analogous to that just described has been charging thatconductor, pari ^;ass», with <strong>the</strong> one first mentioned. By <strong>the</strong>se means wehave two excited or charged conductors.1867. If, before charging <strong>the</strong>se conquerors, two scalps <strong>of</strong> hair be severallysituated on <strong>the</strong>m, it will be perceived that, as <strong>the</strong> charging proceeds,<strong>the</strong> hairs on each <strong>of</strong> <strong>the</strong> scalps rise, and endeavour to keep away from eacho<strong>the</strong>r. But, meanwhile, <strong>the</strong> whole <strong>of</strong> <strong>the</strong> hair on ei<strong>the</strong>r is attracted bythat on <strong>the</strong> o<strong>the</strong>r conductor.Moreover, on touching both conductors withany metallic rod, simultaneously, <strong>the</strong> whole <strong>of</strong> <strong>the</strong> excitement disappears,and <strong>the</strong> hairs assume <strong>the</strong>ir normal position.1868. In producing this discharge, iron is not more efi"ective than anyo<strong>the</strong>r metal. It is, in fact, known to be less competent for this species <strong>of</strong>conduction, than copper, silver,or gold.1869. When <strong>the</strong> conductors are excited <strong>the</strong>y have a powerful efi'ectupon gold leaves, suspended as in <strong>the</strong> electrometer.1870. The state <strong>of</strong> <strong>the</strong> conductors, when excited, as described here, issaid to be static. Such a state <strong>of</strong> excitement is distinguished as a staticalcharge <strong>of</strong> electricity.

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