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

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APPENDIX. 449superficially from ono to tlio o<strong>the</strong>r, parallel to <strong>the</strong> axis <strong>of</strong> <strong>the</strong> includediron, instead <strong>of</strong> pursuing <strong>the</strong> circuitous channel afforded by <strong>the</strong> helix with<strong>the</strong> intensity requisite to <strong>the</strong> polarization <strong>of</strong> <strong>the</strong> ponderable atoms.The extreme Dircrsttjj, ast rcsj)ccts strikiiKj Distance, hctween <strong>the</strong> directEffects <strong>of</strong> Frictional Electricity and those directly arisinj from GalvanicReaction.46. The intensity <strong>of</strong> <strong>the</strong> excitement produced by different electricalmachines is estimated to be as <strong>the</strong> relative lengths <strong>of</strong> <strong>the</strong> sparks whichproceed from <strong>the</strong>ir prime conductors respectively. Admitting that <strong>the</strong>relative intensity were merely as <strong>the</strong> length <strong>of</strong> <strong>the</strong> spark, not as <strong>the</strong> square<strong>of</strong> that length, still <strong>the</strong>re would be an infinite difference between <strong>the</strong> intensity<strong>of</strong> a voltaic scries and that <strong>of</strong> electrical machines, if measured bythis test. Large electrical machines, like that at <strong>the</strong> Polytechnic Institution,London, give sparks at twenty inches and more ; while, agreeably toGassiott's experiments, a Grovcs's battery <strong>of</strong> 320 pairs, in full power, wouldnot, before contact, give a spark at any distance, however minute. Itfollows, that, as respects <strong>the</strong> species <strong>of</strong> intensity which is indicated bylength <strong>of</strong> sparks, or striking distance, <strong>the</strong> diflFerence between <strong>the</strong> electricity<strong>of</strong> <strong>the</strong> most powerful voltaic series and electrical machines is not to berepresented by any degree <strong>of</strong> disjmrify; it proves that galvanism properand electricity proper arc heterogeneous.47. It should be recollected that <strong>the</strong> intensity <strong>of</strong> galvanic action in aseries <strong>of</strong> 320 pairs, excepting <strong>the</strong> loss from conduction, would be to that<strong>of</strong> one pair as 320 to 1.* Of course, <strong>the</strong> striking distance <strong>of</strong> a battery<strong>of</strong> one pair would be 320 times less than nothing : 320 below zero.48. We may infer that <strong>the</strong> undulatory polarization <strong>of</strong> e<strong>the</strong>reo-ponderablematter is <strong>the</strong> primary, direct, and characteristic effect<strong>of</strong> galvanic excitement,in its more energetic modifications. Yet, that by peculiar carein securing insulation, as in <strong>the</strong> water batteries <strong>of</strong> Cross and Gassiott,e<strong>the</strong>real undulations may be produced, with <strong>the</strong> consequent accumulation<strong>of</strong> e<strong>the</strong>real polarity requisite to give sparks before contact, agreeably to <strong>the</strong>experiments <strong>of</strong> those ingenious philosophers.49. Hence it may be presumed that, during intense e<strong>the</strong>reo-ponderablepolarization, superficial e<strong>the</strong>real waves may always be a secondary effect,although <strong>the</strong> conducting power <strong>of</strong> <strong>the</strong> reagents, requisite to <strong>the</strong> constitution<strong>of</strong> powerful galvanic batteries, is inconsistent with that accumulation<strong>of</strong> e<strong>the</strong>real polarity which constitutes a statical spark-giving charge.50. As all <strong>the</strong> members forming a voltaic series have to be discharged* According to Colomb's experiments, electrical attraction and repulsion arc invcrselj'as <strong>the</strong> squares <strong>of</strong> <strong>the</strong> distances: ought not <strong>the</strong> inductive power <strong>of</strong> statical charges whichis produced by those forces, and which precedes and determines <strong>the</strong> length <strong>of</strong> <strong>the</strong> resultingspark, to obey <strong>the</strong> same law ?If this calculation be correct, <strong>the</strong> intensity must be as <strong>the</strong> squares <strong>of</strong> <strong>the</strong> striking distances,as indicated by sparks.It may be urged that <strong>the</strong> striking distances, as measured by <strong>the</strong> length <strong>of</strong> <strong>the</strong> sparks,is in <strong>the</strong> compound ratio <strong>of</strong> <strong>the</strong> quantity and intensity. As to <strong>the</strong> quantity, however,galvanic sources have always been treated as pre-eminent in efficacy, so that on that side<strong>the</strong>re could be no disparity. Moreover, I have found, that in galvanic apparatus <strong>of</strong> onlyone, or even <strong>of</strong> two pairs, as in <strong>the</strong> calorimotors, <strong>the</strong> intensity lessened as <strong>the</strong> surfaceswere enlarged. IJy a pair <strong>of</strong> fifty square feet <strong>of</strong> zinc surface, a white heat could not beproduced in a wire <strong>of</strong> any size, however small. The calorific power <strong>of</strong> such apparatuscan only be made evident by <strong>the</strong> production <strong>of</strong> a comparatively very low temperature, ina comparatively very large mass.29

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