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

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386 OF MATTER, MIND, AND SPIRIT.<strong>the</strong> axis, arc jerked out <strong>of</strong> <strong>the</strong> normal position with an inconceivable quickness,<strong>the</strong> discharge, however, not affecting successive parts <strong>of</strong> <strong>the</strong> lengthabsolutely at oucc, but successively; so that <strong>the</strong>re is a time required fur<strong>the</strong> process, however inconceivably minute it may appear to us. Theeffect upon <strong>the</strong> filaments <strong>of</strong> filings, at <strong>the</strong> different ends <strong>of</strong> <strong>the</strong> wire, areperfectly simultaneous, and <strong>the</strong> effect analogous, but different in this respect,that <strong>the</strong> positive poles are presented externally at one end, <strong>the</strong> negativeat <strong>the</strong> o<strong>the</strong>r, so that, when <strong>the</strong> polarizing affections meet at an intermediatepoint within <strong>the</strong> wire, neutrality ensues.1880. Thus it will be perceived that no current passes through <strong>the</strong>wire, any more than <strong>the</strong> water which is seen to form a w'ave, on one side<strong>of</strong> a lake, passes with <strong>the</strong> wave which is seen apparently to proceed to <strong>the</strong>o<strong>the</strong>r side. Notoriously, in this case, nothing passes but <strong>the</strong> momentum,which is successively imparted to successive portions <strong>of</strong> <strong>the</strong> interveningwater ;so, in <strong>the</strong> galvanic discharge, successive portions <strong>of</strong> <strong>the</strong> interveningwire are affected by <strong>the</strong> original disturbing jerks, <strong>of</strong> which <strong>the</strong> powerpasses from each portion to that next beyond it, just as <strong>the</strong> momentum in<strong>the</strong> case <strong>of</strong> <strong>the</strong> aqueous wave.1881. Upon <strong>the</strong>se considerations I hold myself as warranted in calling<strong>the</strong> affections <strong>of</strong> <strong>the</strong> wire, as described, leaves <strong>of</strong> polarization, not that <strong>the</strong>affection <strong>of</strong> <strong>the</strong> wire has <strong>the</strong> smallest similitude to that with which waterproduces waves, but that, in both cases, <strong>the</strong>re is a successive communication<strong>of</strong> a property. It is well known that <strong>the</strong>re is this analogy in <strong>the</strong> two cases;in ei<strong>the</strong>r, opposite waves, on due meeting, produce reciprocal neutrality.1882. The neutralization <strong>of</strong> <strong>the</strong> electro-polarity induced upon <strong>the</strong>charged conductors (1867) by touching both at <strong>the</strong> same time by a conductingrod, is effected in some degree analogously to <strong>the</strong> process in <strong>the</strong> voltaicdischarge ; since waves <strong>of</strong> opposite polarization are produced at each extremity,and, rushing toward an intermediate point, arc neutralized bymeeting. But <strong>the</strong> polarization in <strong>the</strong> case <strong>of</strong> <strong>the</strong> conductors, as has beenstated, (1874,) is superficial, and extends not only to <strong>the</strong> surfaces <strong>of</strong> <strong>the</strong>conductors, but likewise to <strong>the</strong> surrounding e<strong>the</strong>r and air, and does notlaffect <strong>the</strong> ponderable atoms <strong>of</strong> <strong>the</strong> wire unless <strong>the</strong> charge be too great topass in this superficial manner. In that case, being condensed upon <strong>the</strong>wire to a state <strong>of</strong> great intensity, it causes a polarization <strong>of</strong> <strong>the</strong> atomscomposing it,similar to that <strong>of</strong> <strong>the</strong> voltaic discharge, though less durable.1883. From <strong>the</strong> preceding exposition it follows that <strong>the</strong> conduction andinsulation <strong>of</strong> that species <strong>of</strong> electricity which is excited by an electricalmachine or o<strong>the</strong>r frictional processes, exists upon <strong>the</strong> superficies <strong>of</strong> insulatedmasses, or that <strong>of</strong> <strong>the</strong> circumambient particles <strong>of</strong> <strong>the</strong> air or e<strong>the</strong>r.This frictional electricity likewise passes preferably over <strong>the</strong> surfaces <strong>of</strong>conductors, so that <strong>the</strong> moistened surfiice <strong>of</strong> glass, or o<strong>the</strong>r non-conductors,conveys it with enormous facility. It is notorious, that when <strong>the</strong> air ismoist, electrical machines are paralyzed. But this cannot be in conse-

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