rrnts,; mm,- #\, '^S^ uJ-.-^ te9-§ r-r- ^^m3^ ^' ,# % ELECTRIC PHENOMENA. BY D-^ J. Rosenthal. BERLIN 1872. C. G. LUDERITZ'sche Verlagsbuchhandlung. CARL HABEL. 33 Wilhelm Strasse 33. LONDON, NEW-YORK, WILLIAMS & NORGATE ^' WESTERMANN & Co. GERMAN AND FOREIGN BOOKSELLERS 14 Henrietta Street, Covent Garden. 524 Broadway. ^<*|^ Libra/ry, J. HE greater the progress, wliicli Natural History makes in the knowledge of facts and their inner coherence, the more easy it is to understand those causes which lay the founda- tion of the facts. Whilst formerly, as an explanation for al- most every phenominal appearance, the existence of its own peculiar substance was admitted (for example "Caloric", which was considered as imponderous, or, still earHer, that so-caUed "Phlogiston", which is supposed to contain such a negative weight, that through its existence the other bodies which are connected with it, become much lighter) ; we now attain, more and more, the knowledge, that every phenomenon of Nature is to be traced back to the motions of the smallest particles of which all matter is composed. The phenomena on which I intend to discourse, are very remote from this notion. However minutely they may have been investigated separately, and whatever great results they may have led to in a practical sense, in order to explain them fully, it is necessary for us to make an assumption ("hypo- thesis" as it is called by men of science), for the accuracy of which we have no proof, and it is only devised for the pur- pose of concentrating the whole series of phenomena into a general point of view. The value of such suppositions con- 1872. IL 1. (125) A3 4 Quarterly German Magazine, sists principally in their use as a medium of instruction, and they can be abandoned as soon as they evince themselves as inefficient, or we can find more simple and therefore better ones. According to the supposition in question, there are two highly subtile, imponderable and elastic fluids, which are so refined, that we are not able to weigh them in the most ac- curate scales, but infer their existence from their effects. These fluids are called positive and negative electricity. Each has the quality to repel that body, which is impregnated with its own identical fluid, and on the other hand, to attract that 9 which possesses the opposite, and this attraction and repulsion take place in inverse ratio to the quadrat of the distance from one another; i. e., if two electrical fluids are twice or three times as far from one another, then their repulsive or attrac- tive influence is only of one fourth or one ninth of the power it would be, were a simple distance between them. These two fluids always exist, where solid substance is to be found, they cling to the smallest particles of matter, but nevertheless they are capable of passing from one molecule to the other in one and the same body, as well as from one body to another. Generally these two fluids are present in equal quantities in aU bodies, and the result thereof is, that they cannot exercise any sensible influence outwards. We then caU the bodies neutral-electric or non-electric. When, however, in a body one of the fluids is found in a larger quantity than the other, its stronger effect asserts itself and we call the body electric and indeed positive-electric^ if the positive fluid exists in excess, and negative-electric^ if the ne- gative fluid preponderates. Among the means, which effect such an unequal distri- (126; On Electric Phenomena. 5 Tbution of electric fluid, friction takes the first place. If we rub a stick of sealing-wax witli a piece of woollen cloth, and then touch with the sealing-wax a light little ball made of the pith of the elder-tree and suspended by a silken-thread, we shall find, that the ball is at first attracted by the sealing- wax, but as soon as it conies in contact with it, it is quickly repelled. It is evident, that this last repulsion can only be caused by the fact, that the stick of sealing-wax has imparted to the baU a small part of that electricity, which has been excited by friction, and that now the state of electricity in the sealing-wax and the little ball being similar, they reci- procally repulse each other. As the ball is very light and hangs quite free, the electric fluid carries with it the material particles to which it adheres, and thus, the repulsion, which takes place between the invisible electric fluids becomes per- ceptible to us through the movement of the visible substance. If we now rub a piece of glass and touch with it a second ball hung up in a similar manner, and of the same kind as the before-mentioned, we attain just the same result. The piece of glass becomes electric through friction; it also imparts to the baU through contact a portion of its electricity and the electricity of a similar kind contained in the glass and the ball, repulse one another. If we now bring the piece of glass in contact with the ball, which was first touched with the sealing-wax, it wiU be attracted by it, and likewise, the ball, which was first touched by the piece of glass, will be attracted by the seaHng-wax. "We conclude therefrom, that the electricity, which was excited in the glass and the sealing- wax, are of a different kiud, and we call that excited in the glass positive or vitreous electricity^ and that in the sealing- wax, negative or resinous electricity. Indeed, the electricity (127) 6 Quarterly German Magazine.' of all resins is (like sealing-wax) negative, when excited by- friction; and this phenomenon was first remarked in Amber., which belongs also to these resinous substances and the whole series of phenomena is called electricity from the Grecian name for amber (Elektron). If we bring the two balls together, the one which had been touched by the glass and the other by the sealing-wax, they will attract each other equally, as they are laden withj electricity of a similar kind; but at the moment of colHsioi they fall away from one another, and prove themselves non-electric. The two opposite states of electricity have united themselves and the balls contain again both electricities in equal quantities und are therefore non-electric. We win now rub against each other a piece of glass and a piece of ribbon which is tightly stretched out, and then touch the two balls, which have become non-electric, the one with the piece of glass, the other wi\h the piece of ribbon. Both appear again electric, and indeed, the ball touched by the glass will be repelled, while, on the other hand, it will be attracted by the ribbon. The case is just the contrary with the other baU. We then see, that both the bodies, which have been rubbed against one another, have become electrical, but that both receive an opposite state of electri- city. This proposition is always valid, when two bodies are rubbed together, and w^e leam from it, that no electricity can j he excited by friction^ but that only an ulterior distHbution qf^ both the electric fluids takes jilace, so that in the one a 5wr- • plus of positive electricity is accumulated^ and in the other of \ negative. If we rub a rod of metal, which we hold in the hand, with wool, we cannot prove, that there exists the slightest (123) On Electric Phenomena. 7 face of electricity in it. If we, however, fasten the rod to handle of glass or sealing-wax, or if we WTap the part of which we take hold in silk, and then rub it, it will become strongly electrical, and we can observe all the same pheno- mena which we learned from the piece of glass or the sealiag- T^ax. As soon as we touch any part of it with the hand, then all electricity immediately vanishes from it. If we continue to rub a piece of sealing-wax or a glass rod at one end, and then test another part, wliich has not been rubbed, with the ball of pith, we shall find them quite non-electric. On the