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Nikola Tesla - Free-Energy Devices

Nikola Tesla - Free-Energy Devices

Nikola Tesla - Free-Energy Devices

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384 INVENTIONS OF NIKOLA TE8LA.may remain lighted if the plate be interposed, or may even increasein luminosity. The effect depends on the position of theplate and tube relatively to the coil, and may be always easilyforetold by assuming that conduction takes place from one terminalof the coil to the other. According to the position of theplate, it mayeither divert from or direct the current to the tube.In another line of work the writer has in frequent experimentsmaintained incandescent lamps of 50 or 100 volts burning at anydesired candle power with both the terminals of each lamp connectedto a stout copper wire of no more than a few feet inlength. These experiments seem interesting enough, but theyare not more so than the queer experiment of Faraday, whichhas been revived and made much of by recent investigators, andin which a discharge is made to jump between two points of abent copper wire. An experiment may be cited here which mayseem equally interesting. If a Geissler tube, the terminals ofwhich are joined by a copper wire, be approached to the coil, certainlyno one would be prepared to see the tube light up.Curiously enough, it does light up, and, what ismore, thewire does not seem to make much difference. Now one isapt to think in the first moment that the impedance of thewire might have something to do with the phenomenon. Butthis is of course immediately rejected, as for this an enormousfrequency would be required. This result, however, seemspuzzling only at h'rst for ; upon reflection it is quite clear thatthe wire can make but little difference. Itmay be explained inmore than one way, but it agrees perhaps best with observationto assume that conduction takes place from the terminals of thecoil through the space. On this assumption, if the tube with thewire be held in any position, the wire can divert little more thanthe current which passes through the space occupied by the wireand the metallic terminals of the tube ; through the adjacentspace the current passes practically undisturbed. For this reason,if the tube be held in any position at right anglesto the linejoining the binding posts of the coil, the wire makes hardly anydifference, but in a position more or less parallel with that lineit impairs to a certain extent the brilliancy of the tube and itsfacility to light up. Numerous other phenomena may be explainedon the same assumption. For instance, if the ends of thetube be provided with washers of sufficient size and held in theline joining the terminals of the coil, it will not light up, andthen nearly the whole of the current, which would otherwise

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