Page:United States patent 645576.pdf/5

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645,576

from two hundred and thirty thousand to two hundred and fifty thousand times per second. The high-tension coil A in the form of a fiat spiral was composed of fifty turns of heavily 380insulated cable No. 8 wound in one single layer, the turns beginning close to the primary loop and ending near its center. The outer end of the secondary or high-tension coil A was connected to the ground, as 385illustrated, while the free end was led to a terminal placed in the rarefied air stratum through which the energy was to be transmitted, which was contained in an insulating-tube of a length of fifty feet or more, within which a 390barometric pressure varying from about one hundred and twenty to one hundred and fifty millimeters was maintained by means of a mechanical suction-pump. The receiving transformer was similarly proportioned, the 395ratio of conversion being the reciprocal of that of the transmitter, and the primary high-tension coil A′ was connected, as illustrated, with the end near the low-tension coil C′ to the ground and with the free end to a wire 400or plate likewise placed in the rarefied air stratum and at the distance named from the transmitting-terminal. The primary and secondary circuits in the transmitting apparatus being carefully synchronized, an electromotive405 force from two to four million volts and more was obtainable at the terminals of the secondary coil A, the discharge passing freely through the attenuated air stratum maintained at the above barometric pressures, and 410it was easy under these conditions to transmit with fair economy considerable amounts of energy, such as are of industrial moment, to the receiving apparatus for supplying from the secondary coil C′ lamps L or kindred 415devices. The results were particularly satisfactory when the primary coil or system A′, with its secondary C′, was carefully adjusted, so as to vibrate in synchronism with the transmitting coil or system A C. I have, 420however, found no difficulty in producing with apparatus of substantially the same design and construction electromotive forces exceeding three or four times those before mentioned and have ascertained that by their 425means current impulses can be transmitted through much denser air strata. By the use of these I have also found it practicable to transmit notable amounts of energy through air strata not in direct contact with the 430transmitting and receiving terminals, but remote from them, the action of the impulses, in rendering conducting air of a density at which it normally behaves as an insulator, extending, as before remarked, to a considerable 435distance. The high electromotive force obtained at the terminals of coil or conductor A was, as will be seen, in the preceding instance, not so much due to a large ratio of transformation as to the joint effect of the 440capacities and inductances in the synchronized circuits, which effect is enhanced by a high frequency, and it will be obviously understood that if the latter be reduced a greater ratio of transformation should be resorted to, especially in cases in which it may be deemed445 of advantage to suppress as much as possible, and particularly in the transmitting-coil A, the rise of pressure due to the above effect and to obtain the necessary electromotive force solely by a large transformation ratio.450

While electromotive forces such as are produced by the apparatus just described may be sufficient for many purposes to which my system will or may be applied, I wish to state that I contemplate using in an industrial 455undertaking of this kind forces greatly in excess of these, and with my present knowledge and experience in this novel field I would estimate them to range from twenty to fifty million volts and possibly more. By the use460 of these much greater forces larger amounts of energy may be conveyed through the atmosphere to remote places or regions, and the distance of transmission may be thus extended practically without limit.465

As to the elevation of the terminals D D′ it is obvious that it will be determined by a number of things, as by the amount and quality of the work to be performed, but the local density and other conditions of the atmosphere,470 by the character of the surrounding country, and such considerations as may present themselves in individual instances. Thus if there by high mountains in the vicinity the terminals should be at a greater475 height, and generally they should always be, if practicable, at altitudes much greater than those of the highest objects near them in order to avoid as much as possible the loss by leakage. In some cases when small amounts480 of energy are required to the high elevation of the terminals, and more particularly of the receiving-terminal D′, may not be necessary, since especially when the frequency of the currents is very high, a sufficient amount485 of energy may be collected at that terminal by electrostatic induction from the upper air strata, which are rendered conducting by the active terminal of the transmitter or through which the currents from the same are 490conveyed.

With reference to the facts which have been pointed out above it will be seen that the altitudes required for the transmission of considerable amounts of electrical energy in 495accordance with this method are such as are easily accessible and at which terminals can be safely maintained, as by the aid of captive balloons supplied continuously with gas from reservoirs and held in position securely500 by steel wires or by any other means, devices, or expedients, such as may be contrived and perfected by ingenious and skilled engineers. From my experiments and observations I conclude that with electromotive impulses505 not greatly exceeding fifteen or twenty million volts the energy of many thousands of horse-power may be transmitted over vast distances, measured by many hundreds and510