Weagant's Anti-Static Invention. The Wireless Age, April 1999 by Elmer E. Bucher
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The Wireless Age
April 1919 

Pages 11 - 20
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18                                                            THE WIRELESS AGE                                              April, 1919
could the static currents be balanced, and also, the converse.
     One experiment, seemingly supporting this erroneous belief, made use of a far distant loop, connected to the
tween the ground and the horizontal aerial is increased, its action becomes more nearly that of an ordinary antenna ; and that, because it is then not in the most effective position relative to the incoming signal to collect the
receiving apparatus through long low horizontal leads, and another loop with short leads erected at the receiving station, as in figure 9.  This arrangement was found for the time being to give somewhat better results than that in figure 6, and the improvement was found to result from the more perfect balance thus secured, in spite of the loss of signal.
     However, as mentioned above, it was discovered later that the horizontal leads of the two loops as in figure 6, picked up some of the static and signal energy and, as a result, the static currents in a set of leads and in the loop tended to flow in the same or opposite direction.  Adjustments that were made in the circuit shown in figure 6, to balance out static currents in the loop, before this fact was recognized, caused the static currents in the leads under some circumstances to add; but the simple expedient of placing reversing switches in the circuits solved the problem.
     The results thereafter obtained with the Weagant system were found to be better with the use of greater rather than less effective separation, by an amount proportional to the separation.
     It was observed that, in all arrangements employing two closed circuit loops connected to a central receiving station by long horizontal leads, local tuning of each loop was necessary.  This was not a very convenient procedure with aerials .3 miles apart, for it became necessary to station an operator at each loop and to inform him, by telephone, what adjustments were to be made.

UNDERGROUND AND SURFACE-GROUND HORIZONTAL
AERIALS

     The low horizontal aerial for radio reception was first used by Marconi.  An antenna of the same type employed by Weagant in the spring of 1914, at New Orleans, gave a distinctly better signal to static ratio, than the large earthed aerial. Later comparisons with a loop aerial showed the two to be substantially identical in that respect.
      One important deduction resulting from these tests was the fact that the long horizontal aerials laid under ground, on the surface of the ground, or suspended above the ground, may act as a loop aerial.  Because of the capacity to earth (as shown diagrammatically in figure 10) a return path for the currents exists between the ends, which effectively completes the circuit.
     It has, been noted particularly that, as the distance be-

maximum of energy, the signals are less in strength than would be secured with less spacing.
     Quoting Mr. Weagant
     "The usually accepted explanation of the working of the horizontal aerial is that the wave front of the signal wave is tilted forward and that consequently there is a component of electric force in the direction of its length.  It is to be noted, however, that under some circumstances such an aerial may be acting equally well as a loop.  An aerial of this type is shown, in figure 10, lying on the

surface of the ground and it is evident that by virtue of its capacity to the true conducting earth, a return path between its ends exists and, therefore, it is a form of loop; which method of consideration will account for many of the observed facts, such as its directivity, in a satisfactory way.  It will also account for one observed fact which the usual methods of explanation do not account for, namely, that when an aerial of this type is laid on the ground, or buried underneath it, its effectiveness as an aerial does not increase indefinitely with length, but rapidly reaches an optimum value dependent on the cir-cumstances obtaining.  This can readily be accounted for under the present hypothesis by the fact that as, the length


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