circuit. This was the fundamental working hypothesis
on which the Weagant system is based.
A series of experiments to verify
the hypothesis then followed.
OBSERVATIONS ON TWO LOOPS, THE PLANES
OF WHICH
ARE PERPENDICULAR
For one thing it was found that two
loops, the planes of which were perpendicular, were connected to a common
receiving apparatus, as in figure 5, the static currents could not be
balanced out. The experiment justified the assumption that
electromagnetic
waves responsible for static currents are heterogeneously polarized; that
is, tha axes of the oscillators producing them assumed all possible angles
in space; and the highly damped waves resulting therefrom are propagated
in a direction perpendicular to the earth's surface.
In other words, to the unscientific
mind, these static waves may be described as an electric shower which acts
upon an aerial, perpendicular to the earth. |
AN EARLY FORM OF WEAGANT'S STATIC
ELIMINATOR
To determine the correctness
of the hypothesis that static is propagated vertically and to ascertain
if it were possible on this assumption to devise a system whereby the static
currents could be balanced out while the signal was retained, Mr. Weagant
erected at Belmar, N. J., the aerials and apparatus shown in figure 6.
Two closed loops A and B, each consisting of a single turn of wire 400
feet high with a base line of 1,000 feet, were spaced 5,000 feet from center
to center. Two wires, brought from each loop to a receiving station
located at the center, were supported on ten-foot poles, 6 feet apart.
These leads were connected to the primary coils of a goniometer of the
type used in direction finders ; the secondary coil was connected to a
sensitive oscillation detector. It was this apparatus that permitted
the reception of transatlantic signals through static interference of great
intensity, whereas without it, it was impossible to distinguish the wireless
signal.
The connections to the receiving
tuner and detector are shown .in figure 6, where loop A has the loading
coils L-1 and L-2, the resistances R-1 and R-2, and the coil,
 |