Hertzian Wave Wireless TelegraphyFleming, J. A. (John Ambrose), Sir
Science
Hertzian Wave Wireless Telegraphy
Fleming, J. A. (John Ambrose), Sir
Electric waves; Telegraph, Wireless
capacity, but that which is stored up in the much larger capacity
represented by the primary condenser or, as it may be called, the
electrical wind chest. By the second arrangement we have therefore the
means of radiating more or less continuous trains of electric waves,
corresponding with each spark discharge. To create powerful
oscillations in the aerial, one condition of success is that there
shall be an identity in time-period between the circuit of the aerial
and that of the primary condenser. The aerial is an open circuit which
has capacity with respect to the earth, and it has also inductance,
partly due to the wire of the aerial and partly due to the secondary
circuit of the oscillation transformer in series with it. The primary
circuit or spark circuit has capacity--viz., the capacity of the
energy-storing condenser--and it has also inductance--viz., the
inductance of the primary circuit of the oscillation transformer. We
shall consider at a later stage more particularly the details of
syntonising arrangements, but meanwhile it may be said that one
condition for setting up powerful waves by means of the above
arrangement is that the electrical time-period of both the two
circuits mentioned shall be the same. This involves adjusting the
inductance and capacity so that the product of conductance and
capacity for each of these two circuits is numerically the same.
Instead of employing an oscillation transformer between the condenser
circuit and the aerial, the aerial may be connected directly to some
point on the condenser circuit at which the potential oscillations are
large, and we have then another arrangement devised by Professor Braun
(see Fig. 14). In this case, in order to accumulate large potential
oscillations at the top of the aerial, it is, as we have seen,
necessary that the length of the aerial shall be one quarter the
length of the wave. If, therefore, the electrical oscillations in the
condenser circuit are at the rate of N per second, in other words,
have a frequency N, the wave-length correponding to this frequency is
given by the expression,
3×10^{10}/N cms.
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