Hertzian Wave Wireless TelegraphyFleming, J. A. (John Ambrose), Sir
Science
Hertzian Wave Wireless Telegraphy
Fleming, J. A. (John Ambrose), Sir
Electric waves; Telegraph, Wireless
The number 3×10^{10} is the value in centimetres per second of the
velocity of the electromagnetic wave, and is identical with that of
light. The corresponding resonant length of the aerial is therefore
one-fourth of this wave-length, or 3×10^{10}/4N. Generally speaking,
however, it will be found that with any length of aerial which is
practicable, say, 200 feet or 6,000 cms., this proportion necessitates
rather a high frequency in the primary oscillation circuit. In the
case considered--viz., for an aerial 200 feet in height--the
oscillations in the primary circuit must have a frequency of one and a
quarter million. This high frequency can only be obtained either by
greatly reducing the inductance of the primary discharge circuit, or
reducing the capacity. If we reduce the capacity, we thereby greatly
reduce the storage of energy, and it is not practicable to reduce the
inductance below a certain amount.
[Illustration: FIG. 14.--BRAUN'S RADIATOR. B, battery; I, induction
coil; K, key; S, spark-gap; L, inductance coil; C, condenser; A,
aerial.]
Summing up, it may be said that there are three, and, as far as the
writer is aware, at present only three, modes of exciting the
electrical oscillations in an aerial wire. First, the aerial may
itself be used as an electrical reservoir and charged to a high
potential and suddenly discharged to the earth. This is the original
Marconi method. The second method, due to Braun, consist of attaching
the aerial to some point on an oscillation circuit consisting of a
condenser, an inductance coil and a spark gap, in series with one
another, and charging and discharging the condenser across the spark
gap so as to create alterations of potential at some point on the
oscillation circuit. The length of the aerial must then be so
proportioned as above described that it is resonant to this frequency.
Thirdly, we may employ the arrangement involving an oscillation
transformer, in which the oscillations in the primary condenser
circuit are made to induce others in the aerial circuit, the
time-period of the two circuits being the same. This method may be
called the Braun-Marconi method. Professor Slaby has combined together
in a certain way the original Marconi simple aerial with the resonant
quarter-wave-length wire of Braun. He constructs what he calls a
_multiplicator_, which is really a wire wound into a loose spiral
connected at one point to an oscillation circuit consisting of a
condenser inductance, the length of this wire being proportioned so
that there is a great resonance or multiplication of tension or
potential at its free end. This free end is then attached to the lower
end of an ordinary Marconi aerial, and serves to charge it with a
higher potential than could be obtained by the use of the induction
coil directly attached to it.
* * * * *
Public-domain text, read in full here on John Shaqi.
Reviews
Reviews
No reviews yet
Be the first to share your thoughts on this work.
Join the Discussion
Join the discussion
Sign in to leave a comment or review.
Sign InorCreate an account