Hertzian Wave Wireless TelegraphyFleming, J. A. (John Ambrose), Sir
Science
Hertzian Wave Wireless Telegraphy
Fleming, J. A. (John Ambrose), Sir
Electric waves; Telegraph, Wireless
Nothing is more remarkable, however, than the small amount of energy
which, if properly utilised in electric wave making, will suffice to
influence a sensitive receiver at a distance of even one or two
hundred miles. Suppose, for instance, that we charge a condenser
consisting of a battery of Leyden jars, having a capacity of one
seventy-fifth of a microfarad, to a potential of 15,000 volts; the
energy stored up in this condenser is then equal to 1·5 joules, or a
little more than one foot-pound. If this energy is discharged in the
form of a spark five millimetres in length through the primary coil of
an oscillation transformer, associated with an aerial 150 feet in
height, the circuits being properly tuned by Mr. Marconi's method,
then such an aerial will affect, as he has shown, one of Mr. Marconi's
receivers, including a nickel silver filings coherer tube, at a
distance of over two hundred miles over sea. Consider what this means.
The energy stored up in the Leyden jars cannot all be radiated as wave
energy by the aerial, probably only half of it is thus radiated. Hence
the impartation to the ether at any one locality of about half a
foot-pound of energy in the form of a long Hertzian wave is sufficient
to affect sensitive receivers situated at any point on the
circumference of a circle of 200 miles radius described on the open
sea. Hertzian wave telegraphy is sometimes described as being
extravagant in power, but, as a matter of fact, the most remarkable
thing about it is the small amount of power really involved in
conducting it. On the other hand, Hertzian wave manufacture is not
altogether a matter of power. It is much more dependent upon the
manner in which the ether is struck. Just as half an ounce of dynamite
in exploding may make more noise than a ton of gunpowder, because it
hits the air more suddenly, so the formation of an effective wave in
the ether is better achieved by the right application of a small
energy than by the wrong mode of application of a much larger amount.
If we translate this fact into the language of electronic theory, it
amounts simply to this. It is the electron alone which has a grip of
the ether. To create an ether wave, we have to start or stop crowds of
electrons very suddenly. If in motion, their motion implies energy,
but it is not only their energy which is concerned in the wave making,
but the acceleration, positive or negative--_i.e._, the quickness with
which they are started or stopped. It is possible we may discover in
time a way of manufacturing long ether waves without the use of an
electric spark, but at present we know only one way of doing
this--viz., by the discharge of a condenser, and in the discharge of
large condensers of very high potentials it is difficult to secure
that extreme suddenness of starting the discharge which we can do in
the case of smaller capacities and voltages.
Public-domain text, read in full here on John Shaqi.
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