PROFESSOR OF ELECTRICAL ENGINEERING, UNIVERSITY COLLEGE, LONDON.

The immense public interest which has been aroused of late years in

the subject of telegraphy without connecting wires has undoubtedly

been stimulated by the achievements of Mr. Marconi in effecting

communication over great distances by means of Hertzian waves. The

periodicals and daily journals, which are the chief avenues through

which information reaches the public, whilst eager to describe in a

sensational manner these wonderful applications of electrical

principles, have done little to convey an intelligible explanation of

them. Hence it appeared probable that a service would be rendered by

an endeavour to present an account of the present condition of

electric wave telegraphy in a manner acceptable to those unversed in

the advanced technicalities of the subject, but acquainted at least

with the elements of electrical science. It is the purpose of these

articles to attempt this task. We shall, however, limit the discussion

to an account of the scientific principles underlying the operation of

this particular form of wireless telegraphy, omitting, as far as

possible, references to mere questions of priority and development.

The practical problem of electric wave wireless telegraphy, which has

been variously called Hertzian wave telegraphy, Marconi telegraphy, or

spark telegraphy (_Funkentelegraphie_), is that of the production of

an effect called an electric wave or train of electric waves, which

can be sent out from one place, controlled, detected at another place,

and interpreted into an alphabetic code. Up to the present time, the

chief part of that intercommunication has been effected by means of

the Morse code, in which a group of long and short signs form the

letter or symbol. Some attempts have been made with more or less

success to work printing telegraphs and even writing or drawing

telegraphs by Hertzian waves, but have not passed beyond the

experimental stage, whilst wireless telephony by this means is still a

dream of the future.

We shall, in the first place, consider the transmitting arrangements

and, incidentally, the nature of the effect or wave transmitted; in

the second place, the receiving appliances; and, finally, discuss the

problem of the isolation or secrecy of the intelligence conveyed

between any two places.

The transmitter used in Hertzian wave telegraphy consists essentially

of a device for producing electric waves of a type which will travel

over the surface of the land or sea without speedy dissipation, and

the important element in this arrangement is the _radiator_, by which

these waves are sent out. It will be an advantage to begin by

explaining the electrical action of the radiator, and then proceed to

discuss the details of the transmitting appliances.

It will probably assist the reader to arrive most easily at a general

idea of the functions of the various portions of the transmitting

arrangements, and in particular of the radiator, if we take as our

starting point an analogy which exists between electric wave

generation for telegraphic purposes and air wave generation for sound

signal purposes. Most persons have visited some of the large

lighthouses which exist around our coasts and have there seen a steam

or air _siren_, as used for the production of sound signals during

fogs. If they have examined this appliance, they will know that it

consists, in the first place, of a long metal tube, generally with a

trumpet-shaped mouthpiece. At the bottom of this tube there is a fixed

plate with holes in it, against which revolves another similarly

perforated plate. These two plates separate a back chamber or wind

chest from the tube, and the wind chest communicates with a reservoir

of compressed air or a high-pressure steam boiler. In the

communication pipe there is a valve which can be suddenly opened for a

longer or shorter time. When the movable plate revolves, the

coincidence or non-coincidence of the holes in the two plates opens or

shuts the air passage way very rapidly. Hence when the blast of air or

steam is turned on, the flow is cut up by the revolving plates into a

series of puffs which inflict blows upon the stationary air in the

siren tube. If these blows come at the rate, say, of a hundred a

second, they give rise to aerial oscillations in the tube, which

impress the ear as a deep, musical note or roar; and this continuous

sound can be cut up by closing the valve intermittently into long and

short periods, and so caused to signal a letter according to the Morse

code, denoting the name of the lighthouse. In this case the object is

to produce: first, aerial vibrations in the tube, giving rise to a

train of powerful air waves; secondly, to intermit this wave-train so

as to produce an intelligible signal; and thirdly, to transmit this

wave as far as possible through space.

The production of a sound or air wave can only be achieved by

administering a very sudden blow to the general mass of the air in the

tube. This impulse must be sufficient to call into operation the

inertia and elastic qualities of the air. It is found, moreover, that

the amplitude of the resulting wave, or the loudness of the sound, is

increased by suitably proportioning the length of the siren pipe and

the frequency of the air puffs; whilst the distance at which it is

heard depends also in some degree upon the form of the mouthpiece.

Inside the siren tube, when it is in operation, the air molecules are

in rapid vibratory motion in the direction of the length of the tube.

If we could at any one instant examine the distribution and changes of

air pressure in the tube, we should find that at some places there are

large, and at others small, variations in air pressure. These latter

places are called the _nodes_ of pressure. At the pressure nodes,

however, we should find large variations in the velocity of the air

particles, and these points are called the _antinodes_ of velocity. In

those places at which the pressure variation is greatest, the velocity

changes are least, and _vice versa_. Outside the tube, as a result of

these air motions in it, we have a hemispherical air wave produced,

which travels out from the mouthpiece as a centre; and if we could

examine the distribution of air pressure and velocity through all

external space, we should find a distribution which is periodic in

space as well as time, constituting the familiar phenomenon of an air

wave.

Turning then to consider the production of an electric, instead of an

air wave, we notice in the first place that the medium with which we

are concerned is the _ether_ filling all space. This ether permits the

production of physical changes in it which are analogous to, but not

identical in nature with, the pressures and movements which constitute

a sound wave. The Hertzian radiator is an appliance for acting on the

ether as the siren acts on the air. It produces a wave in it, and it

can be shown that all the parts of the above described siren apparatus

have their electrical equivalents in the transmitter employed in

Hertzian wave wireless telegraphy.

To understand the nature of an electric wave we must consider, in the

first place, some properties of the ether. In this medium we can at

any place produce a state called _electric displacement_ or _ether

strain_ as we can produce compression or rarefaction in air; and, just

as the latter changes are said to be created by mechanical force, so

the former is said to be due to _electric force_. We can not define

more clearly the nature of this ether strain or displacement until we

know much more about the structure of the ether than we do at present.

We can picture to ourselves the operation of compressing air as an

approximation of the air molecules, but the difficulty of

comprehending the nature of an electric wave arises from the fact that

we cannot yet definitely resolve the notion of electric strain into

any simpler or more familiar ideas.

We have to be content, therefore, to disguise our present ignorance by

the use of some descriptive term, such as _electric strain_,

_electrostatic strain_ or _ether strain_, to describe the directed

condition of the space around a body in a state of electrification

which is produced by electric force. This electric strain is certainly

not of the nature of a compression in the ether, but much more akin to

a twist or rotational strain in a solid body.

For our present purpose it is not so necessary to postulate any

particular theory of the ether as it is to possess some consistent

hypothesis, in terms of which we can describe the phenomena which

will concern us. These effects are, as we shall see, partly states of

electrification on the surface or distributions of electric current in

wires or rods, and partly conditions in the space outside them, which

we are led to recognise as distributions of electric strain and of an

associated effect called _magnetic flux_.

We find such a theory at hand at the present time in the electronic

theory of electricity, which has now been sufficiently developed and

popularised to make it useful as a descriptive hypothesis.[2] This

theory has the great recommendation that it offers a means of

abolishing the perplexing dualism of ether and ponderable matter, and

gives a definite and, in a sense, objective meaning to the word

electricity. In this physical speculation, the chief subject of

contemplation is the electron, or ultimate particle of negative

electricity, which, when associated in greater or less number with a

matrix of some description, forms the atom of ponderable matter. To

avoid further hypothesis, this matrix may be called the _co-electron_;

and we shall adopt the view that a single chemical atom is a union of

a _co-electron_ with a surrounding envelope or group of electrons, one

or more of the latter being detachable. We need not stop to speculate

on the structure of the atomic core or co-electron, whether it is

composed of positive and negative electrons or of something entirely

different. The single electron is the indivisible unit or atomic

element of so-called negative electricity, and the neutral chemical

atom deprived of one electron is the unit of positive electricity. On

this hypothesis, the chemical atom is to be regarded as a microcosm, a

sort of a solar system in miniature, the component electrons being

capable of vibration relatively to the atomic centre of mass.

Furthermore, from this point of view it is the electron which is the

effective cause of radiation. It alone has a grip on the ether whereby

it is able to establish wave motion in the latter.

Dr. Larmor has developed in considerable detail an hypothesis of the

nature of an electron which makes it the centre or convergence-point

of lines of a self-locked ether strain of a torsional type. The notion

of an atom merely as a "centre of force" was one familiar to Faraday

and much supported by Boscovich and others. The fatal objection to the

validity of this notion as originally stated was that it offers no

possibility of explaining the inertia of matter. On the electronic

hypothesis, the source of all inertia is the inertia of the ether, and

until we are able to dissect this last quality into anything simpler

than the time-element involved in the production of an ether strain or

displacement, we must accept it as an ultimate fact, not more

elucidated because we speak of it as the inductance of the electron.

We postulate, therefore, the following ideas: We have to think of the

ether as a homogeneous medium in which a strain of some kind, most

probably of a rotational type, is possible. This strain appears only

under the influence of an appropriate stress called the electric

force, and disappears when the force is removed. Hence to create this

strain necessitates the expenditure of energy. An electron is a

centre or convergence-point of lines of permanent ether strain of such

nature that it cannot release itself. To obtain some idea of the

nature of such a structure, let us imagine a flat steel band formed

into a ring by welding the ends together. There is then no torsional

strain. If, however, we suppose the band cut in one place, one end

then given half a turn and the cut ends again welded, we shall have on

the band a self-locked twist, which can be displaced on the band, but

which can not release itself or be released except by cutting the

ring. Hence we see that to make an electron in an ether possessing

torsional elasticity would require creative energy, and when made, the

electron cannot destroy itself except by occupying simultaneously the

same place as an electron of opposite type. Every electron extends,

therefore, as Faraday said of the atom, throughout the universe, and

the properties that we find in the electron are only there because

they are first in the universal medium, the ether. Every line of ether

or electric strain must, therefore, be a self-closed line, or else it

must terminate on an electron and a co-electron.

So far we have only considered the electron at rest. If, however, it

moves, it can be mathematically demonstrated that it must give rise to

a second form of ether strain which is related to the electric strain

as a twist is related to a thrust or a vortex ring to a squirt in

liquid or a rotation to a linear progression. The ether strain which

results from the lateral movement of lines of electric strain is

called the _magnetic flux_, and it can be mathematically shown that

the movement of an electron, consisting when a rest of a radial

convergence of lines of electric strain, must be accompanied by the

production of self-closed lines of magnetic flux, distributed in

concentric circles or rings round it, the planes of these circles

being perpendicular to the direction of motion of the electron.

This electronic hypothesis, therefore, affords a basis on which we can

build up a theory affording an explanation of the nature of the

intimate connection known to exist between ether, matter and

electricity. The electron is the connecting link between them all, for

it is in itself a centre of convergent ether strain; isolated, it

presents itself as electricity of the negative or resinous kind; and,

in combination with co-electrons and other electrons, it forms the

atoms of ponderable matter. At rest the electron or the co-electron

constitutes an electric charge, and when in motion it is an electric

current. A steady flux or drift of electrons in one direction and

co-electrons in the opposite direction is a continuous electric

current, whilst their mere oscillation about a mean position is an

alternating current. Furthermore, the vibration of an electron, if

sufficiently rapid, enables it to establish what are called electric

waves in the ether, but which are really detached and self-closed

lines of ether strain distributed in a periodic manner through space.

We have, therefore, to start with, three conceptions concerning the

electron, viz.: Its condition when at rest; its state when in uniform

motion; and its operations when in vibration or rapid oscillation. In

the first case, by our fundamental supposition, it consists of lines

of ether strain of a type called the electric strain, radiating

uniformly in all directions. When in uniform motion, it can be shown

that these lines of electric strain tend to group themselves in a

plane perpendicular to the line of motion drawn through the electron,

and their lateral motion generates another class of strain called the

magnetic strain, disposed in concentric circles described round the

electron and lying in this equatorial plane.

The proof of the above propositions cannot be given verbally, but

requires the aid of mathematical analysis of an advanced kind. The

reader must be referred for the complete demonstration to the writings

of Professor J. J. Thomson[3] and Mr. Oliver Heaviside.[4]

In the third case, when the electron vibrates, we have a state in

which self-closed lines of electric strain and magnetic flux are

thrown off and move away through the ether constituting electric

radiation, The manner in which this happens was first described by

Hertz in a Paper on "Electric Oscillations treated according to the

Method of Maxwell."[5] As this phenomenon lies at the very root of

Hertzian wave wireless telegraphy, we must spend a moment or two in

its careful examination.

Let us imagine two metal rods placed in line and constituting what is

called a linear oscillator. Let these rods have adjacent ends

separated by a very small air space, and let one rod be charged with

positive and the other with negative electricity. On the electronic

theory this is explained by stating that there is an accumulation of

electrons in one and of co-electrons in the other. These charges

create a distribution of electric strain throughout their

neighbourhood, which follows approximately the same law of

distribution as the lines of magnetic force of a bar magnet, and may

be roughly represented as in Fig. 1. Suppose then that the air gap is

destroyed, these charges move towards each other and disappear by

uniting, the lines of electric strain then collapse, and as they

shrink in give rise to circular lines of magnetic flux embracing the

rods. This external distribution of magnetism constitutes an electric

current in the rods produced by the movement of the two opposite

electric charges. At this stage it may be explained that the electrons

or atoms of electricity can in some cases make their way freely

between the atoms of ponderable matter. The former are incomparably

smaller than the latter, and in those cases in which this electronic

movement can take place easily, we call the material a good conductor.

[Illustration: FIG. 1.--LINES OF ELECTRIC STRAIN BETWEEN A POSITIVE

AND NEGATIVE ELECTRON AT REST.]

Suppose then the electric charges reappear in reversed positions and

go through an oscillatory motion. The result in the external space

would be the alternate production of lines of electric strain and

magnetic flux, the direction of these lines being reversed each half

cycle. Inside the rods we have a movement of electrons and

co-electrons to and fro, electric charges at the ends of the rods

alternating with electric currents in the rods, the charges being at a

maximum when the current is zero, and the current at a maximum when

the charges have for the moment disappeared. Outside the rods we have

a corresponding set of charges, lines of electric strain stretching

from end to end of the rod, alternating with rings of magnetic flux

embracing the rod. So far we have supposed the oscillation to be

relatively a slow one.

[Illustration: FIG. 2.--SUCCESSIVE STAGES IN THE DEFORMATION OF A LINE

OF STRAIN BETWEEN POSITIVE AND NEGATIVE ELECTRONS IN RAPID

OSCILLATION, SHOWING CLOSED LOOP OF ELECTRIC STRAIN THROWN OFF.]

Imagine next that the to and fro movement of the electrons or charges

is sufficiently rapid to bring into play the inertia quality of the

medium. We then have a different state of affairs. The lines of strain

in the external medium cannot contract or collapse quickly enough to

keep up with the course of events, or movements of the electrons in

the rods, and hence their regular contraction and absorption is

changed into a process of a different kind. As the electrons and

co-electrons, _i.e._, the electric charges, vibrate to and fro, the

lines of electric strain connecting them are nipped in and thrown off

as completely independent and closed lines of electric strain, and at

each successive alternation, groups or batches of these loops of

strain are detached from the rod, and, so to speak, take on an

independent existence. The whole process of the formation of these

self-closed lines of electric strain is best understood by examining a

series of diagrams which roughly represent the various stages of the

process. In Fig. 2 we have a diagram (_a_) the curved line in which

delineates approximately the form of one line of electric strain round

a linear oscillator, with spark gap in the centre, one half being

charged positively and the other negatively. Let us then suppose that

the insulation of the spark gap is destroyed, so that the opposite

electric charges rush together and oscillate to and fro. The strain

lines at each oscillation are then crossed or decussate, and the

result, as shown in Fig. 2, _d_, is that a portion of the energy of

the field is thrown off in the form of self-closed lines of strain

(see Fig. 2, _e_). At each oscillation of the charges the direction of

the lines of strain springing from end to end of the radiator is

reversed. It is a general property of lines of strain whether electric

or magnetic, that there is a tension along the line and a pressure at

right angles. In other words, these lines of electric strain are like

elastic threads, they tend to contract in the direction of their

length and press sideways on each other when in the same direction.

Hence it is not difficult to see that as each batch of self-closed

lines of strain is thrown off, the direction of the strain round each

loop is alternately in one direction and in the other. Hence these

loops of electric strain press each other out, and each one that is

formed squeezes the already formed loops further and further from the

radiator. The loops, therefore, march away into space (see Fig. 2,

_f_). If we imagine ourselves standing at a little distance at a point

on the equatorial line and able to see these loops of strain as they

pass, we should recognise a procession of loops, consisting of

alternately directed strain lines marching past. This movement through

the ether of self-closed lines of electric strain constitutes what is

called electric radiation.

Hence along a line drawn perpendicular to the radiator through its

centre, there is a distribution of electric strain normal to that

line, which is periodic in space and in time. Moreover, in addition to

these lines of electric strain, there are at right angles to them

another set of self-closed lines of magnetic flux. Alternated between

the instants when the electric charges at the ends of the radiator are

at their maximum, we have instants when the radiator rod is the seat

of an electric current, and hence the field round it is filled with

circular lines of magnetic flux coaxial with the radiator. As the

current alternates in direction each half period, these rings of

magnetic flux alternate in direction as regards the flux, and hence we

must complete our mental picture of the space round the radiator rods

when the charges are oscillating by supposing it filled with

concentric rings of magnetic flux which are periodically reversed in

direction, and have their maximum values at those instants and places

where the lines of electric strain have their zero values.

Accordingly, along the equatorial line we have two sets of strains in

the ether, distributed periodically in space and in time. First, the

lines of electric strain in the plane of the radiator, and, secondly,

the lines of magnetic flux at right angles to these. At any one point

in space these two changes, the strain and the flux, succeed each

other periodically, being, however, at right angles in direction. At

any one moment these two effects are distributed periodically or

cyclically through space, and these changes in time and space

constitute an _electric wave_ or electromagnetic wave.

We may then summarise the above statements by saying that the most

recent hypothesis as to the nature of electrical action and of

electricity itself is briefly comprised in the following statements:

The universally diffused medium called the ether has had created in

it certain centres of strain or radiating points from which proceed

lines of strain, and these centres of force are called electrons.

Electrons must, therefore, be of two kinds, positive and negative,

according to the direction of the strain radiating from the centre.

These electrons in their free condition constitute what we call

electricity, and the electrons themselves are the atoms of electricity

which, in one sense, is, therefore, as much material as that which we

call ordinary gross or ponderable matter.

Collocations of these electrons constitute the atoms of gross matter,

and we must consider that the individuality of any atom is not

determined merely by the identity of the electrons composing it, but

by the permanence of their arrangement or form. In any mass of

material substance there is probably a continual exchange of electrons

from one atom to another, and hence at any one given moment, whilst a

number of the electrons are an association forming material atoms,

there will be a further number of isolated but intermingled electrons,

which are called the free electrons. In substances which we call good

conductors, we must imagine that the free electrons have the power of

moving freely through or between the material atoms, and this movement

of the electrons constitutes a current of electricity; whilst a

superfluity of electrons of either type in any one mass of matter

constitutes what we call a charge of electricity. Hence an electrical

oscillation, which is merely a very rapid alternating current taking

place in a conductor, is on this hypothesis assumed to consist in a

rapid movement to and fro of the free electrons. We may picture to

ourselves, therefore, a rod of metal in which electrical oscillations

are taking place, as similar to an organ-pipe or siren tube in which

movements of the air particles are taking place to and fro, the free

electrons corresponding with the air particles.

Owing to the nature of the structure of an electron, it follows,

however, that every movement of an electron is accompanied by changes

in the distribution of the electric strain or ether strain taking

place throughout all surrounding space, and, as already explained,

certain very rapid movements of the electrons have the effect of

detaching closed lines of strain in the ether which move off through

space, forming, when cyclically distributed, an electric wave.

[Illustration: FIG. 3.--SIMPLE MARCONI RADIATOR. B, battery; I,

induction coil; K, signalling key; S, spark gap; A, aerial wire; E,

earth plate.]

We may next proceed to apply these principles to the explanation of

the action of the simplest form of Hertzian wave telegraphic radiator,

viz., the Marconi aerial wire. In its original form this consists of a

long vertical insulated wire, A, the lower end of which is attached to

one of the spark balls S of an induction coil, I, the other spark ball

being connected to earth E, and the two spark balls being placed a few

millimetres apart (see Fig. 3). When the coil is set in action

oscillatory or Hertzian sparks pass between the balls, electric

oscillations are set up in the wire and electric waves are radiated

from it. Deferring for the moment a more detailed examination of the

operations of the coil and at the spark gap, we may here say that the

action which takes place in the aerial wire is as follows: The wire is

first charged to a high potential, let us suppose, with negative

electricity. We may imagine this process to consist in forcing

additional electrons into it, the induction coil acting as an electron

pump. Up to a certain pressure the spark gap is a perfect insulator,

but at a critical pressure, which for spark gap lengths of four or

five millimetres and balls about one centimetre in diameter

approximates to three thousand volts per millmetre, the insulation of

the air gives way, and the charge in the wire rushes into the earth.

In consequence, however, of the inertia of the medium or of the

electrons, the charge, so to speak, overshoots the mark, and the wire

is then left with a charge of opposite sign. This again in turn

rebounds, and so the wire is discharged by a series of electrical

oscillations, consisting of alternations of static charge and electric

discharge. We may fasten our attention either on the events taking

place in the vertical wire or in the medium outside, but the two sets

of phenomena are inseparably connected and go on together. When the

aerial wire is statically charged, we may describe it by saying that

there is an accumulation of electrons or co-electrons in it. Outside

the wire there is, however, a distribution of electric strain the

strain lines proceeding from the wire to the earth (see Fig. 4).

[Illustration: FIG. 4.--LINES OF ELECTRIC STRAIN (DOTTED LINES)

EXTENDING BETWEEN A MARCONI AERIAL, A, AND THE EARTH _ee_ BEFORE

DISCHARGE.]

The wire has _capacity_ with respect to the earth, and it acts like

the inner coating of a Leyden jar, of which the dielectric is the air

and ether around it, and the outer coating is the earth's surface.

When the discharge takes place, we may consider that electrons rush

out of the wire and then rush back again into it. At the moment when

the electrons rush out of or into the aerial wire, we say there is an

electric current flowing into or out of the wire, and this electron

movement, therefore, creates the magnetic flux which is distributed in

concentric circles round the wire. This current, and, therefore,

motion of electrons, can be proved to exist by its heating effect upon

a fine wire inserted in series with the aerial, and in the case of

large aerials it may have a mean value of many amperes and a maximum

value of hundreds of amperes. Inside the aerial wire we have,

therefore, alternations of electric potential or charge and electric

current, or we may call it electron-pressure and electron-movement.

There is, therefore, an oscillation of electrons in the aerial wire,

just as in the case of an organ-pipe there is an oscillation of air

molecules in the pipe. Outside the aerial we have variations and

distributions of electric strain and magnetic flux. The resemblance

between the closed organ-pipe and the simple Marconi aerial is, in

fact, very complete. In the case of the closed organ-pipe, we have a

longitudinal oscillation of air molecules in the pipe. At the open end

or mouthpiece, where we have air moving in and out, the air movement

is alternating and considerable, but there is little or no variation

of air pressure. At the upper or closed end of the pipe we have great

variation of air pressure, but little or no air movement (see Fig. 5).

Compare this now with the electrical phenomena of the aerial. At the

spark ball or lower end we have little or no variation of potential or

electron pressure, but we have electrons rushing into and out of the

aerial at each half oscillation, forming the electric discharge or

current. At the upper or insulated end we have little or no current,

but great variations of potential or electron pressure. Supposing we

could examine the wire inch by inch, all the way up from the spark

balls at the bottom to the top, we should find at each stage of our

journey that the range of variation and maximum value of the current

in the wire became less and those of the potential became greater. At

the bottom we have nearly zero potential or no electric pressure, but

large current, and at the top end, no current, but great variation of

potential.

[Illustration: FIG. 5.--AMPLITUDE OF PRESSURE VARIATION IN A CLOSED

ORGAN PIPE, INDICATED BY THE ORDINATES OF THE DOTTED LINE _xy_.]

We can represent the amplitude of the current and potential values

along the aerial by the ordinates of a dotted line so drawn that its

distance from the aerial represents the potential oscillation or

current oscillation at that point (see Fig. 6).

This distribution of potential and current along the wire does not

necessarily imply that any one electron moves far from its normal

position. The actual movement of any particular air molecule in the

case of a sound wave is probably very small, and reckoned in

millionths of an inch. So also we must suppose that any one electron

may have a small individual amplitude of movement, but the

displacement is transferred from one to another. Conduction in a solid

may be effected by the movement of free electrons intermingled with

the chemical atoms, but any one electron may be continually passing

from a condition of freedom to one of combination.

[Illustration: FIG. 6.--(_a_) DISTRIBUTION OF ELECTRIC PRESSURE IN A

MARCONI AERIAL, A, (_b_) DISTRIBUTION OF ELECTRIC CURRENT IN A MARCONI

AERIAL, AS SHOWN BY THE ORDINATES OF THE DOTTED LINE _xy_.]

So much for the events inside the wire, but now outside the wire its

electric charge is represented by lines of electric strain springing

from the aerial to the earth. It must be remembered that every line of

strain terminates on an electron or a co-electron. Hence, when the

discharge or spark takes place between the spark balls, the rapid

movement of the electrons in the wire is accompanied by a

redistribution and movement of the lines of strain outside. As the

negative charge flows out of the aerial the ends of the strain lines

abutting on to it run down the wire and are transferred to the earth,

and at the next instant this semi-loop of electric or ether strain,

with its ends on the earth, is pushed out sideways from the wire by

the growth of a new set of lines of ether strain in an opposite

direction. The process is best understood by consulting a series of

diagrams which represent the distribution and approximate form of a

few of the strain lines at successive instants (see Fig. 7). In

between the lines of formation of the successive strain lines between

the aerial and the earth, corresponding to the successive alternate

electric charges of the aerial with opposite sign, there are a set of

concentric rings of magnetic flux formed round it which are

alternately in opposite directions, and these expand out, keeping step

with the progress of the detached strain loops and having their planes

at right angles to the latter. As the semi-loops of electric strain

march outwards with their feet on the ground, these strain lines must

always be supposed to terminate on electrons, but not continually on

the same electrons. Since the earth is a conductor, we must suppose

that there is a continual migration of the electrons forming the atoms

of the earth, and that when one electron enters an atom, another

leaves it. Hence, corresponding to the electric wave in the space

above, there are electrical changes in the ground beneath. This view

is confirmed by the well-known fact that the achievement of Hertzian

wave telegraphy is much dependent on the nature of the surface over

which it is conducted, and can be carried on more easily over good

conducting material, like sea water, than over badly conducting dry

land.

[Illustration: FIG. 7.--SUCCESSIVE STAGES IN THE PRODUCTION OF A

SEMI-LOOP OF ELECTRIC STRAIN BY A MARCONI AERIAL RADIATOR.]

The matter may be viewed, however, from another standpoint. Good

conductors are opaque to Hertzian waves; in other words, are

non-absorptive. The energy of the electric wave is not so rapidly

absorbed when it glides over a sea surface as when it is passing over

a surface which is an indifferent conductor, like dry land. In fact,

it is possible by the improvement of the signals to detect a heavy

fall of rain in the space between two stations separated only by dry

land. It is, however, clear that on the electronic theory the

progression of the lines of electric strain can only take place if the

surface over which they move is a fairly good conductor, unless these

lines of strain form completely closed loops. Hence we may sum up by

saying that there are three set of phenomena to which we must pay

attention in formulating any complete theory of the aerial. The first

is the operation taking place in the vertical wire, which is described

by saying that electrical oscillations or vibratory movements of

electrons are taking place in it, and, on our adopted theory, it may

be said to consist in a longitudinal vibration of electrons of such a

nature that we may appropriately call the aerial an ether organ-pipe.

Then in the next place, we have the distribution and movement of the

lines of electric strain and magnetic flux in the space outside the

wire, constituting the electric wave; and lastly, there are the

electrical changes in the conductor over which the wave travels, which

is the earth or water surrounding the aerial. In subsequently dealing

with the details of transmitting arrangements, attention will be

directed to the necessity for what telegraphists call a "good earth"

in connection with Hertzian wave telegraphy. This only means that

there must be a perfectly free egress and ingress for the electrons

leaving or entering the aerial, so that nothing hinders their access

to the conducting surface over which the wave travels. There must be

nothing to stop or throttle the rush of electrons into or out of the

aerial wire, or else the lines of strain cannot be detached and and

travel away.

We may next consider more particularly the energy which is available

for radiation and which is radiated. In the original form of simple

Marconi aerial, the aerial itself when insulated forms one coating or

surface of a condenser, the dielectric being the air and ether around

it, and the other conductor being the earth. The electric energy

stored up in it just before discharge takes place is numerically equal

to the product of the capacity of the aerial and half the square of

the potential to which it is charged.

If we call C the capacity of the aerial in microfarads, and V the

potential in volts to which it is raised before discharge, then the

energy storage in joules E is given by the equation,

Hertzian Wave Wireless Telegraphy · 第 5 / 10 题