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EDISON'S work in stock printers and
telegraphy had marked him as a rising man in the
electrical art of the period but his invention of
quadruplex telegraphy in 1874 was what
brought him very prominently before the notice of
the public. Duplex telegraphy, or the sending
of two separate messages in opposite directions
at the same time over one line was known and
practiced previous to this time, but quadruplex
telegraphy, or the simultaneous sending of four
separate messages, two in each direction, over
a single line had not been successfully
accomplished, although it had been the subject
of many an inventor's dream and the object of
anxious efforts for many long years.
In the early part of 1873, and for some
time afterward, the system invented by Joseph
Stearns was the duplex in practical use. In
April of that year, however, Edison took up
the study of the subject and filed two
applications for patents. One of these
applications[23] embraced an invention by
which two messages could be sent not only
duplex, or in opposite directions as above
explained, but could also be sent
"diplex"--that is to say, in one direction,
simultaneously, as separate and distinct
messages, over the one line. Thus there was
introduced a new feature into the art of
multiplex telegraphy, for, whereas duplexing
(accomplished by varying the strength of the
current) permitted messages to be sent
simultaneously from opposite stations, diplexing
(achieved by also varying the direction of the
current) permitted the simultaneous transmission
of two messages from the same station and their
separate reception at the distant station.
The quadruplex was the tempting goal toward
which Edison now constantly turned, and after
more than a year's strenuous work he filed a
number of applications for patents in the late
summer of 1874. Among them was one which
was issued some years afterward as Patent No.
480,567, covering his well-known
quadruplex. He had improved his own diplex,
combined it with the Stearns duplex and thereby
produced a system by means of which four messages
could be sent over a single line at the same
time, two in each direction.
As the reader will probably be interested to
learn something of the theoretical principles of
this fascinating invention, we shall endeavor to
offer a brief and condensed explanation thereof
with as little technicality as the subject will
permit. This explanation will necessarily be of
somewhat elementary character for the benefit of
the lay reader, whose indulgence is asked for an
occasional reiteration introduced for the sake of
clearness of comprehension. While the apparatus
and the circuits are seemingly very intricate,
the principles are really quite simple, and the
difficulty of comprehension is more apparent than
real if the underlying phenomena are studied
attentively.
At the root of all systems of telegraphy,
including multiplex systems, there lies the
single basic principle upon which their
performance depends--namely, the obtaining of
a slight mechanical movement at the more or less
distant end of a telegraph line. This is
accomplished through the utilization of the
phenomena of electromagnetism. These phenomena
are easy of comprehension and demonstration. If
a rod of soft iron be wound around with a number
of turns of insulated wire, and a current of
electricity be sent through the wire, the rod
will be instantly magnetized and will remain a
magnet as long as the current flows; but when
the current is cut off the magnetic effect
instantly ceases. This device is known as an
electromagnet, and the charging and discharging
of such a magnet may, of course, be repeated
indefinitely. Inasmuch as a magnet has the
power of attracting to itself pieces of iron or
steel, the basic importance of an electromagnet
in telegraphy will be at once apparent when we
consider the sounder, whose clicks are familiar
to every ear. This instrument consists
essentially of an electro- magnet of horseshoe
form with its two poles close together, and with
its armature, a bar of iron, maintained in
close proximity to the poles, but kept normally
in a retracted position by a spring. When the
distant operator presses down his key the circuit
is closed and a current passes along the line and
through the (generally two) coils of the
electromagnet, thus magnetizing the iron core.
Its attractive power draws the armature toward
the poles. When the operator releases the
pressure on his key the circuit is broken,
current does not flow, the magnetic effect
ceases, and the armature is drawn back by its
spring. These movements give rise to the
clicking sounds which represent the dots and
dashes of the Morse or other alphabet as
transmitted by the operator. Similar
movements, produced in like manner, are availed
of in another instrument known as the relay,
whose office is to act practically as an
automatic transmitter key, repeating the
messages received in its coils, and sending them
on to the next section of the line, equipped
with its own battery; or, when the message is
intended for its own station, sending the
message to an adjacent sounder included in a
local battery circuit. With a simple circuit,
therefore, between two stations and where an
intermediate battery is not necessary, a relay
is not used.
Passing on to the consideration of another phase
of the phenomena of electromagnetism, the
reader's attention is called to Fig. 1, in
which will be seen on the left a simple form of
electromagnet consisting of a bar of soft iron
wound around with insulated wire, through which
a current is flowing from a battery. The arrows
indicate the direction of flow.
All magnets have two poles, north and south.
A permanent magnet (made of steel, which, as
distinguished from soft iron, retains its
magnetism for long periods) is so called because
it is permanently magnetized and its polarity
remains fixed. In an electromagnet the
magnetism exists only as long as current is
flowing through the wire, and the polarity of
the soft-iron bar is determined by the
DIRECTION of flow of current around it
for the time being. If the direction is
reversed, the polarity will also be reversed.
Assuming, for instance, the bar to be end-on
toward the observer, that end will be a south
pole if the current is flowing from left to
right, clockwise, around the bar; or a north
pole if flowing in the other direction, as
illustrated at the right of the figure. It is
immaterial which way the wire is wound around the
bar, the determining factor of polarity being
the DIRECTION of the current. It will
be clear, therefore, that if two EQUAL
currents be passed around a bar in opposite
directions (Fig. 3) they will tend to
produce exactly opposite polarities and thus
neutralize each other. Hence, the bar would
remain non-magnetic.
As the path to the quadruplex passes through the
duplex, let us consider the Stearns system,
after noting one other principle--namely, that
if more than one path is presented in which an
electric current may complete its circuit, it
divides in proportion to the resistance of each
path. Hence, if we connect one pole of a
battery with the earth, and from the other pole
run to the earth two wires of equal resistance as
illustrated in Fig. 2, equal currents will
traverse the wires.
The above principles were employed in the
Stearns differential duplex system in the
following manner: Referring to Fig. 3,
suppose a wire, A, is led from a battery
around a bar of soft iron from left to right,
and another wire of equal resistance and equal
number of turns, B, around from right to
left. The flow of current will cause two equal
opposing actions to be set up in the bar; one
will exactly offset the other, and no magnetic
effect will be produced. A relay thus wound is
known as a differential relay--more generally
called a neutral relay.
The non-technical reader may wonder what use
can possibly be made of an apparently
non-operative piece of appara- tus. It must
be borne in mind, however, in considering a
duplex system, that a differential relay is used
AT EACH END of the line and forms part
of the circuit; and that while each relay must
be absolutely unresponsive to the signals
SENT OUT FROM ITS HOME
OFFICE, it must respond to signals
transmitted by a DISTANT OFFICE.
Hence, the next figure (4), with its
accompanying explanation, will probably make the
matter clear. If another battery, D, be
introduced at the distant end of the wire A the
differential or neutral relay becomes actively
operative as follows: Battery C supplies wires
A and B with an equal current, but battery D
doubles the strength of the current traversing
wire A. This is sufficient to not only
neutralize the magnetism which the cur- rent in
wire B would tend to set up, but also--by
reason of the excess of current in wire A--to
make the bar a magnet whose polarity would be
determined by the direction of the flow of
current around it.
In the arrangement shown in Fig. 4 the
batteries are so connected that current flow is
in the same direction, thus doubling the amount
of current flowing through wire A. But suppose
the batteries were so connected that the current
from each set flowed in an opposite direction?
The result would be that these currents would
oppose and neutralize each other, and,
therefore, none would flow in wire A.
Inasmuch, however, as there is nothing to
hinder, current would flow from battery C
through wire B, and the bar would therefore be
magnetized. Hence, assuming that the relay is
to be actuated from the distant end, D, it is
in a sense immaterial whether the batteries
connected with wire A assist or oppose each
other, as, in either case, the bar would be
magnetized only through the operation of the
distant key.
A slight elaboration of Fig. 4 will further
illustrate the principle of the differential
duplex. In Fig. 5 are two stations, A the
home end, and B the distant station to which a
message is to be sent. The relay at each end
has two coils, 1 and 2, No. 1 in each case
being known as the "main-line coil" and 2 as
the "artificial-line coil." The latter, in
each case, has in its circuit a resistance,
R, to compensate for the resistance of the main
line, so that there shall be no inequalities in
the circuits. The artificial line, as well as
that to which the two coils are joined, are
connected to earth. There is a battery, C,
and a key, K. When the key is depressed,
current flows through the relay coils at A, but
no magnetism is produced, as they oppose each
other. The current, however, flows out
through the main-line coil over the line and
through the main-line coil 1 at B, completing
its circuit to earth and magnetizing the bar of
the relay, thus causing its armature to be
attracted. On releasing the key the circuit is
broken and magnetism instantly ceases.
It will be evident, therefore, that the
operator at A may cause the relay at B to act
without affecting his own relay. Similar
effects would be produced from B to A if the
battery and key were placed at the B end.
If, therefore, like instruments are placed at
each end of the line, as in Fig. 6, we have
a differential duplex arrangement by means of
which two operators may actuate relays at the
ends distant from them, without causing the
operation of the relays at their home ends. In
practice this is done by means of a special
instrument known as a continuity preserving
transmitter, or, usually, as a transmitter.
This consists of an electromagnet, T,
operated by a key, K, and separate battery.
The armature lever, L, is long, pivoted in
the centre, and is bent over at the end. At a
point a little beyond its centre is a small piece
of insulating material to which is screwed a
strip of spring metal, S. Conveniently placed
with reference to the end of the lever is a bent
metallic piece, P, having a contact screw in
its upper horizontal arm, and attached to the
lower end of this bent piece is a post, or
standard, to which the main battery is
electrically connected. The relay coils are
connected by wire to the spring piece, S, and
the armature lever is connected to earth. If
the key is depressed, the armature is attracted
and its bent end is moved upward, depressing the
spring which makes contact with the upper screw,
which places the battery to the line, and
simultaneously breaks the ground connection
between the spring and the upturned end of the
lever, as shown at the left. When the key is
released the battery is again connected to
earth. The compensating resistances and
condensers necessary for a duplex arrangement are
shown in the diagram.
In Fig. 6 one transmitter is shown as
closed, at A, while the other one is open.
From our previous illustrations and explanations
it will be readily seen that, with the
transmitter closed at station A, current flows
via post P, through S, and to both relay
coils at A, thence over the main line to
main-line coil at B, and down to earth through
S and the armature lever with its grounded
wire. The relay at A would be unresponsive,
but the core of the relay at B would be
magnetized and its armature respond to signals
from A. In like manner, if the transmitter at
B be closed, current would flow through similar
parts and thus cause the relay at A to respond.
If both transmitters be closed simultaneously,
both batteries will be placed to the line, which
would practically result in doubling the current
in each of the main-line coils, in consequence
of which both relays are energized and their
armatures attracted through the operation of the
keys at the distant ends. Hence, two messages
can be sent in opposite directions over the same
line simultaneously.
The reader will undoubtedly see quite clearly
from the above system, which rests upon varying
the STRENGTH of the current, that two
messages could not be sent in the same direction
over the one line at the same time. To
accomplish this object Edison introduced another
and distinct feature--namely, the using of the
same current, but ALSO varying its
DIRECTION of flow; that is to say,
alternately reversing the POLARITY of the
batteries as applied to the line and thus
producing corresponding changes in the polarity
of another specially constructed type of relay,
called a polarized relay. To afford the reader
a clear conception of such a relay we would refer
again to Fig. 1 and its explanation, from
which it appears that the polarity of a
soft-iron bar is determined not by the strength
of the current flowing around it but by the
direction thereof.
With this idea clearly in mind, the theory of
the polarized relay, generally called "polar"
relay, as presented in the diagram (Fig.
7), will be readily understood.
A is a bar of soft iron, bent as shown, and
wound around with insulated copper wire, the
ends of which are connected with a battery, B,
thus forming an electromagnet. An essential
part of this relay consists of a swinging
PERMANENT magnet, C, whose polarity
remains fixed, that end between the terminals of
the electromagnet being a north pole. Inasmuch
as unlike poles of magnets are attracted to each
other and like poles repelled, it follows that
this north pole will be repelled by the north
pole of the electromagnet, but will swing over
and be attracted by its south pole. If the
direction of flow of current be reversed, by
reversing the battery, the electromagnetic
polarity also reverses and the end of the
permanent magnet swings over to the other side.
This is shown in the two figures of Fig. 7.
This device being a relay, its purpose is to
repeat transmitted signals into a local circuit,
as before explained. For this purpose there are
provided at D and E a contact and a back stop,
the former of which is opened and closed by the
swinging permanent magnet, thus opening and
closing the local circuit.
Manifestly there must be provided some
convenient way for rapidly transposing the
direction of the current flow if such a device as
the polar relay is to be used for the reception
of telegraph messages, and this is accomplished
by means of an instrument called a
pole-changer, which consists essentially of a
movable contact piece connected permanently to
the earth, or grounded, and arranged to connect
one or the other pole of a battery to the line
and simultaneously ground the other pole. This
action of the pole-changer is effected by
movements of the armature of an electromagnet
through the manipulation of an ordinary telegraph
key by an operator at the home station, as in
the operation of the "transmitter," above
referred to.
By a combination of the neutral relay and the
polar relay two operators, by manipulating two
telegraph keys in the ordinary way, can
simultaneously send two messages over one line in
the SAME direction with the SAME
current, one operator varying its strength and
the other operator varying its polarity or
direction of flow. This principle was covered
by Edison's Patent No. 162,633, and
was known as the "diplex" system, although,
in the patent referred to, Edison showed and
claimed the adaptation of the principle to duplex
telegraphy. Indeed, as a matter of fact, it
was found that by winding the polar relay
differentially and arranging the circuits and
collateral appliances appropriately, the polar
duplex system was more highly efficient than the
neutral system, and it is extensively used to
the present day.
Thus far we have referred to two systems, one
the neutral or differential duplex, and the
other the combination of the neutral and polar
relays, making a diplex system. By one of
these two systems a single wire could be used for
sending two messages in opposite directions, and
by the other in the same direction or in opposite
directions. Edison followed up his work on the
diplex and combined the two systems into the
quadruplex, by means of which FOUR messages
could be sent and received simultaneously over
the one wire, two in each direction, thus
employing eight operators--four at each
end--two sending and two receiving. The
general principles of quadruplex telegraphy are
based upon the phenomena which we have briefly
outlined in connection with the neutral relay and
the polar relay. The equipment of such a system
at each end of the line consists of these two
instruments, together with the special form of
transmitter and the pole-changer and their keys
for actuating the neutral and polar relays at the
other, or distant, end. Besides these there
are the compensating resistances and condensers.
All of these will be seen in the diagram
(Fig. 8). It will be understood, of
course, that the polar relay, as used in the
quadruplex system, is wound differentially, and
therefore its operation is somewhat similar in
principle to that of the differentially wound
neutral relay, in that it does not respond to
the operation of the key at the home office, but
only operates in response to the movements of the
distant key.
Our explanation has merely aimed to show the
underlying phenomena and principles in broad
outline without entering into more detail than
was deemed absolutely necessary. It should be
stated, however, that between the outline and
the filling in of the details there was an
enormous amount of hard work, study, patient
plodding, and endless experiments before Edison
finally perfected his quadruplex system in the
year 1874.
If it were attempted to offer here a detailed
explanation of the varied and numerous operations
of the quadruplex, this article would assume the
proportions of a treatise. An idea of their
complexity may be gathered from the following,
which is quoted from American Telegraphy and
Encyclopedia of the Telegraph, by William
Maver, Jr.:
"It may well be doubted whether in the whole
range of applied electricity there occur such
beautiful combinations, so quickly made, broken
up, and others reformed, as in the operation of
the Edison quadruplex. For example, it is
quite demonstrable that during the making of a
simple dash of the Morse alphabet by the neutral
relay at the home station the distant
pole-changer may reverse its battery several
times; the home pole-changer may do likewise,
and the home transmitter may increase and
decrease the electromotive force of the home
battery repeatedly. Simultaneously, and, of
course, as a consequence of the foregoing
actions, the home neutral relay itself may have
had its magnetism reversed several times, and
the SIGNAL, that is, the dash, will have
been made, partly by the home battery, partly
by the distant and home batteries combined,
partly by current on the main line, partly by
current on the artificial line, partly by the
main-line `static' current, partly by the
condenser static current, and yet, on a
well-adjusted circuit the dash will have been
produced on the quadruplex sounder as clearly as
any dash on an ordinary single-wire sounder."
We present a diagrammatic illustration of the
Edison quadruplex, battery key system, in
Fig. 8, and refer the reader to the above or
other text-books if he desires to make a close
study of its intricate operations. Before
finally dismissing the quadruplex, and for the
benefit of the inquiring reader who may vainly
puzzle over the intricacies of the circuits shown
in Fig. 8, a hint as to an essential
difference between the neutral relay, as used in
the duplex and as used in the quadruplex, may be
given. With the duplex, as we have seen, the
current on the main line is changed in strength
only when both keys at OPPOSITE stations
are closed together, so that a current due to
both batteries flows over the main line. When a
single message is sent from one station to the
other, or when both stations are sending
messages that do not conflict, only one battery
or the other is connected to the main line; but
with the quadruplex, suppose one of the
operators, in New York for instance, is
sending reversals of current to Chicago; we can
readily see how these changes in polarity will
operate the polar relay at the distant station,
but why will they not also operate the neutral
relay at the distant station as well? This
difficulty was solved by dividing the battery at
each station into two unequal parts, the smaller
battery being always in circuit with the
pole-changer ready to have its polarity reversed
on the main line to operate the distant polar
relay, but the spring retracting the armature of
the neutral relay is made so stiff as to resist
these weak currents. If, however, the
transmitter is operated at the same end, the
entire battery is connected to the main line,
and the strength of this current is sufficient to
operate the neutral relay. Whether the part or
all the battery is alternately connected to or
disconnected from the main line by the
transmitter, the current so varied in strength
is subject to reversal of polarity by the
pole-changer; but the variations in strength
have no effect upon the distant polar relay,
because that relay being responsive to changes in
polarity of a weak current is obviously
responsive to corresponding changes in polarity
of a powerful current. With this distinction
before him, the reader will have no difficulty
in following the circuits of Fig. 8, bearing
always in mind that by reason of the differential
winding of the polar and neutral relays, neither
of the relays at one station will respond to the
home battery, and can only respond to the
distant battery--the polar relay responding
when the polarity of the current is reversed,
whether the current be strong or weak, and the
neutral relay responding when the line- current
is increased, regardless of its polarity. It
should be added that besides the system
illustrated in Fig. 8, which is known as the
differential principle, the quadruplex was also
arranged to operate on the Wheatstone bridge
principle; but it is not deemed necessary to
enter into its details. The underlying
phenomena were similar, the difference
consisting largely in the arrangement of the
circuits and apparatus.[24]
Edison made another notable contribution to
multiplex telegraphy some years later in the
Phonoplex. The name suggests the use of the
telephone, and such indeed is the case. The
necessity for this invention arose out of the
problem of increasing the capacity of telegraph
lines employed in "through" and "way"
service, such as upon railroads. In a railroad
system there are usually two terminal stations
and a number of way stations. There is
naturally much intercommunication, which would
be greatly curtailed by a system having the
capacity of only a single message at a time.
The duplexes above described could not be used
on a railroad telegraph system, because of the
necessity of electrically balancing the line,
which, while entirely feasible on a through
line, would not be practicable between a number
of intercommunicating points. Edison's
phonoplex normally doubled the capacity of
telegraph lines, whether employed on way
business or through traffic, but in actual
practice made it possible to obtain more than
double service. It has been in practical use
for many years on some of the leading railroads
of the United States.
The system is a combination of telegraphic
apparatus and telephone receiver, although in
this case the latter instrument is not used in
the generally understood manner. It is well
known that the diaphragm of a telephone vibrates
with the fluctuations of the current energizing
the magnet beneath it. If the make and break of
the magnetizing current be rapid, the vibrations
being within the limits of the human ear, the
diaphragm will produce an audible sound; but if
the make and break be as slow as with ordinary
Morse transmission, the diaphragm will be
merely flexed and return to its original form
without producing a sound. If, therefore,
there be placed in the same circuit a regular
telegraph relay and a special telephone, an
operator may, by manipulating a key, operate
the relay (and its sounder) without producing a
sound in the telephone, as the makes and breaks
of the key are far below the limit of
audibility. But if through the same circuit,
by means of another key suitably connected there
is sent the rapid changes in current from an
induction-coil, it will cause a series of loud
clicks in the telephone, corresponding to the
signals transmitted; but this current is too
weak to affect the telegraph relay. It will be
seen, therefore, that this method of duplexing
is practiced, not by varying the strength or
polarity, but by sending TWO KINDS OF
CURRENT over the wire. Thus, two sets
of Morse signals can be transmitted by two
operators over one line at the same time without
interfering with each other, and not only
between terminal offices, but also between a
terminal office and any intermediate office, or
between two intermediate offices alone.
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