THE TELEPHONE
VIBRATIONS.-Every manifestation
in nature is by way of vibration. The beating
of the heart, the action of the legs in walking, the
winking of the eyelid; the impulses from the sun,
which we call light; sound, taste and color appeal
to our senses by vibratory means, and, as we have
hereinbefore stated, the manifestations of electricity
and magnetism are merely vibrations of different wave
lengths.
THE ACOUSTIC TELEPHONE.-That
sound is merely a product of vibrations may be proven
in many ways. One of the earliest forms of telephones
was simply a “sound” telephone, called
the Acoustic Telephone. The principle
of this may be illustrated as follows:
Take two cups (A, B), as in Fi,
punch a small hole through the bottom of each, and
run a string or wire (C) from the hole of one cup to
that of the other, and secure it at both ends so it
may be drawn taut. Now, by talking into the cup
(A) the bottom of it will vibrate to and fro, as shown
by the dotted lines and thereby cause the bottom of
the other cup (B) to vibrate in like manner, and in
so vibrating it will receive not only the same amplitude,
but also the same character of vibrations as the cup
(A) gave forth.
SOUND WAVES.-Sound waves
are long and short; the long waves giving sounds which
are low in the musical scale, and the short waves high
musical tones. You may easily determine this by
the following experiment:
Stretch a wire, as at B (Fi,
fairly tight, and then vibrate it. The amplitude
of the vibration will be as indicated by dotted line
A. Now, stretch it very tight, as at C, so that the
amplitude of vibration will be as shown at E. By putting
your ear close to the string you will find that while
A has a low pitch, C is very much higher. This
is the principle on which stringed instruments are
built. You will note that the wave length, which
represents the distance between the dotted lines A
is much greater than E.
HEARING ELECTRICITY.-In
electricity, mechanism has been made to enable man
to note the action of the current. By means of
the armature, vibrating in front of a magnet, we can
see its manifestations. It is now but a step
to devise some means whereby we may hear it. In
this, as in everything else electrically, the magnet
comes into play.
In the chapter on magnetism, it was
stated that the magnetic field extended out beyond
the magnet, so that if we were able to see the magnetism,
the end of a magnet would appear to us something like
a moving field, represented by the dotted lines in
Fi.
The magnetic field is shown in Fi at only one end, but its manifestations are alike
at both ends. It will be seen that the magnetic
field extends out to a considerable distance and has
quite a radius of influence.
THE DIAPHRAGM IN A MAGNETIC FIELD.-If,
now, we put a diaphragm (A) in this magnetic field,
close up to the end of the magnet, but not so close
as to touch it, and then push it in and out, or talk
into it so that the sound waves strike it, the movement
or the vibration of the diaphragm (A) will disturb
the magnetic field emanating from the magnet, and this
disturbance of the magnetic field at one end of the
magnet also affects the magnetic field at the other
end in the same way, so that the disturbance there
will be of the same amplitude. It will also display
the same characteristics as did the magnetic field
when the diaphragm (A) disturbed it.
A SIMPLE TELEPHONE CIRCUIT.-From
this simple fact grew the telephone. If two magnets
are connected up in the same circuit, so that the
magnetic fields of the two magnets have the same source
of electric power, the disturbance of one diaphragm
will affect the other similarly, just the same as
the two magnetic fields of the single magnet are disturbed
in unison.
HOW TO MAKE A TELEPHONE.-For
experimental and testing purposes two of these telephones
should be made at the same time. The case or holder
(A) may be made either of hard wood or hard rubber,
so that it is of insulating material. The core
(B) is of soft iron, 3/8 inch in diameter and 5 inches
long, bored and threaded at one end to receive a screw
(C) which passes through the end of the case (A).
The enlarged end of the case should
be, exteriorly, 2-1/4 inches in diameter, and the
body of the case 1 inch in diameter.
Interiorly, the large end of the case
is provided with a circular recess 1-3/4 inches in
diameter and adapted to receive therein a spool which
is, diametrically, a little smaller than the recess.
The spool fits fairly tight upon the end of the core,
and when in position rests against an annular shoulder
in the recess. A hollow space (F) is thus provided
behind the spool (D), so the two wires from the magnet
may have room where they emerge from the spool.
The spool is a little shorter than
the distance between the shoulder (E) and the end
of the casing, at G, and the core projects only a short
distance beyond the end of the spool, so that when
the diaphragm (H) is put upon the end of the case,
and held there by screws (I) it will not touch the
end of the core. A wooden or rubber mouthpiece
(J) is then turned up to fit over the end of the case.
The spool (D) is made of hard rubber,
and is wound with N silk-covered wire, the windings
to be well insulated from each other. The two
ends of the wire are brought out, and threaded through
holes (K) drilled longitudinally through the walls
of the case, and affixed to the end by means of screws
(L), so that the two wires may be brought together
and connected with a duplex wire (M).
As the screw (C), which holds the
core in place, has its head hidden within a recess,
which can be closed up by wax, the two terminals of
the wires are well separated so that short-circuiting
cannot take place.
TELEPHONE CONNECTIONS.-The
simplest form of telephone connection is shown in
Fi. This has merely the two telephones (A
and B), with a single battery (C) to supply electricity
for both. One line wire (D) connects the two
telephones directly, while the other line (E) has the
battery in its circuit.
COMPLETE INSTALLATION.-To
install a more complete system requires, at each end,
a switch, a battery and an electro-magneto bell.
You may use, for this purpose, a bell, made as shown
in the chapter on bells.
Fi shows such a circuit.
We now dispense with one of the line wires, because
it has been found that the ground between the two
stations serves as a conductor, so that only one line
wire (A) is necessary to connect directly with the
telephones of the two stations. The telephones
(B, B’, respectively) have wires (C, C’)
running to the pivots of double-throw switches (D,
D’), one terminal of the switches having wires
(E, E’), which go to electric bells (F, F’),
and from the bells are other wires (G, G’),
which go to the ground. The ground wires also
have wires (H, H’), which go to the other terminals
of the switch (D, D’). The double-throw
switch (D, D’), in the two stations, is thrown
over so the current, if any should pass through, will
go through the bell to the ground, through the wires
(E, G or E’, G’).
Now, supposing the switch (D’),
in station 2, should be thrown over so it contacts
with the wire (H’). It is obvious that the
current will then flow from the battery (I’)
through wires (H’, C’) and line (A) to
station 1; then through wire C, switch D, wire E to
the bell F, to the ground through wire G. From wire
G the current returns through the ground to station
2, where it flows up wire G’ to the battery,
thereby completing the circuit.
The operator at station 2, having
given the signal, again throws his switch (D’)
back to the position shown in Fi, and the operator
at station 1 throws on his switch (D), so as to ring
the bell in station 2, thereby answering the signal,
which means that both switches are again to be thrown
over so they contact with the battery wires (H and
H’), respectively. When both are thus thrown
over, the bells (G, G’) are cut out of the circuit,
and the batteries are both thrown in, so that the
telephones are now ready for talking purposes.
MICROPHONE.-Originally
this form of telephone system was generally employed,
but it was found that for long distances a more sensitive
instrument was necessary.
LIGHT CONTACT POINTS.-In
1877 Professor Hughes discovered, accidentally, that
a light contact point in an electric circuit augmented
the sound in a telephone circuit. If, for instance,
a light pin, or a nail (A, Fi should be used
to connect the severed ends of a wire (B), the sounds
in the telephone not only would be louder, but they
would be more distinct, and the first instrument made
practically, to demonstrate this, is shown in Fi.
HOW TO MAKE A MICROPHONE.-This
instrument has simply a base (A) of wood, and near
one end is a perpendicular sounding-board (B) of wood,
to one side of which is attached, by wax or otherwise,
a pair of carbon blocks (C, D). The lower carbon
block (C) has a cup-shaped depression in its upper
side, and the upper block has a similar depression
in its lower side. A carbon pencil (E) is lightly
held within these cups, so that the lightest contact
of the upper end of the pencil with the carbon block,
makes the instrument so sensitive that a fly, walking
upon the sounding-board, may be distinctly heard through
the telephone which is in the circuit.
MICROPHONE THE FATHER OF THE TRANSMITTER.-This
instrument has been greatly modified, and is now used
as a transmitter, the latter thereby taking the place
of the pin (A), shown in Fi.
AUTOMATIC CUT-OUTS FOR TELEPHONES.-In
the operation of the telephone, the great drawback
originally was in inducing users of the lines to replace
or adjust their instruments carefully. When switches
were used, they would forget to throw them back, and
all sorts of trouble resulted.
It was found necessary to provide
an automatic means for throwing in and cutting out
an instrument, this being done by hanging the telephone
on the hook, so that the act merely of leaving the
telephone made it necessary, in replacing the instrument,
to cut out the apparatus.
Before describing the circuiting required
for these improvements, we show, in Fi, a section
of a transmitter.
A cup-shaped case (A) is provided,
made of some insulating material, which has a diaphragm
(B) secured at its open side. This diaphragm
carries the carbon pencil (C) on one side and from
the blocks which support the carbon pencil the wires
run to binding posts on the case. Of course the
carbon supporting posts must be insulated from each
other, so the current will go through the carbon pencil
(C).
COMPLETE CIRCUITING WITH TRANSMITTER.-In
showing the circuiting (Fi it will not be possible
to illustrate the boxes, or casings, which receive
the various instruments. For instance, the hook
which carries the telephone or the receiver, is hinged
within the transmitter box. The circuiting is
all that it is intended to show.
The batteries of the two stations
are connected up by a wire (A), unless a ground circuit
is used. The other side of each battery has a
wire connection (B, B’) with one terminal of
the transmitter, and the other terminal of the transmitter
has a wire (C, C’) which goes to the receiver.
From the other terminal of the receiver is a wire (D,
D’) which leads to the upper stop contact (E,
E’) of the telephone hook. A wire (F, F’)
from the lower stop contact (G, G’) of the hook
goes to one terminal of the bell, and from the other
terminal of the bell is a wire (H, H’) which
makes connection with the line wire (A). In order
to make a complete circuit between the two stations,
a line wire (I) is run from the pivot of the hook
in station 1 to the pivot of the hook in station 2.
In the diagram, it is assumed that
the receivers are on the hooks, and that both hooks
are, therefore, in circuit with the lower contacts
(G, G’), so that the transmitter and receiver
are both out of circuit with the batteries, and the
bell in circuit; but the moment the receiver, for
instance, in station 1 is taken off the hook, the latter
springs up so that it contacts with the stop (E),
thus establishing a circuit through the line wire
(I) to the hook of station 2, and from the hook through
line (F’) to the bell. From the bell, the
line (A) carries the current back to the battery of
station (A), thence through the wire (B) to the transmitter
wire (C) to receiver and wire (D) to the post (E),
thereby completing the circuit.
When, at station 2, the receiver is
taken off the hook, and the latter contacts with the
post (E’), the transmitter and receiver of both
stations are in circuit with each other, but both bells
are cut out.