ELECTRIC BELLS. Bells or gongs struck by hammers vibrated
by an electro-magnet placed in an electric circuit. The. apparatus
and accessories consist of the bell, the push-button or circuit-closer,
the conducting wire, and the battery. The battery may be composed
of any of the constant elements described under ELECTRO-GALVANIC BATTERIES.
For household purposes the Leclanche cell will be found
excellently well suited, the number of elements used being regulated
by the extent and consequent resistance of the circuit.
The button or circuit-closer consists of two metallic strips
p and g, Fig. 1171, placed one above the other.
In its normal state the upper strip is separated from the lower
one by a spring. To the strips p and g the conducting
wires a and c are secured, and as the strips are
separated the circuit remains open. It is closed when desired
by pressing the knob p'. The button is inclosed in a wooden
or rubber ease.

Fig. 1172 is a convenient device for combining a number of keys
within a small compass, Eight push-buttons, corresponding to as
many distinct circuits, are arranged at equal distances around
a cylindrical case, within which the connections between the metallic
strips and wires are made. Each wire is separately insulated
by a silk covering, and all are made into a single strand as they
leave the case.
The ordinary, form of bell used for giving single taps is shown
in Fig. 1173. It consists of an electro-magnet M M, opposite
the poles n s of which is placed the armature with its
clapper k. The latter in its normal position is held back
from the bell G by a spiral spring attached to the movable
upright d, which serves to regulate its tension. The stroke
of the armature is limited by the setscrew r.
By a slight modification of the connections in the bell instrument,
the apparatus can be used both as a vibrator and as an instrument
to give single taps.

The general plan is shown in Fig. 1174, in which Hand e
are the electromagnet and armature. S is a switch which
can be turned on B or E at pleasure. When it is
on E, the apparatus becomes a vibrating instrument; when
turned on B,. there is no interruption of the current with
the attraction of the armature, and the instrument simply responds
by single taps to each closing of the circuit by the push-button.
The path of the current, when the switch is on B
and E respectively, is sufficiently evident from the figure
without further description.
When it is desirable to produce a very loud sound, the double bells and double electromagnets are usually employed in the vibrating apparatus. In general, the principle of all vibrating bells is that of the self-acting make and break; but, when the contacts are rigid points, the vibrations of the armature take place only within narrow limits, and the arrangement cannot very well be utilized for ringing a bell. Siemens has devised a plan, in his dial instruments, which answers the purpose much better, by giving the armature a greater range of movement; but the adaptation of this device to the ringing of bells for simple calls is a little troublesome, and in fact, for general use, would be altogether too complicated. By far the most preferable way of obtaining the desired range of stroke is that already described, in which a spring of some kind forms part of the path for the current, and which, with the attraction of the armature, follows the latter for such a distance as may be required.
When one battery is to serve for operating several of the bells
above described, the vibrators can not all be placed in one circuit,
as each one interrupts the circuit independently of the others;
and it is impossible, or rather impracticable, to make the armatures
of the various instruments so that they will all vibrate in exactly
the same time, or always be in unison.
The plan generally adopted for such cases is shown in Fig. 1175,
where each bell, I, II, III, has a separate conducting
wire of its own, as represented by the numerals 1, 2, 3, and a
return wire, L L, serves for all. If, now, one of the
bells is operated by the pressure of a push-button in 1, 2, or
3, as the case may be, it acts without in any way interfering
with the others, as they are all quite independent of the circuit
thus interrupted.
The fault just noticed in connection with the vibrating armature,
causing a break at each vibration, may be remedied in a very easy
manner simply by causing the armature to cut its own magnet out
of circuit after each attraction.
The principle works very satisfactorily, and will be readily
understood by reference to Fig. 1176. m m are the coils
of the electromagnet; a, the armature, to which the clapper
k is attached by means of a rather stiff spring; and f
, an elastic steel spring, which readily follows the to-and-fro
movement of the armature for a short distance. As will be seen,
a current arriving at C passes through the wire 1, coils
m m, and wire 2, to the line L ; the armature is
thus attracted to the spring f. The forward movement of
the armature brings the spring f against a contact c
, and forms the shunt quite independent of the armature.
As the resistance of this route is exceedingly small compared
to that of the helices, almost the entire current passes by the
new path, and the cores become demagnetized. The retractile force
of the spring now preponderates, and the armature falls against
the back stop, breaking the shunt circuit on its way. As this
arrangement does not break the main circuit, any desired number
can be placed in the same line and worked without interfering
with each other.
When the bell system is to be used for long distances, or when
a very loud ringing is desired, for which purpose the main line
current, as a rule, is not sufficient, a relay and local battery
are generally used; and with the heaviest apparatus, requiring
still more power, the ringing is done by means of weights.
Fig. 1177 represents an arrangement devised by Aubine, in which
a single set of electro-magnets, M M, serve both for the
relay and the call. A small projection on the upper end of the
armature a, when the latter is in its normal position, supports
the lever 3, keeping it from making contact with spring 4, and
at the same time holding it firmly against spring 2. When now
a current is sent into the line, it passes along the connection
1 to spring 2, thence to lever 3 and its connecting wire to spring
f and armature a, and from there on through the coils to
earth. This causes an attraction of the armature; lever 3 falls
down on spring 4 and closes the local circuit, which again results
in a magnetization of the core. The armature is thus made to
vibrate in the manner already described, and a violent ringing
is set up, which continues until, by pressure on the knob b
, lever 3 is again raised and supported by the armature projection.
(See "Talking Phonograph, and other Novelties," Prescott,
New York, 1879, from which the foregoing is abridged.)
Your Comments Welcomed! Copyright © 1995 Roger Corrie