LOCK-OUT PARTY-LINE SYSTEMS
The party-line problem in rural districts is somewhat different from
that within urban limits. In the latter cases, owing to the closer
grouping of the subscribers, it is not now generally considered
desirable, even from the standpoint of economy, to place more than
four subscribers on a single line. For such a line selective ringing
is simple, both from the standpoint of apparatus and operation; and
moreover owing to the small number of stations on a line, and the
small amount of traffic to and from such subscribers as usually take
party-line service, the interference between parties on the same line
is not a very serious matter.
For rural districts, particularly those tributary to small towns,
these conditions do not exist. Owing to the remoteness of the stations
from each other it is not feasible from the standpoint of line cost to
limit the number of stations to four. A much greater number of
stations is employed and the confusion resulting is distressing not
only to the subscribers themselves but also to the management of the
company. There exists then the need of a party-line system which will
give the limited user in rural districts a service, at least
approaching that which he would get if served by an individual line.
The principal investment necessary to provide facilities for telephone
service is that required to produce the telephone line. In many cases
the cost of instruments and apparatus is small in comparison with the
cost of the line. By far the greater number of subscribers in rural
districts are those who use their instruments a comparatively small
number of times a day, and to maintain an expensive telephone line for
the exclusive use of one such subscriber who will use it but a few
minutes each day is on its face an economic waste. As a result, where
individual line service is practiced exclusively one of two things
must be true: either the average subscriber pays more for his service
than he should, or else the operating company sells the service for
less than it costs, or at best for an insufficient profit. Both of
these conditions are unnatural and cannot be permanent.
The party-line method of giving service, by which a single line is
made to serve a number of subscribers, offers a solution to this
difficulty, but the ordinary non-selective or even selective party
line has many undesirable features if the attempt is made to place on
it such a large number of stations as is considered economically
necessary in rural work. These undesirable features work to the
detriment of both the user of the telephone and the operating company.
Many attempts have been made to overcome these disadvantages of the
party line in sparsely settled communities, by producing what are
commonly called lock-out systems. These, as their name implies, employ
such an arrangement of parts that when the line is in use by any two
parties, all other parties are locked out from the circuit and cannot
gain access to it until the parties who are using it are through.
System after system for accomplishing this purpose has been announced
but for the most part these have involved such a degree of complexity
and have introduced so many undesirable features as to seriously
affect the smooth operation of the system and the reliability of the
service.
We believe, however, in spite of numerous failures, that the lock-out
selective-signaling party line has a real field of usefulness and that
operating companies as well as manufacturing companies are beginning
to appreciate this need, and as a result that the relief of the rural
subscriber from the almost intolerable service he has often had to
endure is at hand. A few of the most promising lock-out party-line
systems now before the public will, therefore, be described in some
detail.
Poole System. The Poole system is a lock-out system pure and simple,
its devices being in the nature of a lock-out attachment for
selective-signaling lines, either of the polarity or of the harmonic
type wherein common-battery transmission is employed. It will be here
described as employed in connection with an ordinary harmonic-ringing
system.
In Fig. 188 there is shown a four-station party line equipped with
Poole lock-out devices, it being assumed that the ringers at each
station are harmonic and that the keys at the central office are the
ordinary keys adapted to impress the proper frequency on the line for
ringing any one of the stations. In addition to the ordinary talking
and ringing apparatus at each subscriber's station, there is a relay
of special form and also a push-button key.
[Illustration: Fig. 188. Poole Lock-Out System]
Each of the relays has two windings, one of high resistance and the
other of low resistance. Remembering that the system to which this
device is applied is always a common-battery system, and that,
therefore, the normal condition of the line will be one in which there
is a difference of potential between the two limbs, it will be evident
that whenever any subscriber on a line that is not in use raises his
receiver from its hook, a circuit will be established from the upper
contact of the hook through the lever of the hook to the
high-resistance winding _1_ of the relay and thence to the other side
of the line by way of wire _6_. This will result in current passing
through the high-resistance winding of the relay and the relay will
pull up its armature. As soon as it does so it establishes two other
circuits by the closure of the relay armature against the contacts _4_
and _5_.
The closing of the contact _4_ establishes a circuit from the upper
side of the line through the upper contact of the switch hook, thence
through the contacts of the push button _3_, thence through the
low-resistance winding _2_ of the relay to the terminal _4_, thence
through the relay armature and the transmitter to the lower side of
the line. This low-resistance path across the line serves to hold the
relay armature attracted and also to furnish current to the
transmitter for talking. The establishment of this low-resistance path
across the line does another important thing, however; it practically
short-circuits the line with respect to all the high-resistance relay
windings, and thus prevents any of the other high-resistance relay
windings from receiving enough current to actuate them, should the
subscriber at any other station remove his receiver from the hook in
an attempt to listen in or to make a call while the line is in use. As
a subscriber can only establish the proper conditions for talking and
listening by the attraction of this relay armature at his station, it
is obvious that unless he can cause the pulling up of his relay
armature he can not place himself in communication with the line.
The second thing that is accomplished by the pulling up of the relay
armature is the closure of the contacts _5_, and that completes the
talking circuit through the condenser and receiver across the line in
an obvious fashion. The result of this arrangement is that it is the
first party who raises his receiver from its hook who is enabled to
successfully establish a connection with the line, all subsequent
efforts, by other subscribers, failing to do so because of the fact
that the line is short-circuited by the path through the
low-resistance winding and the transmitter of the station that is
already connected with the line.
A little target is moved by the action of the relay so that a visual
indication is given to the subscriber in making a call to show whether
or not he is successful in getting the use of the line. If the relay
operates and he secures control of the line, the target indicates the
fact by its movement, while if someone else is using the line and the
relay does not operate, the target, by its failure to move, indicates
that fact.
When one party desires to converse with another on the same line, he
depresses the button _3_ at his station until after the called party
has been rung and has responded. This holds the circuit of his
low-resistance winding open, and thus prevents the lock-out from
becoming effective until the called party is connected with the line.
The relay armature of the calling party does not fall back with the
establishment of the low-resistance path at the called station,
because, even though shunted, it still receives sufficient current to
hold its armature in its attracted position. After the called party
has responded, the button at the calling station is released and both
low-resistance holding coils act in multiple.
[Illustration: ONE WING OF OPERATING ROOM, BERLIN, GERMANY Ultimate
Capacity 24,000 Subscribers' Lines and 2,100 Trunk Lines.
Siemens-Halske Equipment. Note Horizontal Disposal of Multiple Jack
Field.]
No induction coil is used in this system and the impedance of the
holding coil is such that incoming voice currents flow through the
condenser and the receiver, which, by reference to the figure, will be
seen to be in shunt with the holding coil. The holding coil is in
series with the local transmitter, thus making a circuit similar to
that of the Kellogg common-battery talking circuit already discussed.
A possible defect in the use of this system is one that has been common
to a great many other lock-out systems, depending for their operation
on the same general plan of action. This appears when the instruments
are used on a comparatively long line. Since the locking-out of all the
instruments that are not in use by the one that is in use depends on
the low-resistance shunt that is placed across the line by the
instrument that is in use, it is obvious that, in the case of a long
line, the resistance of the line wire will enter into the problem in
such a way as to tend to defeat the locking-out function in some cases.
Thus, where the first instrument to use the line is at the remote end
of the line, the shunting effect that this instrument can exert with
respect to another instrument near the central office is that due to
the resistance of the line plus the resistance of the holding coil at
the end instrument. The resistance of the line wire may be so high as
to still allow a sufficient current to flow through the high-resistance
coil at the nearer station to allow its operation, even though the more
remote instrument is already in use.
Coming now to a consideration of the complete selective-signaling
lock-out systems, wherein the selection of the party and the locking
out of the others are both inherent features, a single example of the
step-by-step, and of the broken-line selective lock-out systems will
be discussed.
Step-by-Step System. The so-called K.B. system, manufactured by the
Dayton Telephone Lock-out Manufacturing Company of Dayton, Ohio,
operates on the step-by-step principle. The essential feature of the
subscriber's telephone equipment in this system is the step-by-step
actuating mechanism which performs also the functions of a relay. This
device consists of an electromagnet having two cores, with a permanent
polarizing magnet therebetween, the arrangement in this respect being
the same as in an ordinary polarized bell. The armature of this magnet
works a rocker arm, which, besides stepping the selector segment
around, also, under certain conditions, closes the bell circuit and
the talking circuit, as will be described.
[Illustration: Fig. 189. K.B. Lock-Out System]
Referring first to Fig. 189, which shows in simplified form a
four-station K.B. lock-out line, the electromagnet is shown at _1_ and
the rocker arm at _2_. The ratchet _3_ in this case is not a complete
wheel but rather a segment thereof, and it is provided with a series
of notches of different depths. It is obvious that the depth of the
notches will determine the degree of movement which the upper end of
the rocker arm may have toward the left, this being dependent on the
extent to which the pawl _6_ is permitted to enter into the segment.
The first or normal notch, _i.e._, the top notch, is always of such a
depth that it will allow the rocker-arm lever _2_ to engage the
contact lever _4_, but will not permit the rocker arm to swing far
enough to the left to cause that contact to engage the bell contact
_5_. As will be shown later, the condition for the talking circuit to
be closed is that the rocker arm _2_ shall rest against the contact
_4_; and from this we see that the normal notch of each of the
segments _3_ is of such a depth as to allow the talking circuit at
each station to be closed. The next notch, _i.e._, the second one in
each disk, is always shallow, as are all of the other notches except
one. A deep notch is placed on each disk anywhere from the third to
the next to the last on the segment. This deep notch is called the
_selective notch_, and it is the one that allows of contact being made
with the ringer circuit of that station when the pawl _6_ drops into
it. The position of this notch differs on all of the segments on a
line, and obviously, therefore, the ringer circuit at any station may
be closed to the exclusion of all the others by stepping all of the
segments in unison until the deep notch on the segment of the desired
station lies opposite to the pawl _6_, which will permit the rocker
arm _2_ to swing so far to the left as to close not only the circuit
between _2_ and _4_, but also between _2_, _4_, and _5_. In this
position the talking and the ringing circuits are both closed.
The position of the deepest notch, _i.e._, the selective notch, on the
circumference of the segment at any station depends upon the number of
that station; thus, the segment of Station 4 will have a deep notch in
the sixth position; the segment for Station 9 will have a deep notch
in the eleventh position; the segment for any station will have a deep
notch in the position corresponding to the number of that station plus
two.
From what has been said, therefore, it is evident that the first, or
normal, notch on each segment is of such a depth as to allow the
moving pawl _6_ to fall to such a depth in the segment as to permit
the rocker arm _2_ to close the talking circuit only. All of the other
notches, except one, are comparatively shallow, and while they permit
the moving pawl _6_ under the influence of the rocker arm _2_ to move
the segment _3_, yet they do not permit the rocker arm _2_ to move so
far to the left as to close even the talking circuit. The exception is
the deep notch, or selective notch, which is of such depth as to
permit the pawl _6_ to fall so far into the segment as to allow the
rocker arm _2_ to close both the talking and the ringing circuits.
Besides the moving pawl _6_ there is a detent pawl _7_. This always
holds the segment _3_ in the position to which it has been last moved
by the moving pawl _6_.
The actuating magnet _1_, as has been stated, is polarized and when
energized by currents in one direction, the rocker arm moves the pawl
_6_ so as to step the segment one notch. When this relay is energized
by current in the opposite direction, the operation is such that both
the moving pawl _6_ and the detent pawl _7_ will be pulled away from
the segment, thus allowing the segment to return to its normal position
by gravity. This is accomplished by the following mechanism: An
armature stop is pivoted upon the face of the rocker arm so as to swing
in a plane parallel to the pole faces of the relay, and is adapted,
when the relay is actuated by selective impulses of one polarity, to be
pulled towards one of the pole faces where it acts, through impact with
a plate attached to the pole face of the relay, as a limiting means
for the motion of the rocker arm when the rocker arm is actuated by the
magnet. When, however, the relay is energized by current in the
opposite direction, as on a releasing impulse, the armature stop swings
upon its pivot towards the opposite pole face, in which position the
lug on the end of the armature stop registers with a hole in the plate
on the relay, thus allowing the full motion of the rocker arm when it
is attracted by the magnet. This motion of the rocker arm withdraws the
detent pawl from engagement with the segment as well as the moving
pawl, and thereby permits the segment to return to its normal position.
As will be seen from Fig. 189, each of the relay magnets _1_ is
permanently bridged across the two limbs of the line.
Each station is provided with a push button, not shown, by means of
which the subscriber who makes a call may prevent the rocker arm of
his instrument from being actuated while selective impulses are being
sent over the line. The purpose of this is to enable one party to make
a call for another on the same line, depressing his push button while
the operator is selecting and ringing the called party. The segment at
his own station, therefore, remains in its normal position, in which
position, as we have already seen, his talking circuit is closed; all
of the other segments are, however, stepped up until the ringing and
talking circuits of the desired station are in proper position, at
which time ringing current is sent over the line. The segments in Fig.
189, except at Station C, are shown as having been stepped up to the
sixth position, which corresponds to the ringing position of the
fourth station, or Station D. The condition shown in this figure
corresponds to that in which the subscriber at Station C originated
the call and pressed his button, thus retaining his own segment in its
normal position so that the talking circuits would be established with
Station D.
When the line is in normal position any subscriber may call central by
his magneto generator, not shown in Fig. 189, which will operate the
drop at central, but will not operate any of the subscribers' bells,
because all bell circuits are normally open. When a subscriber desires
connection with another line, the operator sends an impulse back on
the line which steps up and locks out all instruments except that of
the calling subscriber.
[Illustration: Fig. 190. K.B. Lock-Out Station]
A complete K.B. lock-out telephone is shown in Fig. 190. This is the
type of instrument that is usually furnished when new equipment is
ordered. If, however, it is desired to use the K.B. system in
connection with telephones of the ordinary bridging type that are
already in service, the lock-out and selective mechanism, which is
shown on the upper inner face of the door in Fig. 190, is furnished
separately in a box that may be mounted close to the regular telephone
and connected thereto by suitable wires, as shown in Fig. 191. It is
seen that this instrument employs a local battery for talking and also
a magneto generator for calling the central office.
The central-office equipment consists of a dial connected with an
impulse wheel, together with suitable keys by which the various
circuits may be manipulated. This dial and its associated mechanism
may be mounted in the regular switchboard cabinet, or it may be
furnished in a separate box and mounted alongside of the cabinet in
either of the positions shown at _1_ or _2_ of Fig. 192.
In order to send the proper number of impulses to the line to call a
given party, the operator places her finger in the hole in the dial
that bears the number corresponding to the station wanted and rotates
the dial until the finger is brought into engagement with the fixed
stop shown at the bottom of the dial in Fig. 192. The dial is then
allowed to return by the action of a spring to its normal position,
and in doing so it operates a switch within the box to make and break
the battery circuit the proper number of times.
_Operation._ A complete description of the operation may now be had in
connection with Fig. 193, which is similar to Fig. 189, but contains
the details of the calling arrangement at the central office and also
of the talking circuits at the various subscribers' stations.
[Illustration: Fig. 191. K.B. Lock-Out Station]
Referring to the central-office apparatus the usual ringing key is
shown, the inside contacts of which lead to the listening key and to
the operator's telephone set as in ordinary switchboard practice.
Between the outside contact of this ringing key and the ringing
generator there is interposed a pair of contact springs _8-8_ and
another pair _9-9_. The contact springs _8_ are adapted to be moved
backward and forward by the impulse wheel which is directly controlled
by the dial under the manipulation of the operator. When these springs
_8_ are in their normal position, the ringing circuit is continued
through the release-key springs _9_ to the ringing generator. These
springs _8_ occupy their normal position only when the dial is in its
normal position, this being due to the notch _10_ in the contact wheel.
At all other times, _i.e._, while the impulse wheel is out of its
normal position, the springs _8-8_ are either depressed so as to engage
the lower battery contacts, or else held in an intermediate position so
as to engage neither the battery contacts nor the generator contacts.
[Illustration: Fig. 192. Calling Apparatus K.B. System]
When it is desired to call a given station, the operator pulls the
subscriber's number on the dial and holds the ringing key closed,
allowing the dial to return to normal. This connects the impulse
battery to the subscriber's line as many times as is required to move
the subscriber's sectors to the proper position, and in such direction
as to cause the stepping movement of the various relays. As the
impulse wheel comes to its normal position, the springs _8_,
associated with it, again engage their upper contacts, by virtue of
the notch _10_ in the impulse wheel, and this establishes the
connection between the ringing generator and the subscriber's line,
the ringing key being still held closed. The pulling of the
transmitter dial and holding the ringing key closed, therefore, not
only sends the stepping impulses to line, but also follows it by the
ringing current. The sending of five impulses to line moves all of the
sectors to the sixth notch, and this corresponds to the position
necessary to make the fourth station operative. Such a condition is
shown in Fig. 193, it being assumed that the subscriber at Station C
originated the call and pressed his own button so as to prevent his
sector from being moved out of its normal position. As a result of
this, the talking circuit at Station C is left closed, and the talking
and the ringing circuit of Station D, the called station, are closed,
while both the talking and the ringing circuits of all the other
stations are left open. Station D may, therefore, be rung and may
communicate with Station C, while all of the other stations on the
line are locked out, because of the fact that both their talking and
ringing circuits are left open.
[Illustration: Fig. 193. Circuit K.B. System]
When conversation is ended, the operator is notified by the usual
clearing-out signal, and she then depresses the release button, which
brings the springs _9_ out of engagement with the generator contact
but into engagement with the battery contact in such relation as to
send a battery current on the line in the reverse direction from that
sent out by the impulse wheel. This sends current through all of the
relays in such direction as to withdraw both the moving and the
holding pawls from the segments and thus allow all of the segments to
return to their normal positions. Of course, in thus establishing the
release current, it is necessary for the operator to depress the
ringing key as well as the release key.
A one-half microfarad condenser is placed in the receiver circuit at
each station so that the line will not be tied up should some
subscriber inadvertently leave his receiver off its hook. This permits
the passage of voice currents, but not of the direct currents used in
stepping the relays or in releasing them.
The circuit of Fig. 193 is somewhat simplified from that in actual
practice, and it should be remembered that the hook switch, which is
not shown in this figure, controls in the usual way the continuity of
the receiver and the transmitter circuits as well as of the generator
circuits, the generator being attached to the line as in an ordinary
telephone.
Broken-Line System. The broken-line method of accomplishing
selective signaling and locking-out on telephone party lines is due to
Homer Roberts and his associates.
[Illustration: Fig. 194. Roberts Latching Relay]
To understand just how the principles illustrated in Figs. 186 and 187
are put into effect, it will be necessary to understand the latching
relay shown diagrammatically in its two possible positions in Fig. 194,
and in perspective in Fig. 195. Referring to Fig. 194, the left-hand
cut of which shows the line relay in its normal position, it is seen
that the framework of the device resembles that of an ordinary
polarized ringer. Under the influence of current in one direction
flowing through the left-hand coil, the armature of this device
depresses the hard rubber stud _4_, and the springs _1_, _2_, and _3_
are forced downwardly until the spring _2_ has passed under the latch
carried on the spring _5_. When the operating current through the coil
_6_ ceases, the pressure of the armature on the spring _1_ is relieved,
allowing this spring to resume its normal position and spring _3_ to
engage with spring _2_. The spring _2_ cannot rise, since it is held by
the latch _5_, and the condition shown in the right-hand cut of Fig.
194 exists. It will be seen that the spring _2_ has in this operation
carried out just the same function as the switch lever performed as
described in connection with Figs. 186 and 187. An analysis of this
action will show that the normal contact between the springs _1_ and
_2_, which contact controls the circuit through the relay coil and the
bell, is not broken until the coil _6_ is de-energized, which means
that the magnet is effective until it has accomplished its work. It is
impossible, therefore, for this relay to cut itself out of circuit
before it has caused the spring _2_ to engage under the latch _5_. If
current of the proper direction were sent through the coil _7_ of the
relay, the opposite end of the armature would be pulled down and the
hard rubber stud at the left-hand end of the armature would bear
against the bent portion of the spring _5_ in such manner as to cause
the latch of this spring to release the spring _2_ and thus allow the
relay to assume its normal, or unlatched, position.
A good idea of the mechanical construction of this relay may be
obtained from Fig. 195. The entire selecting function of the Roberts
system is performed by this simple piece of apparatus at each station.
[Illustration: Fig. 195. Roberts Latching Relay]
The diagram of Fig. 196 shows, in simplified form, a four-station
line, the circuits being given more in detail than in the diagrams of
Chapter XVI.
It will be noticed that the ringer and the relay coil _6_ at the
first station are bridged across the sides of the line leading to the
central office. In like manner the bell and the relay magnets are
bridged across the two limbs of the line leading into each succeeding
station, but this bridge at each of the stations beyond Station A is
ineffective because the line extension _R__{x} is open at the next
station nearest the central office.
[Illustration: Fig. 196. Simplified Circuits of Roberts System]
In order to ring Station A it is only necessary to send out ringing
current from the central office. This current is in such direction as
not to cause the operation of the relay, although it passes through
the coil _6_. If, on the other hand, it is desired to ring Station B,
a preliminary impulse would be sent over the metallic circuit from the
central office, which impulse would be of such direction as to operate
the relay at Station A, but not to operate the bell at that station.
The operation of the relay at Station A causes the spring _2_ of this
relay to engage the spring _3_, thus extending the line on to the
second station. After the spring _2_ at Station A has been forced into
contact with the spring _3_, it is caught by the latch of the spring
_5_ and held mechanically. When the impulse from the central office
ceases, the spring _1_ resumes its normal position, thus breaking the
bridge circuit through the bell at that station. It is apparent now
that the action of coil _6_ at Station A has made the relay powerless
to perform any further action, and at the same time the line has been
extended on to the second station. A second similar impulse from the
central office will cause the relay at Station B to extend the line on
to Station C, and at the same time break the circuit through the
operating coil and the bell at Station B. In this way any station may
be picked out by sending the proper number of impulses to operate the
line relays of all the stations between the station desired and the
central office, and having picked out a station it is only necessary
to send out ringing current, which current is in such direction as to
ring the bell but not to operate the relay magnet at that station.
In Fig. 197, a four-station line, such as is shown in Fig. 196, is
illustrated, but the condition shown in this is that existing when two
preliminary impulses have been sent over the line, which caused the
line relays at Station A and Station B to be operated. The bell at
Station C is, therefore, the only one susceptible to ringing current
from the central office.
[Illustration: Fig. 197. Simplified Circuits of Roberts System]
Since only one bell and one relay are in circuit at any one time, it
is obvious that all of the current that passes over the line is
effective in operating a single bell or relay only. There is no
splitting up of the current among a large number of bells as in the
bridging system of operating step-by-step devices, which method
sometimes so greatly reduces the effective current for each bell that
it is with great difficulty made to respond. All the energy available
is applied directly to the piece of apparatus at the time it is being
operated. This has a tendency toward greater surety of action, and the
adjustment of the various pieces of apparatus may be made with less
delicacy than is required where many pieces of apparatus, each having
considerable work to do, must necessarily be operated in multiple.
The method of unlatching the relays has been briefly referred to.
After a connection has been established with a station in the manner
already described, the operator may clear the line when it is proper
to do so by sending impulses of such a nature as to cause the line
relays of the stations beyond the one chosen to operate, thus
continuing the circuit to the end of the line. The operation of the
line relay at the last station brings into circuit the coil _8_, Figs.
196 and 197, of a grounding device. This is similar to the line relay,
but it holds its operating spring in a normally latched position so as
to maintain the two limbs of the line disconnected from the ground.
The next impulse following over the metallic circuit passes through
the coil _8_ and causes the operation of this grounding device which,
by becoming unlatched, grounds the limb _L_ of the line through the
coil _8_. This temporary ground at the end of the line makes it
possible to send an unlocking or restoring current from the central
office over the limb _L_, which current passes through all of the
unlocking coils _7_, shown in Figs. 194, 196, and 197, thus causing
the simultaneous unlocking of all of the line relays and the
restoration of the line to its normal condition, as shown in Fig. 196.
[Illustration: Fig. 198. Details of Latching Relay Connections]
As has been stated, the windings _7_ on the line relays are the
unlatching windings. In Figs. 196 and 197, for the purpose of
simplicity, these windings are not shown connected, but as a matter of
fact each of them is included in series in the continuous limb _L_ of
the line. This would introduce a highly objectionable feature from the
standpoint of talking over the line were it not for the balancing
coils _7_^{1}, each wound on the same core as the corresponding
winding _7_, and each included in series in the limb _R_ of the line,
and in such direction as to be differential thereto with respect to
currents passing in series over the two limbs of the line.
The windings _7_ are the true unlocking windings, while the windings
_7_^{1} have no other function than to neutralize the inductive
effects of these unlocking windings necessarily placed in series in
the talking circuit. All of these windings are of low ohmic
resistance, a construction which, as has previously been noted, brings
about the desired effect without introducing any self-induction in
the line, and without producing any appreciable effect upon the
transmission. A study of Fig. 198 will make clear the connections of
these unlocking and balancing windings at each station.
The statement of operation so far given discloses the general method
of building up the line in sections in order to choose any party and
of again breaking it up into sections when the conversation is
finished. It has been stated that the same operation which selects the
party wanted also serves to give that party the use of the line and to
lock the others off. That this is true will be understood when it is
stated that the ringer is of such construction that when operated to
ring the subscriber wanted, it also operates to unlatch a set of
springs similar to those shown in Fig. 194, this unlatching causing
the proper connection of the subscriber's talking circuit across the
limbs of the line, and also closing the local circuit through his
transmitter. The very first motion of the bell armature performs this
unlatching operation after which the bell behaves exactly as an
ordinary polarized biased ringer.
[Illustration: Fig. 199. Broken-Back Ringer]
The construction of this ringer is interesting and is shown in its two
possible positions in Fig. 199. The group of springs carried on its
frame is entirely independent of the movement of the armature during
the ringing operation. With reversed currents, however, the armature
is moved in the opposite direction from that necessary to ring the
bells, and this causes the latching of the springs into their normal
position. In order that this device may perform the double function
of ringer and relay the tapper rod of the bell is hinged on the
armature so as to partake of the movements of the armature in one
direction only. This has been called by the inventor and engineers of
the Roberts system a _broken-back ringer_, a name suggestive of the
movable relation between the armature and the tapper rod. The
construction of the ringer is of the same nature as that of the
standard polarized ringer universally employed, but a hinge action
between the armature and the tapper rod, of such nature as to make the
tapper partake positively of the movements of the armature in one
direction, but to remain perfectly quiescent when the armature moves
in the other direction, is provided.
[Illustration: Fig. 200. Details of Ringer Connection]
How this broken-back ringer controls the talking and the locking-out
conditions may best be understood in connection with Fig. 200. The
ringer springs are normally latched at all stations. Under these
conditions the receiver is short-circuited by the engagement of
springs _10_ and _11_, the receiver circuit is open between springs
_10_ and _12_, and the local-battery circuit is open between springs
_9_ and _12_. The subscribers whose ringers are latched are,
therefore, locked out in more ways than one.
When the bell is rung, the first stroke it makes unlatches the springs,
which assume the position shown in the right-hand cut of Fig. 199, and
this, it will be seen from Fig. 200, establishes proper conditions for
enabling the subscriber to transmit and to receive speech.
The hook switch breaks both transmitter and receiver circuits when down
and in raising it establishes a momentary circuit between the ground
and the limb _L_ of the line, both upper and lower hook contacts
engaging the hook lever simultaneously during the rising of the hook.
The mechanism at the central office by which selection of the proper
station is made in a rapid manner is shown in Fig. 201. It has already
been stated that the selection of the proper subscriber is brought
about by the sending of a predetermined number of impulses from the
central office, these impulses passing in one direction only and over
the metallic circuit. After the proper party has been reached, the
ringing current is put on in the reverse direction.
[Illustration: Fig. 201. Central-Office Impulse Transmitter]
The operator establishes the number of impulses to be sent by placing
the pointer opposite the number on the dial corresponding to the
station wanted. The ratchet wheel is stepped around automatically by
each impulse of current from an ordinary pole changer such as is
employed in ringing biased bells. When the required number of impulses
has been sent, a projection, carried on a group of springs, drops into
a notch on the drum of the selector shaft, which operation instantly
stops the selecting current impulses and at the same time throws on
the ringing current which consists of impulses in the reverse
direction. So rapidly does this device operate that it will readily
follow the impulses of an ordinary pole changer, even when this is
adjusted to its maximum rate of vibration.
[Illustration: VIEW OF A LARGE FOREIGN MULTIPLE SWITCHBOARD]
_Operation._ Space will not permit a full discussion of the details of
the central-office selective apparatus, but a general resumé of the
operation of the system may now be given, with the aid of Fig. 202,
which shows a four-station line with the circuits of three of the
stations somewhat simplified. In this figure Station A, Station B,
and Station D are shown in their locked-out positions, A and B having
been passed by the selection and ringing of Station C, while Station D
is inoperative because it was not reached in the selection and the
line is still broken at Station C. Station C, therefore, has
possession of the line.
When the subscriber at Station C raised his receiver in order to call
central, a "flash" contact was made as the hook moved up, which
momentarily grounded the limb _L_ of the line. (See Fig. 200.) This
"flash" contact is produced by the arrangement of the hook which
assures that the lower contact shall, by virtue of its flexibility,
follow up the hook lever until the hook lever engages the upper
contact, after which the lower contact breaks. This results in the
momentary connection of both the upper and the lower contacts of the
hook with the lever, and, therefore, the momentary grounding of the
limb _L_ of the line. This limb always being continuous serves, when
this "flash" contact is made, to actuate the line signal at the
central office.
[Illustration: Fig. 202. Circuits of Roberts Line]
Since, however, all parties on the line are normally locked out of
talking circuits, some means must be provided whereby the operator may
place the signaling party in talking connection and leave all the
other instruments on the line in their normally locked-out position.
In fact, the operator must be able automatically to pick out the
station that signaled in, and operate the ringer to unlatch the
springs controlling the talking circuit of that station. Accordingly
the operator sends impulses on the line, from a grounded battery,
which are in the direction to operate the line relays and to continue
the line circuit to the station calling. When, after a sufficient
number of impulses, this current reaches that station it finds a path
to ground from the limb _L_. This path is made possible by the fact
that the subscriber's receiver is off its hook at that station. In
order to understand just how this ground connection is made, it must
be remembered that each of the ringer magnets is energized with each
selecting impulse, but in such a direction as not to ring the bells,
it being understood that all of the ringer mechanisms are normally
latched. When the selecting impulse for Station C arrives, it passes
through the ringer and the selecting relay coils at that station and
starts to operate the remainder of the ringers sufficiently to cause
the spring _12_ to engage the spring _13_. This establishes the ground
connection from the limb _L_ of the line, the circuit being traced
through limb _L_ through the upper contact of the switch, thence
through springs _12_ and _13_ to ground, and this, before the line
relay has time to latch, operates the quick-acting relay at the
central office, which acts to cut off further impulses, and thus
automatically stops at the calling station. Ringing current in the
opposite direction is then sent to line; this unlatches the ringer
springs and places the calling subscriber in talking circuit. When the
operator has communicated with the calling subscriber, and found, for
example, that another party on another similar line is desired, she
turns the dial pointer on the selector to the number corresponding to
the called-for party's number on that line, and presses the signal
key. Pressing this key causes impulses to "run down the line,"
selecting the proper party and ringing his bell in the manner already
described. The connection between the two parties is then established,
and no one else can in any possible way, except by permission of the
operator, obtain access to the line.
It is obvious that some means must be provided for restoring the
selecting relays to normal after a conversation is finished. By
referring to Fig. 194 it will be seen that the upper end of the latch
spring _5_ is bent over in such a manner that when the armature is
attracted by current flowing through the coil _7_, the knob on the
left-hand end of the armature on rising engages with the bent cam
surface and forces back the latch, permitting spring _2_ to return to
its normal position.
To restore the line the operator sends out sufficient additional
selective impulses to extend the circuit to the end of the line, and
thus brings the grounder into circuit. The winding of the grounder is
connected in such a manner that the next passing impulse throws off
its latch, permitting the long spring to contact with the ground
spring. The operator now sends a grounded impulse over the continuous
limb _L_ of the line which passes through the restoring coils _7_ at
all the stations and through the right-hand coil of the grounding
device to ground. The selecting relays are, therefore, simultaneously
restored to normal. The grounder is also energized and restored to its
normal position by the same current.
If a party in calling finds that his own line is busy and he cannot
get central, he may leave his receiver off its hook. When the party
who is using the line hangs up his receiver the fact that another
party desires a connection is automatically indicated to the operator,
who then locks out the instrument of the party who has just finished
conversation and passes his station by. When the operator again throws
the key, the waiting subscriber is automatically selected in the same
manner as was the first party. If there are no subscribers waiting for
service, the stop relay at central will not operate until the grounder
end of the line is unlatched, the selecting relays being then restored
automatically to normal.
The circuits are so organized that at all times whether the line is
busy or not, the movement up and down of the switch hook, at any
sub-station, operates a signal before the operator. Such a movement,
when made slowly and repeatedly, indicates to the operator that the
subscriber has an emergency call and she may use her judgment as to
taking the line away from the parties who are using it, and finding
out what the emergency call is for. If the operator finds that the
subscriber has misused this privilege of making the emergency call,
she may restore the connection to the parties previously engaged in
conversation.
One of the salient points of this Roberts system is that the operator
always has control of the line. A subscriber is not able even to use
his own battery till permitted to do so. A subscriber who leaves his
receiver off its hook in order that he may be signaled by the operator
when the line is free, causes no deterioration of the local battery
because the battery circuit is held open by the switch contacts
carried on the ringer. It cannot be denied, however, that this system
is complicated, and that it has other faults. For instance, as
described herein, both sides of the line must be looped into each
subscriber's station, thus requiring four drop, or service, wires
instead of two. It is possible to overcome this objection by placing
the line relays on the pole in a suitably protected casing, in which
case it is sufficient to run but two drop wires from the nearer line
to station. There are undoubtedly other objections to this system, and
yet with all its faults it is of great interest, and although radical
in many respects, it teaches lessons of undoubted value.
CHAPTER XVIII
ELECTRICAL HAZARDS
All telephone systems are exposed to certain electrical hazards. When
these hazards become actively operative as causes, harmful results
ensue. The harmful results are of two kinds: those causing damage to
property and those causing damage to persons. The damage to persons
may be so serious as to result in death. Damage to property may
destroy the usefulness of a piece of apparatus or of some portion of
the wire plant. Or the property damage may initiate itself as a harm
to apparatus or wiring and may result in greater and extending damage
by starting a fire.
Electrical currents which endanger life and property may be furnished
by natural or artificial causes. Natural electricity which does such
damage usually displays itself as lightning. In rare cases, currents
tending to flow over grounded lines because of extraordinary
differences of potential between sections of the earth's surface have
damaged apparatus in such lines, or only have been prevented from
causing such damage by the operation of protective devices.
Telegraph and telephone systems have been threatened by natural
electrical hazards since the beginning of the arts and by artificial
electrical hazards since the development of electric light and power
systems. At the present time, contrary to the general supposition, it
is in the artificial, and not in the natural electrical hazards that
the greater variety and degree of danger lies.
Of the ways in which artificial electricity may injure a telephone
system, the entrance of current from an external electrical power
system is a greater menace than an abnormal flow of current from a
source belonging to the telephone system itself. Yet modern practice
provides opportunities for a telephone system to inflict damage upon
itself in that way. Telephone engineering designs need to provide
means for protecting _all_ parts of a system against damage, from
external ("foreign") as well as internal ("domestic") hazards, and to
cause this protection to be inclusive enough to protect persons
against injury and property from damage by any form of overheating or
electrolytic action.
A part of a telephone system for which there is even a remote
possibility of contact with an external source of electrical power,
whether natural or artificial, is said to be _exposed_ to electrical
hazard. The degree or character of possible contact or other
interference often is referred to in relative terms of _exposure_. The
same terms are used concerning inductive relations between circuits.
The whole tendency of design, particularly of wire plants, is to
arrange the circuits in such a way as to limit the exposure as greatly
as possible, the intent being to produce a condition in which all
parts of the system will be _unexposed_ to hazards.
Methods of design are not yet sufficiently advanced for any plant to
be formed of circuits wholly unexposed, so that protective means are
required to safeguard apparatus and circuits in case the hazard,
however remote, becomes operative.
Lightning discharges between the clouds and earth frequently charge
open wires to potentials sufficiently high to damage apparatus; and
less frequently, to destroy the wires of the lines themselves.
Lightning discharges between clouds frequently induce charges in lines
sufficient to damage apparatus connected with the lines. Heavy rushes
of current in lines, from lightning causes, occasionally induce
damaging currents in adjacent lines not sufficiently exposed to the
original cause to have been injured without this induction. The
lightning hazard is least where the most lines are exposed. In a small
city with all of the lines formed of exposed wires and all of them
used as grounded circuits, a single lightning discharge may damage
many switchboard signals and telephone ringers if there be but 100 or
200 lines, while the damage might have been nothing had there been 800
to 1,000 lines in the same area.
Means of protecting lines and apparatus against damage by lightning
are little more elaborate than in the earliest days of telegraph
working. They are adequate for the almost entire protection of life
and of apparatus.
Power circuits are classified by the rules of various governing bodies
as high-potential and low-potential circuits. The classification of
the National Board of Fire Underwriters in the United States defines
low-potential circuits as having pressures below 550 volts;
high-potential circuits as having pressures from 550 to 3,500 volts,
and extra high-potential circuits as having pressures above 3,500
volts. Pressures of 100,000 volts are becoming more common. Where
power is valuable and the distance over which it is to be transmitted
is great, such high voltages are justified by the economics of the
power problem. They are a great hazard to telephone systems, however.
An unprotected telephone system meeting such a hazard by contact will
endanger life and property with great certainty. A very common form of
distribution for lighting and power purposes is the three-wire system
having a grounded neutral wire, the maximum potential above the earth
being about 115 volts.
Telephone lines and apparatus are subject to damage by any power
circuit whether of high or low potential. The cause of property damage
in all cases is the flow of current. Personal damage, if it be death
from shock, ordinarily is the result of a high potential between two
parts of the body. The best knowledge indicates that death uniformly
results from shock to the heart. It is believed that death has
occurred from shock due to pressure as low as 100 volts. The critical
minimum voltage which can not cause death is not known. A good rule is
never willingly to subject another person to personal contact with any
electrical pressure whatever.
Electricity can produce actions of four principal kinds:
physiological, thermal, chemical, and magnetic. Viewing electricity as
establishing hazards, the physiological action may injure or kill
living things; the thermal action may produce heat enough to melt
metals, to char things which can be burned, or to cause them actually
to burn, perhaps with a fire which can spread; the chemical action may
destroy property values by changing the state of metals, as by
dissolving them from a solid state where they are needed into a state
of solution where they are not needed; the magnetic action introduces
no direct hazard. The greatest hazard to which property values are
exposed is the electro-thermal action; that is, the same useful
properties by which electric lighting and electric heating thrive may
produce heat where it is not wanted and in an amount greater than can
safely be borne.
The tendency of design is to make all apparatus capable of carrying
without overheating any current to which voltage within the telephone
system may subject it, and to provide the system so designed with
specific devices adapted to isolate it from currents originating
without. Apparatus which is designed in this way, adapted not only to
carry its own normal working currents but to carry the current which
would result if a given piece of apparatus were connected directly
across the maximum pressure within the telephone system itself, is
said to be self-protecting. Apparatus amply able to carry its maximum
working current but likely to be overheated, to be injured, or perhaps
to destroy itself and set fire to other things if subjected to the
maximum pressure within the system, is not self-protecting apparatus.
To make all electrical devices self-protecting by surrounding them
with special arrangements for warding off abnormal currents from
external sources, is not as simple as might appear. A lamp, for
example, which can bear the entire pressure of a central-office
battery, is not suitable for direct use in a line several miles long
because it would not give a practical signal in series with that line
and with the telephone set, as it is required to do. A lamp suitable
for use in series with such a line and a telephone set would burn out
by current from its own normal source if the line should become
short-circuited in or near the central office. The ballast referred to
in the chapter on "Signals" was designed for the very purpose of
providing rapidly-rising resistance to offset the tendency toward
rapidly-rising current which could burn out the lamp.
As another example, a very small direct-current electric motor can be
turned on at a snap switch and will gain speed quickly enough so that
its armature winding will not be overheated. A larger motor of that
kind can not be started safely without introducing resistance into the
armature circuit on starting, and cutting it out gradually as the
armature gains speed. Such a motor could be made self-protecting by
having the armature winding of much larger wire than really is
required for mere running, choosing its size great enough to carry the
large starting current without overheating itself and its insulation.
It is better, and for long has been standard practice, to use starting
boxes, frankly admitting that such motors are not self-protecting
until started, though they are self-protecting while running at normal
speeds. Such a motor, once started, may be overloaded so as to be
slowed down. So much more current now can pass through the armature
that its winding is again in danger. Overload circuit-breakers are
provided for the very purpose of taking motors out of circuit in cases
where, once up to speed, they are mechanically brought down again and
into danger. Such a circuit-breaker is a device for protecting against
an _internal_ hazard; that is, internal to the power system of which
the motor is a part.
Another example: In certain situations, apparatus intended to operate
under impulses of large current may be capable of carrying its normal
impulses successfully but incapable of carrying currents from the same
pressure continuously. Protective means may be provided for detaching
such apparatus from the circuit whenever the period in which the
current acts is not short enough to insure safety. This is cited as a
case wherein a current, normal in amount but abnormal in duration,
becomes a hazard.
The last mentioned example of damage from internal hazards brings us
to the law of the electrical generation of heat. _The greater the
current or the greater the resistance of the conductor heated or the
longer the time, the greater will he the heat generated in that
conductor._ But this generated heat varies directly as the resistance
and as the time and as the square of the current, that is, the law is
Heat generated = _C^{2}Rt_
in which _C_ = the current; _R_=the resistance of the conductor; and
_t_ = the time.
It is obvious that a protective device, such as an overload
circuit-breaker for a motor, or a protector for telephone apparatus,
needs to operate more quickly for a large current than for a small
one, and this is just what all well-designed protective devices are
intended to do. The general problem which these heating hazards
present with relation to telephone apparatus and circuits is: _To
cause all parts of the telephone system to be made so as to carry
successfully all currents which may flow in them because of any
internal or external pressure, or to supplement them by devices which
will stop or divert currents which could overheat them._
Electrolytic hazards depend not on the heating effects of currents but
on their chemical effects. The same natural law which enables primary
and secondary batteries to be useful provides a hazard which menaces
telephone-cable sheaths and other conductors. When a current leaves a
metal in contact with an electrolyte, the metal tends to dissolve into
the electrolyte. In the processes of electroplating and electrotyping,
current enters the bath at the anode, passes from the anode through
the solution to the cathode, removing metal from the former and
depositing it upon the latter. In a primary battery using zinc as the
positive element and the negative terminal, current is caused to pass,
within the cell, from the zinc to the negative element and zinc is
dissolved. Following the same law, any pipe buried in the earth may
serve to carry current from one region to another. As single-trolley
traction systems with positive trolley wires constantly are sending
large currents through the earth toward their power stations, such a
pipe may be of positive potential with relation to moist earth at some
point in its length. Current leaving it at such a point may cause its
metal to dissolve enough to destroy the usefulness of the pipe for its
intended purpose.
Lead-sheathed telephone cables in the earth are particularly exposed
to such damage by electrolysis. The reasons are that such cables often
are long, have a good conductor as the sheath-metal, and that metal
dissolves readily in the presence of most aqueous solutions when
electrolytic differences of potential exist. The length of the cables
enables them to connect between points of considerable difference of
potential. It is lack of this length which prevents electrolytic
damage to masses of structural metal in the earth.
Electrical power is supplied to single-trolley railroads principally
in the form of direct current. Usually all the trolley wires of a city
are so connected to the generating units as to be positive to the
rails. This causes current to flow from the cars toward the power
stations, the return path being made up jointly of the rails, the
earth itself, actual return wires which may supplement the rails, and
also all other conducting things in the earth, these being principally
lead-covered cables and other pipes. These conditions establish
definite areas in which the currents tend to leave the cables and
pipes, _i.e._, in which the latter are positive to other things. These
positive areas usually are much smaller than the negative areas, that
is, the regions in which currents tend _to enter_ the cables form a
larger total than the regions in which the currents tend _to leave_
the cables. These facts simplify the ways in which the cables may be
protected against damage by direct currents leaving them and also they
reduce the amount, complication, and cost of applying the corrective
and preventive measures.
All electric roads do not use direct current. Certain simplifications
in the use of single-phase alternating currents in traction motors
have increased the number of roads using a system of
alternating-current power supply. Where alternating current is used,
the electrolytic conditions are different and a new problem is set,
for, as the current flows in recurrently different directions, an area
which at one instant is positive to others, is changed the next
instant into a negative area. The protective means, therefore, must be
adapted to the changed requirements.
CHAPTER XIX
PROTECTIVE MEANS
Any of the heating hazards described in the foregoing chapter may
cause currents which will damage apparatus. All devices for the
protection of apparatus from such damage, operate either to stop the
flow of the dangerous current, or to send that flow over some other
path.
Protection Against High Potentials. Lightning is the most nearly
universal hazard. All open wires are exposed to it in some degree.
Damaging currents from lightning are caused by extraordinarily high
potentials. Furthermore, a lightning discharge is oscillatory; that
is, alternating, and of very high frequency. Drops, ringers,
receivers, and other devices subject to lightning damage suffer by
having their windings burned by the discharge. The impedance these
windings offer to the high frequency of lightning oscillations is
great. The impedance of a few turns of heavy wire may be negligible to
alternating currents of ordinary frequencies because the resistance of
the wire is low, its inductance small, and the frequency finite. On
the other hand, the impedance of such a coil to a lightning discharge
is much higher, due to the very high frequency of the discharge.
Were it not for the extremely high pressure of lightning discharges,
their high frequency of oscillation would enable ordinary coils to be
self-protecting against them. But a discharge of electricity can take
place through the air or other insulating medium if its pressure be
high enough. A pressure of 70,000 volts can strike across a gap in air
of one inch, and lower pressures can strike across smaller distances.
When lightning encounters an impedance, the discharge seldom takes
place through the entire winding, as an ordinary current would flow,
usually striking across whatever short paths may exist. Very often
these paths are across the insulation between the outer turns of a
coil. It is not unusual for a lightning discharge to plow its way
across the outer layer of a wound spool, melting the copper of the
turns as it goes. Often the discharge will take place from inner turns
directly to the core of the magnet. This is more likely when the core
is grounded.
_Air-Gap Arrester_. The tendency of a winding to oppose lightning
discharges and the ease with which such discharge may strike across
insulating gaps, points the way to protection against them. Such
devices consist of two conductors separated by an air space or other
insulator and are variously known as lightning arresters, spark gaps,
open-space cutouts, or air-gap arresters. The conductors between which
the gap exists may be both of metal, may be one of metal and one of
carbon, or both of carbon. One combination consists of carbon and
mercury, a liquid metal. The space between the conductors may be
filled with either air or solid matter, or it may be a vacuum.
Speaking generally, the conductors are separated by some insulator.
Two conductors separated by an insulator form a condenser. The
insulator of an open-space arrester often is called the dielectric.
[Illustration Fig. 203. Saw Tooth Arrester]
Discharge Across Gaps:--Electrical discharges across a given distance
occur at lower potentials if the discharge be between points than if
between smooth surfaces. Arresters, therefore, are provided with
points. Fig. 203 shows a device known as a "saw-tooth" arrester
because of its metal plates being provided with teeth. Such an
arrester brings a ground connection close to plates connected with the
line and is adapted to protect apparatus either connected across a
metallic circuit or in series with a single wire circuit.
Fig. 201 shows another form of metal plate air-gap arrester having the
further possibility of a discharge taking place from one line wire to
the other. Inserting a plug in the hole between the two line plates
connects the line wires directly together at the arrester. This
practice was designed for use with series lines, the plug
short-circuiting the telephone set when in place.
A defect of most ordinary types of metal air-gap lightning arresters
is that heavy discharges tend to melt the teeth or edges of the
plates and often to weld them together, requiring special attention
to re-establish the necessary gap.
Advantages of Carbon:--Solid carbon is found to be a much better
material than metal for the reasons that a discharge will not melt it
and that its surface is composed of multitudes of points from which
discharges take place more readily than from metals.
[Illustration Fig. 204. Saw-Tooth Arrester]
[Illustration Fig. 205. Carbon Block Arrester]
Carbon arresters now are widely used in the general form shown in Fig.
205. A carbon block connected with a wire of the line is separated
from a carbon block connected to ground by some form of insulating
separator. Mica is widely used as such a separator, and holes of some
form in a mica slip enable the discharge to strike freely from block
to block, while preventing the blocks from touching each other.
Celluloid with many holes is used as a separator between carbon
blocks. Silk and various special compositions also have their uses.
[Illustration Fig. 206. Arrester Separators]
Dust Between Carbons:--Discharges between the carbon blocks tend to
throw off particles of carbon from them. The separation between the
blocks being small--from .005 to .015 inch--the carbon particles may
lodge in the air-gap, on the edges of the separator, or otherwise, so
as to leave a conducting path between the two blocks. Slight moisture
on the separator may help to collect this dust, thus placing a ground
on that wire of the line. This ground may be of very high resistance,
but is probably one of many such--one at each arrester connected to
the line. In special forms of carbon arresters an attempt has been
made to limit this danger of grounding by the deposit of carbon dust.
The object of the U-shaped separator of Fig. 206 is to enable the
arrester to be mounted so that this opening in the separator is
downward, in the hope that loosened carbon particles may fall out of
the space between the blocks. The deposit of carbon on the inside
edges of the U-shaped separator often is so fine and clings so tightly
as not to fall out. The separator projects beyond the blocks so as to
avoid the collection of carbon on the outer edges.
Commercial Types:--Fig. 207 is a commercial form of the arrangement
shown in Fig. 205 and is one of the many forms made by the American
Electric Fuse Company. Line wires are attached to outside binding
posts shown in the figure and the ground wire to the metal binding
post at the front. The carbon blocks with their separator slide
between clips and a ground plate. The air-gap is determined by the
thickness of the separator between the carbon blocks.
[Illustration: Fig. 207. Carbon Block Arrester]
[Illustration: Fig. 208 Roberts "Self-Cleaning" Arrester]
The Roberts carbon arrester is designed with particular reference to
the disposal of carbon dust and is termed self-cleaning for that
reason. The arrangement of carbons and dielectric in this device is
shown in Fig. 208; mica is cemented to the line carbon and is large
enough to provide a projecting margin all around. The spark gap is not
uniform over the entire surface of the block but is made wedge-shaped
by grinding away the line carbon as shown. It is claimed that a
continuous arcing fills the wedge-shaped chamber with heated air or
gas, converting the whole of the space into a field of low resistance
to ground, and that this gas in expanding drives out every particle of
carbon that may be thrown off. It seems obvious that the wedge-shaped
space offers greater freedom for carbon dust to fall out than in the
case of the parallel arrangement of the block faces.
An outdoor arrester for metallic circuits, designed by F.B. Cook, is
shown in Fig. 209. The device is adapted to mount on a pole or
elsewhere and to be covered by a protecting cap. The carbons are large
and are separated by a special compound intended to assist the
self-cleaning feature. The three carbons being grouped together as a
unit, the device has the ability to care for discharges from one
terminal to either of the others direct, without having to pass
through two gaps. In this particular, the arrangement is the same as
that of Fig. 204.
[Illustration: Fig. 209. Cook Air-Gap Arrester]
A form of Western Electric arrester particularly adapted for outside
use on railway lines is shown with its cover in Fig. 210.
[Illustration: Fig. 210. Western Electric Air-Gap Arrester]
The Kellogg Company regularly equips its magneto telephones with
air-gap arresters of the type shown in Fig. 211. The two line plates
are semicircular and of metal. The ground plate is of carbon,
circular in form, covering both line plates with a mica separator.
This is mounted on the back board of the telephone and permanently
wired to the line and ground binding posts.
[Illustration: OLD SWITCHBOARD OF BELL EXCHANGE SERVING CHINATOWN,
SAN FRANCISCO, CALIFORNIA]
[Illustration: Fig. 211. Kellogg Air-Gap Arrester]
Vacuum Arresters:--All of the carbon arresters so far mentioned depend
on the discharge taking place through air. A given pressure will
discharge further in a fairly good vacuum than in air. The National
Electric Specialty Company mounts three conductors in a vacuum of the
incandescent lamp type, Fig. 212. A greater separation and less
likelihood of short-circuiting can be provided in this way. Either
carbon or metal plates are adapted for use in such vacuum devices. The
plates may be further apart for a given discharge pressure if the
surfaces are of carbon.
[Illustration: Fig. 212. Vacuum Arrester]
Introduction of Impedance:--It has been noted that the existence of
impedance tends to choke back the passage of lightning discharge
through a coil. Fig. 213 suggests the relation between such an
impedance and air-gap arrester. If the coil shown therein be considered
an arrangement of conductors having inductance, it will be seen that a
favorable place for an air-gap arrester is between that impedance and
the line. This fact is made known in practice by frequent damage to
aërial cables by electricity brought into them over long open wires,
the discharge taking place at the first turn or bend in the aërial
cable; this discharge often damages both core and sheath. It is well to
have such bends as near the end of the cable as possible, and turns or
goosenecks at entrances to terminals have that advantage.
[Illustration: Fig. 213. Impedance and Air-Gap]
This same principle is utilized in some forms of arresters, such as
the one shown in Fig. 214, which provides an impedance of its own
directly in the arrester element. In this device an insulating base
carries a grounded carbon rod and two impedance coils. The impedance
coils are wound on insulating rods, which hold them near, but not
touching, the ground carbon. The coils are arranged so that they may
be turned when discharges roughen the surfaces of the wires.
[Illustration: Fig. 214. Holtzer-Cabot Arrester]
Metallic Electrodes:--Copper or other metal blocks with roughened
surfaces separated by an insulating slip may be substituted for the
carbon blocks of most of the arresters previously described. Metal
blocks lack the advantage of carbon in that the latter allows
discharges at lower potentials for a given separation, but they have
the advantage that a conducting dust is not thrown off from them.
[Illustration: Fig. 215. Carbon Air-Gap Arrester]
Provision Against Continuous Arc:--For the purpose of short-circuiting
an arc, a globule of low-melting alloy may be placed in one carbon
block of an arrester. This feature is not essential in an arrester
intended solely to divert lightning discharges. Its purpose is to
provide an immediate path to ground if an arc arising from artificial
electricity has been maintained between the blocks long enough to melt
the globule. Fig. 215 is a plan and section of the Western Electric
Company's arrester used as the high potential element in conjunction
with others for abnormal currents and sneak currents; the latter are
currents too small to operate air-gap arresters or substantial fuses.
Protection Against Strong Currents. _Fuses._ A fuse is a metal
conductor of lower carrying capacity than the circuit with which it is
in series at the time it is required to operate. Fuses in use in
electrical circuits generally are composed of some alloy of lead,
which melts at a reasonably low temperature. Alloys of lead have lower
conductivity than copper. A small copper wire, however, may fuse at
the same volume of current as a larger lead alloy wire.
Proper Functions:--A fuse is not a good lightning arrester. As
lightning damage is caused by current and as it is current which
destroys a fuse, a lightning discharge _can_ open a circuit over which
it passes by melting the fuse metal. But lightning may destroy a fuse
and at the same discharge destroy apparatus in series with the fuse.
There are two reasons for this: One is that lightning discharges act
very quickly and may have destroyed apparatus before heating the fuse
enough to melt it; the other reason is that when a fuse is operated
with enough current even to vaporize it, the vapor serves as a
conducting path for an instant after being formed. This conducting
path may be of high resistance and still allow currents to flow
through it, because of the extremely high pressure of the lightning
discharge. A comprehensive protective system may include fuses, but it
is not to be expected that they always will arrest lightning or even
assist other things in arresting lightning. They should be considered
as of no value for that purpose. Furthermore, fuses are best adapted
to be a part of a general protective system when they do all that they
must do in stopping abnormal currents and yet withstand lightning
discharges which may pass through them. Other things being equal, that
system of protection is best in which all lightning discharges are
arrested by gap arresters and in which no fuses ever are operated by
lightning discharges.
Mica Fuse:--A convenient and widely used form of fuse is that shown in
Fig. 216. A mica slip has metal terminals at its ends and a fuse wire
joins these terminals. The fuse is inserted in the circuit by clamping
the terminals under screws or sliding them between clips as in Figs.
217 and 218. Advantages of this method of fuse mounting for protecting
circuits needing small currents are that the fuse wire can be seen, the
fuses are readily replaced when blown, and their mountings may be made
compact. As elements of a comprehensive protective system, however, the
ordinary types of mica-slip fuses are objectionable because too short,
and because they have no means of their own for extinguishing an arc
which may follow the blowing of the fuses. As protectors for use in
distributing low potential currents from central-office power plants
they are admirable. By simple means, they may be made to announce
audibly or visibly that they have operated.
[Illustration: Fig. 216. Mica Slip Fuse]
[Illustration: Fig. 217. Postal Type Mica Fuse]
[Illustration: Fig. 218. Western Union Type Mica Fuse]
Enclosed Fuses:--If a fuse wire within an insulating tube be made to
connect metal caps on that tube and the space around the tube be
filled with a non-conducting powder, the gases of the vaporized fuse
metal will be absorbed more quickly than when formed without such
imbedding in a powder. The filling of such a tubular fuse also muffles
the explosion which occurs when the fuse is vaporized.
[Illustration: Fig. 219. Pair of Enclosed Fuses]
Fuses of the enclosed type, with or without filling, are widely used
in power circuits generally and are recommended by fire insurance
bodies. Fig. 219 illustrates an arrester having a fuse of the enclosed
type, this example being that of the H. W. Johns-Manville Company.
[Illustration Fig. 220. Bank of Enclosed Fuses]
In telephony it is frequently necessary to mount a large number of
fuses or other protective devices together in a restricted space. In
Fig. 220 a group of Western Electric tubular fuses, so mounted, is
shown. These fuses have ordinarily a carrying capacity of 6 or 7
amperes. It is not expected that this arrester will blow because 6 or
7 amperes of abnormal currents are flowing through it and the
apparatus to be protected. What is intended is that the fuse shall
withstand lightning discharges and when a foreign current passes
through it, other apparatus will increase that current enough to blow
the fuse. It will be noticed that the fuses of Fig. 220 are open at
the upper end, which is the end connected to the exposed wire of the
line The fuses are closed at the lower end, which is the end connected
to the apparatus. When the fuse blows, its discharge is somewhat
muffled by the lining of the tube, but enough explosion remains so
that the heated gases, in driving outward, tend to break the arc which
is established through the vaporized metal.
A pair of Cook tubular fuses in an individual mounting is shown in
Fig. 221. Fuses of this type are not open at one end like a gun, but
opportunity for the heated gases to escape exists at the caps. The
tubes are made of wood, of lava, or of porcelain.
Fig. 222 is another tubular fuse, the section showing the arrangement
of asbestos lining which serves the two purposes of muffling the sound
of the discharge and absorbing and cooling the resulting gases.
[Illustration: Fig. 221. Pair of Wooden Tube Fuses]
_Air-Gap vs. Fuse Arresters._ It is hoped that the student grasps
clearly the distinction between the purposes of air-gap and fuse
arresters. The air-gap arrester acts in response to high voltages,
either of lightning or of high-tension power circuits. The fuse acts in
response to a certain current value flowing through it and this minimum
current in well-designed protectors for telephone lines is not very
small. Usually it is several times larger than the maximum current
apparatus in the line can safely carry. Fuses _can_ be made so delicate
as to operate on the very smallest current which could injure apparatus
and the earlier protective systems depended on such an arrangement. The
difficulty with such delicate fuses is that they are not robust enough
to be reliable, and, worse still, they change their carrying capacity
with age and are not uniform in operation in different surroundings and
at different temperatures. They are also sensitive to lightning
discharges, which they have no power to stop or to divert.
Protection Against Sneak Currents. For these reasons, a system
containing fuses and air-gap arresters only, does not protect against
abnormal currents which are continuous and small, though large enough
to injure apparatus _because_ continuous. These currents have come to
be known as sneak currents, a term more descriptive than elegant.
Sneak currents though small, may, when allowed to flow for a long time
through the winding of an electromagnet for instance, develop enough
heat to char or injure the insulation. They are the more dangerous
because insidious.
[Illustration: Fig. 222. Tubular Fuse with Asbestos Filling]
_Sneak-Current Arresters._ As typical of sneak-current arresters,
Fig. 223 shows the principle, though not the exact form, of an
arrester once widely used in telephone and signal lines. The normal
path from the line to the apparatus is through a small coil of fine
wire imbedded in sealing wax. A spring forms a branch path from the
line and has a tension which would cause it to bear against the ground
contact if it were allowed to do so. It is prevented from touching
that contact normally by a string between itself and a rigid support.
The string is cut at its middle and the knotted ends as thus cut are
imbedded in the sealing wax which contains the coil.
[Illustration: Fig. 223. Principle of Sneak-Current Arrester]
A small current through the little coil will warm the wax enough to
allow the string to part. The spring then will ground the line. Even
so simple an apparatus as this operates with considerable accuracy.
All currents below a certain critical amount may flow through the
heating coil indefinitely, the heat being radiated rapidly enough to
keep the wax from softening and the string from parting. All currents
above this critical amount will operate the arrester; the larger the
current, the shorter the time of operating. It will be remembered that
the law of these heating effects is that the heat generated =
_C^{2}Rt_, so that if a certain current operates the arrester in, say
40 seconds, twice as great a current should operate the arrester in 10
seconds. In other words, the time of operation varies inversely as the
square of the current and inversely as the resistance. To make the
arrester more sensitive for a given current--_i.e._, to operate in a
shorter time--one would increase the resistance of the coil in the wax
either by using more turns or finer wire, or by making the wire of a
metal having higher specific resistance.
The present standard sneak-current arrester embodies the two elements
of the devices of Fig. 223: a _resistance_ material to transform the
dangerous sneak current into localized heat; and a _fusible_ material
softened by this heat to release some switching mechanism.
The resistance material is either a resistance wire or a bit of
carbon, the latter being the better material, although both are good.
The fusible material is some alloy melting at a low temperature. Lead,
tin, bismuth, and cadmium can be combined in such proportions as will
enable the alloy to melt at temperatures from 140° to 180° F. Such an
alloy is a solder which, at ordinary temperatures, is firm enough to
resist the force of powerful springs; yet it will melt so as to be
entirely fluid at a temperature much less than that of boiling water.
[Illustration: Fig. 224. Heat Coil]
_Heat Coil._ Fig. 224 shows a practical way of bringing the heating and
to-be-heated elements together. A copper spool is wound with resistance
wire. A metal pin is soldered in the bore of the spool by an easily
melting alloy. When current heats the spool enough, the pin may slide
or turn in the spool. It may slide or turn in many ways and this
happily enables many types of arresters to result. For example, the pin
may pull out, or push in, or push through, or rotate like a shaft in a
bearing, or the spool may turn on it like a hub on an axle. Messrs.
Hayes, Rolfe, Cook, McBerty, Kaisling, and many other inventors have
utilized these combinations and motions in the production of
sneak-current arresters. All of them depend on one action: the
softening of a low-melting alloy by heat generated in a resistance.
When a heat coil is associated with the proper switching springs, it
becomes a sneak-current arrester. The switching springs always are
arranged to ground the line wire. In some arresters, the line wire is
cut off from the wire leading toward the apparatus by the same
movement which grounds it. In others, the line is not broken at all,
but merely grounded. Each method has its advantages.
Complete Line Protection. Fig. 225 shows the entire scheme of protectors
in an exposed line and their relation to apparatus in the central-office
equipment and at the subscriber's telephone. The central-office
equipment contains heat coils, springs, and carbon arresters. At some
point between the central office and the subscriber's premises, each
wire contains a fuse. At the subscriber's premises each wire contains
other fuses and these are associated with carbon arresters. The figure
shows a central battery equipment, in which the ringer of the telephone
is in series with a condenser. A sneak-current arrester is not required
at the subscriber's station with such equipment.
Assume the line to meet an electrical hazard at the point _X_. If this
be lightning, it will discharge to ground at the central office or at
the subscriber's instrument or at both through the carbon arresters
connected to that side of the line. If it be a high potential from a
power circuit and of more than 350 volts, it will strike an arc at the
carbon arrester connected to that wire of the line in the central
office or at the subscriber's telephone or at both, if the separation
of the carbons in those arresters is .005 inch or less. If the carbon
arresters are separated by celluloid, it will burn away and allow the
carbons to come together, extinguishing the arc. If they are separated
by mica and one of the carbons is equipped with a globule of
low-melting alloy, the heat of the arc will melt this,
short-circuiting the gap and extinguishing the arc. The passage of
current to ground at the arrester, however, will be over a path
containing nothing but wire and the arrester. The resulting current,
therefore, may be very large. The voltage at the arrester having been
350 volts or more, in order to establish the arc, short-circuiting the
gap will make the current 7 amperes or more, unless the applied
voltage miraculously falls to 50 volts or less. The current through
the fuse being more than 7 amperes, it will blow promptly, opening the
line and isolating the apparatus. It will be noted that this
explanation applies to equipment at either end of the line, as the
fuse lies between the point of contact and the carbon arrester.
[Illustration: Fig. 225. Complete Line Protection]
Assume, on the other hand, that the contact is made at the point _Y_.
The central-office carbon arrester will operate, grounding the line and
increasing the amount of current flowing. There being no fuse to blow,
a worse thing will befall, in the overheating of the line wire and the
probable starting of a fire in the central office. It is obvious,
therefore, that a fuse must be located between the carbon arrester and
any part of the line which is subject to contact with a potential which
can give an abnormal current when the carbon arrester acts.
Assume, as a third case, that the contact at the point _X_ either is
with a low foreign potential or is so poor a contact that the
difference of potential across the gap of the carbon arrester is lower
than its arcing point. Current will tend to flow by the carbon
arrester without operating it, but such a current must pass through
the winding of the heat coil if it is to enter the apparatus. The
sneak current may be large enough to overheat the apparatus if allowed
to flow long enough, but before it has flowed long enough it will have
warmed the heat-coil winding enough to soften its fusible alloy and to
release springs which ground the line, just as did the carbon arrester
in the case last assumed. Again the current will become large and will
blow the fuse which lies between the sneak-current arrester and the
point of contact with the source of foreign current. In this case,
also, contact at the point _Y_ would have operated mechanism to ground
the line at the central office, and, no fuse interposing, the wiring
would have been overheated.
_Exposed and Unexposed Wiring._ Underground cables, cables formed of
rubber insulated wires, and interior wiring which is properly done,
all may be considered to be wiring which is unexposed, that is, not
exposed to foreign high potentials, discharges, sneak, or abnormal
currents. _All other wiring_, such as bare wires, aërial cables, etc.,
should be considered as _exposed_ to such hazards and a fuse should
exist in each wire between its exposed portion and the central office
or subscriber's instrument. The rule of action, therefore, becomes:
_The proper position of the fuse is between exposed and unexposed
wiring._
It may appear to the student that wires in an aërial cable with a lead
sheath--that sheath being either grounded or ungrounded--are not
exposed to electrical hazards; in the case of the grounded sheath,
this would presume that a contact between the cable and a high
potential wire would result merely in the foreign currents going to
ground through the cable sheath, the arc burning off the
high-potential wire and allowing the contact to clear itself by the
falling of the wire. If the assumption be that the sheath is not
grounded, then the student may say that no current at all would flow
from the high-potential wire.
Both assumptions are wrong. In the case of the grounded sheath, the
current flows to it at the contact with the high-potential wire; the
lead sheath is melted, arcs strike to the wires within, and currents
are led directly to the central office and to subscribers' premises.
In the case of the ungrounded sheath, the latter charges at once
through all its length to the voltage of the high-potential wire; at
some point, a wire within the cable is close enough to the sheath for
an arc to strike across, and the trouble begins. All the wires in the
cable are endangered if the cross be with a wire of the primary
circuit of a high-tension transmission line. Any series arc-light
circuit is a high-potential menace. Even a 450-volt trolley wire or
feeder can burn a lead-covered cable entirely in two in a few seconds.
The authors have seen this done by the wayward trolley pole of a
street car, one side of the pole touching the trolley wire and the
extreme end just touching the telephone cable.
The answer lies in the foregoing rule. Place the fuse between the wires
which _can_ and the wires which _can not_ get into contact with high
potentials. In application, the rule has some flexibility. In the case
of a cable which is aërial as soon as it leaves the central office,
place the fuses in the central office; in a cable wholly underground,
from central office to subscriber--as, for example, the feed for an
office building--use no fuses at all; in a cable which leaves the
central office underground and becomes aërial, fuse the wires just
where they change from underground to aërial. The several branches of
an underground cable into aërial ones should be fused as they branch.
Wires properly installed in subscribers' premises are considered
unexposed. The position of the fuse thus is at or near the point of
entrance of the wires into that building if the wires of the
subscriber's line outside the premises are exposed, as determined by
the definitions given. If the line is unexposed, by those definitions,
no protector is required. If one is indicated, it should be used, as
compliance with the best-known practice is a clear duty. Less than
what is known to be best is not honest practice in a matter which
involves life, limb, and indefinite degrees of property values.
Protectors in central-battery subscribers' equipments need no
sneak-current arresters, as the condenser reduces that hazard to a
negligible amount. Magneto subscribers' equipments usually lack
condensers in ringer circuits, though they may have them in talking
circuits on party lines. The ringer circuit is the only path through
the telephone set for about 98 per cent of the time. Sneak-current
arresters, therefore, should be a part of subscribers' station
protectors in magneto equipment, except in such rural districts as may
have no lighting or power wires. When sneak-current arresters are so
used the arrangement of the parts then is the same as in the
central-office portion of Fig. 225.
Types of Central-Office Protectors. A form of combined heat coil and
air-gap arrester, widely used by Bell companies for central-office
protection, is shown in Fig. 226. The two inner springs form the
terminals for the two limbs of the metallic-circuit line, while the
two outside springs are terminals for the continuation of the line
leading to the switchboard. The heat coils, one on each side, are
supported between the inner and outer springs. High-tension currents
jump to ground through the air-gap arrester, while sneak currents
permit the pin of the heat coil to slide within the sleeve, thus
grounding the outside line and the line to the switchboard.
[Illustration: Fig. 226. Sneak-Current and Air-Gap Arrester]
_Self-Soldering Heat Coils._ Another form designed by Kaisling and
manufactured by the American Electric Fuse Company is shown in Fig.
227. In this the pin in the heat coil projects unequally from the ends
of the coil, and under the action of a sneak current the melting of
the solder which holds it allows the outer spring to push the pin
through the coil until it presses the line spring against the ground
plate and at the same time opens the path to the switchboard. When the
heat-coil pin assumes this new position it cools off, due to the
cessation of the current, and _resolders_ itself, and need only be
turned end for end by the attendant to be reset. Many are the
variations that have been made on this self-soldering idea, and there
has been much controversy as to its desirability. It is certainly a
feature of convenience.
[Illustration: Fig. 227. Self-Soldering Heat-Coil Arrester]
Instead of using a wire-wound resistance element in heat-coil
construction some manufacturers employ a mass of high-resistance
material, interposed in the path of the current. The Kellogg Company
has long employed for its sneak-current arrester a short graphite rod,
which forms the resistance element. The ends of this rod are
electroplated with copper to which the brass terminal heads are
soldered. These heads afford means for making the connection with the
proper retaining springs.
[Illustration: Fig. 228. Cook Arrester]
Another central-office protector, which uses a mass of special metal
composition for its heat producing element is that designed by Frank B.
Cook and shown in Fig. 228. In this the carbon blocks are cylindrical
in form and specially treated to make them "self-cleaning." Instead of
employing a self-soldering feature in the sneak-current arrester of
this device, Cook provides for electrically resoldering them after
operation, a clip being designed for holding the elements in proper
position and passing a battery current through them to remelt the
solder.
In small magneto exchanges it is not uncommon to employ combined fuse
and air-gap arresters for central-office line protection, the fuses
being of the mica-mounted type already referred to. A group of such
arresters, as manufactured by the Dean Electric Company, is shown in
Fig. 229.
[Illustration: Fig. 229. Mica Fuse and Air-Gap Arresters]
Types of Subscribers' Station Protectors. Figs. 230 and 231 show types
of subscribers' station protectors adapted to the requirements of
central-battery and magneto systems. These, as has been said, should be
mounted at or near the point of entrance of the subscriber's line into
the premises, if the line is exposed outside of the premises. It is
possible to arrange the fuses so that they will be safe and suitable
for their purposes if they are mounted out-of-doors near the point of
entrance to the premises. The sneak-current arrester, if one exists,
and the carbon arrester also, must be mounted inside of the premises or
in a protecting case, if outside, on account of the necessity of
shielding both of these devices from the weather. Speaking generally,
the wider practice is to put all the elements of the subscriber's
station protector inside of the house. It is nearer to the ideal
arrangement of conditions if the protector be placed immediately at the
point of entrance of the outside wires into the building.
[Illustration: Fig. 230. Western Electric Station Arrester]
[Illustration: Fig. 231. Cook Arrester for Magneto Stations]