Part III

THE TRACK CIRCUIT

"Perhaps no single invention in the history of the development of

railway transportation has contributed more towards safety and

despatch in that field than the track circuit. By this invention,

simple in itself, the foundation was obtained for the development of

practically every one of the intricate systems of railway block

signaling in use today wherein the train is, under all conditions,

_continuously active_ in maintaining its own protection.

"In other words, the track circuit is today the only medium recognized

as fundamentally safe by experts in railway signaling whereby _a

train or any part thereof may retain continuous and direct control of

a block signal while occupying any portion of the track guarded by the

signal_."

"To Mr. William Robinson the Patent Office records concede the honor

of having devised the first practical track or 'Rail circuit'. This

comprised what is termed the _closed_ track circuit. * * * Closed

track circuits are very reliable, wholly safe in principle, and simple

of application and maintenance."

The above paragraphs, quoted from the third annual report of the Block

Signal and Train Control Board to the Interstate Commerce Commission

under date of November 22, 1910, ably express in a few words what the

invention of the track circuit has meant to the railroads of this and

other countries. In order, however, that those who are not familiar

with the principles of the track circuit may have some general

knowledge of them, a simple, non-technical description is given, as

prepared some years ago by Mr. J. P. Coleman, of the Union Switch &

Signal Company.

Historical information on the development and use of direct current

and alternating current track circuits for roads using electricity for

propulsion purposes and those using steam will be found in a report on

this subject made by Committee X to the Railway Signal Association in

1910.

The Rail Circuit Principle

By J. P. Coleman.

Assuming that it is clearly understood that the current is generated

at the battery; that it flows from thence through the conductors (of

which the coils of the magnet form part) and back again to the

battery, and that the magnet is simply a device interposed in the

circuit for the purpose of transforming electrical energy into

mechanical (magnetic) energy, and that the latter can exist in an

electro-magnet only with the presence of the former, we are now

prepared to make clear the principle of an electric track section.

To assist in this, let us state an invariable law governing the flow

of currents: _If two or more paths be presented an electric current,

it immediately becomes divided, and flows in each in quantities

directly in proportion to the conductivity of each._

The unit of electrical resistance, whereby the comparative merits of

various materials and sizes of materials as conductors are designated,

is called an _ohm_, (just as the unit of lineal measurement whereby

the comparative lengths and sizes of various objects are designated,

is termed a _foot_) and we will therefore use that term in reference

to the resistance of a conductor.

[Illustration: Fig. 1]

Figure 1 represents an ordinary gravity battery, the conductors from

it, and the electro-magnet to which they connect; also the armature as

attracted by the magnet and overcoming the spring which tends to

withdraw it from the magnet.

Now, as long as the current flows through the magnet, this condition

of things remains unaltered; but let a second path be presented to the

current several hundred times less in resistance than the original

one, and the result is that several hundred parts of the current will

leave the magnet for the "short circuit," and consequently leave so

little remaining in the original one that the effect will be

practically to demagnetize the magnets.

[Illustration: Fig. 2]

Figure 2 will render this very apparent if we will assume the wire of

the magnet R to possess a resistance of 10 ohms, and the conductors

themselves a resistance so low as to be inappreciable and unworthy of

consideration.

[Illustration: Fig. 3]

[Illustration: Fig. 4]

Now, assume the current to be flowing and the magnet to be charged,

and let us take a piece of metal which has an electrical resistance of

1/100 of an ohm, and lay it across the conductors at any point between

the battery and the magnet. The result is, that instead of flowing

through 10 ohms resistance _via_ the magnet, it follows the invariable

rule, and takes that offering but 1/100 of an ohm; or, more to the

point, if we assume the conductors referred to to be one mile of steel

rails each (Fig. 3), and again leave their resistance (which would be

about one ohm each) out of consideration entirely, leaving that of the

magnet as first stated, and assume the bar of 1/100 of an ohm to be an

axle and pair of wheels (_a_) of a train (Fig. 4), which possess the

same resistance, we can readily see that the result would be exactly

the same, _i.e._, instead of all the current passing through the

magnets, as when the rails were unoccupied, the presence of the wheels

upon them would cause 999/1000 of the current to leave the magnet and

pass through _them_; they offering but 999/1000 of the resistance of

the magnets, and thus leaving but 1/1000 of the whole current passing

through them, which being so small a part of so feeble a current is

imperceptible and without sufficient influence to hold the magnet

charged. Therefore, it follows that the instant that a pair of wheels

enters upon a pair of rails which thus form part of the conductors of

an electrical current holding charged a magnet, that magnet becomes

practically demagnetized, and consequently loses all power to overcome

any opposing force in its armature.

When the armature of a magnet is arranged upon a small lever, by

motion of which a second circuit is closed or opened, or two or more

circuits are otherwise controlled, the entire device is termed a

relay. In all forms of this instrument, as is the case with almost

every other electrical instrument, the armature is so arranged as to

fall by gravity, or by tension of a small spring suitably arranged,

away from the cores of the magnets when they become demagnetized.

[Illustration: Fig. 5]

When switches are included in a track section (Fig. 5), it becomes

necessary for safety to have them control the track section in such a

way that unless they are properly set (and locked, if desired) for the

main track, the continuity of the rail circuit is interrupted and the

signal is thereby held at danger. To render more certain this result,

the circuit controller (switch box) at the switch is arranged in such

a way that the track circuit is not only interrupted beyond the

switch, but is also short-circuited by it when the switch is not

properly set. It is also necessary for safety that the side track from

the switch points back to the fouling point (Fig. 5) be included in

the track section: thus insuring that all trains on these tracks are

out of danger of collision with the main track when a "clear" signal

is displayed on it.

In dividing tracks into distinct electrical sections, it becomes

necessary to insulate the rail ends at the terminal of each, from

those of the adjacent sections. If this were not done the current of

each section would traverse the next, and continue on indefinitely,

influencing each other so as to interfere with or totally prevent the

operation of all.

In order that we may fully comprehend the nature of an insulation, let

us make clear a few facts concerning conductors in general. All

materials conduct electricity to a certain extent; but some with much

more freedom than others. Thus, silver, copper, gold, zinc, platinum,

iron, steel, mercury, and other pure metals permit the passage of an

electric current through them with but slight resistance, (although

all offer a certain amount,) and are therefore termed _conductors_.

The following liquids are classed as conductors: concentrated and

diluted acids, saline liquids and water, although they are much less

efficient as such than the metals.

To this list might be added the earth itself and the various

ingredients forming it, the nature of which ingredients determines

very much its efficiency as a conductor. Thus at points abounding in

mineral deposits the earth would be far superior as a conductor to

those parts in which none exist, but at best should be regarded as a

poor conductor.

Next comes a class of materials which offer a great resistance to the

current, and which from that reason are termed non-conductors, or

insulators; of this class, rubber, glass, leather, resin, wood,

brimstone and dry air are the most common.

Wood being a non-conductor, it is very evident that the cross-ties

under the steel rails form an insulation between them and the ground;

also, that if a piece of the same or similar material be placed

between the rail ends, and that if two other pieces of sufficient

strength be substituted for the iron fish-plates at that point, a

secure insulation will be formed between the rails.

It is precisely in this way that the insulation of one rail from

another is effected (Fig. 6) and the long, practical use of many

hundred joints of this sort, has proved it to be a method both

economical and thoroughly efficient.

[Illustration: Fig. 6]

A much more secure _joint_, however, is obtained by insulating the

existing iron fish-plates from the rails by means of heavy fiber

plates, and their bolts from the rails by fiber bushings (Fig. 7).

While this method is superior to the first mentioned one in that it

makes a more secure rail joint, it is no more efficient as an

insulation.

[Illustration: Fig. 7]

One would naturally suppose that owing to the large surface of contact

existing between the rails and their connecting or fish-plates, and

from the apparent security of that contact obtained by the bolts

through them, no trouble would be experienced by the current in

passing from one rail to the other. This, however, is not the case, as

the bolts and even the plates themselves frequently become loose, even

when provided with the best of nut locks, and the rust and dirt

settling between them and the rails oftentimes increase the resistance

of a track section to a serious extent. Again, even when tightly

bolted and locked, these plates form but an imperfect contact, owing

to the scale or rust upon them. Therefore, to insure that the

resistance of a track section may be as low and as constant as

possible, we have found it absolutely necessary to connect each two

adjacent rail ends together by means of a short piece of very strong

wire (Fig. 8).

[Illustration: Fig. 8]

These wires are termed "track wires" (bond wires) and are provided

with a button-head rivet at each end, which is securely soldered

thereto, for the purpose of securing them to the rails. (Bond wires

are now attached to the rails by channel pins or are welded on.) The

connections from the rails to the battery and relay of a track section

are secured to the rails in the same manner. The battery is usually

located in a chute or well sunk in the ground at the terminal of each

section, which is provided with an elevator in which the battery is

placed and by which it may be raised and lowered at will. All wires

when placed underground are run in grooved lumber in order that they

may be secure from injury.

Even in very wet or snowy weather a single jar of gravity battery is

generally found to furnish sufficient current to properly work the

relay at the other end of any section less than three-quarters of a

mile in length; although it frequently happens on longer sections and

occasionally on those of ordinary length that two jars are necessary.

A greater number of jars is never advisable since by increasing the

intensity of the current, the liability of its leaking from one rail

to the other during wet weather is correspondingly increased, and as

this is attended with some uncertainty in the working of the relay of

the section--due to the varying intensity of the current--it should be

carefully guarded against. As two jars of gravity battery are not

sufficient to operate a signal, lock, bell or any similar instrument

with any degree of certainty, it becomes necessary to have a second

set of batteries of a greater number of jars for that purpose. The

armature of the magnet controlled by the track section is therefore

made to control a second circuit using a battery of this sort (Figs.

3, 4 and 5) and which includes the magnet of the signal mechanism. The

use of a relay on a track section is therefore necessary; and when it

becomes necessary to control two or more devices, each requiring

independent circuits, by one track, the use of a relay is

indispensable.

Track Circuit Characteristics

While the fundamental principles of the track circuit are the same

today as they were when it was originally invented by Dr. Robinson in

1872, it has been found that it is not as simple a device as was

formerly supposed to be the case and many problems have arisen which

have required and is requiring the careful study of the signal

engineers. Accordingly, it is well to present briefly some of the

track circuit characteristics as they are known today. In the

following presentation, information has been collected from many

different sources, including abstracts from papers presented on the

track circuit by Mr. A. R. Fugina, signal engineer, and Mr. J. B.

Weigle, signal inspector on the Louisville & Nashville.

There are two general classes of track circuits, direct current and

alternating current, which may be further subdivided between single or

double rail circuits. The essential feature of the track circuit is

the insulation of each section of track from the adjoining sections.

Each rail in the section is connected to the one adjoining by bond

wires, for the purpose of making a continuous conductor from one end

of the section to the other.

Rail Bonding

Under the present methods of bonding, the angle bar carries the

greater part of the current, and bond wires frequently carry as little

as 20 per cent. of it and sometimes even less. The rail resistance is

lowest with new rails, but it gradually gets higher, due to rust and

dirt formations between the angle bar and the rail. But even with new

rail, the rail resistance varies greatly at different periods and even

at different times during any twenty-four hours. This variation is

entirely due to the fact that the angle bars carry more of the current

than the bond wires, and that the bond wires under any condition are

only large enough to carry the smaller part of the current from the

battery. The lower the resistance of the bonds the less variable will

be the rail resistance.

The resistance of the angle bars increases greatly as rail resistance

increases, as a result of which the angle bars rapidly carry less of

the current.

It is not infrequent to find the rail resistance to be as high as 0.20

ohms per 1,000 ft. of track, and we have known it to run as high as

0.264 in new rail, where especial attention had been given to

obtaining as good bonding as possible. Under such conditions the angle

bar carries very little of the current, the capacity of the bond is

not sufficient to carry the current, and the net result is a failing

track circuit, which is probably attributed to bad ballast, zinc

treated ties or other causes.

The principal defect in the track circuit is that of improper bonding.

The only explanation as to why No. 8 iron wires became standard for

bonding appears to be that the bond wires were cut from this size iron

telegraph wire which was in general use at the time rails began to be

bonded. It is important to obtain better bonding to obtain a minimum

constant rail resistance.

It has been recommended that:

First--The use of galvanized wire bonds should be eliminated.

Second--Forty per cent. copper clad bond wires should be used as a

temporary expedient to replace galvanized bond wires.

Third--Except for theft and crystallization, copper bond wires would

be much more advisable.

Fourth--Larger bond wires should be used, these bonds to be at least

equal in carrying capacity to two 46-in. No. 6 solid copper or to two

No. 2, 40 per cent. copper clad wires.

Until recently it has been the general opinion of all experts on the

track circuit that the rail resistance was rather an unimportant

factor and that, as a general rule, the change in rail resistance

could be disregarded in making track circuit investigations and

calculations.

Many bad track circuit conditions have been laid to bad ballast

conditions, zinc treated ties, wet track, etc., which, if carefully

analyzed, would have shown the trouble to be due to extremely high

rail resistance. These faulty conclusions are being drawn nearly every

day.

Single rail track circuits, so called from the fact that but one rail

is insulated, are also used. Installations of this kind are made to

avoid the expense of two insulated joints or where one rail is needed

for another circuit. Such track circuits are more liable to failure

than those having both rails insulated for the reason that the

break-down of one insulated joint will extend the circuit beyond the

proper limit and cause interference of neighboring circuits or

extended shunting of the relay, due to the presence of a train beyond

the insulated joint.

A track circuit may be made to perform two separate functions in which

the direction or polarity as well as the presence of current is made

use of in the relay, provided the first or principal function actuated

by the presence or absence of current does not interfere with the

secondary function, actuated both by the presence of current and its

polarity.

Where switches occur in a track circuit, special means must be

employed to prevent short-circuiting through the switch rods and

leakage of current to the turn-out rail. The usual method is the use

of insulated switch rods with insulated joints in the leads of the

turnout and at the fouling point of the turnout. The switch points are

bonded to the stock rails to insure shunting by a pair of wheels on

any part of the track.

None of the methods employed in running track circuits through

switches show any protection against an open switch. In order to

obtain this protection a switch instrument or switch box is used. This

consists of a device with electrical contacts, the whole mounted on a

switch timber and connected to the switch point by means of a rod so

arranged that when a switch slips open or is thrown open the movement

of the rod actuates contacts which, on being closed, form a closed

path from one rail to the other through wires connecting the rails to

the contacts, thus when the contacts are closed by a switch being

opened, the same effect is produced as if a train was on the circuit,

shunting it out.

On electrically operated roads where tracks are bonded for the return

propulsion current with heavy copper bonds, no additional bond wires

are necessary.

The Track Battery

The usual form of track circuit has a primary battery at one end of

the insulated track section, with the positive terminal of the battery

connected to one rail and the negative terminal to the other, while a

relay at the other end of the section is connected to the rails in a

similar manner. Current flows from the positive side of the battery

through the one rail, the relay and the other rail back to the

battery, thus keeping the relay energized.

For d.c. track circuits, four types of cells have been used to a

greater or less extent, the gravity cell; Lalande (soda) cell; storage

cell and dry cell. The gravity cell has a voltage of about 0.8 or 0.9

volts, the resistance varying with the manner in which the cell is

maintained and averaging about 3 ohms. It will remain active for long

periods on closed circuits without appreciable polarization. Because

of this high internal resistance usually no external resistance is

necessary to be connected between it and the rail of the track. The

e.m.f. of the Lalande (soda) cell may vary from about 0.67 volts to

0.88 volts while the internal resistance will range between 0.019

ohm to 0.4 ohm. Because of the low internal resistance of these cells

it is necessary to use an external resistance of the proper value

between the cell and the rail. The storage cell is made in various

capacities and a fully charged cell on open circuit has a voltage of

approximately 2.1 volts which, when placed on discharge, becomes

approximately 2 volts and drops to about 1.8 volts when completely

discharged. The voltage in this type of cell varies with the density

of the electrolyte and to a certain extent with temperature. It has

practically a negligible internal resistance and it is also necessary

to use an external resistance in the leads between the cell and the

track to prevent a flow of excessive current when a train occupies the

track. The dry cell is used only in emergency cases or occasionally

for open circuit track circuits of 2 or 3 rail lengths, which are

sometimes used as annunciator starts to announce the approach of a

train to a tower-man. It is designed primarily for open circuit work

and will polarize when current beyond a certain figure is drawn

continuously from it.

The Track Relay

The track relay is a development of the instrument of the same name

used in telegraph service. It consists of an electro-magnet of the

horseshoe type with a pivoted armature, carrying one or more fingers

for making or breaking electric circuits for the control of signal

apparatus.

Track relays with resistances of 2 and 4 ohms are usually employed.

From experience with two-ohm relays on the L. & N., covering a great

many of them on all kinds of circuits, the following conclusions are

reached:

The two-ohm relay is more suitable for general use on track

circuits than the four-ohm, provided not less than the R.S.A.

recommended limiting resistance is used between the battery and

track.

The two-ohm relay will operate satisfactorily where the four-ohm

will not on bad track circuits, and with considerably less current

consumption.

The two-ohm relay will operate equally as well on good track

circuits of average length as the four-ohm, there being little

difference in current consumption on this class of circuit. Under

the same conditions longer track circuits may be operated with the

two-ohm relay.

The two-ohm relay is at least as safe as the four ohm. It should be

thoroughly understood that it is as important with the four-ohm relay

as it is with the two-ohm relay to have not less than the R.S.A.

recommended limiting resistance between the battery and track. This is

important with any kind of low internal resistance battery, and under

certain conditions with gravity battery also.

In one case assume a train to be passing from the relay end to the

battery end of a track section and in the other case from the battery

end to the relay end. The effect accomplished is the same except that

the relay will not release so quickly when the train passes from the

battery end towards the relay end, and this is in part due to the

self-induction of the circuit through the relay coils, the rails and

the axles of the train. It is due more, however, to small current

leakage from the adjacent section and the effects of stray currents

which are always present to a greater or less degree. A broken rail

will also generally open the circuit and de-energize the relay.

Circuits for the control of the various signal devices are broken

through the contact points of the track relay.

Track Circuit Maintenance

Cross ties have a relatively high resistance to the passage of

electric current, but when a large number connect the rails many

multiple paths are introduced into the circuit through which the

current may flow from one rail to the other, and, considering them as

a whole, the resistance they offer to the passage of the current

reaches a relatively low value. Consequently there is always a current

leakage from rail to rail through the cross ties and ballast. Every

effort should be made to secure and maintain the best ballast and

drainage possible on d.c. as well as a.c. track circuits. Cinders,

dirty sand, soft water-logged ties and ballast not well cleaned away

from the base of the rail will produce track circuit trouble,

particularly during wet weather, while good rock ballast, sound ties

and clean track give the greatest efficiency.

The use of ties freshly treated with zinc chloride also reduces the

ballast resistance. If too many such ties are used in a track circuit

the current leakage between rails becomes so great that not enough

current reaches the relay to hold it closed, the effect being the same

as if a train is on the track circuit shunting out the relay. For good

results, the number of zinc-treated ties installed per year in any

track circuit should not be greater than 15 per cent. of the total

number of ties in that circuit.

Track Circuit Troubles

Some of the common track circuit ailments are relay and track battery

troubles, defective track connections, poor bonding and broken rails,

short circuits or shunts, excessive leakage and defective insulated

joints, all of which will cause the signals to be set in the danger

position, while defective relays, foreign current and poor wheel

contact may result in a false proceed signal indication with a train

in the block section.

It was the quite general practice to operate bad track circuits by

piling on gravity battery, either in multiple or multiple-series

arrangements to obtain operating results without any regard to the

safety of the circuit and, no doubt, many false proceed failures were

caused thereby.

The effect of temperature changes on track circuit operation are of

considerable importance. The track relay, which is generally housed in

a cast or sheet iron box, probably is affected more by changes in

temperature than any other part of the track circuit. The resistance

of a 2-ohm relay, which is 2 ohm at 70 degrees F., will be 2.22 ohm at

120 degrees F., and 1.69 ohm at 0 degrees F., a variation of .53 ohm.

The pick up and release of the relay, .2 and .1 volt, respectively, at

70 degrees F., will be .22 and .11 volt at 120 degrees F., and .17 and

.085 volt at 0 degrees F. A relay, with a normal resistance of 4 ohm

at 70 degrees F., will be 4.45 ohm at 120 degrees F. and 3.38 ohm at 0

degrees F., a variation of 1.07 ohm. The pick up and release, .3 and

.14 volt, respectively, at 70 degrees F., will be .33 and .16 volt at

120 degrees F. and .25 and .12 volt at zero.

The point which is intended to be brought out by these figures is that

when the temperature of the relay increases, a correspondingly higher

voltage is required to pick up the armature, and when the temperature

decreases the armature will hold up with lower voltage across the

coils. This indicates that a track relay is more liable to fail to

release due to an imperfect train shunt in cold weather than at any

other time.

Some of the best preventatives that may be provided to guard against

false proceed signals due to track relays failing to release with a

train in the circuit, are:

1. Use as much resistance as practicable between battery and

track.

2. Use low resistance bond wires, and maintain bonding in good

shape.

3. Keep ballast well cleared from contact with rails.

4. Maintain insulation in insulated track joints in good condition.

Aside from these simple remedies no definite rule can be given to

combat foreign current. If it is so troublesome that these methods do

not overcome it, the circuit affected must be carefully studied to

determine the source of the foreign current and its path to the rails,

then special means can usually be provided to overcome it.

Ballast Resistance and Leakage

The importance of ballast resistance has long been recognized, and

this always has been considered the great variable, whereas,

investigations show that the ballast resistance is at least no more

variable than the rail resistance, and that of the two it is more

important to reduce the rail resistance to a minimum, and especially

to establish it as a constant.

When the ballast leakage problem was first taken up (on the L. & N.),

various kinds of ballast were measured in both wet and dry weather,

the intention being to determine the lowest possible resistance per

1000 ft. for each kind of ballast. It was proposed in this way to

establish a standard minimum resistance per 1000 ft. for each kind of

ballast. For instance, if a number of measurements in wet weather

showed 8 ohms per 1000 ft. as a minimum for track circuits with

crushed rock ballast, it was the intention to adopt 8 ohms as the

standard minimum ballast resistance per 1000 ft. for all track

circuits where crushed rock ballast was in use. If a number of wet

weather measurements showed 4 ohms per 1000 ft. as a minimum for

cinder ballast, it was the intention to adopt 4 ohms as the standard

minimum ballast resistance per 1000 ft. for all track circuits where

cinder ballast was used. It was the intention to follow out the same

process and establish a standard for all kinds of ballast in use. This

was soon found to be impracticable.

After making many ballast resistance measurements, it was noticed that

the variation of the resistance on any track circuit, as between wet

and dry weather, generally followed quite a definite rule. For

instance: If the resistance per 1000 ft. of dry ballast was found to

be 28 ohms or more, it would be not less than 8 ohms per 1000 ft. when

wet; or if resistance of dry ballast was found to be between 22 and 28

ohms per 1000 ft., it would be not less than 6 ohms per 1000 ft. when

wet.

Once a relay is picked up or energized, but a small amount of current

is required to maintain it in that condition. This is one reason why

it is important to keep the ballast clear of the rails and it is

because of the condition which may cause a relay to remain energized

that rules are in force requiring the signalmen to disconnect a track

relay when track forces are changing out rails.

Combined Rail and Bond Wire Resistance

On circuits newly bonded with two 46-in. galvanized iron wires a

joint, the combined rail and bond wire resistance was found (on the L.

& N.) to vary from .02 ohm per 1000 ft. of track on some circuits to

.265 ohm on others, a difference of over 1300 per cent. This was

rather puzzling. After a great many measurements had been made on

different circuits it was found that no two measurements gave the same

results, notwithstanding the fact that in many circuits the size of

rail, length of bond wires, and age of bonding were exactly the same.

On account of the bonding being new and the channel pins well driven,

the contact between the bond wire and rail was above suspicion. The

only other part of a track circuit that could possibly be the cause of

this difference was in the contact between the angle bars and rails,

and this later proved to be the case. Actual measurements made in the

field proved that when the rail is new and the joint bolts tight,

nearly all of the current flowing from rail to rail passes through the

angle bars, whereas when the rails get old a coating of rust and dirt

forms between the rail and angle bars, forcing practically all of the

current through the bond wires. On most of the circuits measured on

the L. & N. the combined rail and bond wire resistance was found to be

less than .1 ohm per 1000 ft. of track, although many were found to be

between .10 and .30 ohm per 1000 ft. It is interesting to note that

two circuits were found bonded with two 52-in. iron wires, for which

the combined rail and bond wire resistance measured .410 ohm, and that

by adding two 40 per cent. copper clad bond wires to each joint the

combined resistance was reduced to .144 ohm.

The Growth of the Track Circuit

Unfortunately there exists little or no data regarding the mileage of

track circuits installed from the time the first installation was made

by Dr. Robinson at Kinzua, Pa., and Irvineton up to about 1905. During

the period between January 1, 1905, and September 30, 1906, the total

automatic block signal mileage installed was 1,710.6, which brought

the total up to 6,826.9 for the United States. Between September 30,

1906, and January 1, 1908, 3,976.1 miles of automatic signals were

installed, which increased the above total to 10,803.0 miles.

The Block Signal and Train Control Board, seeing the need for accurate

data in the signal field, started the tabulation of such statistics

when it compiled and issued Block Signal Statistics as of January 1,

1908. After this board went out of existence, the Bureau of Safety of

the Interstate Commerce Commission continued the collection and

publication of these data yearly. Perhaps no better word picture can

be given of what Dr. Robinson's invention has meant to the railroads

than to present the story in the form of a table showing the miles of

road and the track equipped with the track circuit since January 1,

1908. In addition to the table, the accompanying chart presents the

information in a graphical form.

[Illustration: Progress Chart of Automatic Signal Installations

Since January 1, 1908.]

Track Circuit Mileage for Automatic and Controlled Manual Signals

in the United States as Taken from I.C.C. Reports

----------+-------------------+---------------------------------------

| Automatic | Controlled Manual

+---------+---------+-------------------+-------------------

| | | Miles of Road | Miles of Track

| Miles | Miles +--------+----------+--------+----------

| of | of | Track |Continuous| Track |Continuous

| Road | Track |Circuits| Track |Circuits| Track

| | | at | Circuits | at | Circuits

| | |Station | |Station |

----------+---------+---------+--------+----------+--------+----------

January 1,|

1908 | 10,819.3| 18,534.1| 726.7 | 212.0 | 2118.0 | 410.8

1909 | 12,174.3| 20,590.9| 407.6 | 572.2 | 978.0 | 1413.0

1910 | 14,238.9| 23,771.3| 385.8 | 491.5 | 953.5 | 1371.3

1911 | 17,709.8| 29,151.6| 483.9 | 439.4 | 1119.3 | 739.9

1912 | 20,300.0| 33,343.8| 402.0 | 295.9 | 955.6 | 496.0

1913 | 22,196.6| 36,873.0| 370.2 | 228.3 | 868.9 | 380.3

1914 | 26,569.3| 44,461.2| 275.7 | 180.3 | 625.3 | 281.6

1915 | 29,863.5| 49,442.1| 250.5 | 145.1 | 549.3 | 185.7

1916 | 30,942.5| 51,119.7| 255.1 | 125.1 | 549.6 | 179.3

1917 | 32,954.6| 53,799.8| 230.3 | 132.0 | 524.8 | 155.5

1918 | 35,193.1| 57,083.6| 208.1 | 131.2 | 451.6 | 154.8

1919 | 36,989.4| 59,458.2| 221.2 | 256.9 | 483.8 | 441.2

1920 | 37,968.8| 60,992.3| 196.3 | 129.2 | 413.3 | 151.4

1921 | 38,543.9| 61,744.5| 206.8 | 125.7 | 422.6 | 166.4

----------+---------+---------+--------+----------+--------+----------

The first yearly report of the Bureau of Safety, I.C.C., on block

signals to contain information as to the miles of road and miles of

track on which alternating current track circuits were installed, was

that issued as of January 1, 1914. Data taken from that report up to

the last one issued is presented in the table below.

Alternating Current Track Circuit Mileage

----------------+---------------+----------------

| Miles of Road | Miles of Track

----------------+---------------+----------------

January 1, 1914 | 3,289.2 | 4,144.6

January 1, 1915 | 2,728.2 | 5,814.9

January 1, 1916 | 3,186.7 | 6,679.0

January 1, 1917 | 3,336.2 | 6,823.6

January 1, 1918 | 3,748.0 | 7,530.1

January 1, 1919 | 4,496.6 | 8,620.2

January 1, 1920 | 4,676.5 | 9,026.0

January 1, 1921 | 4,786.1 | 9,120.2

----------------+---------------+----------------

Alternating current track circuits have certain advantages over direct

current track circuits, particularly in respect to their immunity to

the dangerous effects of foreign direct current to which d.c. track

circuits in some communities are subjected. The above table is

therefore of interest as it shows the application of alternating

current as made to Dr. Robinson's invention of the closed track

circuit.

The Invention of the Track Circuit The history of Dr. William Robinson's invention of the track circuit, the fundamental unit which made possible our present automatic block signaling and interlocking systems · 第 2 / 3 章