The Thompson-Houston
System of Electric
Lighting.

“In its power to assume always that form of energy which happens to be the most useful lies the great importance of electricity.” This importance has been brought to the notice of the public by means of the many recent exhibitions. Public interest has been roused and there is everywhere a desire for information and a guide through this far reaching field for discovery and invention. And, although there are many works treating on electricity and electric light, people specially want a short and concise though thorough description of the various schemes by which electric light is produced. In this thesis the object is to give a brief treatise on one of the many schemes of producing light by electric currents viz—The Thomson-Houston System.

In pursuing the subject of electricity, the first thing noticed is the analogy and difference between the dynamo and its older and more powerful rival the steam engine. The resemblances are, First as in the development of the steam engine, but few of the improvements and inventions in electrical machines were made by mathematical leaders. Watt ran across the idea of the seperate condenser while repairing the Newcomen model and applied the expansion of steam to the steam engine by a mechanical accident rather than by his own ingenuity, and so we find the first designers of the dynamo were mechanics rather than philosophers. Secondly the tendency to disregard old methods and instruments because of new discoveries and inventions has, as in the steam engine, hindered the advancement in electrical science. As an example it has become customary to regard frictional and statical electric machines, for practical purposes, as obsolete, but recent discoveries seem to hint that they may yet be utilized. Lately Prof. Dodge has shown that dust and vapor whirling in the air may be settled by a discharge of electricity consisting of a continuous series of electric sparks. This has been utilized to clear the atmosphere in lead smelting works from the fumes of volatized lead and with its application comes the invention of Wimhurst which produces with a minimum of mechanical labor a continuous series of electric sparks and works admirably.

The differences between the engine’s and dynamo’s developement are: First the marvelously rapid developement of the dynamo as compared with that of the steam engine. Since 1867 when the term “dynamo electric machinery” even to scientific men had but little signification, the dynamo has been brought to a very high degree of perfection. Secondly , the development of the dynamo has reached a much higher degree of perfection than that of the steam engine. Among the best steam engines twenty per cent effeciency is considered as very good while a good dynamo gives out in the form of electricity, ninety per cent of the mechanical energy put in it. But the class of people who improved and made the steam engine what it is were as well educated in one sense as were the men who brought out the dynamo. While it is true that in Watt’s time the knowledge concerning steam was very meagre, yet the practical men who made the dynamo, did it by themselves as nearly all the teachers of electricity knew nothing except what may be called electrical tricks. As has been said ^[1] “The teachers and writers of textbooks, practically did not know that there was anything in common between the electricity from a rubbed glass machine and voltaic electricity, or to be brief, that there was a science of electricity as distinguished from mere natural history.” In fact as late as 1870 there were really no textbooks on electricity. Even now electrical knowledge is so meagre as to warrant the same writer’s expression, “We can not imagine a mechanical engineer mistaking a few inches for a few miles or a grocer compounding an ounce of sugar with a carload, but this gives too truthful an idea of the vagueness that still exists.”

In the distant future, electricity will be used for electric lighting only as subordinate to other uses to which it may be applied such as heating houses, taking place of stoves for cooking, being used as a substitute for the steam engine. In fact the motor is rapidly becoming of as much practical use as the electric light. The principle of the motor is just this; a certain amount of mechanical energy say thirty four horsepower per minute into the form of electric currents, which by the way gives enough current to run 45, 2000 candle power lamps, send the current and distance through suitable conductors and attach them to similar dynamo or dynamos but in such a manner that the current in the second set of dynamos flows in the reverse direction to that of the first; when, the armature of the second dynamo or dynamos will revolve and at the pulley or pulleys of the dynamos, aside from friction, will be given out 95% of the thirty-four horsepower, the loss being due to the resistance of the conductors. Now in practice a motor is placed on the arc light circuit the same as a lamp, for energy less than twelve horsepower. It does not affect the lights and is a clean, neat way of obtaining energy.

But however true the foregoing may be, the greatest present use of electricity is to start and maintain light. There are several so-called systems, embracing dynamos, lamps, regulators, etc, from which I select the Thomson-Houston as the one for the purpose of describing for several reasons, first , it is at least as good as the average system of which there is a mushroom growth; second , valuble information was kindly offered by the parent Company; third , a good plant is near to which free acess was given, and fourth , we have at the Mechanical Hall of this University, a dynamo, loaned by the parent Company, which affords information without any inconvenience. As each part of the system comes up to be described a little of its history will be given. As the first part of a system necessary to be produced is the current generator we will first describe

In considering the current generator the first thing to be decided upon is the definition of the term dynamo. The following is thought to be a correct definition,—A dynamo or dynamo electric machine is a machine which is used to convert energy in the form of mechanical motion into energy of electric currents, or vica-versa . Those used to generate currents of electricity are called dynamos, those used to generate mechanical motion are known as motors.

In attempting to make clear the theory of the dynamo, we will recall some simple experiments. In Fig. 1, send a current around B from right to left. Now A being free to move vertically either up or down, connect its binding posts to a galvanometer (that is, an instrument used to tell the direction of a current and also used to test the relative strength of two or more currents) and move A up suddenly when a current will be generated in A whose direction will be the same as that of the current in B. Now this current is not created energy, because in lifting ^[2] the coil A, work is expending against the attraction between the coils, as between two currents flowing in the same direction there is an attraction. If we pursue this experiment in its various forms we will find the following statement known as Lentz law is true, viz: “If the relative positions of two conductors A and B be changed of which B is traversed by a current, a current is induced in A in such a direction that by its electro dynamic action on the current in B it would have imparted to the conductor a motion of the contrary kind to that by which the inducing action was produced.”

The theory of this law is that around every wire carrying a current there is a magnetic whirl (Fig. 3). Now if the conducting wire be passed through a hole in a horizontal plate of glass and iron filings be sifted upon the latter they will arrange themselves, as shown in Fig. 2., along lines, radial in this case, known as lines of force, which arranging is due to the magnetic attraction of the current in the wire upon the iron filings. Now in B. Fig. 1, every portion of the wire has just such a whirl and just such lines of force, or magnetic field, and when A is moved each part of the wire of A cuts one or more lines of force of the many magnetic fields making up the magnetic field of the entire coil B. Now when the wire of coil A cuts magnetic field of B a current is generated in A acording to the following statement known as Faraday’s Law; “When a conductor in a field of force moves in any way so as to cut the lines of force there is an electromotive force produced in the conductor in such a direction that supposing a figure swimming in the conductor to turn to look along the positive direction of the lines of force (in Fig. 1, toward axis of B), and the conductor be moved to his right, he will be swimming with the current so induced.” Hence in Fig. 1, the current generated in it will be from left to right.

Practically Faraday’s principle means just this: by moving a wire across a space where there are magnetic lines, the motion of the wire as it cuts the magnetic lines sets up around the cutting wire a magnetic whirl or in other words sets up a current in that wire.

The foregoing laws are the “principles of the dynamo,” yet after their deduction, the progress of the evolution of the dynamo was slow and attended by many dificulties. Between 1860 and 1870 however, a working knowledge of these laws became the property of thousands of mechanics, and by comparing the number of inventions before and after that date (1860) the present generous growth of systems, dynamos and lamps, prove that inventions were almost in proportion to the number of people who had any electrical knowledge. In 1866 Wilde produced a toy magneto-electric machine for giving shocks, in which he used excited electromagnets. In the same years Varley and others produced a machine which excited its own field magnets the type of all machines used in practice. With this principle of Varley’s and Pacinnotti’s ring, Gramme produced in 1871 his since famous continuous current generator, one of which the second dynamo electric machine ever brought to this country can now be seen at the engine house at Purdue University. In 1877 Silas Brush brought out his famous dynamo and it may be interesting to know that he designed and had one made without experimenting in the least. In the following year a patent was issued to Messrs. Elihu Thomson and Edwin J. Houston, Professors of electricity in Philadelphia on the present though much improved Thomson Houston Dynamo.

Fig. 1.

Fig. 2.

Fig. 3.

Fig. 4.

Fig. 5.

Fig. 6.

Fig. 7.

To go back to Lentz and Faraday’s laws and carefully consider them we can but assent to S. P. Thompson’s “fifteen propositions on the dynamo” which are:—1. A part of the energy of an electric current exists in the form of a magnetic whirl surrounding the wire.

2. Currents may be generated in a wire by setting up these whirls.

3. We can set up these whirls by increasing or decreasing the relative distance between magnets and wires.

4. To set up and maintain these whirls consumes power.

5. To induce currents in a conductor there must be motion between them so as to alter the number of lines of force (Fig. 4 to 7).

6. Increase in the number of lines of force in the circuit produces a current of the opposite sense to decrease (Fig. 7).

7. Approach induces electromotive force in the opposite direction to that induced by retreat.

8. The stronger the magnetic field the stronger the current.

9. The more rapid the motion the stronger the current.

10. The greater the length of the conductor which cuts lines of force the stronger the current.

11. The shorter the conductor not so employed the stronger the current.

12. Approach being a finite process the approaching and receeding must give alternating directions to the current.

13. By the use of a commutator all the currents can be turned in the same direction.

14. In a steady circuit it makes no difference what kind of magnets are used to procure the requisite magnetic field whether permanent or electromagnets.

15. Hence the current of the generator may be used to excite the magnetism of field magnets.

Now the Thomson-Houston dynamo comes under that class of dynamos in which there is a rotation of coils in a uniform field of force, such rotation (Fig. 6.) being affected round an axis in the plane of the coil. Of course this dynamo is made like all others of its class to have first , as powerful field-magnets as possible, second , the armature or rotating coil has as great a lenght of wire in it as possible the wire being thick to offer little resistance and third , built to stand high rotative speed.

The simple theoretical dynamo is shown at Fig. 8, consisting of a single rectangular loop of wire rotating in the magnetic field formed by large magnets, and in order to take the current so generated from the loop so as to give a continuous current, we use a two part commutator (Fig. 9) consisting of a metal tube split in two and mounted on wood, each half connected to one end of the loop. The current is taken off by brushes which lead to the main circuit. But manifestly this dynamo would give no appreciable current becase it has a very small length of wire on the armature, so a great number of loops were used which at present constitute the so-called drum armature .

We may rotate the loops of wire in Fig. 8, on one of its sides as an axis or even push it farther from the center of revolution than that. To do this, wrap the wire around a ring and connect both ends to a two part commutator (Fig. 10). If instead of the ring in Fig. 10, being solid it be a number of coils of wire and if instead of there being one coil around the ring there be thirty we will have Pacinnotti’s ring before spoken of. If we used four to ten coils or “bobbins” of large size which is shown diagramatically at Fig. 11, we would have the Brush dynamo.

So with exceptions we may say that there are practically two types of dynamos as regards armatures, the ring type as Brush, Pacinnotti’s Gramme, and the drum armature (page 20).

The Thomson-Houston dynamo is like the rest of that dynamo, unique. To quote S. P. Thompson; “The Thomson-Houston spherical armature is unique among armatures, its cup shaped field magnets are unique among field magnets, its three part commutator is unique commutators.”

Fig. 8.
Simple Dynamo.

Fig. 9.

Fig. 10.

Fig. 11.

Fig. 12.

Fig. 13.

An armature of a dynamo is the rotating coil or coils which generates currents of electricity by moving in a magnetic field of force. It is the most important part of a dynamo as it is literally the current generator. So we first consider the Thomson-Houston

It is spheroidal in shape as is noted for the fact of its very seldom burning out , i. e., the electricity heating the wires of the armature to such an extent as to destroy the insulation or fuse the wires, either rendering the armature useless. It is made by keying two dish-shaped iron disks SS Fig. 12, to the shaft x and putting ribs dd about ten in number in the twenty-five light machine, and over the whole putting varnished paper. Then at stated intervals, pegs JJJ are driven into suitable holes in the disks and ribs to help in winding wire on the shell. Next three insulated wires of equal length are joined together at h Fig. 13, and the three wires are then wound over the shell in the following peculiar manner: one half of No. 1 is wound so as to form a zone of a sphere of which the shaft is in the same plane as the center circumference of the zone. The armature is then turned on the shaft as an axis 120° and one half of No. 2 is wound in the same manner as the first half of No. 1. The armature is moved 120° more and all of No. 3 is wound. The armature is then turned back, 120° on the shaft as an axis and the remainder of No. 2 is wound. Lastly the armature is turned back 120° more and the rest of No. 1 is wound. They are bound by wires gg Fig. 13 to hold them when rotating. The object of this rather complicated winding is to get the three coils equi distant from the shaft in order that each coil will generate practically the same current. Now as will be seen the overlapping wires will form a nearly spherical armature. The armature is mounted on the shaft x as an axis which extends far enough out from its bearings to put a pulley on the end H and a commutator on the other end to the three parts of which are fastened the three wires marked one, two, three, Fig. 13.

It has been urged that the repairs of this armature will be larger than on any other armature. If there should be a “burnout” it would necessitate the taking apart of the dynamo and sending the armature to the factory to be rewound. But it never burns out except through positive carelessness and it will be found that the repairs on this armature is less than on the armatures of its several powerful rivals taken separately even though they be of simpler construction.

When the Thomson-Houston armature is rotated between the cup-shaped fieldmagnets alternate currents are generated in each coil in turn and now the next point to be considered is the

which incites the alternate currents so formed into one continuous current. The commutator as before stated is fastened on the shaft at the end one, two, three Fig. 13. It consists of three copper plates in the form of a cylinder each segment A´A´A´ covering 115° of the dotted circle Fig. 14. They are screwed to rod CCC and DDD which are insulated by wood and gutta-percha plates EE from the iron mounting E´´ which is in turnescrewed to shaft by set screws shown. The wires one, two, three, have respectively red, white and blue insulation and are put in binding posts DDD marked one, two, three at the factory and if not so placed may work badly. The current enters D goes to B´B´ which there have direct contact with A .

Fig. 14.
Half Sec. A.B.

Fig. 15. Air blast Nozzles.

Fig. 16. Air blast Mechanism.

Fig. 17. Section of Dynamos.
Spherical Armature in Fig. 13.

Now in a three-part commutator the spark occurring as the segments pass under the brushes would very quickly destroy the surface and interfere with the currents in the coil. This difficulty is overcome by blowing out the spark by an air blast given at just the right place and time. The manner in which the blast is delivered is as follows: the segments of the commutator

are separated by gaps of about 5° and in front of each of the leading brushes there projects a nozzle, Fig. 15, which discharges an air blast alternately three times in each revolution. The blast itself is supplied by an ingenious piece of mechanism known as the

It consists of an elliptical box II whose sides have perforations II where air can enter while inside of this rotates a steel disk keyed to the armature shaft and having radial slots in which slide three wings RRR of ebonite which as they fly around drives air into the holes JJ leading to the nozzles Fig. 15. The result is that, since the spark is done away with, oil can be supplied to the commutator in limited quantities but still amply sufficient to reduce the wear on the commutator to such an extent that the life of a segment is greatly increased. The air blast is fastened to the dynamo frame just behind the commutator and can be see in Fig. 23.

as may be seen from Fig. 17, consists of two flanged iron tubes AA whose end consists of a convex segment of a sphere accurately turned to recieve the armature. Coils of wire CC which are in the outside circuit and through which the entire current flows are wound upon the tubes. After the armature is placed between them the two tubes are bolted together by heavy wrought iron bars BB and the whole carried on the frame work PN shown also at PN Fig. 23. Now a little magnetism only remains in the wrought iron bars and iron frame works when the armature first revolves, but the current even though slight, going through the coils makes an electromagnet out of each tube and heavily magnetizes the wrought iron bars and in two or three seconds after the armature first rotates it is entirely surrounded by a heavy magnetic field. One of the good points of these field magnets is that but very little magnetism is lost as compared with most other dynamos and since it takes power to maintain a heavy magnetic field, this dynamo is in this respect very economical.

Later on we will show that pushing the brushes together or pulling them apart alter the strength of the current, but for the present just accept the fact and we will show how the brushes are varied. It is accomplished by the mechanism shown in Fig. 18. The brushes are fixed to the levers YY and Y ₂ Y ₂ united by the lever l . The automatic movement is obtained by the electromagnet R while a dashpot J prevents too sudden motion. Suppose the brushes to be in the position shown when the current would get too strong owing to lights being cut out. The electromagnet R getting stronger would raise A and reduce the current taken off until current came to normal. If, instead, some lamps were thrown in the current would become weak and the electromagnet R would become weak, drop A which would increase current and this will continue till current reaches normal.

The foregoing regulating gear is used on small dynamos and old style large ones. On the large new style dynamo a more delicate regulating gear is used, the current which operates it being shown at Fig. 19. Normally the electromagnet R is short circuited by the wire r and only acts when this circuit is broken. At some point in the main circuit is a wall controller or controller magnet shown in Fig. 19, at ST, consisting of two electro magnet, Their yoke supported by a spring and the yoke operating the contact lever S. If the current becomes too strong the controller magnet circuit is broken and all the current of the main circuit goes through the electromagnet R which by its sudden increase of strength quickly raises A and thus alters the brushes. This only exists for a moment until the yoke of the controller magets fall because of their decrease of magnets strength, when current again flows through wire r because when yoke drops contact is made. This decreases the strength of electro magnet R thus dropping A and increasing current. Hence S will again raise and break contact and R again rais A . This is continually repeated.

of which there are four in use on all machines, are made of a broad strip of springy copper having six slits two thirds the distance up, and thus touching at several points. They are held by clamps shown at Fig. 23 which also shows the brushes. The brushes are held to the commutator by their own springiness and the variation of position due to strength of current. The brushes are set by a gauge sent with each dynamo which shows length from the end of brush to the holder. The holders are set at the correct angle by a gauge of brass of the shape of a right angled triangle the short side having a wide flange curved to fit the commutator for which it is sent, while the second side as regards length must fit to the holder when swung to it on the commutator as an axis.

After describing the details of the dynamo, we will at once proceed to find how the

In the diagram Fig. 19 the rotation is as in practice against the hands of the watch when seen from the commutator end of shaft. The three coils of the armature are represented by three lines A , B , C , united at their inner extremities each being joined to a segment of the commutator. There are two positive brushes P and F and two negative ones P´ and F´ . The current delivered to P and F goes round one of the field magnet coils, then to the outer circuit consisting of regulating gear, lamps, motors, etc., through the other field magnet coil to brushes P´ and F´. Now from Fig. 20, we observe that supposing the loop to be rotating against the hands of the watch in a magnetic field the diagram represents by arrows the direction of the electro-motive forces induced in those loops. The action is a maximum along the line of the resultant magnetic field m m´ and the minimum along the line n n´ which is at right angles to m m´. The reason that m m´ is not horizontal is that the induced poles of the armature is in advance of the poles of the field magnet and is constantly tending to be drawn back. Applying Fig. 20 to Fig. 19, we see that there will be an outward current in B , an inward one in C , A generating no current for that moment.

Now the following pair of brushes F F´ are shifted backward three times as far as P P´ is shifted forwards. When the current is the greatest possible the brushes P and F and P´ and F´ are 60° apart thus leaving P and F´ and P´ and F´ just 120° apart and since the segments of the commutator are each 120° in length ^[3] there will always be two coils in parralel with one another and in series with the third. Taking one sixth of a revolution and continuing all the way round we find the following tabulated statement showing brushes in contact with coils, to be true viz:—

Now suppose the current to become to strong owing to any cause, the following brushes are made to recede. This can but shorten the time that the brushes are in contact with the commutator when the coil is passing through that position in which it is generating the maximum amount of current and also hasten the time when it goes into parralel with a comparatively idle coil. If the current is to weak then the brushes are made to close up thus reducing the time that the most active coil is in parralel with one less active and also makes the brushes be longer in contact with the segment when the coil is generating its maximum amount of current. The motion of advance and retreat of the brushes is accomplished by the Thomson Regulating Gear before described. On Fig. 23 can be seen all the dynamo’s details except the Controller magnet .

Fig. 18.

Fig. 19.

Fig. 20.

Fig. 21.

Fig. 22.

As regards the Thomson-Houston Dynamo it will be found to produce the steadiest and most uniform current of any dynamo now in use. It regulating gear is the simplest and most natural one ever used. In its ability to reduce the current simaltaneously to one tenth of its former quantity inside of one or two minutes without injury to itself and lamps it stands alone, in practice.

Fig. 23.

Your engraving representing “ Dynamo Electric Machine with Thomsons Spherical Armature ”

—Taken from one of your catalogues, and pasted on a sheet of this paper—

In a system the most important thing next to the dynamo is the lamps. The first experimenter who produced an electric glow was Otto von Guericke. But neither the glow nor electric spark have been used to produce electric light for practical purposes, this was left to the voltaic arc on the one hand and the incandescent lamp on the other. Davy in 1800 mentions experiments in which electric light was obtained by electric sparks between two carbon points. He showed the arc ^[4] light for the first time in 1810 at the Royal Institute, which with Foucalt’s hand regulator (1844) Deleuil lit the Place de la Concorde, Paris. Thomas Wright in London (1845) devised the first apparatus which automatically adjusted the carbons. W. C. Staite used the electric current for the regulation of the carbons in 1848. In 1855 Serrin constructed a lamp which would have been used on a large scale had it not been for the cost of generating electricity. In 1876 Paul Jablochkoff invented his electric candles and in 1881 there were 4000 in use, but as their use increased their defects were found out. Regulated lamps were again brought into use and with them experimenters again endeavored to solve the problem of dividing the electric light. In 1877 Tschikoliff solved the problem in a very simple manner. He reasoned that, if the current be divided and part go through the carbons and make the arc and the rest go through an electromagnet and regulate the arc and the the current unite and when another light is wanted the current be again divided and reunited, the current may be divided any number of times and the scheme work nicely. When put in practice it worked very nicely and is used on most lamps at present. Suppose there be a lamp placed in the circuit. The current divides and the larger half goes through the carbons, as here there is no resistance as the carbons touche, while the remainder, going through a spiral of high resistance, is small. When the carbons burn away a little the arc is formed and the resistance increasing brings the regulating gear into operation. Now the strength of the current is the same after it has gone through the lamp as before because the current is going to get through either one way or the other, hence any number of lamps may go on in series, depending only upon the tension of the current.

Incandescent lamps were produced as early as 1859 but not till 1879 when Swan, Edison, Sawyer and others were they ever in a practical form. The first glow lamp Edison constructed had platinum wire to be heated. He however examined the properties of organic substances and finally fixed on bamboo fibre. The bamboo is divided into fibres one millimeter in diameter and twelve millimeters long. These fibres are pressed in U-shaped moulds and baked in ovens where they are allowed to become carbonized. The carbonized filament is attached to platinum wires which are fused in a glass vessel from which the air has been exhausted. We will speak more fully of the incandescent lamp when describing the Thomson Houston System’s incandescent lamp.

The Thomson Arc lamps was used by the Thomson Houston System since its begining till about two years ago when they stopped manufacturing them, only furnishing broken parts. The arc lamps at present used is

They are manufactured in two styles the single lamp used for stores, buildings etc., and the double lamp used for street service, all night work, etc. The light is produced by the voltaic arc between two carbons, the negative pole or lower carbon burning away about half as fast as the positive pole or upper carbon. The outside view of the single lamp is seen in Fig. 21 and of the double lamp in Fig. 22.

The regulation of the double lamp is diagramatically shown in Fig. 24, which is a plan of the lamp with cover removed, showing only a plan of cylindrical part of the lamp. The wires marked a b c d run along the top in order to be out of the way. In Fig. 24 the current comes in at the binding post and is at A divided into three currents A , B , and C . The current a goes to the yoke I of the electromagnets h and i and when the yoke is not held down by magnets h and i , it goes out wire a to binding post B . This only continues a moment until the current b which goes through the carbons and at the start has almost no resistance offered it, attracts the yoke I thus breaking contact of curcuit a until the current ceases or till both carbons burn away, when in the latter case the resistance of b becoming very high as compared to j and k but little current goes through h and i and I is raised by a weak spring not shown, thus making contact of circuit a , and since current a has little resistance as compared to b or c most of the current goes through it, thus practically making a cut-out. The current b goes round the electro-magnets h and i , then to the “bed” through screw J, the “bed” being a cast iron bottom of the cylinder E Fig. 22. From the bed it goes down carbon holder C (or H ) through carbons and arc to frame bed A Fig. 22. From there it comes up a wire by the side of frame C Fig. 22 and joins other currents at B . The third current a goes through electromagnets j and k and joins other currents at B .

This is when switch F Fig. 22 and M Fig. 24, is turned on . Now since the dynamo will regulate all differences in current the lamps can be turned on or off at will by any one. This is accomplished at the lamp by turning off the switch. When the switch is turned off , the current goes through d to screw K which is then touched by metal L (in contact with binding post B and worked by M ).

It will be perceived that any disorder in a lamp cannot affect other lamps in the circuit and will right itself or if not the lamp can immediately be switched out of circuit.

Now as to the regulating gear. The two carbon holders are held up, H , by clutch operated by springs (not shown) till end N of lever ON is permanently held down, and C , by the raising and falling of yoke D . There is only one arc burning at a time in a double lamp and the so-called positive carbon C burns first. When the lamps are trimmed the switch is first turned off the carbons put in and the switch turned on . This will draw the upper carbons up about a quarter of an inch.

When the current is turned on the circuit aa is almost instantly broken and most of the current goes through c as the distance between carbons being a quarter of an inch the arc has a very large resistance. The electromagnets j an k attract D which lets loose C , which falls to lower carbon, and the resistance being almost nothing, most of the current goes through b . This weakens j and k which lets D up while D takes C up with it thus establishing the arc. The current all goes down C till the enlarged end of C strikes lever ON thus letting H drop and also putting it in electrical contact with “bd,” which it was not in before. After a short time the carbons burn away, the arc becomes longer and establishes itself and the resistance becoming greater in passing from carbon to carbon and a correspondingly less current flows through b and a greater one through c . This makes the electro-magnets j and k strong enough to draw D to them in spite of spring Q . When D is attracted by j and k , C (or H ) falls and again the arc lengthens, always being kept about 3/32 inch long. This is frequently and continually repeated, the delicacy depending upon the strengh of the spring Q as compared to the electromagnets strength.

Fig. 24.

When the carbon in carbon holder C burns to a length of about two inches in attempting to fall to maintain arc’s length, an enlarged port at the top of the carbon holder C strikes and holds down lever ON pivoted at O (and end N held up by a spring P ) thus letting loose a clutch by which electrical contact is made between H and “bed” and letting H fall till it touches lower carbon when an arc is established and regulated just as for C .

The Thomson-Rice single lamp has the same gear with the exception of having only carbon holder C , H , lever ON , and spring clutch and spring P being absent. The single lamp will burn eight hours and the double lamp fourteen hours continuous running.

These lamps are intended only for a steady current and will not cut out of circuit if the current gets too strong. But with the Thomson Houston dynamo the current never gets too strong and because of this there are less power absorbing mechanism and as anything’s functions decrease the remaining functions are increasedly better. As the Thomson-Rice lamp has less functions and power consuming machinery, it can but be the most economical, delicately adjusted and steadiest lamp extant. They are made to stand a current of five amperes above the normal current for a short time, as, when forty lights are simultaneously cut out of a forty-five light circuit, the current runs up about four amperes above the normal current for about one half a minute.

Prof. Thomson has gotten out a divided arc lamp which supplies a light of moderate candle power for locations where a 2000 candle power lamp gives more light than can be economically utilized. It is specially suited for factory and mill use where looms or other tall machines are liable to cast disadvantageous shadows. It is said that these lights are supplied cheaper per candle power than the standard lamp and up to date is sucessful.

He has also arranged apparatus by which arc lamps are run in multiple series, series or multiple arc. It is said that divisions, redivisions and reunions are practicable. This is also sucessful as far as we can find out.

As before stated Edison fixed upon carbonized filament of bamboo. The Sawyer-Man company however applied for a patent on carbonized filament for incandescent lamps on January 19 ^th 1880, and after five years litigation with Thos. A. Edison they were granted a patent No. 317,676, on May first, 1885, covering their invention. The Sawyer-Man lamp Fig. 25, consists of a carbonized connected to platinum wires fused in a glass tube from which all the air possible had been extracted. The light is produced by the glow of the filament and heat of gases given from filament. The life of a lamp is from 1000 to 1500 hrs. and requires a current of 1¼ to 1.3 amperes and give 20 to 25 C.P. When the filament becomes brittle and breaks the tube is unscrewed from the key Fig. 26, and a new one screwed in. They are run on the arc light circuit by the use of an individual distributor Fig. 27 which consists of a brass case containing a magnet in the circuit of the lamps and a resistance coil automatically substituted in case the lamp should break or is turned off by key Fig. 26. The scheme of arranging lamps so as to get the right current is shown at Fig. 28. the number of lamps in a group depending on the current.

Prof. Thomson has gotten out a lamp Fig. 29 in two styles one for 6.8 amperes current and one for 10 amperes current. Three lamps of different candle power, due to different potential differences at binding post of lamp, are use on the same current. The method of connecting them is shown in Fig. 30. It will be perceived that the lamps carry the full current yet have a life of 1000 hrs. or more. This is a great invention indeed doing away with a great loss of power due to high resistance coils. It will be noticed however that a 125 C.P. incandescent lamp uses as much energy as a 2000 C.P. arc light, the 65 C.P. lamp one half as much and the 32 C.P. lamp one fourth as much.

The Thomson Houston system also furnish lightning arresters, ammeters, hanging boards, switchboards, hoods, insulators, lamp arms, etc, but, though in some respects many of these miscellaneous articles are ingenious and novel, yet they are not distinctive of the Thomson Houston or any other system. Be it said however that all these articles fill their proper places. The company also furnish a motor to go on their circuits but for the double reason that of the motor not being strictly related to electric lighting and of being unable to obtain a description of it, it must remain undescribed as far as this thesis is concerned.

After describing all the parts of the system it may be interesting to know how a plant is arranged. The last plate is a photograph of the LaFayette Gas Company’s Plant of the Thomson Houston System taken at ten oclock one night. It shows the engine, dynamos, the wall controller on the left wall, and a view of the lamps which had hoods put before them to prevent the polarization of the negative.

On the accompanying page will be found a table showing experiments with an old style dynamo given Purdue University by the Thomson Houston Company, which dynamo is now in the engine house of the Mechanical Hall.

The dynamo was run by a large pulley (about four and one half feet in diameter) on the same shaft as the fly wheel and beside the latter. Two lamps were put in circuit with a Deprez-Carpentier ammeter and a volt meter of the same make was put in between the brushes. First one lamp (old Thomson style) was switched out of circuit, the dynamo started and when speed was reached the circuit made. The following readings were taken when the engine made 139 & the dynamo 1122 revolutions per minute.

Fig. 25

consisting of drawing of Sawyer Man lamp cut from catalogue, and trimmed to contour of drawing

Fig. 26

a drawing showing action of key in Sawyer Man lamp, cut to contour

Fig. 27

a drawing of the Thomson Rice Individual distributor cut from cataloug and pasted in.

Fig. 28

a drawing cut from pamphlet showing “Method of using Thomson Rice Individual distributor”

Fig. 29

a drawing cut from pamphlet showing “Prof. Thomsons incandescent lamp—series incandescent lamp”

Fig. 30

Drawing showing “method of using the Series Incandescent Lamp manufactured by the Thomson-Houston Elec. Co.” cut from your pamphlet and pasted on a similar sheet.

A photographer of La Fayette photoed the Gas Company’s plant of T & H in this city one evening at 10 o’clock when several lights were burning in room. I had a large one printed and pasted on a piece of bristol board of the same size as this sheet, and put in my original copy.

The source for this e-book was a hand-written thesis.

Footnotes have been moved to the end of the book.

The captions for Figures 23, 25, 26, 27, 28, 29 and 30 are reproduced, however, the original drawings were not bound with the published thesis and are therefore not part of this e-book.

The author’s spelling has been maintained, Some standardization of punctuation was done to improve readability.

The following proper names as used by the author are reproduced here with their more commonly used spelling:

Phrases and titles which the author portrayed by underlying have been presented in italics. Some standardization of these was also done particularly with regard to the presentation of illustration captions.