THE TESLA HIGH FREQUENCY COIL Plate 1. — Complete 12" Apparatus. Frontispiece. THE TESLA HIGH FREQUENCY COIL ITS CONSTRUCTION AND USES BY GEORGE F. HALLER AND ELMER TILING CUNNINGHAM S6 ILLUSTRATIONS NEW YORK D. 23 VAN NOSTRAND COMPANY Murray and 1910 27 Warren Sts. INTRODUCTION In presenting this book on the Tesla authors hope that they have filled No practical library of science. pubhc the coil to the a long felt vacancy in the made attempt has been to give a mathematical explanation of the oscillation transformer, and other parts of the high-frequency apparatus, simple reason that the theory is obtained of no practical use. tried to lead the and connect bells cell up amateur, batteries, and when Neither have the authors is just learning from the elements how to string of the galvanic the working of a high-potential, alternating cur- to but have merely rent, who too complex, for the advanced amateurs manual on made an effort to place in the in electrical science hands of a practical working now the construction of high-frequency coils, so useful in scientific investigation. The coil attention of the authors when was first called to the Tesla they were fortunate enough to be given the use of the 7" standard coil described in the last chapter of this book. it, in A systematic line of experiments was carried on with order to study the effects of a change in the constants of the various circuits. details of construction and All the mechanical were carefully worked out, electrical and authors finally decided to design and construct a larger The coil, as first constructed, was a decided failure, the coil. due to VI Introduction too small a condenser capacity. further For about five experimented on the details of construction and finally arrived at the 12" coil described in this coil months they they feel assured especially designed great volume. is to This as efficient give a latter fact book. as can be made. This It is high-frequency discharge of makes it useful for wireless telegraphy. In conclusion they have to thank Mr. G. O. Mitchell many suggestions They and for for the kindly interest he has taken in this work. this htde book would have been impossible. feel that without his help the writing G. F. H. E. T. C. of. CONTENTS CHAPTER I. II. III. IV. V. VI. VII, VIII. IX. X. PAGE General Survey The The The The The Transformer 4 . Condenser . 20 . Oscillation Transformer Interrupter 24 . . 32 . Construction of the Boxes Assembling . . 7" . Standard Coil 64 72 . Uses of the Coil Dimensions of 60 . . Theory of the Coil Appendix i . 84 . ....... . 97 iii LIST OF PLATES FACING PAGE PLArE I. II. III. I\'. \'. VI. VII. Complete 12" Apparatus Frontispiece Transformer for 12" Apparatus . Oscillation Transformer and Glass for Condenser of 12' Coil . 20 .... 52 Motor-driven Interrupter The Electrolytic Rectifier . Discharge from the 12' Coil The 7' Standard Apparatus . . 52 96 . . 20 .... ... 96 LIST OF FIGURES FIG. 1. Method 2. Secondary Bobbin of Transformer 3. Hand Winder 4. Wire-spool Holder Primary Terminals of Fastening — Completed PAGE Primary 8 ii 13 14 . 5. Frame 6. Section of Completed Transformer for Secondary of Transformer 18 18 . 22 8. Condenser Frame and Brass Condenser Sheet End Support for Secondary of Oscillation Transformer 9. Fibre Strip 25 7. 10. 11. 12. 13. 14. Rod End Support 25 Centre 25 for Primary 28 Primary of Oscillation Transformer . Completed Secondary of Oscillation Transformer Bushings for Support of Oscillator Standards 29 29 . . 30 15. Hard Rubber Block on 16. Simple Primary Air-gap 34 17. Magnetic Interrupter 37 18. Motor Interrupter Fan 19. Brass Angle Piece 20. 21. Hard Rubber Block Section of the Motor 22. Patterns of Base 42 23. Patterns of Yoke 44 24. Section of Completed 25. Rotor Disc 26. Rotor and Clamp Nut 48 27. Stator Disc 49 Oscillation Transformer 38 . 39 40 Interrupter 41 . Molor 45 - 28. Frame 29. Self-starting Device 30. Rectifier Plates 31. Transformer Box for Stator Coils and 30 \\'iring 46 51 . . . . . Diagram Box 32. High-tension 33. Connections for Primary of Transformer 52 58 61 . 63 65 List of Figures xil PAGE FIG. High-tension Bushing 35. and Standards Wiring Diagram Waves on Wires Primary and Core of Transformer Secondary Bobbin of Transformer Plate and Frame of Condenser 36. 37. 38. 3940. Oscillators 92 of 7' Coil 98 of 7" Coil 99 loi Oscillation Transformer of 7' Apparatus Box Apparatus 43. Wiring Diagram Oscillators and Standards for 7' Apparatus 46. 47. 48. 49. 08 - . 42. 44. ^7 . 41. 45. ^ ..... 34. for 7" 104 . 106 107 . . Transformer of Small Coil Completed Transformer of Small Coil Oscillation Primary Spark-gap Wiring Diagram Wiring Diagram 115 . . . 109 113 . 117 118 118 THE TESLA COIL CHAPTER I GENERAL SURVEY By is and most far the largest electricity, for branch of science interesting Maxwell has proven mathematically, and Hertz verified experimentally, that light is an ejectromagnetic disturbance in the ether, and thus added that subject to the realm of Amongst electricity. the various phenomena of electricity, those of the high-tension current are the most interesting and With such a current instructive. all the wonders of the Geissler and Crookes tubes may be seen. With it space, waves for wireless and a great number It is the purpose of this messages may be of other experiments carried out. book to show how a apparatus for producing these currents and sent out into may satisfactory be constructed, also to describe a few of the uses for such a coil. The apparatus, as described in this book, known is most commonly as the Tesla High-Frequency Coil, and consists, in general, of four parts Interrupter; former. 3. Each : i. The Step-Up Transformer; The Condenser; 4. The 2. The Oscillation Trans- of these will be fully considered in subsequent chapters. Before entering upon the description of the Tesla high- frequency apparatus, however, it would be well to make a few general remarks which are of the greatest importance. The Tesla Coil 2 Throughout the whole work must be given ing care most of construction the matter of insulation. to the exact- All the wire used must be carefully tested, and each layer of wire the transformer must be thoroughly shellacked, and then in in- sulated from the next layer, by two turns of carefully oiled In the condenser, which paper. really the vital part of is the apparatus, the glass should be of the best grade obtainable. the must It also be free from It is in high-frequency apparatus, howe^'er, that the greatest and care as regards both construction The taken. & S. B. air bubbles. all insulation must be secondary consists of one layer only of No. 32 wound on gauge, double cotton-covered wire, an octagonal frame, formed of strips of vulcanized fibre fastened two end pieces of wood. to must be taken that would cause a short wound, When winding the wire, no two adjacent wires touch, circuit. When the wire is care for that completely given about five coats of shellac, not only to it is act as an insulator, but also to prevent any slipping of the wires, The primary and a half turns secondary. are band making two around a circular frame surrounding the consists of a thin The frames on which wound must be \'ery firm of copper, the primary and and secondarj sulDstantial, so that ai occasional jar will not displace any of the wires on the secondary. All connections must be soldered, and the connecting wires run through glass tubes. When the apparatus must be constructed. is finished, two carefully made box6 These must be oil tight. This iii General Survey accomplished by mortising boxes, especially shellac. 3 all joints, the joints, and then giving about four or Into one box the transformer other the condenser boxes are filled and fits, and oscillation transformer. with pure paraffine oil, coats five which the of into the Then the the only is efficient insulator for these high-tension currents. Some who intend to build this coil will think that precautions regarding insulation are extreme, but found that, in currents, too lation is all it these will be dealing with high-frequency, high potential much care cannot be taken, for "Good the key to success in high tension work." insu- CHAPTER II THE TRANSFORMER The transformer — sometimes merely an induction a called converter is the number the number an interrupter, In a transformer used to raise or lower the voltage. of watts is connected directly to the coil that is alternating-current mains, without the use of and — in the primary equals approximately of watts in the secondary. In the case of any step-up transformer, the ratio of the number ondary in the of volts in the primary to those set is nearly the amperes decrease The of the no The upon common induction-coil type, volts or 55 volts, efficient and steps it is up to from the mains about 10,000 volts. working of a transformer depends largely The always best to use; for, iron used little on the must be retentivity. fall A of high straight of the current maximum value to zero, the magnetic flux falls maximum value, not to zero, but to a value which its but the oil-immersed, step-up It takes the alternating current the design of the core. is of turns of wire the secondary; in in the inverse ratio. permeability and should have core number the in the sec- transformer used in the coil described in this book transformer. at same as primary to the number up from from its depends The Transformer The on the residual magnetism. open much circuit is when so that magnetism residual than in a closed magnetic less in an open circuit mag- than in a closed one. the electromotive force in the secondary magnetic to the fall in the field, it is an circuit, the current suddenly becomes zero, the netic flux drops lower in As 5 proportional is greater with a straight core than with a closed circuit of iron. The coil designer the iron core is obliged to determine the length of from the experience of matics for calculating it is others, as the too complex, although simple useful in the case of closed circuit transformers. is made have is, to made if If the core too short the secondary coils be made of too large a diameter therefore, a certain length In the case of and the primary magnetizing current will be too long too large, while mathe- which to be efficient. would There will give the best results. transformer the length of the core was this determined after having gained all information possible from certain eminent men who had made matters; in fact, the dimensions of the transformer for were determined this special use The all iron core is made up gauge iron wire 18" long. size with a pair of the bundle are off nary piece of iron pipe, a an internal diameter with these wires. The pliers, and,' sawed wire study of these life way. No. 20 or 22 B. is when assembled, the ends of square with a hack saw. little less An ordi- than 18" long, and having putting the wires surface, & S. cut nearly to first slightly less than 2", When on end on a smooth in this of pieces of a and is in, tightly filled stand the pipe force in each wire until The Tesla Coil 6 it When hits this surface. end is The sawed off «-ith the bundle fire and left upper finished, the a hack saw to exactly i8." tube containing the iron wires or coal is is now placed in a coke there until the fire burns itself out, thus This heating and subsequent slow insuring slow cooling. cooling so softens the iron wires that their retentivity duced to When a minimum. cool, the wires are is re- taken out They and sandpapered to ^emo^'e any superfluous oxide. are then, one by one, dipped into boiling water, wiped dry, and while warm still the shellac is dry they are again packed, as tightly as possible, in the pipe, to hold still packed When are coated with thin shellac varnish. them Then, while in the desired shape. out closely together, they are forced slowly the pipe; starting at the end thus released, they are of tightly bound with a narrow cotton bandage, which can be obtained The bandage from any surgical supply house. should be When between one and two inches wide, but no more. entire core is wrapped with The ends hea\ily shellacked. and smooth; oughly, when after this it will this cloth, the cloth it is of the core are put in a warm the should be now filed flat place to dry thor- be ready for the primary winding. use of the insulating varnish on the iron wires is The to arrest eddy currents as much as possible, thus preventing the iron wire from becoming heated and energy wasted, which would lower the transformers The primary is efficiently. wound in two sections of two layers each, one above the other. No. 12 B. covered is copper wire used. &l S. gauge, double cotton- About 2\ pounds will be The Transformer The primary may be wound by hand, by required. two wooden supports bored in each, it is and having a apart, But fairly well. satisfactory to wind To mount to one. in a lathe, it it, and slip ring fit was formed, Make over the extreme end of the core. it as tightly as possible by placing between fitted The it the and the Now clamp core a few strips of tin or other thin sheet-metal. firmly in the chuck. the if cut a half-inch piece from the end of the pipe in which the core be 2" hole rather difScult to wind the wire tightly in this way, amateur has access it erecting Then, by turning to receive the iron core. would be more it 17" hand the wire may be wound the core by as 7 other end of the core should also with a half-inch piece of pipe and supported at this The one place in the steady rest. piece of pipe is used to prevent any of the wires from being forced in unequally at the points where the chuck clamps and it, the other to afford a smooth bearing surface for the steady any tendency stock, with the centre About I ft. from of turns of tape removed, around At it. Proceed it. may be pressed up against this point end, its now to is several turns wind the wire tightly and Here the winding of stopped for a short time in order to give the wire a good coat of shellac. another coating wound on bind the wire to by taking closely to within i" of the other end. the primary it. the end of the copper wire take a couple around the iron core, about i" from of tape If there is rest. for the core to slip out of the chuck, the tail is given while the wire it, After the shellac has dried, and then is still wet. the second layer When is the winding ' The Tcsla Coil 8 point, a has come to within about six turns of the starting on piece of tape doubled back with its ends projecting beyond the The looped end second layer. unwound of the tape See Fig. outer side of the winding. — Method The winding The of the second layer loop jecting ends. off. By In is drawn this way is as, Completed finished over the piece brought through the loop in tight by pulling on the other the last turn is using this method or fastening getting loose. the la^t "tuTYt. the pro- kept from slipping it is use any bobbin heads for the primary; advantage, must be on of Fastening Primary Terminals Primary. of tape, the last turn being tape. portion of the kf''') Sji-ix^rams showing rnar^rter oC CasientTn^ I. first layer, i. /I Fig on the itself is laid unnecessary this is to a decided with a removable primary, bobbins are always The wire is cut off about 2' from this ending in order to allow layer this of the primary The second and the be described in a later chapter. will thoroughly shellacked, the section is wound directly when wound layer fastened in the is is on top of the to wind diameter total wound is a is larger as before. trifle in four sections. The thickness -J". tube will fit It will first Now The the one fitting inner diameter of the smaller length of the tubes turn out a around with the tube on it, it wooden rod Mount tightly. is 18" and the rod in the lathe clamping one end of the wood in the thin parting tool, cut off seven rings, three i" wide, If their so that the larger With a chuck, and supporting the other end on a centre. off in be greater than 2!", the external diameter of the one being 35". 3^" wide. wound be 2|". necessary to procure two micanite tubes, tightly within the other. same in the same manner will first, thoroughly shellacked, has been put on carefully 164 turns can be and the The secondary tube section first complete. turn last in the 16" making the various is is Each If the wire plenty of wire for same end, and being sure starting at the direction. g which connections, When The Transformer and four, the amateur has no lathe the rings may be cut a mitre box. Out of some quarter-inch sheet-fibre, cut eight circular pieces, 6" in diameter and having a 3" hole Slip one of the 1" rings on the smaller tube, in the centre. and with Le Page's glue fasten tube. Next slip on one it to the extreme end of the of the circular discs of fibre, and then one of the 3J" rings, fastening them with glue. Two more After discs are put on, and then another 3^" ring. The 10 this comes another and a Be ring. and a i" disc This is by a disc ring, followed Then put on two more 3,{" ring. ing 3 1" ring. Coil I'rsld discs and the remain- and followed by the remaining disc sure that each ring carefully glued is Before putting on the discs, small holes should be drilled them, through which to carry the wires. The bobbin for the secondary The bered 2, drilled on about \" 3, 7 6, seen in Fig. is the holes ha\'e 2. romijlcted discs num- have them drilled Obtain a wooden rod upon their outer edge. which the secondary bobbin in the connecting wires fcjr their inner edge, while the others from i'' place. in will lit tightly. It should be i8i" long. winding wire If the coil builder is skilled in the winding may be done there hand; but for an amateur, who has had but with lathe windirig, or for one the following great care the end method is must be taken of the layer is much more who does rapidly than by little that the wire is experience not possess a In winding given. in the lathe, in the lathe, not snapped off when reached, and while the jjaper wrapped on before the next layer is lathe, is being wound. For the hand winder, the wooden rod, on which the secondary bobbin fits tightly, is drilled in at 4" with a litde less than a {" hole. driven into these holes, to serve as an fit tightly, so as to turn project at one end, other end The standards are axh,-. with the cylinder. which is sufficient both ends for about Pieces of |" iron are then is They should About 6" should bent into a handle. 1 !/' at the for a bearing. made of '(" oak, fastened jg|" apart, The Transformer ^ „9 II -^ 1-^ r -I* -Id- <5^ f ^ -I* "1 ^ 4e- :,f^i^,^^-J^.?/-^ long is oak f" square and 2" piece of fastened with two screws to the top of each standard, to serve as a cap. on the its A 2' long. a baseboard to Tesla Coil Tlie 12 I" hole then bored with is This allows the cylinder joint. bearings A when Two necessary. its centre be taken out of to iron washers are slipped over the shaft at the short end to act as a thrust bearing, and two washers, with an open, steel-wire spring them, are put on the other end. This between will give the friction required to enable the amateur to stop the winding at any time, and still be sure that the cylinder will not rotate and so The dimensions loosen the turns of wire. seen in Fig. As it is of the winder are 3. the wire must be wound under some tension, and as tiresome to give the required tension by letting the wire run through the hand, the holder shown in Fig. 4 was devised. It consists of is an axle which fits 4" longer than the spool. There end of this axle for about 2" wooden standards fastened are put between the spool to bear on. up on A An the spool tightly, to a is and which a thread cut on one then mounted in two It is baseboard. and the standards Iron washers for the spool open spring made of piano wire is slipped the threaded end of the shaft, outside of the standards. washer and a nut are now put on A tension to the spring. lock nut is to give the required put on to keep this nut from turning. Care must be taken in the wire. When to detect any breaks that may occur winding the wire it quite frequently The Transformer 13 c o "n -a I M F\ O C5 The Tesla Coil 14 happens that a it is covered by bobbin, little kink cause a break; but because will the cotton insulation, unknown it will To to the coil builder. be wound on detect these breaks immediately, the authors used the following method. is cut out of a piece of sheet brass or copper. and 3" in diameter. This is the It is A ring }" wide fastened by several flat-headed brass screws to one side of the spool on which the wire is / ^ 8 Fig. 4. bought. If the — \\'ire-Spool Holder. wire has been bought from a reliable dealer, the inner end will be found projecting outside of This wire A is strip of sheet that it will is copper or brass, which bear on the ring, the standard, a wire the reel. soldered to the ring on the outside of the spool. is is of such a length fastened to the upper end on the side on which the ring led to one pole of a dry cell. is. From of here The Transformer On 15 the winder a strip of sheet metal the standards. is best to fasten It is It from the handle. it bent so that is fastened to one of to the make good projecting axle, which has been polished to A trical contact. wire one farthest up presses firmly on the it then led from the brush on the is standard to a binding post on the baseboard. receiver now connected is the other pole of the head attachment, is the Bell receiver, easily elec- in series A cell. A telephone with the binding-post and watch-case receiver, with a the best to use. an attachment If the to hold amateur has only to his it head can be arranged. If the amateur may prefers he use a sensitive galva- nometer. Everything To is now ready begin, pass about i' bobbin heads numbered head 2 is. The wrapped on wooden circuit cylinder. through 2, 3, from the side on which bobbin all and then this It will now be the wire seen that there on the used, the needle will be deflected. will its is and the a complete The diaphragm spool. drawn down or break, the diaphragm will return to a click bare part should be the axle between the washer in the telephone receiver is is winding of the secondary. insulation should be scraped off of the end of the wire for about 2", tightly for the of the wire through the hole in the if If a galvanometer the wire should normal position and be heard, or in the case of the galvanometer the needle will return to the zero position. the break should be located and When the wire should not be used in soldering, as a this happens soldered. little left Acid on the wire 6 The Tesla Coil 1 will corrode is and it the best thing to use as a flux. The layer in the section between the bobbin heads first wound from I, 2, is 2 to i, and a good coating of shellac. a Rosin connection. spoil the electrical The edge is wax must not be used when sulation, as the transformer paraffine oil, thus spoling the first its layer, down with a little to increase the in- finished immersed is in All the layers after insulating properties. should start about \" from the inner face of the discs each layer after The given it is which acts as a partial solvent to paraffine wax, and stop the same distance from them. around wound taken around the pre\ious of the paper can be held Parafiine shellac. it is Before winding the next over a turn of paper little one. after it. it is wound and then Be sure to shellac take a turn of paper Continue winding until 61 layers are last layer in place. should be wrapped over with a narrow cotton bandage which is thoroughly shellacked to keep About two feet of wire section for making the various connections. then brought through should be it in place projecting from the left the hole in disc i, This wire and its end is is connected to the axle. Unwind the other wire from the axle and, after polishing the uninsulated part with a piece of emery cloth, t^vist around the end of the wire from the spool, which has been polished, and then solder the connection. bare part of the wire with some insulate The it also \\'rap the silk thread, so as to thorou'^hly it. section between the bobbin heads 3, 4, is now wound. The Transformer The ; layer first is wound from 17 towards j the winder being 4, turned in such a direction that the direction of the current in the wire of this section will That means wound. the opposite be the same as in the one just must be rotated that the winder direction. For convenience, howe\er, winding the secondary bobbin can be taken rod and put back in a reversed position, the winder rotated the is same the wooden off of the ^^hen in in this is done The same as predously. instructions hold for this section as for the pre\"iou5 one. Each layer must be shellacked and wrapped with paper and the winding In must stop before getting this section 71 layers are wound bobbin heads. to the on. About 2' of wire should be brought through the hole in disc 4 to allow for ; connections. The two remaining - now wound sections are in the manner, there being 71 layers in the section between the bobbin heads the discs the 5, 6, Remember 7, 8. same and only 61 to la\ers in the section This method of winding as in the previous coils. A static strains. practical reason that is wires are from the outer layers, thus to bring out a The reason middle . new piece of wire and if for ha^'ing a greater coils w-ill readily direction between keep the direction of the wire has several advantages, one of them being that ; same relieves the leading out all making it an}- are ever number it ahvavs easy broken off. of la}-ers in the be seen from a consideration of the intensity of the lines of magnetic force around a solenoid. Leave the completed secondary in a warm place to thor- The Tesla Coil ^'V <t'V----7f" Fig. 5. — Frame 7i ff for Secondary of Transformer. oughly dry, and in the meantime construct the frame secondary. base is made Working drawings are given in Fig. of a piece of i"x 9" pine 20^" long. and edges are rounded to give it 5. The a better apgearance. for the The comers Three supports of i"x7" pine, 4V' high, are erected at the points m. 1! Fig. 6. ,.r,r..—.nm-rrrr-g^ — Section !lbi'Anm(Trn-F-n-3T^"'T:::r; of Completed Transformer. The Transformer shown in the figure. 3j" in diameter the secondary is is is At the top of each a half-round hole Into these cut. wound. The 19 fits the tube on which distance between the supports 7r. The two are silk now terminals from the middle coils of the secondary soldered together, and the connection wrapped with thread to insulate it. The other two terminals are left alone at present as their connections are described in a later chapter. The reason for using a cotton cloth instead of tape in the construction of the transformer is that oil almost immedi- ately spoils all the adhesive qualities of the type. CHAPTER III THE CONDENSER A CONDENSER is an apparatus for accumulating a large quantity of electricity on a small surface. vary considerably, but in all cases The form may consists essentially of it two conductors separated by a non-conductor or and its The action depends entirely upon induction. thinner and the the dielectric inductive capacity, the greater A denser. potential. is greater dielectric, its specific the capacity of the con- thin dielectric, however, cannot withstand a high Besides the thickness, the dielectric strength de- pends on the character of the material. The condenser used for in this apparatus used is glass and the plates are finished the condenser For the in size, is made immersed especially designed in yV thick and When oil. io"xi2" These sheets may be had them each sheet should be examined If dielectric pure parafi&ne about nine or ten cents apiece. are any air bulAles. The of sheet brass. dielectric 95 sheets of glass, should be obtained. to size for it is long continued use on high voltages. carefully to see any are found in cut In purchasing if there a sheet of glass should be rejected. The brass used is number 32 or 34. Forty-six sheets Plate Plate III. — II. — Transformer for 12" Apparatus. Oscillation Transformer 12" Coil. and Glass for Condenser of The Condenser 8"xio" are required. side In one of the corners of the shorter a tongue 2" wide and is the top of this tongue. wide, a out of little soldering As a right on the is this the tongues cut The extra i" is Rosin, not acid, should be used in the width is used the tongues are cut occupies the part that has been constructed which the condenser is pine. The base long. The sides are is The frame transformer box. built made up is made in out of well dried of a piece of ]" x 11" pine, iif" cutout of y'xi2" material lof" are also cut from j"xi2" wood and long. are 11" long. and ends should be planed up smooth on both sides, so as to make them completed frame is a little less seen in Fig. The than i" thick. 7. Place the condenser frame on a table or some other surface, with one of the ends down. clean so as to remove any dust or moisture. by putting two glass sheets bottom of the frame. glass plates so that there sheet, except in the flat Before putting any of the glass sheets in the frame, they should be carefully the for sheets. in the oscillation sides rolls 8" the only width that can be obtained in When The condenser The bent across in the figure. rule 12" The ends is can be had in cut 3"xi|". to the plates. shown places. it If the brass hp These tongues should always be soldered most for A j" j" long. more should be obtained and them as a flux. position i They should be it. 21 wiped Commence frame so that they reach Place a brass sheet on top of these is a i" margin of glass were the tongue comes out. If all around the the lip on the The Tesla Coil 22 tongue has been bent carefully will just fit up against Without displacing the brass lay two sheets of glass. on top of of glass it it. A brass sheet next put is i" margin around the brass as in the previous the brass come two more but in this There should case the tongue comes out on the reverse side. be a in, the sheets case. After This process sheets of glass. is A. n." "Frame for B."Sha|3= Dotted tort4ue Fig, 7. — Condenser Condenser brass jheet show size op o^ lines w^dn so\<ierG6 on. Frame and Brass Coxdexser Sheet. kept up until the 46 sheets of brass have been put in Three sheets If the glass book last of glass are placed the last sheet will just go few sheets two, to take on top of the and the brass used are the it is last brass plate. size called for in this In forcing in the a good idea to lay a cloth between the last up any excess crack the glass. m place. tightly. pressure, which would otherwise The Condenser Set the condenser upright, when 23 finished, No. 16 bare copper wire about piece of down the lips in turn, the one side, and 3' the and solder a long to each of same is done on the other side. Two frame leather straps should be fastened to the sides of the to lift former box. it by when lowering The into the oscillation trans- object for building the condenser in a separate frame, instead of in the division in the oscillation transformer box, ever require shet is to facilitate rebuilding, due moving should the condenser to the rupturing of the glass . AA'hen the condenser is placed in the box, the end which has the three glass sheets should be placed against the partition, that is, nearest the oscillation transformer. pre\-ent the spark from the This oscillation transformer through into the condenser, instead of following its is to breaking air path. CHAPTER I\' THE OSCILLATION TRANSFORMER It in is this part of the apparatus, so simple in construction, which the most care as regards insulation must be taken. The success of the whole apparatus depends on the care with which this part is The constructed. as two wires touching, or many may cause a short circuit and require It not wise to hurry the work, as is reconstruct it if The end wood. The two eter, and from f " are marked the fibre strips, reconstruction. be necessary to any suitable piece of will it made out of supports for the secondary are 8" in diamto i" in thickness. Eight equidistant points on the periphery and wide cut at these points. These its careless. supports are off least fault, such other small similar mistakes, See Fig. slots J" These 8. on which the secondary strips are 17" long and \" square is deep and \" slots are for wound, to fit into. and are cut from the best vulcanized fibre obtainable, eight being required. In each end of the strips a hole to recei^'e end is drilled a small brass screw, which pieces. A wooden rod about is and countersunk to fasten i" in diameter obtained and a shoulder turned on each end. of the shoulder is \" and its them The to the is now diameter length just equals the width of 24 The the supports, Oscillation Transformer |" i.e., if The used for the ends. wood f" is used, or i" 25 if length of the rod over i" all wood is must be — End Support for S. Secondary of Oscillation Transformer. Fig. only 17". See Fig. 10. of each of the end A h" hole is now drilled in the centre These pieces are now slipped on, pieces. E ITFig. 9. — Fibre one on each end of the rod. supports, after fitting them Strip. Screw the in the slots are parallel to the rod in the centre. If that they any of the strips are 77" 10. — Centre on the and seeing "TT Fig. fibre strips Rod. The Tcsia Coll 20 bent or warped they should be straightened before being fastened in place. A good way them to straighten is to lay them between two boards, placing some heavy weight on the top board, and lea\c them thus over or 5 ounces of Xo. 28 B. &: S. gauge double cotton About 4 covered copper wire Two first method 18" long in \\'a\-s of these methods be described, as satisfactory. cylinder of wood turned out, and on is first will intended for those that have a lathe is A which the wire can be wound them both the authors have found at their disposal. There required for the secondary. is are several equally good on the frame. The night. it 4" in diameter and are screwed the eight ends are in strips of fibre, so that their line, and that they the amateur has a couple of clamps strike one another. made of strips of sheet iron with a bolt through the ends, matters by clamping them around the will greatly help about 6" apart, first file taken order to A It light cut is a No. 18 thread is now strips to within cut, starting an inch of clean cut the tool there is mounted on the the In must be \cry sharp and several light cuts should be taken instead of one. strips are strips, should be cut just as deep as possible. make a it and then they are polished with from the end of the i" other end. A and moving them as needed. off the strips, and sandpaper. about If frame again it will When the be seen that a continuous groove in which the wires will lie with- out touching one another. The secondary frame in the lathe so that it is now supported between just turns easily. centres Around one end Oscillalion Transformer Till' wrap about of one of the strips be used for connections. to wire tightly on the groove cut for making for of shellac A this is dry keeping the wire in the When all finished, a where they gi\'en to the wires is is wind the extra should be left at the connections. When strips. i' This of Xo. 2S wire. i' Starting at this point frame, always About it. ~i the wire is rest the end hea\y coat on the fibre heavily shellacked. brush should be used so as not to displace any of soft The secondary should now be the wires. placed in a warm place to dry. The following method can be used in case a lathe A available. around the secondary frame. smoothl}'. and shellacked The wire is make two wrapped on in place. It wood wound then to silk It is here that shellac dissoh'ed in be used. turns tightl}', thread turns, to is is wound on keep them apart, heavily shellacked at the ^^'hen should not on, starting about i" same time between it and might be mentioned alcohol from the end up to within an inch of the other end. silk not spool of silk thread and some silk are re- There must be enough quired. is is all and the frame put wound in a warm A the the wire place to thoroughly dry. Get t\vo pieces of of each J"xi2" pine 12" long and find the centre by the intersection of their diagonals. points as centres describe two circles, with radii on each board. With 4I'' these and 5^' Di\"ide the circles ha\-ing the radius 5}" into 36 equal parts. These points can be located with a protractor or mariner's compass, there being one e\ery 10°. 28 Tlie Tesla Coil At each of these points drill boards cut out a piece i"x At a planing may in a \" hole. See Fig. ii. i". buy eighteen mill dowels, 36" long. -]" gwe you These Each one should be be had for one cent apiece. two, which will In each corner of these \" rods, thirty-six cut 18" long. Fasten one of the 12" end pieces to each of the ends of the Sb- ^ holes o \ o \ o \ o o Ai -5i- I o v \/, ,0^ ^-o' /^' Fig, II. — End Support for Primary. completed secondary frame, by four flat-headed brass screws. See that the circular end pieces of the secondary just the smaller circles now drawn on the boards. The fit on ^" rods are driven into place, thus forming a circular cage on which the primary is wound. For the primary get an i" wide. 8' piece of No. 36 copper ribbon AAYap the end of the ribbon once around the end The the dowel of A Oscillation Transformer shown Fig. in 29 and solder 12 in it piece of copper wire should also be soldered Starting from here on place. here. two and a half turns around take — Primary of Oscillation TRANSrORMER. Fig. 12. This the secondary frame. the you dowel diametrically Wrap started. and solder it the in place. will bring you to the end of opposite the dowel from which ribbon once around A this dowel piece of wire should also be — Completed Sec13. ondary or Oscillation Fig. Transformer. soldered on. spaced. fasten The turns of the ribbon Get four pieces of them the other, as braces should be equally i"xi" pine 183" long and from the one end of the frame to the pieces fitting in the corners that were cut out for them. The Tcsla Coil 3° J I I I I - Bushings for Support of Oscillator Standards. ^ / ~^ z "¥" -e "^ 4- Fig. 15. — Hard Rubber Block on Oscillation Transformer. The Oscillation Turn two bushings out They are shown the shoulder centre, at and is The A I" thick. two opposite points Two pieces of 31 of a piece of f" brass or copper rod. in Fig. 14. the shoulder Transformer is length over §" hole drilled to recei\"e and is slightly V' and down the all is drilled countersunk two small brass screws. vulcanized fibre or ebonite J"xi'', 2" long, with a 5" hole drilled h" from the end, are fastened to the middle of the top side of the made The bushings primary frame. are fitted into the holes and screwed in place. just The wires from the secondary are soldered onto these bushings. ^^'hen this all is done the that needs to be oscillation transformer done is to connect completed oscillation transformer is it up is finished properly. seen in plate III. and The CHAPTER V THE INTERRUPTER Let us now consider that important part of the apparatus, The the primary spark-gap. stated, is to provide a denser charged to is function of this, as previously path of high resistance until the con- Then capacity. full its it suddenly breaks down, and allows the current to surge back and across it, until the current other factors in the damped is After circuit. forth out by resistance and the oscillations ceased, the ideal spark-gap should return to have maximum its disruptive strength before the condenser can be charged by the next cycle from the secondary of the transformer. In practice this is far from being the case. The air between the discharging balls becomes heated, and offers a comparatively low-resistance path for the current. This results in an arc being formed, which prevents the condenser from performing its which confronts the designer of this The tially is to find some way to get rid heated air and thus prevent the arc being formed. object of this chapter accomplishing The The mechanical problem function. is to this result, show several ways of par- but in no case perfectly. simplest form of spark-gap for the primary of the oscillation transformer, one which has given 32 fair results Tlte Interrupter ^li with the writers, consists of merely two adjustable brass No balls. provision made is for blowing out the arc that forms, so that considerable of the energy of the transformer Nevertheless sufficient oscillations are set up is wasted. to bring the coil to within i" or 2" of maximum its length of spark discharge. Most amateur struction, their a designer coil is be very anxious work apparatus coil builders will, at this point in the con- A are. may what to see be obtained with the simple air-gap. more acquainted with is the possibilities of good idea of the working value of the When the workings of a Tesla he can construct that one of the spark wipe-outs which best suited to the current that he has at his disposal. THE SIMPLE AIR-GAP Two standards of brass J" in diameter and 4" long are mounted on a piece 5" apart. A each rod and of -^^" hole is hard rubber. They should be about drilled J" from the upper end of is taped with a standard \" machine screw tap. These two holes must be Next two pieces for the whole of standards. Two in line. of \" brass rod 3!" in length are threaded their length to balls Y in fit the holes tapped in the diameter are turned out of brass or are procured from a dealer These and threaded Two balls are drilled to in physical fit supplies. in the brass rods. vulcanized fiber rods are turned out of f" rod, 3" in length, and a \" shield 2" in diameter end of each handle. The handle is is drilled screwed on one and tapped for The Tcsla Coil 34 i" to is fit on which it is safeguard the operator's hand to fibre the brass rod screwed. The from sliding shield off the handle and coming into contact with the transformer which would probably be current, fatal. Connection can be made to the brass standard near the bottom by drilling -6 -*Afcl*' an ^ !_ IEHIImQ) -^ J '• 0/-/'A/-)'/'/-, <- e .f c Fig. i6. — Simple Primary Air-cap. a small hole through them, and then drilling and tapping another hole at right angles to the to first, for a thumb screw bind the wire. A set screw at the top of the standards to clamp the rods in place after they to the operator. have been adjusted See Fig. i6. will be a convenience The Interrupter 35 THE AIR-BLAST INTERRUPTER In order to of much make more the air-gap getting rid efficient, between the spark terminals, a of the heated gases mechanical means can be used of forcing in cold driving out much To higher. efficiently hard glass tubing is is accomplish drawn out opening ^\" in diameter. ard and This is this a nozzle having an into mounted on a brass standto a foot used in the laboratory to operate a blast is lamp or any other suitable supply of compressed good blast of air to form, thus a piece of f" connected by means of a rubber tube bellows such as air, heated gases and keeping the resistance the will effectually air. A wipe out any arc that tends thereby increasing the disruptive length of the bright oscillation transformer discharge. however, that occupying so it is The a tedious task to much operator will find, pump a foot bellows, of his time as to handicap him in per- forming experiments with the high-frequency discharge, and he will soon decide that the best policy is to construct either a magnetic wipe-out or a motor-driven interrupter. THE MAGNETIC INTERRUPTER The magnetic blow-out is well suited for those who have a source of direct current at their disposal; either the lighting circuit or a suitable battery current. have only the alternating current and no- volt For those who who wish to use the magnetic wipe-out the writers have added to this chapter a simple home-made electrolytic rectifier of their own design The Tesla 36 which will give Coil a current suitable for magnetizing the magnet of this interrupter. Two standards of the same interrupter, but 6" in length form as those used and having spark in the simple balls I" instead of J" in diameter, are mounted on a hard rubber base 10" x The fibre terrupter. handles and shields are also necessary for Two this in- electromagnet bobbins 5^" long and having an iron core |" in diameter with An are procured. 7". iron has 2 holes drilled in it heads 3" in diameter fibre yoke made from i"xj" iron in the the bobbins are fastened to 7" long middle i^" from both ends, and it by a screw in the core. Two polar pieces of f " square iron, filed into an egg-shaped point The are screwed to the upper ends of the core. are wound wire, if full of No. 14 B. & S. gauge cotton-covered magnet they are to be operated on a battery current of from eight to ten volts such as a plunge battery. rent of rectifier bobbins 1 10 volts is If a direct cur- available No. 24 should be used. described at the end of this chapter is If the used No. 22 wire should be used as the voltage of the rectified current on no volts alternating is about 90 volts. be thoroughly saturated in order to The magnets must give the best results. After the magnets are finished they should be fastened to the hard rubber base, at right angles to the rods carrying the spark balls, balls of the by two screws through the iron yoke. The spark-gap should be between the projections of the magnet. A sheet of mica is bent around the polar projections of the magnets in order to prevent the spark from jumping to the cores of the magnets. Fig. 17. The Interrupter of the coils are so connected that the current The ends them will traverse outer ter- suitable binding-posts and the finished. is Fig. The The in opposite directions. minals are brought out to interrupter 37 17. — ^Maonitic Inieehupter. principle of this piece of apparatus based on Da\'y's is experiment in which he found that the electric arc is extin- guished upon the approach of a magnet. THE MOTOR-DRIVEN INTERRUPTER This interrupter is the one the writers used in their earlier experiments with the 7" standard part of this book. It consists coil described in the latter run on the alternating current at no volts, driving disc having a number of projections bolted face, and a brass separating at will. builder it oscillator so may direct current mounted from the projections on the The motor may be possess. A of motor essentially of a fan a brass around its that the distance disc can be varied any suitable design that the small battery motor rimning on can be pressed into service if the amateur does The Tesla Coil 38 not care to go to the expense of purchasing a fan motor or The has not the facihties for building one. directions for building a suitable induction motor are given at the end of this chapter. /bbei" Fig. i8. To make — Motor Interrupter Fan. the disc for this interrupter turn out of \" sheet brass a circular piece lo" in diameter. may be able it Lay off eter on its no lathe If is avail- procured at a model maker's quite reasonably. face respectively. two concentric Di\ide the circles, 8" inner of and 9}" these in diam- into thirty equal divisions and draw radial lines from the centre of the disc through each of the points marked o£F, thus dividing The same number the outer circle into the through each of Drill a hole circles A and tap them number Interrupter to 39 of equal divisions. the points laid off on both a standard 4-36 machine screw. jQt made by bending of brass angle pieces I, j'g" brass Two holes coontersunk ->i^ Brass Angle Piece. into the form shown are drilled flat'-headed in the figure are procured. and tapped in fit a standard 4-36 pieces are screwed to each one to machine screw. These the brass disc with j" screws. A \" hole is drilled in the centre of the disc holes are drilled on a circle and having a radius of three ig" |". Next The Tesla Coil 40 turn out a circular block of hard rubber 2" in diameter and the same shape as in Fig. 20. The brass disc is screwed with three brass wood screws {" long and the whole to it is fastened the to insulated from & To it. % shaft of the motor so as 20, plate a brush to bear — Hard Rubber Block. on the back near the centre of a piece of y^" sheet spring brass. and Y be well I Fig. 10" long to mal<:e electrical contact with the brass wide. It is is cut out This piece should be mounted on a piece of hard rubber with a suitable binding-post, so as to press against the back of the disc. For the other side of the spark-gap a standard mounted on hard rubber similar spark-gap is to the one described used, but instead of being 4" long for the simple it is 6" in length The Interrupter and the brass diameter. The ball is fibre best if it is slightly less 41 than \" in handle and shield are necessary in order to adjust the length of spark-gap while the coil operation. — r is in The Interrupter 43 A SiLVLL SELF-ST.\RTIXG SDsGLE-PHASE IXDUCTIOX MOTOR To build a motor, to run on the single-phase alternating current of perhaps is tools no running a fan interrupter, volts, suitable for ver}' The difficult. builder will require and a much greater knowledge of machine shop prac- construct an efficient motor than to build tice to parts of Tesla apparatus combined. had but litde experience in For those who have an alternating-current fan direct -current batter}- book may be complete the coil builder will have all The motor. following description of the building of this motor in order that this of the all motor construction, the writers suggest that the amateur purchase motor or a suitable more in itself is and given so that the necessary data to build the complete apparatus without reference to other works. The first step in the construction patterns for the base to make the necessary There are two castings The base supporting the punchinss for the stator cast directly on the standard which supports the motor. required. is and yokes. is The It that the drawint;. Fig. 23. will give the required dimensions. is assumed that the amateur pattern-maker an iron casting mould was made, is therefore shrinkage in the pattern in order to enough. One is aware smaller than the pattern from which must be allowed be sure that the casting eighth of an inch to the foot is will for be large about the proper amount. Turn out a circular piece 5 " in diameter and i" in thick- 77/r 44 ncss. Then a rod i" in 'Icslii ('nil diameter, and 6" long, swelling into a graceful enlargement at the lower enrl, is turned out and fastened with glue and nails to the centre of the < in iilar disc. -^ 1- -,'^ - D-^ for jiUUifr heads I'lO, A piece of wood the figure. The is 23, PAn;.i':.'s oi' YoKE. cut out of ;" stock to the form radius of curvature of the arr so that the stator will and nailed — fit it accurately. to the top of the upright. This shown in must be 2\" jjiere is The whole glued pattern is The Inlcmipter iliilllllllilMI'Hliii A Fig. ;:4. — Section of Completed Motor. 45 Tlic 46 gi\cn two coals of lampblack to make of the rotor shaft jet black. 'I'his we must make tompktt's llic pattern castings are of the stator. and of the made from They a pattern lor a yoke. turn out of \\" sloik a circular we this pattern disc 5I" in diameter Two it shellac \'arnisii, containing suOicicnt In order to pro\i(le a su|)porl for (he bearing for the base. To make l)csl Tcsla Coil same form this palleni, as in the drawing. one to lit each end not only ser\e to furnish bearings the rotor, but also to enclose the entire for motor and thus keep out moisture and dust. Vie. 25, — Rotor Disc, After the patterns arc shellacked they should be sent to a foundry where the castings can be obtained quite reasonably. It requires journal. one casting of the base and two of the yoke When chipped and The all the castings arc obtained they should be the roughness filed rotor consists of a or number off. of iron discs 2\" in diameter The Interrupter and having twelve f " holes j^g" thickness; about forty of These high. discs can be help of a lathe and around the edge and a They should be made hole in the centre. j^|§Q-" in drilled 47 made by drill press, A sufficient number turned down from a shown in the figure, to motor will not is or they can be obtained already in electrical sup- them are mounted on a of make shaft, As a pile 2v" in height. have a very heavy load thrown on sufficient to i" f" rod of cold rolled steel to the size not be necessary to key fit pile the coil builder wfith the stamped out from any of the large dealers plies. of iron about them making a them A to the shaft. the will it it, good driving They can be keep them from turning. in the figure. The conductors consist of twelve s" copper rods 2f" long. One clamped in position by the nut shown of these rods should be driven in each of the holes the edge of the discs both sides. To and should project J" short-circuit them, beyond them on two heavy rings made by bending two pieces of \" copper rod into a an outside diameter of if" are soldered rods. in Use sufficient solder in around making circle having to the ends of the these connections order to prevent heating at the connections by the induced current in the rotor. The This completes the next thing to consider this case is rotor. the stator punchings. In they will not be punched out, but will be cut out on either a shaper or milling machine, or cut out by hand after as drilling. much metal has been removed as The diameter ing on Fig. 27. of these discs To make is is possible by given in the draw- them, cut roughly out of tHtt" 48 The Tesla Coil hi %k -%%. o "T «)i» I s o ^ The Interrupter 49 The Tesla Coil JO iron about loo pieces 6" in diameter, with a pair of snips. A I" hole is drilled in the centre of them and the whole number and turned are clamped on a mandrel between two nuts down in Next four a lathe to si". the figure, and a tube i" in external diameter and J" fibre internal diameter Y' holes are drilled as in driven in each hole. is length, with hexagonal nuts and A J" stud 3I" in f" iron washers, binds the After tightening up the nuts the bolts can discs together. be slightly riveted to guard against possible loosening. whole is clamped either a chuck and the centre in Next the 2f" in diameter. slots are is bored out A file. to cut as in the figure, on a milling machine or shaper or by the use saw and The of a hack large bulk of the metal can be removed by mounted on the pedestal drilling. When the stator is complete it is with four cap screws which screw into the bottom edge. The two ends are fastened to the stator with four l" screws i" long. way between The the nuts binding the stator discs together. order that the heads be drilled The fit up against the is stator four holes should next wrapped with paper until and the heads are bolted on are to be permanently. It is well to can always be put back in the same between the shaft and the journal of In to allow the nuts to project into the heads. rotor into the stator grade fillister holes for these screws are drilled mid- Babbit metal in the mark them place. is obtainable. it way fits they so that they Then filled just the space with the best Cardboard washers slipped over the shaft prevent the babbit from running out. The The used next thing to do is the size are No. The 22. shown in wrapped with 28. ' is wind 51 the stator coils. wound in a The wire wooden frame After the coils are tape, shellacked, wound and allowed to of they dry by Before the coils can be put into place, means must be provided This to coils are Fig. thoroughly baking. is Interruptef for making the motor self-starting. accomplished by means of a short-circuited copper The Tesla Coil 52 The pieces. brought out pieces six coils are in series, the to suitable end terminals being binding-posts fastened and suitably insulated from it. A end to the coating of black paint completes the motor. Although the induction motor at varying loads, we can secure is a constant-speed motor some slight speed regulation, 4Short circuited of Wo, 14- Bare cortduc/br Wi>«, Cof>(>er showing €haf]e of wire bff[ore alijj^in^ into slots Fig. which is 29 — Self-starting Device. a great advantage in operating the by coil, inter- posing a liquid resistance in series with the motor. resistance consists essentially of as is plates suspended in an cell, ha\'ing jar, such two metal electrolyte, so that the distance be- tween them can be varied at erally any suitable glass used in a Daniell or Gra\'ity This used as the electrolyte. will. Copper sulphate is gen- Plate Plate I\'. \'. — Motor-driven — The Interrupter. Electrohnic Rectifier. The Interrupter 53 AN ELECTROLYTIC CURRENT RECTIFIER It to was only make that the authors decided which has proven highly rectifier, advantages are that Its moment public the results of their experiments on an electro- current lytic at the last it easily is quires only slight attention, its efficiency the current which a small set will rectify To a great many this description it may seem The the Tesla apparatus. reasons appeared, to the authors at the is built, very large. is is entirely foreign to circuits will if need about 80 or go volts pressure, can hardly be obtained from the lighting which are generally alternating or from to substitute however for so doing, least, sufficiently great, for a source of direct current at Then having re- very high, and amateur constructs the magnetic wipe-out he since this current it out of place in putting in which of a rectifier, satisfactory. and cheaply he this source of direct current a D. C. motor batteries. will for the induction be able motor de- scribed in this chapter. The the method current is greater due. number of rectifiers now on the market use of choking out the one half of the alternating- wave and The it is to this fact that their low efficiency high efficiency of the apparatus devised by the authors depends on what might be called the alternate path connection or method; that current to traverse, one of is, there are two paths for the enormous resistance and one of very low resistance. The idea of this form of rectifier came to the authors in The Tesla Coil 54 the following They were experimenting on some way. cathode tubes of peculiar construction, using a 12" induction The coil. current from the secondary of this coil latory in character, of course. It charge through the tube was ^-ery was observed that the unsteady, especially the interruptions were not very rapid. ments was carried out effect, to oscil- is A line dis- when of experi- determine the cause of this unusual' with the result that the resistance was found to be enormously greater for currents in the one direction through the tube than in the opposite direction, due entirely to the difference in the forms of the two electrodes. After discovering this fact they wondered lytic cell if some electro- might not be made which would possess the same properties and could be used nating currents. From to rectify the ordinary a previous study of the alter- effects of various electrodes on the electrolysis of certain solutions we arrived at se\'eral cells which exhibited these properties to a marked extent. It tial was found that an aluminium electrode was the thing in every of forming cell, together with some acid an oxide with aluminium. The salt essen- capable other electrode might be any conductor unaffected by the solution. Some of the conductors suitable for the other electrode are iron, carbon, gave more or bonate, acid and less lead, and the following satisfactory results. solutions Acid sodium sodium phosphate, acid potassium car- tartrate, potassium alum, and in fact most of the ionizable, acid sulphates, carbonates, tartrates, all and phosphates. slightly The Interrupter By merely putting one of these method this gives an cells in the circuit, the one wave may be choked half of the alternating current But 55 Thus than 50%. efficiency of less out. the authors were led to devise the alternate-path method. Before describing this method, however, in detail the properties of a single cell. we After a current passed for a few minutes through one of the of oxide tically is will take cells, While this does is prac- not prevent the difference of potential from being maintained across the it is a coating formed on the aluminium electrode which a non-conductor. up cell, does prevent the ions from giving up their charge and in way this vanic it acts like a polarized copper plate in a single gal- cell. when This condition of the aluminium of the current the is enormous resistance When on the anode. aluminium becomes the cathode there merely the resistance of the electrolyte encountered. possessing this property cell As stated circuit exists the reversal is Any called asymmetric. before, a single cell would choke out the one by being merely put in the half of the alternating wave, but as this gives an intermittent current, the following the method devised by the authors. in all. and one The Two is Three is cells are needed of these consist of one electrode of aluminium of iron, with a solution of third has between them. sodium acid carbonate. two aluminium plates and one iron plate The same On looking at Fig. the current can flow 30 it from trolyte to plates I or 4. solution will is used. be seen that when E is positive either plate 2 or 3 across the elec- The path from 3 to 4 is of enormous resistance, as the I to 2 6 to aluminium AA'hen this H becomes positive the current can flow from or from s to 4. 7 the anode, but the path from is low resistance and hence the current takes of is path. is Tcsla Coil Tlic 56 It takes the path from 6 to 7 as this In this way both waves of the alternat- of low resistance. ing current are used and the only loss is due to the resistance of the electrolyte. Thus in made from the direct current which has a sine wave form, this set the negative values in the alternating have been all positive. The following are plans for a rectifier suitable for use on directly the no- volt-alternating-current light The rectifying cells have glass containing jars. 7" X 6" X 4" inside are cut out of They -J" 5" x 7" are sheet and are all jars are all The aluminium measurements. same the The mains. size plates and shape. The aluminium and four are required. should be comparatively pure to prevent deterioration of the plates due to local action. extent impure may rectify it will the cells are cut from I" sheet. the fail be at a very low Two is making plates it larger is that to. The third is plates are is 8" x iron plates size as This larger 5". The cell. required to necessity for fasten the bind- held three eighths of an inch apart in the following manner: canite or hard rubber (fibre they do if goes between two aluminium it and the extra length ing-post The them are the same be used in the middle to work, and to efficiency. of aluminium plate and the plate the plates are to any If Out of some f" sheet must not be used as it vul- swells in TJic Interrupter water) cut four strips x 61". .1" V' These latter pieces are drilled Some Also cut out four washers diameter and a number of pieces h" square. about in and tapped The washers have a \" thread. \" vulcanite threaded to 57 rod up cut is With a \" nut. fit to hole drilled in them. into about 2" lengths and and washers these strips and plates are held the required distance apart firmly fasten them The together. across the tops of the plates one of the of each A electrodes are put by the solution binding-post As the plates. are longer the plates rubber are used the washers at the bottom. far superior to using iron ones is an insulating bushing. The strips of the the bolts This method of using hard rubber bolts and See Fig. 30. nuts and a standard fit -}" than if is fitting strips across the the jars top of when are wide; on the edges of the sodium acid carbonate be a saturated solution. them with fastened at the top the they will be suspended in the in place strips resting electrolyte, and jars. used, should is Other solutions than this can be used, although the authors obtained the best results with this one. Besides it is about the cheapest of all the possible electrolytes. In selecting an electrolyte the following factors must be taken into consideration. It must have low resistance, must be a stable compound, and when no current it it is flowing must not attack the aluminium plate and only slightly attack it when To make mounted current is passing. the set con\'enient to in a handle the jars should be wooden frame, with the cell containing the The Tcsla Coil 58 -->fi'bai* wojW D.C, A.c. :; r lauRE. Fig 30. ehowr'tig — Rectifier faos'ition o£ 1fia ce)/5 and eledrtdcs Plates and Wiring Diagram. The Interrupter two aluminium electrodes are shown With 59 in the middle. The in the figure. this electrolyte the few minutes, it aluminium plates will take a The form in a being merely necessary to short circuit the D. C. taps with a resistance and allowing the full connections rectifier to load current. efficiency of the apparatus will be somewhat increased by using a cooling worm, as the electrolyte when cool has the greatest current density. It will be necessary to depending on the use the renew the set is given electrolyte at intervals, CHAPTER \T THE CONSTRUCTION OF THE BOXES The is next thing to consider in the building of a Tcsla the boxes which contain the transformer One box coil. for transformer, condenser, might be used, but for a coil Two be objectionable. They and ha\'e the A up inside is where they are is so to the placed on top of the box. most substantial box, but it harder is filling up the pores in the wood does to which not sink does in a softer wood. it the best material to use as the joints will require which pine which lead to the fact that the shellac \'arnish considerable oil, is the safe, except those oak with the same readiness as Pine if advantage of taking owing tight, used for into to handle, of having all the high-potential connections interrupter which make weight would form can be used separately, single box, however, has the Oak makes and high-tension coil of this size the advantage of not being too bulky room and less and high-tension separate boxes give the ideal result. the transformer in this desired. coil may filling will up to make them imper\-ious to paraffine soak through almost anything in time. Sugar be readily stained and looks very neat when \-ar- nished. For the sides and ends of the transformer 60 box it requires — The Conslniclion of the Boxes 6i a piece of straight-grained pine free from knots, ij" x lo", 6" long. The bottom 26" long, and pieces to the size The end made i"x pieces shown in Fig. 31, must be mortised of a piece of i 11", 2' long. and plane J" x 14", Cut the the edges true. into the sides i" from the These tongues and grooves may be cut with a saw end. and should be the top of a piece of chisel TOP a rabbeting plane if is not at hand. l/IEW-Tiivy rm^vtj After the sides COVER -i'i' Zoi" iA zsi- -iSif' 0000 I®! '®l l@| I® i®| I I® I©' I® i@| I® i@| W T SIDE VIEW END VIEW ' Fig. 31. Teansfokmer Box. and ends are finished the tongues heavy coat of shellac, hol, and while still and grooves are given a which has been dissolved wet are put together. in grain alco- Six long brass screws with round heads are to be used in each board to hold the sides. A on the screw brass washer to prevent the Y l^i diameter should be placed head from sinking into the wood. Next the edges should be gone over with a plane sary so that the bottom board will fit if neces- flush in all places. The 62 Tcsla Coil TJic bottom board that it is be i" wider than the width of the box, so to laps over V' is cut to size, a finish, on each \\'\\tn the side. bottom board the edges are rounded off with a plane to and then is it fastened to the box with long headed brass screws, placed every four inches along the A and ends. box The coating of shellac is ilat- sides given to the edges of the bottom on, just before putting the gi\-e to help make it tight. screws must be forced in until they are flush with the wood. Next the inside should be given five or six coats of shellac, paying especial care each coat A to to get into the joints, and allowing dry before applying the next. small brass cock in the end near the bottom box ience in emptying the it it in so that the box of will not leak is The box for the high-frequency coil of the transformer box. working drawings the condenser it oil. oil. and condenser must partition oscillation transformer, should be bored in circulation of the A is construction as in the case The dimensions in Fig. 32. and its a conven- such that a siphon quick enough for an occasional emptying of the have the same care taken in is but the labor of putting its oil, are given in the is put in between but several holes near the bottom to allow of the free This box must also have several coats of shellac, as the insulating oil used will leak through in spite of all the precaution taken. After the boxes are finished they should be stained or varnished to suit the taste of the builder. looks well, and as it is dark it covers Walnut up a multitude stain of faults Boxes 63 boxes are well made a good The Construction of in the wood working. ciling followed by If the the several coats of shellac makes a very good finish. TOV VIEW COVER REMOVED COVER .1 "?+= h— /? ii :=F^ -36?- J6i :^i CHAPTER VII ASSEMBLING It for not wise to hurry is the if when assembling high-tension wires brush-discharge effects will are the apparatus, not properly insulated, be noticed on operating. In nine cases out of ten poor insulation will result in puncturing his condenser and probably burning out Care should be taken former. mount First to the transformer in the transformer into its box bring his trans- follow these directions. its its After lowering box. four primary leads to The two four heavy binding-posts on the end of the box. terminals inner of two sections are brought the to two adjacent binding-posts, and the two outer ones to the other two, in such a manner that connecting electrically the two middle binding-posts puts the sections in circuiting the See the two outer pairs throws the sections diagram. This is across two binding-posts, or fits and short- in parallel. accomplished by means of a piece of fiat brass with slots filed in which series it so that it just fits by a short piece of brass rod in the holes of the binding-posts. The secondary terminals are soldered directly to two brass rods f" in diameter and 3" long, which extend through the opposite end of the box for ij". 64 These rods are insulated Assembling by two heavy hard rubber or lows: is A turned full 2" piece of down diameter of the rod. Fig. 33. in the The A §" hole bushings fibre i^" is flange them and as fol- drilled on one end the down the centre bushinsrs should be a driving — Connections 8" made rod 2" in diameter fit both for Primary of Transformer. end of the box and over the brass are 6" apart brings fibre hard rubber or to iV', except for a of the bushing. 65 up from rod. The the bottom of the box. well above the level of the oil, rods This thus assuring no leakage at this point. The leads from the sections should be led to the brass rods through glass tubing bent in the desired shape. is drilled and tapped in the end of each rod to fit A hole a standard The Tesla Coil 66 Another hole brass set screw. the first drilled at right angles to about \" from the end of the rod to meet the This makes an hole. is efficient first binding-post to hold the con- ductor. This finishes the connections can now be placed box is filled former. free in the position on the transformer, which which with enough pure paraffine This cover the trans- oil to should be of the best quality obtainable, oil from moisture and impurities, such as lating purposes. The to occupy. it is It is used for insu- should be allowed to soak into The primary sections for 24 hours before using. all the terminals are connected to a source of alternating current by means of a suitable switch The next step is and fuse capable of carrying 30 amperes. putting in the connections and terminals in the high-tension box. I FiG. 34 - - h- High-tension Bushing, Three brass rods similar box, with the in the end same form to those used in the transformer of bushings, are driven through holes of the high-tension oscillation transformer. I -- box next to one end of the These holes should be about from the bottom and 3" apart. The brass 6" rods project Assembling The bushings and I" williin the box. tight rods can be made oil by giving them a good coating of Le Page's glue before driving A 67 them into place. 2" strip of wood is box below these rods, glued on in the lower inside end of the to prevent the end of the oscillation transformer from coming in contact with them. i!.;.c: Fig. .35, The condenser wire to ' *^ is — Oscillators is first it is soldered. glass tube suitably bent the box. A wire is and Standards. lowered into place in the box and a run from one terminal which <J} The to the nearest outer brass rod, wire should be enclosed in a and should follow the lower edge of run from the other terminal of the con- The Tesla Coil 68 denser in a similar manner to the other outer brass rod. A follows the other lower edge of the box. from this of the A conductor at a point opposite wire is also soldered to the is from the condenser lead band and led oscilla- Tlie tap wire into place. soldered to one end of the primary the wire from the middle brass rod to the other end of the band. These leads should be run They should as directly as possible. The is It to be. is The middle brass rod. now lowered is where one terminal primary band of the oscillation transformer tion transformer oil. to tap wire in glass tubes also be kept and under the connections are shown in Fig. 36. o o Fig. 36. is — Wiring Diagram. connections have been securely soldered the box After all filled with oil, so that the entire apparatus is completely immersed. The Two oscillators fibre or in length, and standards can now be hard rubber bushings 2]" and having a flange ]" thick in constructed. diameter and and 3" in diameter turned on one end, are set in two holes cut in the directly above the holes lation transformer. A in the brass J" hole is bushings on the drilled i.\" co\'er oscil- through the centre Assemhling Two of each bushing. tubes should fit J" brass rods 10" long are enclosed The The ends the rods tightly. rods project from the fibre the bushings diameter and gY' in outside in fibre tubes f" on the 69 and can be The lo^ig- of the brass slightly tapered to fit oscillation transformer. oscillators consist of screwed on the end of two two brass balls i" in diameter ^f/' brass rods 12" long, which are to slide easily in two holes drilled \" from the top of the standards through both the fibre and the rod. at the top of each standard will A set screw be of convenience in clamping the rods in any desired position. may be In order that the discharge gap the coil in operation is are screwed for about on the ends of the in diameter rods, carrying the oscillators, li". the standards through the bushings in the cover Slide until the rods make good second box. It contact with the bushings on the This completes the connections oscillation transformer. the adjusted while two vulcanite handles f" now be should position at the high-tension ing a space of about i^' end for the of placed the in its in final transformer, leav- interrupter between the two boxes. The built particular form of interrupter which has already been is connected to the binding-posts of the high-tension coil as in the wiring diagram. These leads and those from the transformer to the high-tension 12 B. & S. est glass box should be of No. gauge hard copper wire and enclosed tubing obtainable. They should be in the heavi- as straight and The Tesla Coil yo as short as is safety in operating the consistent with pri- mary spark-gap. A suitable panel switchboard, with the necessary fuses, transformer and interrupter acquisition to the apparatus, but matter makes a sv/itches, it is desirable This not essential. left to the taste of the individual worker. is When the connections have has dri\en out all the air that all it been made and the can, oil open the interrupter gap about i" and cautiously close the transformer switch. If no excessi\'e load is by the 30 ampere in series, closed if until one is taken by the transformer as manifested fuses or an alternating-current ammeter obtainable, the spark-gap can be slowly the condenser discharges across it. Then, if the directions have been carefully followed in building the apparatus, a heavy, bluish white, snapping discharge of over 12" in length will pass between the oscillators, upon the further adjustment of the interrupter gap. When the transformer is used on 55 volts the primary sections should be connected in parallel in series. parallel If the sections on no volts, If fault may it ought to, no volts in and hence the con- puncture. by any chance a discharge should may be due be due for the voltage output of the secondary would be about double what denser and on the primary were connected to several things. to the fact that the sections fail to take place, the In most cases will on the primary or secondary of the transformer are connected in opposition. mine whether the transformer it is working To deter- satisfactorily or Assembling not, disconnect from the it -ji apparatus and see rest of the if an arc discharge of at least 6 or 8 inches can be drawn out bet\\"een and color This arc two electrodes. is generally of a yellow extinguished by any draught of easily you do not obtain a 6 or 8 inch arc test the sections to see they are connected in the right manner, no arc error has is it lies does not lie in the transformer, in the condenser; charge, determined by its if they are and some To test this is most If there most likely connect the trans- if is a condenser dis- none obtained, your likely short-circuited or which can only be remedied by its even punctured, reconstruction. next place to look for trouble is in the oscillation Ring out by means of a magneto the primary transformer. no open circuits, circuit bet«'een the primary and secondary circuits to see that there are and then there see it is bluish white color, can be obtained primary spark-gap. condenser The if highly improbable, then former up with the condenser and s;e in the and If been made in the construction. If the fault that which results, still air. if and secondar}-. due to is any short If these parts are all right the fault may be poor insulation, in having the turns of the secondary touching. The remedy Finally look and is ob^ious. see that aU the electrical connections are as they should be, then the apparatus cannot fail to discharge over a 15" air-gap. CHAPTER VIII THE THEORY OF THE TESLA COIL Although, the authors stated that in the introduction, they would not attempt to give a mathematical explanation of the coil, they feel that a few facts regarding the theory still would not be out improvements the to the reader. amateur wishes The as of place here, in that is first well to sets It will also suggest certain be of assistance own the transformer. is The Its action, electro- alternating current flowing in the up an alternating magnetic field, which being linked with the secondary induces an electromotive in it. When the secondary is open there is except induction, is that thrown on necessary its magnetize high the self- core. to the secondary, the current through the primary automatically adjusts is to force theoretically no current passing through the primary, due to As a load if design. almost everybody, depends on magnetic induction. primary may to construct a coil of his thing to consider known it itself as the self-induction decreased by the opposing ampere turns of the second- ary, that is, if the transformer is self-regulating for vary- ing loads. The normal used current through the primary of the transformer in the 12" coil is from 22 72 to 25 amperes, the secondary Theory of the Coil voltage being about seventy-five hundred, age in the secondary To -3 and thus fifty-five volts the amper- oT- get the required voltage of seventy-five secondary on to about is 73 in the primary hundred it in the necessary is connect the two sections of the primary in parallel, as this On has the effect of cutting the .primary turns in two. one hundred and ten volts the sections are connected in The series. use of the transformer in the Tesla apparatus merely to charge a condenser, and thus nary induction coil or even a static it is is seen that an ordi- machine of the proper dimensions could be used, but they are not nearly as handy. Another important matter tion of a transformer to be tions ary. is a to secure The in connection with the construc- used for creating electric oscilla- sufficiently small resistance in the second- reason for this is that the transformer is used to charge a condenser. When an electromotive force a condenser, the full is applied to the terminals of difference of potential is not created between the terminals of the condenser immediately, but The time rises gradually. depends on capacity (C) its charging circuit. of the condenser, in a required to charge the condenser and The product and the resistance {R) of the CR is called the time constant practically the condenser time equal to ten times the time constant. constant is to is charged The time be reckoned as the product of the capacity (Q in microfarads and the resistance {R) of the charging circuit in megohms.- The The time is gi\en in fractions of a second. condenser, more than anything else, constitutes the The Tesla Coil 74 essential part of the Tesla coil. It plays the same part the mechanical interrupter in the ordinary induction Its action, lies in however, purely electrical and up the currents setting When any is condenser is of its great advantage enormous frequency. may discharged, the discharge one of several forms, depending only on the three constants of the discharging circuit and The resistance. discharge as coil. take electrical — inductance, capacity, may be either oscillatory or entirely unidirectional, consisting only of a gradual equali- zation of the potentials on the two plates. This tration. may be made clear by the following mechanical Suppose a glass U-tube to illus- be partly fdled with mercury, and the mercury to be displaced so that the one side of the tube in is is higher than in the other. then a force due to the difference of the liquid to return to the mercury that so it is is now level, an equal height in allowed to return, but released slowly, position without oscillations. it If, level There tending to cause both limbs. is goes back to If constrained, its original however, the constraint is suddenly removed, then owing to the inertia of the mercury it overshoots the position of equilibrium and oscilla- tions are created. If the the liquid viscous, being damped out by What we these is rough in the call inertia in material resistance experienced electrical interior, or oscillations will quickly subside, friction. with the inductance of an the tube substances corresponds electric circuit and the by a liquid moving resistance of a circuit. If frictional in the tube, with we suppose the Theory of the Coil U-tube at its above to include air 75 mercury and tiie would circuit. necessary conditions for the creation of mechanical oscillations in a material system or substance are that there must be a self-recovering the matter displaced displaceability of must possess inertia; some in kind, and other words, moved must tend to go back to the restraining force is removed, and must overshoot the thing when be closed up ends, the compressibility of the enclosed air correspond to the electrical capacity in a The to original position its the position of equilibrium in so doing. Frictional resist- ance causes decay in the amplitude of the oscillations by dissipating their energy as heat. In the same way the conditions for establishing oscillations in a circuit is that it electrical must connect two bodies having electrical capacity with respect to each other, such and the as the plates of a condenser, possess inductance tions, the and low sudden release circuit Under resistance. itself must these condi- of the electric strain results in the production of an oscillatory electric current in the circuit, provided the resistance of the circuit critical value. We is less than a certain have these conditions present when the two coatings of a Leyden jar are connected by a heavy copper wire. Professor William in titled Lord Kelvin, published 1853 a paper on "Transient Electric Currents" in which the discharge of the in Thomson, Leyden jar was mathematically treated a manner that elucidated important If we consider the case of a facts. Leyden jar or condenser charged The Tesla Coil 76 through a circuit having inductance and resistance, then in up in the act of discharge the electrostatic energy stored the condenser is con\'erted into electric current energy dissipated as heat in the connecting and At any moment circuit. the rate of decrease of the energy in the jar is equal to the rate of dissipation of the energy in the discharging circuit plus the rate of change of the kinetic or magnetic energy associated with the circuit. From Lord Kelvin these facts up an equation sets of energy, vi^hich leads to a certain class of differential equation The solutions in this case depend on between the constants inductance, resistance, ha\ing two solutions. relation the and capacity. If Z= inductance, C= solutions are determined If is 4U — greater than if by the — LC J^C or capacity, that , R= resistance, then the relative values of is, if R is greater thanl/lr:, V (J T is — R greater than 4 , the charge in the jar dies gradually as the time increases, in such a discharge current The charge ratio — R circuit, stant {T') is is is is called the that the time constant (Z) of the CR of the condenser circuit. less manner away always in one direction. and the product unidirectional circuit — and LC. when is dis- called the time con- Hence the discharge the time constant of the inductive than half the geometric stants of the inductive circuit mean and condenser of the time concircuit: Theory of the Coil however, If, — 77 T (^ J? is than less 4 — R the discharge current will be oscillatory, the current decaying in accordance with the damped law of a When rent oscillation train. the discharge is so highly oscillatory that the cur- not uniformly distributed through the cross-section is of the conductor, then the ordinary resistance (R) and ductance (L) must be replaced by the high-frequency ance and inductance of the circuit. AA'hen the discharge takes the oscillatory quency is R is son with form the fre- given by the expression, 2- If in- resist- > LC can be neglected in compari- very small, then , 4L- and then the frequenc}- is given by the expres- sion, In this equation both the quantities in electromagnetic C and L must be measured units or both in practical units, viz., in henrys and farads. In the majority of cases are practically used, cuit is easily negligible, measured which in the resistance of and the inductance electric the is small and hence in centimeters or absolute C. one milli-henry being equal to oscillations oscillatory cir- G. S. units, a million centimeters (10°). The Tesla Coil 78 Also capacity the microfarad being measured best is microfarads; one in one millionth part of a farad or the IO-" of an absolute C. G. S., unit (electromagnetic) of capacity. Hence when L is expressed in centimeters and C in micro- farads, the expression for the natural frequency of the circuit becomes n= X 1= VCL 5.033 10" storing capacity of a condenser The energy CV, the expression - where C is given by the capacity of the con- is 2 V denser and The main the charging voltage. thing in constructing condensers to be used on high charging voltages all is the solid dielectric. this number is reduced when cost and internal energy in ebonite, mica, tions, are suitable, constant is and also great. and micanite are of these flint glass high, being Glass from is is 5 to 10, brittle, loss Glass of certain composi- in the dielectric are considered. is There are only a few dielectrics suitable for high-tension work, and practically the best, as and its its all that dielectric dielectric strength however, and liable to have flaws which sooner or later give way. The capacity of a condenser depends on the area of the plates, their distance apart used, and farads, is where and the constant of the dielectric expressed by the following formula in micro- K is the dielectric constant, the plates expressed in square centimeters, apart in centimeters, 5 the total area of and D the distance Tlieory of the Coil KS ^_ The constant 9 x lo'^ 79 comes from the one micro- fact that farad equals 900,000 electrostatic units of capacity. The oscillation transformer construction are that its it is nothing but a modified trans- The former with an air core. only important facts about should be built to withstand great between the turns, and that the primary voltage differences should have as small an inductance as to is make is practicable, in order No the frequency as great as possible. gained by having many close turns in the primary, because the increase of inductive effect increase in the number advantage on the secondary, due of primary turns, is to an about exactly annulled by the decreased current through the primary due to its own The greater inductance. function of the interrupter may be formed gap, for if The to destroy any arc that across the terminals of the primary spark- this arc is not wiped out there will be no true oscillatory discharge in the one. is reason for this is condenser circuit or only a feeble that as long as the arc discharge continues, the secondary terminals of the transformer are reduced to nearly the same potential, or at most by a few hundred The volts. function of the primary spark-gap voltage to which to charge the condenser. tial difference differ only between the spark balls is is to regulate the Since the poten- almost equal to the potential difference across the condenser, the condenser will discharge at a voltage determined by the length of the air- The Tcsla Coil 8o Now gap. there is suited for each coil As a rule it is a certain length of spark-gap which and it can easily be determined by out until a point it trial. ahnost reached, is out any further would cause to cease pass- it This spark length almost always gives the best ing. best best to start with a rather short spark-gap, gradually lengthening when opening it is this chapter In the earlier part of it was stated results. that the high- frequency resistance and inductance should be substituted and inductance, when dealing for the ordinary resistance with circuits which are subject to the action of electric The processes and means used lations. ment high-frequency measurements. difference between the two cases The main is to measure- for the and potentials when applied to of low-frequency alternating currents are not always applicable or correct either reason for the be found in the that a high-frequency current does not penetrate merely a surface or skin When tra^'ersed 1. The is, effect. resistance of the conductor, direct currents five be considered. for high-frequency currents that into the by an alternating current, there are qualities of a circuit to fact conductor of good conductivity, but interior of a thick solid is oscil- which is always greater than for the ordinary currents; and alternating currents up to about a frequency of loo per second. 2. The inductance of the conductor depends on metrical form, material, insulator. The tance becomes. and the nature its geo- of the surrounding greater the frequency, the smaller the induc- Theory of 3. The the Coil capacity of the conductor, depending on tion with regard to the return circuit on the 4. dielectric constant of the The 8i dielectric and other posi- its circuits and surrounding insulator. conductance of the insulator surrounding the conductor. 5. The energy dissipating power, due to other causes than conductance, such as dielectric hysteresis, which exist in Under the dielectric. this heading comes the from the brush discharges through the air loss of energy between the con- ductors. If the constants of a circuit for low-frequency currents are known, the values of the constants be calculated fairly correct. can, however, be delicate measured and inconvenient isfactory. The directly, for use for high frequencies can high-frequency constants but the apparatus is rather and besides not always If the coil builder cares to sat- measure the constants of a circuit for himself, he will find the description of the necessary instruments in other books as it is beyond the scope of this work. Ha\-ing now briefly treated theoretically the principal parts, the authors will try to parts work on all four of show how these together to form the Tesla high-frequency appara- tus. The condenser is of the transformer connected in series with the secondary and thus is being continually charged. \Vhen the potential difference betweeen the plates of the condenser reaches a certain critical value determined by the length of the primary spark-gap, the diameter of the spark The Tcsla Coil 82 balls, etc., a discharge takes place which oscillates through and back and the primary of the oscillation transformer The frequency forth across the primary spark-gap. current depends entirely, as of the circuit. On first shown thought, one of the on the constants before, would think that the condenser would discharge through the closed circuit in the transformer secondary rather than little jump the air-gap, but a show consideration of the matter will that the induc- tance of this circuit to electric oscillations of this nature Another matter so great that no discharge can take place. that might be touched gap. on here is the resistance of the spark- Before any discharge has passed and under normal conditions the resistance of the spark-gap voltage required to break about 10,000. air After the down one initial is very great: the centimeter of air being discharge has passed and the becomes heated and ionized the resistance may drop low as two or three ohms. part in the The is damping This fact plays as an important of the oscillation trains. discharge from the condenser which oscillates through the primary of the oscillation transformer sets alternating magnetic field, is rapidly which being linked with the ondary induces an electromotive force induction in this case up a in it. The law sec- for the not nearly as simple as in the case of the ordinary transformer, the capacities of the circuits playing an important part. If the capacity of the circuits is certain critical value, the induction capacities of the circuits, while if is in the below a ratio of the greater the induction de- pends on the relation between the number of turns in the Theory of primary and secondary. voltage The the Coil 83 formulae for calculating the difference across the secondary in either case are extremely complex, involving the damping factor, the capacities of the circuits, and other Drude and Bjerknes constants. have treated the subject of the oscillation transformer analytically in an admirable maimer. The frequency of the spark in the large spark-gap is not a simple one but consists of se\eral, one being the natural period of vibration of the secondary and one a forced vibration of the secondary, due to the fact that the secondary are never exactly in tune. There is primary and also a certain small current of a high frequency, due entirely to the constants of the spark balls and connectors, which act as a condenser. The Tesla much to coil in its present form is still be improved upon and wished very crude leaving for. The problem that presents itself in the construction of Tesla coils tically the same one is prac- that presents itself in selective wireless telegraphy, so that the solution of the one will solve the other. CHAPTER IX USES OF THE COIL The Tesla coil readily lends itself to a great number of experiments, some interesting in their effect, others useful in scientific Waves research. X-Ray be sent out into space, illuminated, number The brush beautiful of other things done. high potential current obtained from this coil pos- due that are not possessed by either a static in which to its high frequency Ruhmkorff induction the machine. These properties are best seen effects, may shown, and a great effects sesses certain interesting properties coil or wireless messages for tubes excited, Geissler tubes may the Appendix. in the beautiful brush be obtained even with the coil described All of these experiments on the brush discharge should be performed in the dark, as they then show to the best These effects, advantage. besides affording a great scientific \alue. non is and it is due It is a known pleasing sight, are of fact that the phenome- molecules near the terminal, to the agitation of the thought, since the brush is hot, that some heat must be developed by the impact of the molecules against the minal or each other. A little 84 ter- consideration of the matter Uses of the Coil leads us to the conclusion that which would give intense much from reason for putting amateur new The suffi- been light and But heat. this is stray- the practical nature of this book; the only it in being, that it might suggest to the lines for experiment. following have we could but reach if enough frequencies, we could produce a brush ciently high ing too 85 on experiments from taken Nikola brush the Tesla's discharge "Experiments with Alternate Currents of High Potential and High Fre- quency." There is practically nothing except some wire and a few on the brush supports required for discharge, and thus they can be performed by every one. the first all these experiments In experiment two insulated wires about 10 feet long are stretched across the room. tances of a foot and a half They are supported at dis- by insulating cords. attached to each terminal of the wires is coil is put in action the wires are seen to coil. One of the When the be strongly illumi- nated by the streams issuing abundantly from their whole surface. (This experiment must be shown in the dark, of course.) The cotton covering on the wire, although it may be very thick, does not affect the result. To produce the best of the wires must be effect the carefully adjusted. the wires at the start very long cutting off lengths first until primary gap and the length It is best to take and then adjust them by long pieces and then shorter and shorter the correct length is reached. When this adjustment has been obtained and the wires are fed by either The Tesla Coil 86 from them the 12" or 7" coil, the hght will be sufficient to distinguish objects in the troom. Another way of brush easily exhibiting the by effect is attaching the end of 10 or 20 feet of No. 36 insulated copper ' wire to the one terminal of the coil and the opposite end to an insulating support, lea\-ing the wire hanging clear. Upon touching the remaining terminal with a bit of metal held in the hand, the wire will break forth into numberless streams or threads of light palpitating in unison with the discharge of the condenser. The luminous intensity of the streams increased by focusing illustrated them upon a small coil a is sphere. The is ter- wire bent into a circle about one foot in centre of the sphere should be in a line at right angles to the plane of the circle at is set up, To centre. its a luminous hollow cone dark one half of the brass sphere minated. one of the attached and to the other terminal a small brass diameter discharge This surface. To by the following experiment. minals of the in the can be considerably is is When the formed, and seen strongly illu- get the best results possible with this experi- ment, the area of the sphere should be equal to the area of the wire. Another way may be shown in is which the luminous effect of the discharge as follows: two circles of rather stout wire, one being about 32" in diameter and the other and to each of the terminals of the attached. same The two plane. When circles coil 12", are formed, one of the circles must be concentric and the coil is is in the turned on the whole space Uses of the Coil between the wires uniformly is intensity of the streams that objects in the 87 tilled forming this room can be The with streams. luminous disc is such plainly distinguished even though at a considerable distance. By this time the experimenter will realize that to pass ordinary luminous discharges through gases, no particular degree of exhaustion is essential, and necessary, but a very high frequency is of course a shows us that the attempts of the molecules or vacuum atoms the use of sure. is when to need not be limited be looked forward light will light is to the to, and be produced without any vessel whatever and with When This high potential. produce hght by the agitation of a gas tube, but the time that in the near future, to fairly air at ordinary pres- obtained this way, there will be no chemical process nor consumption of material, but merely a transfer of energy, and the probability would have an is that such a light efficiency far exceeding that of of the present incandescent lights, even the best which waste so much of the energy in heat. The Geissler effect can be readily bui^nt-out incandescent globe, in been destroyed. To show it shown by using only a which the vacuum has not the bulb should be suspended from an insulating knob, so that the discharge through the centre of the bulb. in order to see the will pass The room should be dark changes that take place in the globe. putting the coil in action the bulb lights pulsating, delicate purple hue. This color generally turns to a lovely pale green, up with a in a On gently few minutes and then sometimes, TJie 88 but rarely, this changes tensity of the light of the colors is something minutes the filament is A in- discharge it is peculiar thing always happens is found used, namely, that in a few to be completely shattered. it is only necessary to hold the globe in the hand, without any connections to the By moving The be admired. to a bulb with a good filament With The light. too long through the tube as liable to pierce the glass. the 12" coil white to a delicate not very great, but the delicateness is must not be continued if Tesla Coil the bulb around coil, for it to light up. in the vicinity of the spark, various changes in the intensity of the light will be seen. If the amateur may tubes, these is fortunate enough to possess be lit up by connecting them, an adjustable spark-gap, coil tubes will to the coil. some Geissler in series with In the case of the large light up when merely brought into the vicinity of the discharge. The is best X-ray tube to use with this Tesla coil known as a double-focus tube, although may be used of the ing light, coil the terminals X-ray tube are alternately cathode and anode, when an alternating current able, what any other tube As with not quite as good results. is if X-rays is used the pulsating or rather may be called light, va:ry- would be objection- but due to the high frequency of the current from the pulsations are not noticeable. focus tube flector is used the rays are reflected and then from the other double the space is filled tube had been used. When first the double- from one in rapid succession, with the rays than if this re- and thus a single-focus Uses of the Coil If the tube 12" coils, it is a small one and used on either the 7" or is should be connected in series with an adjustable spark-gap, to prevent any injury to this On it. starting the coil spark-gap should be open as far as possible and then gradually closed until the best result should be it 89 felt now and then to see becomes too hot the is if it The obtained. tube has become hot, and if should be stopped and the spark- coil gap lengthened. may For those amateurs who desire to use this coil for wireless telegraphy, the authors merely state that able, is it suit- with a few minor changes, in most of the systems using For a step-up transformer. referred to a large number detail information they are of admirable books, especially devoted to this subject, written by very eminent men in this field. But opens after all the great field of experimental investigation itself to enter the realm the possessors of one of these coils first the field in is, field of electric waves. The subject results are expected itself is still in its when netic disturbances are verified in It is infancy the laws of electromag- a convincing manner. not the easiest subject to experiment in by any means, on the other hand it is the most difficult. In order to carry out any of the experiments at satisfactory results a large and they which Hertz made himself famous, the that and great when mathematically investigated by Maxwell; electric wiring is room required. of a large barn, provided free A from all all and get metallic objects good place is in the loft no better place can be had. It The Tesla Coil QO was in a large barn that the authors verified some of Hertz's experiments on electric In dealing with waves. waves there are two disturbances to be taken into account, the electromagnetic and the electrostatic. two on ing both which is the all wires. A method electromagnetic and also sta- be given for obtain- will stationary the that can consistently be There are waves and the classes of waves, the electromagnetic tionary waves electric waves, brought within the scope of this work. D. E. Jones has made a translation from the German of the original papers of Heinrich Hertz, dealing with the experiments and results which have The knobs a short distance apart. to the his name famous. radiator or oscillator used by Hertz consists of two metallic plates, having attached to in made secondary of the coil. them short rods ending These knobs are connected Hence, as the secondary motive force accumulates, the plates are brought ence of potential and lines of stretch out We sponding points on the negative. a differ- displacement electrostatic from the positive side of the to electro- oscillator to corre- have thus a strong electrostatic displacement created along the lines of force. When the potential dilTerence reaches a certain point de- pending on the length of the spark-gap, the breaks down and a air current flows from the one other across the spark-gap. It is insulation plate to the merely the discharge of a condenser, for the two plates on the oscillator form a condenser, with air as a dielectric. around a magnetic This creates in the space flux, the direction of which is everywhere Uses of the Coil normal 91 The to the direction of the electric displacement. energy electrostatic is thus transformed into electrokinetic energy. the If some of the energy As the intermittent this is way sufficiently therefore we have groups the electromagnetic waves are set In order to of trains which spread out through the off have the breaking sudden a displacement wa\e. off as in operation and oscillations started is thrown coil is continually waves thrown In oscillation electric down up of electric dielectric. in the air. of the air sufficiently sharp to obtain the oscillations, at least three things are necessary: the spark-ball surfaces no ultra-violet light must fall must be bright and on the balls, and the clean, balls must be a certain distance apart, best determined by experience. The form of resonator de\ised by Hertz consists merely of a nearly closed ring or rectangle of wire the ends of which end in metallic balls placed very close together. ball is adjustable have been many The one by the use of a micrometer screw. modifications of this resonator, the authors found most satisfactory There but the one was where a neon or carbon dioxide Geissler tube of the spectrum variety was connected directly across the spark-gap. Instead of getting a spark then the tube becomes illuminated. By tor, using this resonator and the before-meintioned oscilla- the magnitude of the electric displacements in the space surrounding the oscillator can be Hertz's great air. This is work was mapped in setting out. up stationary waves in accomplished by having a large metal plate The Tcsla Coil 92 set up in the radiator is set room up to act as in front of a it, reflector. at By reflector the The this with is it, its so parallel to the holding the resonator parallel to the metallic nodes and antinodes can be easily traced out. size of the plates on the radiator used by Hertz The experiment was i6" square. of about coil some distance from that the plane of the plates on the oscillator reflector. The No. 6 copper wire, 14" m in resonator was a ring in diameter. n w a^ Fig. 37. To used. set — Waves on Wires. up stationary waves on wires Two similar plates to those the on the same radiator is oscillator are gotten Uses of tlie Coil 93 and mounted a short distance from the plates of the radiator. The plates are all parallel and have two from them across the room as shown Thus the wires are parallel wires led in the figure. electrostatically connected to the Hertz radiator and the plates rapidly alternate in potential, and this applies to the ends of This electromotive force. potential which If the light. tionary the EMF wires creates an alternating electric waves of travel along the wires with the velocity of length of the wire waves of electric current is suitably adjusted, sta- and potential are set up by the interference of the direct and reflected waves. To tion try the and interference of electric waves, two brass rods ending consisting of in a zinc box must be very tained. experiments on reflection, refraction polariza- of parabolic form is in balls required. sensitive, for otherwise The prisms and a small oscillator no lenses used are and mounted The resonator results will be ob- moulded from either paraffine or pitch. As before stated the authors said that they would merely outline the experiments possible with the Tesla coil, and for the detailed information the translations of Hertz's original works must be consulted, unless the amateur has knowledge of German course be far more to sufficient read the originals, which will of satisfactory. There are several experiments which can be readily performed with this apparatus and which would appeal to those having no knowledge of electric phenomena. ments have but little practical value, These experi- the only reason for The Tesla Coil 94 them being citing some that they may who should chance friend furnish entertainment to The into his shop. writers saw them performed on the vaudeville stage with an first Oudin resonator which To is far inferior to the Tesla coil. begin the performance the operator should make a few general statements as to the voltage required to leap such as 30,000 for different air-gaps, Then show 2", etc. and After he has about 55,000 for the discharge across the 6" or 12" gap the spectator imagine let i", what voltage that represents. become somewhat impressed with the intensity of the discharge, the operator can approach one of the oscil- and allow lators this his hand when motion in constant There point. this current effects result so is To his bare hand. without severe burning of the hand, he should keep do on one on the spark to play is is prevent the spark from playing only a very slight sensation traversing your body and no shown The next experiment felt injurious The the authors are aware. far as best hand when to effect in the dark. the coil is is one to grasp in operation and oscillator with the to have an assistant touch the operator's bare elbow with a cotton cloth dipped in alcohol. To The handkerchief immediately get the result without rather tightly bursts in flame. any uncertainty the cloth around the assistant's modification of the same experiment is hand. any of the audience are inclined as to lighting cigars to An wrapped amusing to touch the cloth to the hair of the operator, showing that the hair If is is not ignited. smoke, a suggestion on a windy night without the annoyance Uses of the Coil of matches blowing out 95 The will be greatly appreciated. operator has merely to bring a piece of metal, such as a nail, held in the and hand to within h" of light the cigar A one of the spark terminals from the spark. gas flame can be lit with the bare fingers by grasping one oscillator with the bare hand and approaching the burner with the finger of the other hand so that a spark will The the metal tip of the burner. more spectacular by letting the jump have made A^riters spark jump from the to this tip of the tongue. In these experiments an assistant should adjust the spark- gap so that no more current passes than is to To is necessary. This prevent the spark from burning the operator. convince the audience of the tremendous voltage passing through the operator's body he has merely to bring one hand up to a lighted incandescent globe, while he grasps one terminal of the coil On with the other hand. approach of the hand the filament the near will violently vibrate and then shatter, blackening the bulb and of course extinguishing the lamp. Lighting Geissler tubes held in the hand or even in the mouth by approaching them ment to the oscillators is an experi- that never fails to bring forth the applause of those present. Perhaps the most spectacular experiment, one which unaccountable for by the every-day electrician house wiring and has never been brought high-frequency- currents is the lighting of in is who does touch with an ordinary incan- The Tesla Coil 96 descent lamp with traversing current the the operator's body. Before performing this experiment some few remarks on the quantity of current necessary to full brightness on the no- volt to bring the filament circuits should be made, They can those present are ignorant of electrical matters. if thus see that the energy C. P. lamp therefore is \olts this equivalent to 55 watts, is and that this means approximately The ^^ reason taken with impunity is of an why \ no ampere, while according ampere this amount At taken through the operator's body. to the best authorities age human. an ordinary 16 required to light is fatal amount to the aver- of energy can be not definitely known, but it is thought be due to the fact that the high-frequency current does to not penetrate into the interior of a solid conductor, but follows the surface. The This is known as the skin effect. operator, to get the best results, should stand on an insulated stool and grasp one terminal of the coil with one hand, and approach with a piece of metal held tightly in the hand or mouth one lead of a lamp, the other lead of has been previously grounded. to bright red gap up to its and if an The lamp assistant adjusts the best working distance, the to full brightness. will which come up primary spark- lamp may be brought Plate VI. — Discharge from Plate VII. — The the 12" Coil. 7" Standard Apparatus. CHAPTER X DIMENSIONS OF For think chapters, spark amateurs those is 7" who, STANDARD COIL ha\'ing read previous the an apparatus giving a twelve-inch that too large for their limited uses, this chapter has been added. This coil is by no means to be thought of as a toy, for the authors themselves used the very apparatus described in this chapter in carrying out their X-ray and Geissler tubes. first experiments with the Wireless messages were also sent successfully over a distance of three miles in wet weather. This was the greatest available distance over which the authors could try the coil, so that three miles should not be maximum considered the In clear transmitting distance. weather messages could easily be sent a distance of about fifty miles, provided your antennae is well insulated from grounds. Because does not apparatus this mean regards insulation entirely on this that is any not as powerful as the other, less care should be and mechanical construction, whether the coil builder is to get mittent spark or a fat crackling one. between this for The taken it as depends a thin, inter- only difference apparatus and the larger one, besides that of 97 The Tesla Coil 98 size, is in the construction of the transformer and then they are only The built trivial. core of the transformer up of pieces of long after the is & No. 32 B. manner described in care should be taken in annealing wires as was done The primary is 38. 2f" in diameter S. and is gauge iron wire 13" Chapter II. The same and insulating the iron before. wound other, as seen in Fig. 38. Fig and condenser — Primary in two sections adjacent Each section is to each wound towards and Core of Transpoemer of 7" Coil. the centre, starting i" from the ends of the core, for a distance of 5". There are six layers of No. 16 B. & S. cotton covered copper wire in each section. thoroughly shellacked are held At least when put on and left for layer is the terminal wires by the same method as described two feet should be gauge double Each in Chapter II. bringing out the terminals to the binding-posts. The secondary is wound in two sections. gauge double cotton covered copper wire is No. 32 B. & S. The tube used. Dimensions of on which wound it is thickness of the wall Standard Coil 99 has an internal diameter of 4" and the It is 11" ^^". is They are 6" in diameter 4g" in diameter cut out of the centre. made from long and The bobbin heads the best vulcanized fibre. of j" sheet fibre. 7" are cut out and have a hole Four of these are w^ II ^^--^^—^4^11 -4^ ! Fig. 39, They shown the in the ->'i^ 7" Coil, are slipped on the tube to the positions The figure. heads of each section two sections -^i- Secondary Bobbin of Transformer of - required. in J 2}/'. is 3 J", distance between and The bobbin heads can be same manner bobbin the the distance between the held in place by cutting as described in Chapter II the rings out of a very thin fibre tube, or in this case it will be sufficient to wrap some heavy brown paper several times around the tube between the bobbin heads. a layer on the secondary, shellac turn of paper. \" of the In this way bobbin heads. it After winding and wrap it with one build up the secondary to within When the last layer is put on it The Tesla Coil loo wrapped with is several turns of paper which is shellacked This completes the construction of the transformer. in place. \A'hen finished it should be left for some time in a warm dry place as behind the stove, to thoroughly dry the shellac. The reason for this is that green shellac a is fairly good con- ductor. For the condenser, twenty-eight sheets of brass 6" x lo" are required. No. 32 or 34 sheet has a lug i^' long on it soft sheet brass and i]" wide is Each used. either cut direcdy Whether they or soldered on in the upper corner. are cut directly on the sheet or are soldered on will depend on the width are cut lip is \Mth of the brass sheet used. on the sheet or soldered on with 8" and 7" is liable sooner or later to give reconstruction of the condenser. clean before putting The frame is made Any should be rejected way, thus causing the Wipe each sheet of glass in to the condenser. The constructed from well seasoned pine. two sides are made is it it i" Thirty x 12" are required. sheet of glass that has an air bubble in it A brass. See Fig. 40. bent across the top of each lug. sheets of glass -^q" thick as 12" brass they from J" x 12" pine 4" long. of a piece of I" x 4" pine 8" long. The The base tened to the sides by some flat-headed brass screws. is base fas- The heads of the screws should be sunk flush with the wood. On the one side of the frame two strips J" x i" are fastened; one at the top and the other at the bottom of the frame. See figure. the side The frame on which the is now strips laid on a flat surface with have just been fastened down. Dimensions of I 7" S/andard Coil t:: f^l" Sirijit I I ^it'^l'strik I I I I > I ^ i^Cstrl^ --3" . ^ ^ Fig, 40. — Plate and Frame of Condensek. lOI The Tesla Coil 102 A glass plate is placed in the frame after having been wiped dry and clean so that Then a brass sheet glass at the should just is touches the bottom of the frame. it laid in so that there i" is bottom and a V' margin on the margin of The sides. fit lip Without against the upper edge of the glass. displacing the brass sheet place a sheet of glass on top of This it. the lug is followed with a sheet of brass, but in this case on the brass the previous one. to brought out on the opposite side is Continue this process until the 28 Two sheets of glass have been put in place. are placed on top of the last brass sheet. glass sheets Also remember to bring the lugs from the brass sheets out on alternate sides. Mortices should be cut in the top and bottom of the upper ends of the sides a last little deeper than the point to which the These are glass sheet reaches. of pine l" X i" similar to those should be screwed the glass. strip A and the down in turn down These piece of paper or cloth placed between the and solder a piece of copper already been tinned, to each of the the one side and another wire About No. 16 bare wire side. extra wire should be left to The receive two strips other side. glass will prevent the breaking of the latter. which has on the other to tjie so that they press firmly against Set the condenser upright wire, on oscillation make transformer is all lips to all the lips will do. Enough necessary connections. constructed in the same manner as the one for the 12" for the secondary are 6" in diameter and are turned out of i" material. coil. Eight equidistant The circular supports slots are cut in the per- Dimensions of iphery Y square. long. A rod 11" long the figure 41. The f' Standard Coil square and 11" fibre strips are A" is turned out 103 to the size shown in diameter and has a A" shoulder It is i" in turned on each end. This rod holds the two supports for the secondary apart. If the grooves of winding the wire in should be cut on the fibre to be used, the thread is strips before mounting them on the supports. In the original coil the wire was merely wound on three supports 3" wide mounted on a hexagonal end piece. fibre The wire was wound contact this method it adjacent turns were and the whole was thoroughly shellacked. method new, that no so of winding gave good in Although results while the coil was was found after some usage that the wires became loosened, thereby reducing the effecti\-e sparking distance. A better way howe\-er, is to use The scribed in Chapter 1\. one of the methods de- wire used is Xo. 28 B. gauge double cotton covered copper wire and was & S. wound 18 turns to the inch. The end pieces for the primary are cut out of h" material The and are 9" square. dowels fit used in all. is 8". diameter of the After the secondary The which the There are twenty -four \" maple dowels is are screwed to the secondary frame, in place. circle in wound and these end pieces the dowels slipped length of the frame o^'e^ all is The 12" primary winding consists of one and a half turns of a copper ribbon -i" wide. The the ^^'inding stretch other, A turns should be equally spaced from the one end of the frame copper wire is and to the soldered on to each end of the The Tesla Coil 104 UJ -*IT'-| T.OC I r — T- I 1 o , f„0 1^ I- t3 DC (I ' I to ° '^ I "-• I U=-i I ' "^ K IP il-jt I — -^ i^; (Jj CO -^J' « o i4 Ti is! H z o ii --./ 4 ^ g^ f Dimensions of primary band for making i"x|", 12" long, strip tiie is Standard Coil 105 A hard rubber connections. screwed across the top of the Two completed oscillation transformer. in it 8-y apart. holes are drilled Into these two bushings, similar to those used in the 12" coil and described in Chapter IV, are When the secondary terminals are soldered to oscillation transformer is mounted in seasoned oak. Chapter VI apply cover is The box is All the directions given The divided into two halves, one carrying the interrupter oscillators. connections from the interrupter to the condenser are made through the hinges so that the cover without disturbing the connections. A may of holes drilled in it of the box. It is It is put in be- has a number to allow of the free circulation of the Suitable handles are put at each end of the transformer be swung back partition tween the transformer and the condenser. The The to the construction of this box. and the other the discharge The the one box. dimensions of this box are given in Fig. 42. in them complete. All the parts of the 7" coil are built out of f" well fitted. is now set on end box oil. for carrying it. in the smaller division held in place by two yoke-shaped, supports fastened to the inside of the box and core between the two sections of the secondary. wooden encircling the The primary terminals are brought to four heavy binding-posts at the upper end of the box. They should be soldered on in the order as for the transformer on the large shorting, the coil, two middle posts puts the sections that is, same so that in series shorting the two outer pairs gives a parallel connection. and Tlie Tesla Coil roo K > Dimensions of The condenser and in place, Standard Coil 7" oscillation transformer are is sec- in glass tubes, From one suitably bent, directly to the condenser. condenser a wire now put The between the two. the condenser being ondary terminals from the transformer are led the 107 side of an end of the primary band led to on the oscillation transformer. The remaining end of the copper band and the other side of the condenser are directly connected to the two hinges of the cover carrying the interrupter. All connections should be carefully soldered. should be of about No. 20 B. in glass tubes & S. They gauge copper wire, enclosed and kept under the oil as much as possible. o o Fig. 43. — Wiring Any one of the forms of V can be used with the coil; Diagram. interrupters described in Chapter the coil in question being equipped with the motor interrupter. The connections between the primary spark-gap and hinges can be run in glass tubes lying in grooves cut in the I" under side of the cover. A piece of hard rubber sheet should be screwed over the grooves wherever there transformer shown or is any danger of shorting to the core of the primary terminals. in the wiring diagram. The connections are io8 Tcsla Coll TJic The two brass oscillators consist of screwed on the end of two rods 7" long, which are -^^" brass from the top of the drilled \" two holes to slide easily in standards, through both the fibre diameter balls J" in and the rod. A set screw at the top of each standard will be of convenience in clamping the rods in any desired position. The standards Two are constructed as follows. hard rubber bushings 2" in diameter and iV' having a flange \" thick and 2^" end are set in is and diameter turned on one in two holes cut in the cover directly abo^•e the on the holes in the brass bushings A I" hole fibre or in length oscillation transformer. Two through the centre of each bushing. drilled f " brass rods 8" long are enclosed in fibre tubes f " in outside diameter and 7 V' The ends tightly. and should be The long. should tubes of the brass rods project tapered to slightly fit fit the from the the bushings rods fibre on the oscillation transformer. may In order that the discharge gap the coil is in operation, are screwed for about The two on the ends of the be adjusted while handles I" in diameter rods, carrying the oscillators, i\". standards are cover until they now slid make good the oscillation transformer. up ^'ulcanite through the bushings in the contact with the bushings on When to the alternating current the coil mains, it is will now connected break forth in may be a beautiful 7" discharge. If everything found in the is not as it ought manner described in to be, the trouble Chapter VII. - Dimensions of 7" Standard Coil 7 i f m§$$^^^ 5 \- Oscillator **« i %5tandar.i> 7 Coil s" BUSHINQ FiG, 44, — Oscillators hrasfi rod Foil 7 COIL and Standards for 7" Apparatus. log APPENDIX For those of our readers disposal, and who who have desire to carry limited Besides many this who possess an ordinary induction three inch spark, which they may This coil is it not is coil, is available, giving a two or article. immersed, hence no boxes oil cities, substitute for the trans- former to be described in the present required, as Appendix are not situated in where an alternating-current lighting supply but at their on some of the many experi- ments possible with high-tension currents, has been added. means will be simply mounted on a base in a place free from dust and moisture. regarding insulation A large amount of the precautions and other things can be dispensed with, thereby reducing the cost of the materials to within the reach of almost every one. While speaking of cost, let us state that to purchase a coil giving a 12" spark from the regular dealers coil in tion would mean an outlay a single box is of about The worth S165. by the amateur, not considering exceed S50 for the 12" coil and $25 $300, while the 7" cost of construc- his time, should not for the 7" coil. This piece of apparatus giving about a not exceed Sio to build at home. It is 3'' spark should large enough for most of the experiments on Roentgen and Geisler tubes and for wireless work o\-er short distances. The Tesla Coil 112 The above sums include simple the The interrupter. others will bring the price up in proportion. The high-frequency coil is made Cut out two as follows: end pieces of i" wood lo" square and describe on each one two concentric having diameters of 9 and circles, On respectively. these circles bore a come 36" Y dowels. mill These are made of hard wood and Cut each dowel long. inches Next procure from a planing apart as in the figure. about twenty number 7 of \" holes i" into 12" lengths and fit one in each of the holes on the smaller circle of one of the boards. When they are place the other board all in other end of the dowels. The empty is The B. & S. until the secondary is put on the outer circle of holes is left wound. secondary winding consists of one layer of No. 32 gauge double cotton covered copper wire. winding about Y from the ends. Begin the Shellac the wire with several coats of the best orange shellac when the winding is finished. The dowels ing for the primary are next put in place by push- them through the holes from one end. tightly the holes may be reamed 18 bare wire are wound on out. coil is six turns of then mounted on a base. Two No. oscillators The ends of mounted on a with standards are provided for the terminals of the secondary. pletes the high-tension coil. too it. the primary are connected to two binding-posts piece of hard rubber. fit the outer dowels, each turn being over an inch from the one next to The whole Next If they This com- A ppendix ^- ^-- 1 "3 Tesla Coil '^^'^ 114 The condenser lo" X 12", with a piece of tin The method of glass. Lay a follows: While top of it, 8" x 10" between each sheet foil on a smooth leaving an inch margin of glass On table and wet place a sheet of still corner lay a strip of tin glass. glass of arranging this condenser glass plate coat of shellac. window consists of fifteen sheets of it On a on tin foil around. all as is gi\e one projecting an inch beyond the foil top of this lay a second sheet of glass and another sheet of tin only the strip in this case foil, on the opposite Continue side. This of glass are used up. is brought out this until the fifteen sheets will give seven sheets of tin foil, with the strips coming out on the one side and seven projecting on the other The side. strips may be fused together with a hot iron and a copper wire soldered on. condenser best is mounted The bound together with in a box. transformer for use with the It formers already described. of No. 20-22 iron lY and when II in is wrapped with The after the & S. trans- core consists of a bundle The method described two sections one above the other. Each or 50-55 volt same as the two diameter in The primary insulating tape. of fastening the layers. No. 16 B. 1 00-110 wires, well annealed. formed is the next piece of apparatus is essentially the is and This completes the condenser. alternating-current circuits to construjt. The whole insulating tape See Fig. i is Chapter is for the wound method section consists of one layer of gauge double cotton covered copper wire. After the primary is wound wrap on well shellacked until the diameter is several layers of paper built up to 2}". Appendix "5 The Tesla Coil ii6 The secondary winding two sections of copper wire. First of & No. 32 B. saw out of wood, 4" in diameter this transformer consists of gauge double cotton covered S. of \" stock four circular pieces and having a 2 J" hole in the centre. shown Slip these on the primary to the positions The two end in the figure. ones are |" from the ends of the core and the middle ones are \" apart. Wind formed layer the wire of the secondary until the diameter and wrap a piece The whole is 3J". just shellac each on before beginning the of paper mounted on a coil is on the two spools Thoroughly next. suitable base, the primary terminals being connected to binding-posts. If the transformer current, the series. If, be operated on the loo-iio to is volt two sections of the primary are connected on the other hand, it is to in be u^ed on the 50-55 volt current the sections are joined in parallel. It is well, however, in either case to bring the primary terminals out to four separate binding-posts. tions may Always be be readily certain, the windings in the In order to set made Then for the desired connec- either series or parallel. though, that the current will traverse same direction. up the high oscillations we must introduce a spark-gap in series with the secondary of the transformer The method and the high-tension coil. primary spark-gap given as follows: Procure two pieces is of making this of vulcanized fibre rod |" in diameter 4 inches long. Drill' a j" hole in each V' from one end. holes Next bore two 6" apart in the base of the transformer as shown -|" in Fig. 47. — Appendix 117 Drive the fibre supports into these holes with the holes in the fibre in line. The spark-gap fibre tube is made of two }" brass rods 6" long with long slipped over the end to act as an insu- 2'' One lating handle. lead of the secondary of the transformer goes directiy to one rod, the other goes to the primary of the high-tension The coil. high-tension coil is return wire from the primary of the soldered to the other side of the spark-gap. The diagram shows how the condenser is connected and also the connections just described. —6 ^H ^-- 1- --^ i Fig. 47. There care is Prim-^ry Spakk-g.\p. no interrupter used with must be taken that the spark is apparatus so that this long enough to prevent arcing. Those possessing a suitable induction to substitute this for may do so the transformer coil and who wish and primarj' spark-gap by changing one connection. Disconnect one terminal of the secondary from the discharger the and connect secondary terminal to a binding-post suitably insulated by hard rubber. One terminal of the primary of the high- The Tesla Coil ii8 tension coil is connected to the spark-gap instead of the sec- ondary of the induction tension coils primary The coil. is other terminal of the high- connected to the new binding-post. A glance at the figure will make this plain and also the method Fig. 48.*-^ Fig. 49. of connecting WriUNG Diagram. — Wiring up the condenser. Diagram. When making between the various parts of the apparatus the wires in glass tubes The and to it is connections well to enclose keep them back out of the way. operator will soon find that ordinary insulation is of Appendix no value whatever in dealing so that all terminals with these high-tension currents, must be kept apart a distance greater than that of the high-tenson discharge gap. caution is 119 If this pre- not observed you will have some very beautiful brush discharges close proximity. all along the conductors that are in too
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