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equivalent amount of heat is obtained by dividing the expression by J, the mechanical equivalent of heat.

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In an induction coil, electricity of large current and low pressure is converted into an equivalent electrical energy of small current and high pressure, by means of a bar of soft iron or a bundle of wires, wrapped with two coils of insulated wire of different lengths and diameters. An alternating current being sent through the shorter wire alternately magnetizes and demagnetizes the iron bar with reversed magnetic polarity, and reversals of magnetism in this bar in turn produce an alternating current in the circuit of which the secondary coil is a portion; the secondary current being as stated above of high potential and small quantity.

By suitable structural changes, an induction coil can be inverted as to its functions, and used to convert small electric currents into large ones, with inverse changes in potential.

THE APPARATUS.

The electricity is generated by one of two methods. In the direct system, the dynamo is contained in the machine below the clamps, and the armature contains two windings; the one being a fine winding which is in series with the field magnet coils, and the other winding being merely a bar of copper in the form of a letter U or less than a single coil. This bar being of very low resistance, the maximum current is sufficient for welding purposes, and the terminals are connected directly to the copper clamps. Alternating currents are generated in this machine, and used for welding, in order to avoid commutators, which are necessary in direct current machines. It should be remembered that in all dynamos the electricity is generated in alternating currents, and that these currents are in proper turn fed to brushes of opposite polarity, and thus rendered continuous. In an alternating current dynamo, the electricity is conducted from the armature to rings instead of to a commutator, and is thus better suited for large currents, and some forms of the apparatus do not require rings or any moving contacts. There is no electrical reason why an alternating current should be used except the convenience of its manipulation. In fact, the con

tinuous current supplied by secondary batteries has been used for this purpose.

Another form of apparatus termed the indirect system is more conveniently suited for large work, or in places where a number of welding machines are operated by the current from a single dynamo. The welding current is produced by conversion of the comparatively high tension current by means of an inverted induction coil, termed a transformer. The primary circuit from the dynamo is conducted through many turns of fine wire wound around a soft iron ring, and upon this same ring is a single turn of a large copper bar in which the welding current is produced by inductive effect. These currents receive 4,000 to 15,000 alternations per minute. The welding currents are not changed suddenly or by switches, as such manipulation would not be desirable or even practicable with the great currents used; but in the direct welding machine, a set of resistance coils is placed in the fine circuit which passes around the field magnets, and by interposing more or less of the resistance coils in this circuit, the strength of the magnets is diminished or increased, and the welding current altered accordingly.

With the indirect machine, the amount of the secondary or welding current is controlled by varying the current in the primary coil by means of a kicking coil, or by a variable shunt to the field coils and in other ways.

In either case the apparatus is simple and ir full and complete control at will of the operator by movement of a lever, and this action controls the heat.

THE PROCESS.

In the electric welding process, the two pieces to be joined are secured in firm end contact by a pair of adjustable copper clamps which are placed upon the top of the apparatus. An electric current of large volume is passed through the pieces, and the contact between them being of less conductivity than the homogeneous metal, heating ensues at this place, as the juncture is brought to the proper temperature by the gradual motion of the regulating lever, and as the metal softens, the clamps are pressed towards each other to insure a continuous metallic union across the bar.

The weld begins at the center and proceeds radially towards the surface, as the temperature becomes greater than at the interior.

The heating is further increased by the fact that the resistance of the hot metal is greater than that of cold metal.

The enormous electric currents used in this welding process sometimes reach 50,000 amperes, but with an electro-motive force of half a volt, and therefore not capable of giving any sensation to a person.

It would be injudicious to offer any premium upon ignorance, but the operation of electric welding is one of the simplest of mechanical processes, requiring but little skill on the part of the operator in comparison with that exact training of hand and eye and long experience necessary for ordinary welding. The operator must understand the color of the proper welding heat of the metal under treatment, but this is readily learned. The work is not manipulated during the process, except when it is desired to reduce the burr at the weld, and is at all times under observation, and its heat subject to entire control by means of a lever which graduates the strength of the current.

The dynamo generating the electricity is self-regulating, and requires no attention except for lubrication.

There is no unnecessary waste of fuel, the heating being local, and does not extend far from the weld; cotton-covered wire onefourth of an inch in diameter can be welded without searing the insulation over three-fourths of an inch from the weld.

The time for making a weld varies from a fraction of a second to about two minutes, according to the work; although nothing over two inches diameter has yet been welded, but larger machines are process of construction.

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It is not necessary to provide motive power fully equal to the maximum deniand, as the time is so short that the momentum of a flywheel will serve the same purpose as in a drop press, and give up the surplus energy required.

The power is inversely proportional to the time and appears to be about proportional to the 2.3 power of the diameter in inches, with a slight variation in favor of quick work caused by differences in rates of thermal conductivity of the material.

APPLICATIONS.

The process is far cheaper than that of hand welding, and also extends to other methods of manufacture, but the comparative expense differs according to the previous conditions in every place where it has been applied thus far.

Its applications in practical work thus far have been confined to butt welding for many purposes, such as continuous wire work, carriage work, axles and tires, cotton bale ties, barrel hoops and wire cables and many miscellaneous purposes. Axes are made of drop forgings, joining the tool steel edge to a mild steel poll, bars are heated in the middle and upset forming collars, and pipes are joined together a matter of great value in ice machines. The list might be continued to greater length, but this indicates the range of its practical uses at this early day.

STRENGTH OF ELECTRIC WELDS.

The value of the process, for most purposes, independent from any scientific interest or mechanical ingenuity shown in the apparatus, must be that of the resistance of the welds under tensile

stress.

It will be readily understood however, that, as this process accomplishes many things hitherto impossible, aside from any question of ultimate strength, it is fitted for applications in many constructions where it saves labor and time; provided only that the joints be in all cases sufficiently good for the purpose for which the article is designed. A large field thus opens up in the execution of ornamental design in metal work, where it will supplant screws, rivets or solder for fastenings, and in other evident applications.

There is no reason why such a weld should be stronger than the rest of the bar, but if averaging of equal strength, some of the breaks would occur at the weld. There have been many tests made on various testing machines, but it has been considered preferable to submit only the official record of tests made on the Emery Testing Machine at the U. S. Arsenal at Watertown, Mass.

ORDNANCE DEPARTMENT, U. S. A.

REPORTS OF TESTS BY TENSION OF BARS JOINED BY ELECTRIC WELDS, AT THE TESTING MACHINE, U. s. ARSENAL, WATERTOWN, MASS.

SECTIONAL AREAS.

TENSILE STRENGTH.

Test No.

Marks.

Metal.

Length

Total

At Weld.

Of Bar.

Total

Lbs.

Lbs. sq. in. Position of Fracture. Appearance of Fracture. in bar.

Remarks.

Ins. Inches.

Sq. In. Inches

Sq. In.

4695

Wrt. Iron.

31.75 1.74 diam.=2.39

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1.02.40.408 21,920 53,730

1.50 diam. 1.77 79,640

45,070 34 in. from middle of Fibrous gr. spot at circum- Weld finished with hammer weld. 1.21 57,900 49,500 At weld.. 7.85 42,690 54,380 3 inches from weld.

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11.9

1.02 x .40 .408 21,840 53,530

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12.8 1.17x .48= .562 12.9 1.14 x .45= .513 12.9 1.13 x .49= .513 12.9 1.18x .51= .602 12.8 1.18x .47= .555 12. Not welded 12.

49 diam.=.189

13.35 .50 66 .193

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Octagonal Steel. 16.

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53,480 At weld..

.408 20,400

50,000

Dull Fibrous, in part gr. and spongy

.408 22,240

.408 21,780

.50 diam.=.196 12,520

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.196 11,160 56,940 At the grip.

54,510 2 inches from weld... Fibrous. 53.380 3.7 63,880

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.186 7,690 39,230 At weld.

.196 10,260 52,350 14 inch from weld.

.196 10,280 52,450 1.6
.186 11,080 56,530 1.75
.190 10,270 52,400 1.8
.196 11,170 56,990 1.5
.196 10,060 51,330 1.7
.196 10,120 51,630,1.5
.302 15,700 51,990

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Fibrous.

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.360 45,800 127,220

.360 45,670 126,860 At face of grips..

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