As important as the measurements of the astronomer are those of the electrician. It was as recently as 1819 that Oersted, a Danish physicist, published a discovery which became a foundation stone of electrical engineering, and upon which rises the art of electrical measurement. He observed that when an electric current is passing through a wire, a nearby magnetic needle tends to place itself at right angles to the wire, the deflection varying with the strength of the current. When instead of a wire, a coil, duly insulated, is employed to carry the current, effects much more decided are displayed. At first current-measurers, or galvanometers, employed simple compass needles; these proved to be unsatisfactory. They were affected by the variations which occur in the intensity of the earth’s magnetism; and no matter how carefully a needle was made, it varied in strength from week to week, from year to year; again, a current might be so strong as to create magnetism overwhelming in comparison with that of the earth, and quite beyond the measuring power of a compass needle. A galvanometer on a plan due to Professor James Clerk Maxwell, employs a permanent magnet, or an electro-magnet, which is stationary, between the poles of which may freely turn a coil bearing the current to be measured. This current in the case of an ocean cable is so weak that no other means of indication will serve. Lord Kelvin’s recording apparatus for such a cable is a galvanometer on this principle. In order to concentrate the lines of magnetic force on the vertical sides of the coil, a piece of soft iron, D, is fixed between the poles of the magnet. This iron becomes magnetized by induction, so as to produce a very powerful field of force, in the minute spaces between it and the two magnetic poles, through which spaces the vertical sides of the coil are free to move. Instruments of this kind, developed by D’Arsonval, are known by his name.
Weston Instruments.
Instruments for electrical measurement, with stationary magnets and moving coils, of great excellence, are manufactured by the Weston Company, Waverly Park, New Jersey. Their accuracy rests upon several important discoveries by Dr. Edward Weston: first, a method of making a magnet which is really permanent, retaining its original strength for a long time: second, by the preparation of a remarkable group of alloys which under ordinary variations of temperature manifest scarcely any change in conductivity, and which set up but little thermo-electric action as they touch other metals in an instrument. Let us see how a Weston voltmeter, or measurer of electric pressure, is constructed.
Weston voltmeter.
A light rectangular coil of copper wire, C, is wound on an aluminium frame pivoted in jeweled bearings so as to be free to rotate in the ring-like space between an inner cylindrical soft iron core, K, and the pole pieces P and P of the permanent magnet, M. A light aluminium pointer, p, is attached to the coil and is free to move across the scale, D. The current enters the coil through the two spiral springs S and S, which serve also to control the movement of the coil. When a current passes through the coil the dynamic action between the current and the magnetic field tends to rotate the coil, and the position of equilibrium between this force and the torsion of the springs, indicated by the pointer, measures the current passing through the coil. Because the magnetic field is practically unvarying throughout, and the torsion of the springs is proportionate to their deflection, the scale is virtually uniform. This is not assumed in their manufacture, however, for each instrument is calibrated by direct reference to standards. As the aluminium frame moves through the magnetic field, slight currents are generated within the metal; these serve to dampen vibrations so that the pointer comes to rest almost instantly without friction. That the magnetic field may have the utmost strength, the air gap in which the coil rotates is made as narrow as possible; this is ensured by workmanship of the highest skill, and by tools specially designed. The hardened steel pivots are ground and centered as in the best watch-making: the coil is balanced by means of adjustable weights so that none but electrical forces may come into play. In a Weston voltmeter of regular type, the maximum current required for a full scale-deflection is only 0.01 ampere. Instruments of much higher sensibility are constructed for measuring insulation, requiring but 0.0006 ampere for the same deflection. So much for the task of measuring electrical pressure.
For measuring electrical currents, which differ from pressures as the quantity of water flowing in a pipe differs from the pressure of that water as shown in a common gauge, a Weston ammeter, or ampere-meter, may be employed. It is similar to the voltmeter just described, being in fact a milli-voltmeter actuated by the difference in electrical potential, or pressure, between the terminals of a standard resistance, the shunt, through which a definite fraction of the current passes. It is as if a known part of the flow of a river being measured, the volume of the whole stream is learned.
The two principal alloys discovered by Dr. Weston, and used in his instruments, are manganin and nickelin. Manganin has about twenty-five times the resistance of copper, and increases in resistance about 0.00001 for each degree Centigrade through which its temperature rises. Nickelin has about twenty-nine times the resistance of copper, and decreases in resistance about 0.00004 for each degree Centigrade through which its temperature rises. These and other alloys used in construction are carefully worked and annealed according to methods perfected in years of experience. After a wire for an instrument is drawn, its fibres, being in a state of unequal strain, undergo an artificial aging process so that their resistance shall remain unchanged after adjustment. The Weston instruments are based on the international volt and ampere adopted by the National Bureau of Standards at Washington. Instruments of the regular portable type have a guaranteed accuracy of one part in 400, while the laboratory standard semi-portable instruments are guaranteed to one part in 1000. Weston voltmeters and ammeters are constantly being checked after years of active service, and are found correct within the guaranteed limits of accuracy.
This remarkable success testifies to the importance of asking, What properties are needed in the material of which an instrument is to be built? That question duly answered, it becomes a task for research to provide these materials, that skill may put them together in compact and convenient form.[29]