Methods of Measuring Electrical Resistance

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Here a and /3 are thrown, the one in series with A and the FIG. 609b.
other in series with B. Thus the equation of the bridge in this case becomes, (A + a) b - (B + 0) a = 0. (2) In the actual employment of the Kelvin double bridge the resist- ART. 610] THE MEASUREMENT OF LOW RESISTANCE 117 ance d can never be made zero, -tho it should be made as small as possible.
Referring to Fig. 609a, A and B are two low resistances (pro- vided with potential points at 1, 2, and 1', 2') which are to be comp
...ared, the resistance of both A and B being that included between potential points. The resistance d, called the " yoke, " connects A and B. Besides being made as low as possible it is arranged to be easily removed as, for example, by withdrawing a copper link from two mercury cups. The other four resistances a, b and a, /3 are relatively high resistances and are called the ratio coils. Because there are two pairs of ratio coils the net-work is called a " double bridge. " 610. Theory of the Kelvin Double Bridge.

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