Consider a circuit consisting of four equal resistors R 1, R 2, R 3, R 4 connected in a bridge configuration (figure 2). If we supply it with a current source P along a diagonal, we have at equilibrium a zero voltage between B and D. The variation of any one of the resistors causes a voltage Vs to appear between B and D, which can be measured by an instrument G. For very small variations in resistance (of the order of a few microohms in the case of gauges), the output voltage Vs is practically proportional to the relative variations in resistance ΔR /R of each of the gauges. Neglecting higher-order terms, it is :
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