. W HEATSTONE B RIDGE As an application of Kirchhoff’s rules consider the circuit shown in Fig. . , which is called the Wheatstone bridge .
The bridge has four resistors R , R , R and R . Across one pair of diagonally opposite points (A and C in the figure) a source is connected. This ( i.e. , AC) is called the battery arm.
Between the other two vertices, B and D, a galvanometer G (which is a device to detect currents) is connected. This line, shown as BD in the figure, is called the galvanometer arm. For simplicity, we assume that the cell has no internal resistance. In general there will be currents flowing across all the resistors as well as a current I g through G.
Of special interest, is the case of a balanced bridge where the resistors are such that I g = . We can easily get the balance condition, such that there is no current through G. In this case, the Kirchhoff’s junction rule applied to junctions D and B (see the figure)