A cell of E.M.F. E and internal resistance r supplies currents for the same time t through external resistance R1 and R2 respectively. If the heat produced in both cases is the same then the internal resistance is |
$\frac{1}{r} = \frac{1}{R_1} + \frac{1}{R_2}$ $ r = \frac{R_1 + R_2}{2}$ $ r = \sqrt{R_1R_2}$ $ r = R_1+R_2$ |
$ r = \sqrt{R_1R_2}$ |
$ H_1 = (\frac{E}{r+R_1})^2 R_1 t$ $ H_2 = (\frac{E}{r+R_2})^2 R_2 t$ $ H_1 = H_2$ $ \Rightarrow R_1(r+R_2)^2 = R_2(r+R_1)^2$ $ r^2(R_1 - R_2) - R_1 R_2 ( R_1 - R_2)=0$ $ since , R_1 -R_2 \text{ is not equal to zero}$ $\Rightarrow r = \sqrt{R_1R_2}$ |