When two cells are connected in series, the total emf is the sum of the individual emfs, and the total resistance is the sum of the internal resistances and the external resistance.
Let the emf of each cell be \( E \), the internal resistances of the two cells be \( r_1 \) and \( r_2 \), and the external resistance be \( R \). The potential difference across the first cell is zero, which means no current flows through the first cell.
This implies that the potential drop across the internal resistance of the first cell is exactly equal to the emf of the second cell.
Using Ohm's law and the conditions provided, we get the relationship: \[ R = r_1 - r_2 \]
Thus, the correct value of \( R \) is: \[ \text{(3) } r_1 - r_2 \]
The graph between variation of resistance of a wire as a function of its diameter keeping other parameters like length and temperature constant is
A wire of resistance $ R $ is bent into a triangular pyramid as shown in the figure, with each segment having the same length. The resistance between points $ A $ and $ B $ is $ \frac{R}{n} $. The value of $ n $ is:
Two point charges M and N having charges +q and -q respectively are placed at a distance apart. Force acting between them is F. If 30% of charge of N is transferred to M, then the force between the charges becomes:
If the ratio of lengths, radii and Young's Moduli of steel and brass wires in the figure are $ a $, $ b $, and $ c $ respectively, then the corresponding ratio of increase in their lengths would be: