Consider a circuit where a cell of emf \( E_0 \) and internal resistance \( r \) is connected across the terminal A and B as shown in the figure. The value of \( R \) for which the power generated in the circuit is maximum, is given by:
Step 1: The total resistance in the circuit is the sum of the internal resistance \( r \) and the external resistance \( R \).
Step 2: The power generated in the circuit is given by:
\[ P = \frac{E_0^2}{R_{\text{total}}} \times R = \frac{E_0^2}{(R + r)^2} \times R, \]
where \( R_{\text{total}} = R + r \) is the total resistance in the circuit.
Step 3: To find the value of \( R \) that maximizes the power, we take the derivative of the power with respect to \( R \) and set it equal to zero:
\[ \frac{dP}{dR} = \frac{E_0^2 (R + r) - E_0^2 R \times 2(R + r)}{(R + r)^4} = 0. \]
Simplifying, we find:
\[ (R + r) - 2R = 0, \]
\[ R = 3r. \]
Thus, the value of \( R \) for which the power is maximum is \( R = 3r \).
A battery of emf \( E \) and internal resistance \( r \) is connected to a rheostat. When a current of 2A is drawn from the battery, the potential difference across the rheostat is 5V. The potential difference becomes 4V when a current of 4A is drawn from the battery. Calculate the value of \( E \) and \( r \).
A constant voltage of 50 V is maintained between the points A and B of the circuit shown in the figure. The current through the branch CD of the circuit is :
A quantity \( X \) is given by: \[ X = \frac{\epsilon_0 L \Delta V}{\Delta t} \] where:
- \( \epsilon_0 \) is the permittivity of free space,
- \( L \) is the length,
- \( \Delta V \) is the potential difference,
- \( \Delta t \) is the time interval.
The dimension of \( X \) is the same as that of: