The circuit has a 3 V cell connected to resistances of \(1 \, \Omega\), \(4 \, \Omega\), and \(4 \, \Omega\). The total resistance \(R_{\text{total}}\) of the circuit is calculated as:
\[ R_{\text{total}} = R_{\text{internal}} + R_{\text{external}} \]
The external resistance is a parallel combination of \(4 \, \Omega\) and \(4 \, \Omega\):
\[ R_{\text{parallel}} = \frac{1}{4} + \frac{1}{4} = 2 \, \Omega. \]
Thus, the total resistance becomes:
\[ R_{\text{total}} = 1 \, \Omega + 2 \, \Omega = 3 \, \Omega. \]
The current in the circuit is:
\[ i = \frac{\text{EMF}}{R_{\text{total}}} = \frac{3 \, \text{V}}{3 \, \Omega} = 1 \, \text{A}. \]
The terminal potential difference \(V_{\text{terminal}}\) is given by:
\[ V_{\text{terminal}} = \text{EMF} - i R_{\text{internal}} = 3 \, \text{V} - (1 \, \text{A} \cdot 1 \, \Omega) = 2 \, \text{V}. \]
Final Answer: 2 V
Two cells of emf 1V and 2V and internal resistance 2 \( \Omega \) and 1 \( \Omega \), respectively, are connected in series with an external resistance of 6 \( \Omega \). The total current in the circuit is \( I_1 \). Now the same two cells in parallel configuration are connected to the same external resistance. In this case, the total current drawn is \( I_2 \). The value of \( \left( \frac{I_1}{I_2} \right) \) is \( \frac{x}{3} \). The value of x is 1cm.
Let \( T_r \) be the \( r^{\text{th}} \) term of an A.P. If for some \( m \), \( T_m = \dfrac{1}{25} \), \( T_{25} = \dfrac{1}{20} \), and \( \displaystyle\sum_{r=1}^{25} T_r = 13 \), then \( 5m \displaystyle\sum_{r=m}^{2m} T_r \) is equal to: