
Here, \(R_2\), \(R_3\), and \(R_4\) are in parallel. The equivalent resistance of these resistors is given by:
\[ \frac{1}{R_{234}} = \frac{1}{R_2} + \frac{1}{R_3} + \frac{1}{R_4} = \frac{1}{8} + \frac{1}{4} + \frac{1}{8} \]
\[ R_{234} = 2 \, \Omega \]
This resistance is in series with \(R_1\), so the total equivalent resistance is:
\[ R_{\text{total}} = R_1 + R_{234} = 10 \, \Omega + 2 \, \Omega = 12 \, \Omega \]
The current supplied by the battery is:
\[ I = \frac{V}{R_{\text{total}}} = \frac{12 \, V}{12 \, \Omega} = 1 \, \text{A} \]

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.
Current passing through a wire as function of time is given as $I(t)=0.02 \mathrm{t}+0.01 \mathrm{~A}$. The charge that will flow through the wire from $t=1 \mathrm{~s}$ to $\mathrm{t}=2 \mathrm{~s}$ is:
Let R = {(1, 2), (2, 3), (3, 3)}} be a relation defined on the set \( \{1, 2, 3, 4\} \). Then the minimum number of elements needed to be added in \( R \) so that \( R \) becomes an equivalence relation, is: