When resistors are connected in parallel, the voltage across each resistor is identical. Initially, we determine the equivalent resistance (\(R_\text{eq}\)) of the parallel arrangement:
\[ \frac{1}{R_\text{eq}} = \frac{1}{R_1} + \frac{1}{R_2} = \frac{1}{1\ \Omega} + \frac{1}{3\ \Omega} = \frac{4}{3}\ \Omega \] \[ R_\text{eq} = \frac{3}{4}\ \Omega \]
Subsequently, employing Ohm’s law (\(V = IR\)), we ascertain the voltage across the parallel combination:
\[ V = I \times R_\text{eq} = 1\ \text{A} \times \frac{3}{4}\ \Omega = \frac{3}{4}\ \text{V} \]
Given that the voltage is uniform across each resistor in a parallel circuit, the voltage across the \(3\ \Omega\) resistor is also \(\frac{3}{4}\ \text{V}\). We can now calculate the current (\(I_2\)) through the \(3\ \Omega\) resistor utilizing Ohm’s law once more:
\[ I_2 = \frac{V}{R_2} = \frac{\frac{3}{4}\ \text{V}}{3\ \Omega} = \frac{1}{4}\ \text{A} = 0.25\ \text{A} \]
Consequently, the current traversing the \(3\ \Omega\) resistor amounts to \(0.25\) amperes.
