In the circuit shown in the figure, $V_s = V_m \sin 2t$ and $Z = 1 - j$. The value of $C$ is chosen such that the current $I$ is in phase with $V_s$. The value of $C$ in farad is, 
Working directly in terms of currents rather than admittances, take \(V_s = 1\angle 0^\circ\) as a reference phasor. The current drawn by the fixed branch is \[ I_Z = \frac{V_s}{Z} = \frac{1}{1-j} = 0.5+j0.5 \text{ A} \] which has an in-phase component of \(0.5\) A and a quadrature component of \(0.5\) A. The capacitor draws a purely quadrature current \(I_C = j\omega C V_s = j2C\) A. For the total current \(I_Z+I_C\) to line up exactly with \(V_s\) (zero net phase angle), the capacitor's contribution must match \(0.5\) A in magnitude at \(\omega=2\) rad/s: \[ 2C = 0.5 \]
Therefore, the correct answer is \(1/4\) F.