In an RLC circuit with sinusoidal voltage, the impedance can be expressed as:
\[
Z = R + j\left( \omega L - \frac{1}{\omega C} \right)
\]
where \( \omega = 2 \) rad/s (angular frequency), \( R = \frac{1}{3} \, \Omega \), \( L = \frac{1}{4} \, H \), and \( C = 3 \, F \).
The impedance will give us the current, which is:
\[
I(t) = \frac{V(t)}{Z}
\]
Substituting the given values into the formula, we get the current as \( 25 \sin(2t + 53.1^\circ) \), where the phase angle comes from the argument of the impedance.
Final Answer:
\[
\boxed{25 \sin(2t + 53.1^\circ)}
\]