Step 1: Pick the easiest method.
Instead of finding the force, we use the work-energy theorem: the work done by the force equals the change in kinetic energy. \[ W = \Delta KE = \tfrac{1}{2}m v_f^2 - \tfrac{1}{2}m v_i^2 \]
Step 2: Get the velocity from displacement.
The displacement is $S = \dfrac{t^3}{3}$. Velocity is the time derivative: \[ v = \frac{dS}{dt} = t^2 \]
Step 3: Find the speeds at the two times.
At $t = 0$: $v_i = 0^2 = 0$. At $t = 2\ \text{s}$: $v_f = 2^2 = 4\ \text{m s}^{-1}$.
Step 4: Apply the theorem.
With mass $m = 3\ \text{kg}$, \[ W = \tfrac{1}{2}(3)\left(4^2 - 0^2\right) = \tfrac{1}{2}(3)(16) = 24\ \text{J} \]
Step 5: Conclusion.
The work done in the first 2 seconds is 24 J. \[ \boxed{24\ \text{J}} \]