Step 1: Recall the work-energy theorem.
The work done by all forces on an object equals the change in its kinetic energy:
\[
W_\text{net} = K_f - K_i
\]
Step 2: Identify which force components do work.
The displacement is $\vec{s} = 6\hat{i}$, which is purely in the $x$-direction.
Work is done only by the component of force parallel to the displacement.
So only $F_x = 4\,\text{N}$ does work; the $y$-component ($-15\hat{j}$) does no work because it is perpendicular to the displacement.
Step 3: Compute the work done by the x-component of force.
\[
W = F_x \times s_x = 4 \times 6 = 24\,\text{J}
\]
Step 4: Verify using dot product.
\[
W = \vec{F} \cdot \vec{s} = (4\hat{i} - 15\hat{j}) \cdot (6\hat{i}) = 24 + 0 = 24\,\text{J}
\]
Step 5: Apply the work-energy theorem.
Initial kinetic energy $K_i = 7\,\text{J}$.
\[
W = K_f - K_i \implies K_f = K_i + W = 7 + 24 = 31\,\text{J}
\]
Step 6: State the final answer.
\[
\boxed{31\,\text{J}}
\]