Step 1: Use the work-energy theorem.
According to the work-energy theorem,
\[
W=\Delta K
\]
where
\[
W=\text{work done}
\]
and
\[
\Delta K=K_f-K_i
\]
Step 2: Find the work done by the force.
Given,
\[
\vec{F}=4\hat{i}-15\hat{j}
\]
and displacement
\[
\vec{s}=6\hat{i}
\]
Work done is the dot product:
\[
W=\vec{F}\cdot \vec{s}
\]
\[
=(4\hat{i}-15\hat{j})\cdot (6\hat{i})
\]
\[
=24
\]
Thus,
\[
W=24\,\text{J}
\]
Step 3: Find the final kinetic energy.
Initial kinetic energy:
\[
K_i=7\,\text{J}
\]
Using
\[
W=K_f-K_i,
\]
we get
\[
24=K_f-7
\]
\[
K_f=31\,\text{J}
\]
Step 4: Final conclusion.
Hence, the kinetic energy at the end of the displacement is
\[
\boxed{31\,\text{J}}
\]