Concept:
For a body rolling without slipping,
\[
mgh
=
\frac12 mv^2+\frac12 I\omega^2.
\]
For a solid sphere,
\[
I=\frac{2}{5}mR^2.
\]
The rotational kinetic energy is
\[
K_r=\frac12 I\omega^2.
\]
Step 1: Express rotational kinetic energy in terms of translational kinetic energy.
Since
\[
v=R\omega,
\]
\[
K_r
=
\frac12\left(\frac25mR^2\right)\omega^2
=
\frac15 mv^2.
\]
Also,
\[
K_t
=
\frac12 mv^2.
\]
Hence,
\[
K_r=\frac25K_t.
\]
Step 2: Use conservation of energy.
\[
mgh
=
K_t+K_r
=
K_t+\frac25K_t
=
\frac75K_t.
\]
Therefore,
\[
K_t
=
\frac57 mgh.
\]
Thus,
\[
K_r
=
\frac25\left(\frac57 mgh\right)
=
\frac27 mgh.
\]
Step 3: Substitute the given values.
\[
K_r
=
\frac27(3)(10)(7).
\]
\[
K_r
=
60\,\text{J}.
\]
Step 4: Write the final answer.
\[
\boxed{K_r=60\,\text{J}}
\]
\[
\boxed{\text{Answer = (D)}}
\]