Concept:
By Stokes' Theorem,
\[
\iint_S (\nabla\times\vec{F})\cdot\vec{N}\,dS
=
\oint_C \vec{F}\cdot d\vec{r},
\]
where \(C\) is the boundary of the surface \(S\).
If the surface is a closed surface (such as a sphere), then its boundary is empty. Hence, the line integral is zero.
Equivalently,
\[
\nabla\cdot(\nabla\times\vec{F})=0,
\]
and applying the Divergence Theorem also gives zero flux of the curl through any closed surface.
Step 1: Identify the nature of the surface.
The given surface
\[
x^2+y^2+z^2=a^2
\]
is a closed sphere.
Hence,
\[
\partial S=\varnothing.
\]
Step 2: Apply Stokes' Theorem.
Therefore,
\[
\iint_S(\nabla\times\vec{F})\cdot\vec{N}\,dS
=
\oint_{\partial S}\vec{F}\cdot d\vec r.
\]
Since
\[
\partial S=\varnothing,
\]
the line integral is
\[
\oint_{\partial S}\vec{F}\cdot d\vec r=0.
\]
Thus,
\[
\iint_S(\nabla\times\vec{F})\cdot\vec{N}\,dS=0.
\]
Hence,
\[
\boxed{(D)\;0.}
\]