To solve this problem, we apply the Divergence Theorem, also known as Gauss's theorem. The Divergence Theorem relates the flux of a vector field through a closed surface to the divergence of the field inside the volume bounded by the surface.
We are given that \( \vec{F} = \nabla \times \vec{G} \). Therefore, \(\vec{F}\) is a curl of some vector field \(\vec{G}\).
The Divergence Theorem states:
\[\iint_S \vec{F} \cdot \vec{n} \, ds = \iiint_E \nabla \cdot \vec{F} \, dV\]
Where \( S \) is the boundary of the volume \( E \) and \(\vec{n}\) is the outward normal to \( S \). However, in our case, since \( \vec{F} = \nabla \times \vec{G} \), we use the identity:
\[\nabla \cdot (\nabla \times \vec{G}) = 0\]
The divergence of a curl is always zero. Thus, we have:
\[\iiint_E \nabla \cdot (\nabla \times \vec{G}) \, dV = 0\]
Therefore, by the Divergence Theorem:
\[\iint_S \vec{F} \cdot \vec{n} \, ds = \iiint_E \nabla \cdot \vec{F} \, dV = \iiint_E 0 \, dV = 0\]
Hence, the integral over the closed surface \( S \) is zero.