Step 1: Set up the divergence theorem.
$S$ is a closed sphere, so the flux integral converts into a volume integral by the divergence theorem: $\alpha = \iiint_V (\nabla \cdot \vec{F})\, dV$, where $V$ is the solid ball bounded by $S$.
Step 2: Compute the divergence.
Differentiate each component of $\vec{F} = (2x+3z)\hat{i}+(xz-y)\hat{j}+(y^2+2z)\hat{k}$ along its own axis and add:
\[ \nabla \cdot \vec{F} = 2 + (-1) + 2 = 3 \]
This is constant everywhere, so $\alpha = 3V$.
Step 3: Shift to the centre and switch to spherical coordinates.
Let $u=x-3, v=y+1, w=z-2$. This shift keeps volumes unchanged and turns the ball into $u^2+v^2+w^2 \le 81$. Using $u=r\sin\phi\cos\theta, v=r\sin\phi\sin\theta, w=r\cos\phi$, the volume element is $r^2\sin\phi\, dr\, d\phi\, d\theta$.
\[ \alpha = 3\int_0^{2\pi}\int_0^{\pi}\int_0^{9} r^2 \sin\phi \, dr\, d\phi\, d\theta \]
Step 4: Evaluate the three integrals one at a time.
\[ \int_0^9 r^2\, dr = \frac{729}{3} = 243, \qquad \int_0^{\pi}\sin\phi\, d\phi = 2, \qquad \int_0^{2\pi} d\theta = 2\pi \]
Multiply these with the constant $3$:
\[ \alpha = 3 \times 243 \times 2 \times 2\pi = 2916\pi \]
Step 5: Find the required value.
\[ \frac{1}{36\pi}\alpha = \frac{2916\pi}{36\pi} = 81 \]
Final Answer:
The required value works out to $81$, the same result the shortcut ball-volume formula would give.
\[ \boxed{81} \]