We are given the vector field:
\[
\vec{v} = x^3 \hat{i} + y^3 \hat{j} + z^3 \hat{k}.
\]
By the Gauss divergence theorem, the outward flux of the vector field over the surface of a closed surface \( S \) is given by:
\[
\iint_S \vec{v} \cdot \hat{n} \, dA = \iiint_V (\nabla \cdot \vec{v}) \, dV,
\]
where \( \nabla \cdot \vec{v} \) is the divergence of \( \vec{v} \).
The divergence of \( \vec{v} \) is:
\[
\nabla \cdot \vec{v} = \frac{\partial}{\partial x} (x^3) + \frac{\partial}{\partial y} (y^3) + \frac{\partial}{\partial z} (z^3) = 3x^2 + 3y^2 + 3z^2 = 3(x^2 + y^2 + z^2).
\]
Since we are integrating over the surface of a unit sphere (where \( x^2 + y^2 + z^2 = 1 \)), the integral becomes:
\[
\iiint_V 3 \, dV = 3 \times \text{Volume of the unit sphere}.
\]
The volume of a unit sphere is \( \frac{4}{3}\pi \), so the outward flux is:
\[
3 \times \frac{4}{3}\pi = 4\pi.
\]
Numerically,
\[
4\pi \approx 12.566.
\]
Thus, the value of the outward flux is approximately \( 12.6 \).