Step 1: Recognize the tool needed.
The integral asks for the flux of \(\vec{F}\) through a closed surface, the unit sphere. The divergence theorem converts a closed surface integral into a volume integral of the divergence:
\[
\oiint_S \vec{F}\cdot d\vec{s}=\iiint_V (\nabla\cdot\vec{F})\,dV
\]
Step 2: Compute the divergence of \(\vec{F}\).
\[
\vec{F}(x,y,z)=\sin(y)\,\hat{x}+\cos(x)\,\hat{y}+5\,\hat{z}
\]
\[
\nabla\cdot\vec{F}=\frac{\partial}{\partial x}\big(\sin(y)\big)+\frac{\partial}{\partial y}\big(\cos(x)\big)+\frac{\partial}{\partial z}(5)
\]
Step 3: Evaluate each partial derivative.
\(\sin(y)\) does not depend on \(x\), so \(\dfrac{\partial}{\partial x}\big(\sin(y)\big)=0\). \(\cos(x)\) does not depend on \(y\), so \(\dfrac{\partial}{\partial y}\big(\cos(x)\big)=0\). The constant \(5\) does not depend on \(z\), so \(\dfrac{\partial}{\partial z}(5)=0\).
Step 4: Add up the divergence.
\[
\nabla\cdot\vec{F}=0+0+0=0
\]
The divergence is zero everywhere in space, not just on the sphere.
Step 5: Apply the divergence theorem.
Since \(\nabla\cdot\vec{F}=0\) at every point inside the unit ball,
\[
\iiint_V (\nabla\cdot\vec{F})\,dV=\iiint_V 0\,dV=0
\]
Step 6: Final conclusion.
\[
\boxed{0.0}
\]