Concept:
A very important vector identity is:
\[
\nabla\cdot(\nabla\times \vec A)=0
\]
for any sufficiently differentiable vector field \(\vec A\).
This means the divergence of the curl of any vector field is always zero.
Step 1: Understand the identity.
The curl of a vector field is
\[
\nabla\times \vec a
\]
Taking divergence of this curl gives
\[
\nabla\cdot(\nabla\times \vec a)
\]
This expression is always zero.
Step 2: Check option (A).
\[
\nabla\cdot \vec a=0
\]
This is not always true for every vector field.
It is true only for solenoidal vector fields.
Step 3: Check option (B).
\[
\nabla\times \vec a=0
\]
This is not always true for every vector field.
It is true only for irrotational vector fields.
Step 4: Select the universal identity.
The identity that always holds is
\[
\nabla\cdot(\nabla\times \vec a)=0
\]
Step 5: Final answer.
\[
\boxed{\nabla\cdot(\nabla\times \vec a)=0}
\]