Correct answer is (c) \(div(\vec{V})=0\)
The best explanation: Taking the continuity equation,
\(\frac{\partial\rho}{\partial t}+\nabla.(\rho \vec{V})=0\)
For incompressible flow, ρ is constant
\(\frac{\partial\rho}{\partial t}+\nabla.(\rho \vec{V})=0\)
The resulting equation is
\(\nabla.(\rho \vec{V})=0\)
\(\rho\nabla.(\vec{V})=0\)
\(\nabla.(\vec{V})=0\)
Thus, for incompressible flow, divergence of \(\vec{V}=0\).