Step 1: Check for compressibility by evaluating the divergence of the velocity field.
The divergence of \( \vec{V} \) is given by:
\[
\nabla \cdot \vec{V} = \frac{\partial V_x}{\partial x} + \frac{\partial V_y}{\partial y}.
\]
Substituting \( V_x = 3 \) and \( V_y = 5x \):
\[
\nabla \cdot \vec{V} = 0 + 0 = 0.
\]
Since the divergence is zero, the fluid is incompressible.
Step 2: Check for rotational or irrotational flow by evaluating the curl of the velocity field.
The curl of \( \vec{V} \) in two dimensions is given by:
\[
\nabla \times \vec{V} = \left( \frac{\partial V_y}{\partial x} - \frac{\partial V_x}{\partial y} \right) \hat{k}.
\]
Substituting the components:
\[
\nabla \times \vec{V} = (5 - 0) \hat{k} = 5 \hat{k}.
\]
Since the curl is not zero, the flow is rotational.