In fluid dynamics, when a velocity potential (\(\phi\)) exists, the flow is described as irrotational. This is because the existence of a velocity potential implies that the flow is conservative, allowing us to define a scalar function whose gradient gives the velocity field. For a flow to be irrotational, the curl of the velocity vector field must be zero:
\(\nabla \times \mathbf{V} = 0\)
Since \(\mathbf{V} = \nabla \phi\), the curl of a gradient is always zero, i.e.,
\(\nabla \times \nabla \phi = 0\)
Thus, the presence of a velocity potential (\(\phi\)) indicates an irrotational flow, aligning with the properties of potential flow where no vortices are present.