For irrotational flow, the vorticity ($\vec{\omega}$) must be zero: \[ \vec{\omega} = \nabla \times \vec{v} = 0. \] In three-dimensional flow, this condition implies that each component of vorticity must vanish. For the specific component: \[ \omega_z = \frac{\partial v}{\partial y} - \frac{\partial w}{\partial x} = 0. \] Thus, for irrotational flow: \[ \frac{\partial v}{\partial y} = \frac{\partial w}{\partial x}. \]