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: \[ \frac{\partial v}{\partial y} = \frac{\partial w}{\partial x}. \]
Match List-I with List-II\[ \begin{array}{|c|c|} \hline \textbf{Type of fluids} & \textbf{Relationship between shear stress and velocity gradient} \\ \hline (A) \text{Newtonian fluid} & (III) \text{Linear} \\ (B) \text{Non-Newtonian fluid} & (IV) \text{Non-linear} \\ (C) \text{Ideal Fluid} & (I) \text{Zero velocity gradient} \\ (D) \text{Ideal Plastic} & (II) \text{With definite yield stress and linear relationship} \\ \hline \end{array} \]