In a static fluid, the pressure variation is governed by the equation:
\[\frac{dp}{dy} = -Y,\]
where:
$p$ is the pressure,
$y$ is the vertical direction,
$Y$ is the specific weight of the fluid $= \rho g$,
$-$ sign indicates that pressure decreases as we move upward.
The specific weight $Y$ is the product of the fluid density $\rho$ and gravitational acceleration $g$, so the pressure variation depends on both.
Match List-I with List-II\[ \begin{array}{|c|c|} \hline \textbf{Type of fluids} & \textbf{Relationship between shear stress and velocity gradient} \\ \hline (A) \text{Newtonian fluid} & (III) \text{Linear} \\ (B) \text{Non-Newtonian fluid} & (IV) \text{Non-linear} \\ (C) \text{Ideal Fluid} & (I) \text{Zero velocity gradient} \\ (D) \text{Ideal Plastic} & (II) \text{With definite yield stress and linear relationship} \\ \hline \end{array} \]