The upward buoyant force that is exerted on a body immersed in a fluid, whether fully or partially, is equal to the weight of the fluid that the body displaces.
The pressure drop in an incompressible and Newtonian fluid in laminar flow flowing through a long cylindrical pipe of constant cross section is inversely proportional to the fourth power of the radius of the pipe.
The speed of efflux of a fluid through a sharp-edged hole at the bottom of a tank filled to a depth h is the same as the speed that a body (in this case a drop of water) would acquire in falling freely from a height h: v=2gh.
Describes the capillary pressure difference sustained across the interface between two static fluids, such as water and air, due to the phenomenon of surface tension.