Navier-Stokes equations

Navier Stokes equations

These equations were derived independently by G.G Stokes and M. Navier in the 19th century, and describe the motion of a non-turbulent Newtonian fluid.

In its general form the equation that describes the motion is:

$\rho \left(\frac{\partial \bf{v}}{\partial t} + \bf{v} \cdot \nabla \bf{v} \right) = -\nabla p + \nabla \cdot \bf{T} + \bf{f}$

where \rho denotes density, p pressure, v is velocity, T is the stress tensor, and f is forces acting on the fluid.


2011-03-29 17:43