A planar called a parallel shear flow has the form

u(x1,x2,x3)=(U(x2),0,0),u(x_1,x_2,x_3)=(U(x_2),0,0),

where the velocity is parallel to a fixed direction and its speed varies transversely. It is incompressible, and U(x2)U'(x_2) measures its shear. Its vorticity is (0,0,U(x2))(0,0,-U'(x_2)).

Advection and evolution

For this profile, (u)u=0(u\cdot\nabla)u=0, since the field is independent of x1x_1. Allowing U=U(t,x2)U=U(t,x_2), the unforced Navier–Stokes equation with constant pressure reduces to tU=νx22U\partial_tU=\nu\partial_{x_2}^2U.

Terminology

Shear can also describe differential motion in more general geometries. In a rotating flow, variation of angular velocity with radius is differential rotation, and its shear expressions include the cylindrical geometry.

References