Relative to the zz-axis, the axial velocity is the scalar uz=uezu_z=u\cdot e_z; its vector contribution is uzezu_z e_z. Along a particle trajectory, dz/dt=uz(t,X(t))dz/dt=u_z(t,X(t)).

Axial flow

A purely axial flow has u=uzezu=u_z e_z, while a general flow can have axial motion together with radial motion and swirl. “Axial outflow” describes motion away from a specified central region along the axis; its sign can differ on the two sides of that region.

For a purely axial differentiable flow, incompressibility requires zuz=0\partial_z u_z=0. Radial components can balance a nonzero axial derivative in a general incompressible flow.