Flow velocity
In fluid dynamics the flow velocity, or velocity field, of a fluid is a vector field which is used to mathematically describe the motion of a fluid. The length of the flow velocity vector is the flow speed.
Contents
Definition
The flow velocity u of a fluid is a vector field
\[ \mathbf{u}=\mathbf{u}(\mathbf{x},t)\]
which gives the velocity of an element of fluid at a position \(\mathbf{x}\,\) and time \( t\, \).
The flow speed q is the length of the flow velocity vector[1]
\[q = || \mathbf{u} ||\]
and is a scalar field.
Uses
The flow velocity of a fluid effectively describes everything about the motion of a fluid. Many physical properties of a fluid can be expressed mathematically in terms of the flow velocity. Some common examples follow:
Steady flow
The flow of a fluid is said to be steady if \( \mathbf{u}\) does not vary with time. That is if
\[ \frac{\partial \mathbf{u}}{\partial t}=0.\]
Incompressible flow
A fluid is incompressible if the divergence of \(\mathbf{u}\) is zero:
\[ \nabla\cdot\mathbf{u}=0.\]
That is, if \(\mathbf{u}\) is a solenoidal vector field.
Irrotational flow
A flow is irrotational if the curl of \(\mathbf{u}\) is zero:
\[ \nabla\times\mathbf{u}=0. \]
That is, if \(\mathbf{u}\) is an irrotational vector field.
Vorticity
The vorticity, \(\omega\), of a flow can be defined in terms of its flow velocity by
\[ \omega=\nabla\times\mathbf{u}.\]
Thus in irrotational flow the vorticity is zero.
The velocity potential
If an irrotational flow occupies a simply-connected fluid region then there exists a scalar field \( \phi \) such that
\[ \mathbf{u}=\nabla\mathbf{\phi} \]
The scalar field \(\phi\) is called the velocity potential for the flow. (See Irrotational vector field.)
Notes and references
- ↑ Courant, R.; Friedrichs, K.O. (1977) (5th ed.), Springer, ISBN 0-387-90232-5, p. 24