Velocity potential
Template:Short description Template:More citations needed Within the applied mathematical study of fluid dynamics and continuum mechanics, a velocity potential is a scalar potential used in potential flow theory. It was introduced by Joseph-Louis Lagrange in 1788.[1]
Suppose a smooth vector field in a simple connected region represents the flow velocity of a fluid at each point. This flow field is said to be irrotational when If the flow field is irrotational, then it can be also be represented as the gradient of a scalar function :
is known as a velocity potential for Template:Math. Velocity potentials are unique up to a constant and a function solely of the temporal variable. So if is a velocity potential, then generates the same flow field as .
The Laplacian of a velocity potential is equal to the divergence of the corresponding flow. Hence if a velocity potential satisfies Laplace equation, the flow is incompressible.
Unlike a stream function, a velocity potential can exist in three-dimensional flow.
Usage in acoustics
In theoretical acoustics,[2] it is often desirable to work with the acoustic wave equation of the velocity potential instead of pressure Template:Mvar and/or particle velocity Template:Math. Solving the wave equation for either Template:Mvar field or Template:Math field does not necessarily provide a simple answer for the other field. On the other hand, when is solved for, not only is Template:Math found as given above, but Template:Mvar is also easily found—from the (linearised) Bernoulli equation for irrotational and unsteady flow—as