Velocity potential

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.

Suppose a smooth vector field 𝐮 in a simple connected region represents the flow velocity of a fluid at each point. This flow field is said to be irrotational when ∇×𝐮=0. If the flow field is irrotational, then it can be also be represented as the gradient of a scalar function ϕ: 𝐮=∇ϕ =∂ϕ∂x𝐢+∂ϕ∂y𝐣+∂ϕ∂z𝐤.

ϕ is known as a velocity potential for u. Velocity potentials are unique up to a constant and a function solely of the temporal variable. So if ϕ(x,y,z) is a velocity potential, then ϕ(x,y,z)+f(t)+C generates the same flow field as ϕ(x,y,z).

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, it is often desirable to work with the acoustic wave equation of the velocity potential ϕ instead of pressure p and/or particle velocity u. ∇2ϕ−1c2∂2ϕ∂t2=0 Solving the wave equation for either p field or u field does not necessarily provide a simple answer for the other field. On the other hand, when ϕ is solved for, not only is u found as given above, but p is also easily found—from the (linearised) Bernoulli equation for irrotational and unsteady flow—as p=−ρ∂ϕ∂t.

See also

Notes

  1. ↑ Anderson, John (1998). A History of Aerodynamics. Cambridge University Press. ISBN 978-0521669559.[page needed]
  2. ↑ Pierce, A. D. (1994). Acoustics: An Introduction to Its Physical Principles and Applications. Acoustical Society of America. ISBN 978-0883186121.[page needed]