Physics:Lamb surface

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Short description: Smooth, connected 2D surfaces in fluid dynamics

In fluid dynamics, Lamb surfaces are smooth, connected orientable two-dimensional surfaces, which are simultaneously stream-surfaces and vortex surfaces, named after the physicist Horace Lamb.[1][2][3] Lamb surfaces are orthogonal to the Lamb vector [math]\displaystyle{ \boldsymbol{\omega}\times\mathbf{u} }[/math] everywhere, where [math]\displaystyle{ \boldsymbol{\omega} }[/math] and [math]\displaystyle{ \mathbf{u} }[/math] are the vorticity and velocity field, respectively. The necessary and sufficient condition are

[math]\displaystyle{ (\boldsymbol{\omega}\times\mathbf{u})\cdot[\nabla\times(\boldsymbol{\omega}\times\mathbf{u})]=0, \quad \boldsymbol{\omega}\times\mathbf{u}\neq 0. }[/math]

Flows with Lamb surfaces are neither irrotational nor Beltrami. But the generalized Beltrami flows has Lamb surfaces.

See also

References

  1. Lamb, H. (1932). Hydrodynamics, Cambridge Univ. Press,, 134–139.
  2. Truesdell, C. (1954). The kinematics of vorticity (Vol. 954). Bloomington: Indiana University Press.
  3. Sposito, G. (1997). On steady flows with Lamb surfaces. International journal of engineering science, 35(3), 197–209.