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In fluid dynamics, Landau–Squire jet or Submerged Landau jet describes a round submerged jet issued from a point source of momentum into an infinite fluid medium of the same kind. This is an exact solution to the incompressible form of the Navier-Stokes equations, which was first discovered by Lev Landau in 1944 and later by Herbert Squire in 1951. The self-similar equation was in fact first derived by N. A. Slezkin in 1934, but never applied to the jet. Following Landau's work, V. I. Yatseyev obtained the general solution of the equation in 1950.

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  • Jet de Landau-Squire (fr)
  • Landau–Squire jet (en)
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  • In fluid dynamics, Landau–Squire jet or Submerged Landau jet describes a round submerged jet issued from a point source of momentum into an infinite fluid medium of the same kind. This is an exact solution to the incompressible form of the Navier-Stokes equations, which was first discovered by Lev Landau in 1944 and later by Herbert Squire in 1951. The self-similar equation was in fact first derived by N. A. Slezkin in 1934, but never applied to the jet. Following Landau's work, V. I. Yatseyev obtained the general solution of the equation in 1950. (en)
  • En mécanique des fluides le jet de Landau-Squire ou jet de Landau immergé décrit l'influence d'une source ponctuelle dans un écoulement stationnaire, incompressible, en géométrie cylindrique. La solution analytique de ce problème a été donnée par Lev Landau en 1944 et Herbert Squire en 1951. (fr)
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  • In fluid dynamics, Landau–Squire jet or Submerged Landau jet describes a round submerged jet issued from a point source of momentum into an infinite fluid medium of the same kind. This is an exact solution to the incompressible form of the Navier-Stokes equations, which was first discovered by Lev Landau in 1944 and later by Herbert Squire in 1951. The self-similar equation was in fact first derived by N. A. Slezkin in 1934, but never applied to the jet. Following Landau's work, V. I. Yatseyev obtained the general solution of the equation in 1950. (en)
  • En mécanique des fluides le jet de Landau-Squire ou jet de Landau immergé décrit l'influence d'une source ponctuelle dans un écoulement stationnaire, incompressible, en géométrie cylindrique. La solution analytique de ce problème a été donnée par Lev Landau en 1944 et Herbert Squire en 1951. (fr)
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