Explore: Von Karman Equation

modeling of von Kármán vortex street can be performed using different techniques including but not limited to solving the full Navier-Stokes equations with k-epsilon

The Föppl–von Kármán equations, named after August Föppl and Theodore von Kármán, are a set of nonlinear partial differential equations describing the

Theodore von Kármán (Hungarian: (szőllőskislaki) Kármán Tódor [(søːløːʃkiʃlɒki) ˈkaːrmaːn ˈtoːdor], May 11, 1881 – May 6, 1963) was a Hungarian-American

the case of rough pipes in a fully turbulent flow regime (Prandtl-von Kármán equation). In a cylindrical pipe of uniform diameter D, flowing full, the

The Kármán line (or von Kármán line /vɒn ˈkɑːrmɑːn/) is a conventional definition of the edge of space; it is widely but not universally accepted. The

turbulence the Kármán–Howarth equation (after Theodore von Kármán and Leslie Howarth 1938), which is derived from the Navier–Stokes equations, is used to

In fluid dynamics, the von Kármán constant (or Kármán's constant), named for Theodore von Kármán, is a dimensionless constant involved in the logarithmic

for solving integral equation of surface radiation exchanges Nonlinear acoustics Large eddy simulation Föppl–von Kármán equations Timoshenko beam theory

Born–von Karman boundary condition requires the wave function to be periodic on a certain Bravais lattice. Named after Max Born and Theodore von Kármán, this

electrode. Using cylindrical coordinates, the von Karman and Cochran solution to the Navier-Stokes equations yields the two relevant profiles to electrochemical