Richardson criterion sanjidâr-e Richardson Fr.: critère de Richardson A condition for the onset of → instability in multilayer fluids which compares the balance between the restoring force of → buoyancy and the destabilizing effect of the → shear. Etymology (EN): Named after the British meteorologist Lewis Fry Richardson (1881-1953), who
first arrived in 1920 to the dimensionless ratio now called
→ Richardson number. The first formal proof of the criterion, however,
came four decades later for → incompressible flows
(Miles, J. W. 1961, J. Fluid Mech., 10, 496; Howard, L. N., 1961, J. Fluid Mech., 10, 509). |