Monin-obukhov similarity theory
From Glossary of Meteorology
Monin–Obukhov similarity theory[edit | edit source]
A relationship describing the vertical behavior of nondimensionalized mean flow and turbulence properties within the atmospheric surface layer (the lowest 10% or so of the atmospheric boundary layer) as a function of the Monin–Obukhov key parameters.
These key parameters are the height z above the surface, the buoyancy parameter ratio g/Tv of inertia and buoyancy forces, the kinematic surface stress τ0/ρ, and the surface virtual temperature flux where g is gravitational acceleration, Tv is virtual temperature, τ0 is turbulent stress at the surface, ρ is air density, Qv0 is a kinematic virtual heat flux at the surface, Hv0 is a dynamic virtual heat flux at the surface, Cp is the specific heat of air at constant pressure, and is the covariance of vertical velocity w with virtual temperature near the surface. The key parameters can be used to define a set of four dimensional scales for the surface layer: 1) the friction velocity or shearing velocity, a velocity scale, 2) a surface-layer temperature scale, 3) a length scale called the Obukhov length, where k is the von Kármán constant; and 4) the height above ground scale, z. These key scales can then be used in dimensional analysis to express all surface-layer flow properties as dimensionless universal functions of z/L. For example, the mean wind shear in any quasi-stationary, locally homogeneous surface layer can be written as where f is a universal function of the dimensionless height z/L. The forms of the universal functions are not given by the Monin–Obukhov theory, but must be determined theoretically or empirically. Monin–Obukhov similarity theory is the basic similarity hypothesis for the horizontally homogeneous surface layer. With these equations and the hypothesis that the fluxes in the surface layer are uniform with height, the momentum flux, sensible heat flux, and fluxes of water vapor and other gases can be determined.
Compare aerodynamic roughness length, Richardson number.
Compare aerodynamic roughness length, Richardson number.