
Monin-Obukhov Length
    
    Encyclopedia
    
        The Obukhov length is used to describe the effects of buoyancy on turbulent flows, particularly in the lower tenth of the atmospheric boundary layer.  It was first defined by Alexander Obukhov
in 1946, . It is also known as the Monin-Obukhov length because of its important role in the similarity theory developed by Monin and Obukhov .
The Obukhov Length is defined by

where is the frictional velocity,
 is the frictional velocity,  is the mean virtual potential temperature,
 is the mean virtual potential temperature,  is the surface virtual potential temperature flux, k is the von Kármán constant
 is the surface virtual potential temperature flux, k is the von Kármán constant
. The virtual potential temperature flux is given by

where is potential temperature,
 is potential temperature,  is absolute temperature and
 is absolute temperature and  is specific humidity.
 is specific humidity.
By this definition, is usually negative in the daytime since
 is usually negative in the daytime since  is typically positive during the daytime over land, positive at night when
 is typically positive during the daytime over land, positive at night when  is typically negative, and becomes infinite at dawn and dusk when
 is typically negative, and becomes infinite at dawn and dusk when  passes through zero.
 passes through zero.
A physical interpretation of is given by the Monin-Obukhov similarity theory. During the day
 is given by the Monin-Obukhov similarity theory. During the day  it is the height at which the buoyant production of turbulence kinetic energy (TKE) is equal to that produced by the shearing action of the wind (shear production of TKE).
 it is the height at which the buoyant production of turbulence kinetic energy (TKE) is equal to that produced by the shearing action of the wind (shear production of TKE).
        
    
Alexander Obukhov
Alexander Mikhailovich Obukhov   was a Russian physicist and applied mathematician known for his contribution to statistical theory of turbulence and atmospheric physics. He was one of the founders of modern boundary layer meteorology...
in 1946, . It is also known as the Monin-Obukhov length because of its important role in the similarity theory developed by Monin and Obukhov .
The Obukhov Length is defined by

where
 is the frictional velocity,
 is the frictional velocity,  is the mean virtual potential temperature,
 is the mean virtual potential temperature,  is the surface virtual potential temperature flux, k is the von Kármán constant
 is the surface virtual potential temperature flux, k is the von Kármán constantVon Kármán constant
In fluid dynamics, the Von Kármán constant , named for Theodore von Kármán, is a dimensionless constant describing the logarithmic velocity profile of a turbulent fluid flow near a boundary with a no-slip condition...
. The virtual potential temperature flux is given by

where
 is potential temperature,
 is potential temperature,  is absolute temperature and
 is absolute temperature and  is specific humidity.
 is specific humidity.By this definition,
 is usually negative in the daytime since
 is usually negative in the daytime since  is typically positive during the daytime over land, positive at night when
 is typically positive during the daytime over land, positive at night when  is typically negative, and becomes infinite at dawn and dusk when
 is typically negative, and becomes infinite at dawn and dusk when  passes through zero.
 passes through zero.A physical interpretation of
 is given by the Monin-Obukhov similarity theory. During the day
 is given by the Monin-Obukhov similarity theory. During the day  it is the height at which the buoyant production of turbulence kinetic energy (TKE) is equal to that produced by the shearing action of the wind (shear production of TKE).
 it is the height at which the buoyant production of turbulence kinetic energy (TKE) is equal to that produced by the shearing action of the wind (shear production of TKE).
        
    

