Dimensionless Numbers: Difference between revisions
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<div id="Prandtl Number"></div> | |||
;'''Prandtl Number''' | |||
* Definition: <math> Pr = \nu/\alpha </math>, where <math> \nu </math> is the [[#Viscosity|viscosity]], and <math> \alpha </math> is the [[#Diffusivity|thermal diffusivity]]. | |||
* Interpretation: The ratio between the momentum diffusivity (i.e. viscosity) and heat diffusivity. | |||
* Analysis: The typical Prandtl number for water is around 7 for water (At 20 degrees Celsius). See also [[#Schmidt Number|Schmidt number]]. | |||
<div id="Reynolds Number"></div> | <div id="Reynolds Number"></div> | ||
;'''Reynolds Number''' | ;'''Reynolds Number''' | ||
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<div id="Schmidt Number"></div> | <div id="Schmidt Number"></div> | ||
;'''Schmidt Number''' | ;'''Schmidt Number''' | ||
* Definition: <math> Sc = \nu/\kappa </math>, where <math> \nu </math> is the [[#Viscosity|viscosity]], and <math> \kappa </math> is the [[#Diffusivity|diffusivity]]. | * Definition: <math> Sc = \nu/\kappa </math>, where <math> \nu </math> is the [[#Viscosity|viscosity]], and <math> \kappa </math> is the [[#Diffusivity|mass diffusivity]]. | ||
* Interpretation: The ratio between the momentum diffusivity (i.e. viscosity) and mass diffusivity. | * Interpretation: The ratio between the momentum diffusivity (i.e. viscosity) and mass diffusivity. | ||
* Analysis: The typical Schmidt number for water is around 500, depending on the temperature and salinity. For [[#DNS|direct numerical simulations]], <math> Sc = 1 </math> is commonly used in the literature. See also [[#Prandtl Number|Prandtl number]]. | * Analysis: The typical Schmidt number for water is around 500, depending on the temperature and salinity. For [[#DNS|direct numerical simulations]], <math> Sc = 1 </math> is commonly used in the literature. See also [[#Prandtl Number|Prandtl number]]. |
Revision as of 09:50, 28 May 2015
- Prandtl Number
- Definition: , where is the viscosity, and is the thermal diffusivity.
- Interpretation: The ratio between the momentum diffusivity (i.e. viscosity) and heat diffusivity.
- Analysis: The typical Prandtl number for water is around 7 for water (At 20 degrees Celsius). See also Schmidt number.
- Reynolds Number
- Definition: , where and are the characteristic velocity and length scales, and is the dynamic viscosity.
- Interpretation: The ratio of inertial force to viscous force.
- Analysis: Small Reynolds numbers are often associated with viscous flows, whereas large Reynolds numbers are typically found in turbulent flows.
- Gradient Richardson Number
- Definition: , where is the buoyancy frequency and is the background horizontal velocity.
- Interpretation: The ratio between the strength of stratification and velocity shear.
- Analysis: A sufficient condition for the flow to be linearly stable is that the local Richardson number exceed 0.25 throughout the flow. However, does not mean the flow is necessarily unstable (the criterion is not sufficient). When the flow is not a parallel shear flow, the meaning of is not clear.
- Schmidt Number
- Definition: , where is the viscosity, and is the mass diffusivity.
- Interpretation: The ratio between the momentum diffusivity (i.e. viscosity) and mass diffusivity.
- Analysis: The typical Schmidt number for water is around 500, depending on the temperature and salinity. For direct numerical simulations, is commonly used in the literature. See also Prandtl number.