# Dynamic viscosity

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- | The SI | + | The SI unit of dynamic viscosity (Greek symbol: <math>\mu</math>) is pascal-second (<math>Pa\cdot s</math>), which is identical to <math>\frac{kg}{m\cdot s}</math>. |

The dynamic viscosity is related to the kinematic viscosity by | The dynamic viscosity is related to the kinematic viscosity by | ||

- | + | :<math>\mu=\rho\cdot\nu</math> | |

- | <math>\mu=\rho\cdot\nu</math> | + | where <math>\rho</math> is the density and <math>\nu</math> is the [[kinematic viscosity]]. |

- | </ | + | |

+ | For the use in CFD, dynamic viscosity can be defined by different ways: | ||

+ | * as a constant | ||

+ | * as a function of temperature (e.g. piecewise-linear, piecewise-polynomial, polynomial, by [[Sutherland's law]] or by the [[Power-law viscosity law|Power law]]) | ||

+ | * by using Kinetic Theory | ||

+ | * composition-dependent | ||

+ | * by non-Newtonian models | ||

{{stub}} | {{stub}} | ||

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## Latest revision as of 10:03, 12 June 2007

The SI unit of dynamic viscosity (Greek symbol: ) is pascal-second (), which is identical to .

The dynamic viscosity is related to the kinematic viscosity by

where is the density and is the kinematic viscosity.

For the use in CFD, dynamic viscosity can be defined by different ways:

- as a constant
- as a function of temperature (e.g. piecewise-linear, piecewise-polynomial, polynomial, by Sutherland's law or by the Power law)
- by using Kinetic Theory
- composition-dependent
- by non-Newtonian models