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[[Cross fluid]] is a type of [[Generalized Newtonian fluids| Generalized Newtonian fluid]], their viscosity depends upon shear rate by the following equation:
A '''Cross fluid''' is a type of [[generalized Newtonian fluid]] whose [[viscosity]] depends upon shear rate according to the following equation:


<math>
<math>
\mu_\mbox{eff}(\dot \gamma) = \frac {\mu_0}{1 + ({\frac {\mu_0 \dot \gamma} {\tau ^ *}})^{1-n}  }
\mu_{\operatorname{eff}}(\dot \gamma) = \frac {\mu_0}{1 + ({\frac {\mu_0 \dot \gamma} {\tau ^ *}})^{1-n}  }
</math>
</math>


Where <math> \mu_\mbox{eff}(\dot \gamma) </math> is [[viscosity]] as a function of [[shear rate]],
where
<math> \mu_0 </math>, <math> \tau ^ * </math> and ''n'' are coefficients.
:<math> \mu_{\operatorname{eff}}(\dot \gamma) </math> is [[viscosity]] as a function of [[shear rate]],
:<math> \mu_0 </math>, <math> \tau ^ * </math> and ''n'' are coefficients.


At low [[shear rate]] (<math> \mu_0 \dot \gamma <\ <\ \tau^* </math>)Cross fluid behave as a [[Newtonian fluid]] and at high [[shear rate]] (<math> \mu_0 \dot \gamma >\ >\ \tau^* </math>) as [[Power-law fluid]].
At low [[shear rate]] (<math> \mu_0 \dot \gamma \ll \tau^* </math>), cross fluids behave as [[Newtonian fluid]]s and at high [[shear rate]] (<math> \mu_0 \dot \gamma \gg \tau^* </math>) as [[power-law fluid]]s.


== See Also ==
==See also==
*[[Navier-Stokes equations]]
*[[Navier-Stokes equations]]
*[[Fluids]]
*[[Fluid]]
*[[Carreau fluid]]
*[[Carreau fluid]]
*[[Power-law fluid]]
*[[Power-law fluid]]
*[[Generalized Newtonian fluids]]
*[[Generalized Newtonian fluid]]
 
==References==
*Kennedy, P. K., ''Flow Analysis of Injection Molds''. New York. Hanser. ISBN 1569901813


[[Category: Non-Newtonian fluids]]
[[Category: Non-Newtonian fluids]]

Latest revision as of 15:32, 29 April 2009

A Cross fluid is a type of generalized Newtonian fluid whose viscosity depends upon shear rate according to the following equation:

<math> \mu_{\operatorname{eff}}(\dot \gamma) = \frac {\mu_0}{1 + ({\frac {\mu_0 \dot \gamma} {\tau ^ *}})^{1-n} } </math>

where

<math> \mu_{\operatorname{eff}}(\dot \gamma) </math> is viscosity as a function of shear rate,
<math> \mu_0 </math>, <math> \tau ^ * </math> and n are coefficients.

At low shear rate (<math> \mu_0 \dot \gamma \ll \tau^* </math>), cross fluids behave as Newtonian fluids and at high shear rate (<math> \mu_0 \dot \gamma \gg \tau^* </math>) as power-law fluids.

See also

References

  • Kennedy, P. K., Flow Analysis of Injection Molds. New York. Hanser. ISBN 1569901813