Chilton and Colburn J-factor analogy

Chilton and Colburn J-factor analogy is probably the most successful and widely used analogy from heat, momentum, and mass transfer analogies. The basic mechanisms and mathematics of heat, mass, and momentum transport are essentially the same. Among many analogies (like Reynolds analogy, Prandtl-Taylor analogy) developed to directly relate heat transfer coefficients, mass transfer coefficients, and friction factors Chilton and Colburn J-factor analogy proved to be the most accurate.

It is written as follows,

\frac{f}{2} = J_H = \frac{h}{cp \cdot G} \cdot {Pr}^{\frac{2}{3}}= J_D = \frac{k'_c}{\overline{v}} \cdot {Pr}^{\frac{2}{3}}

This equation permits the prediction of an unknown transfer coefficient when one of the other coefficients is unknown. The analogy is valid for turbulent flow in conduits with Re > 10000, 0.7 < Pr < 160, and tubes where L/d > 60 (the same constraints as Seider-Tate). The wider range of data can be correlated by Friend-Metzner analogy.

See also

References

  • Geankoplis, C.J. Transport processes and separation process principles (2003). Fourth Edition, p.475.

External links

-

This article about an engineering topic is a stub. You can help Wikipedia by expanding it.

This article is from Wikipedia. All text is available under the terms of the GNU Free Documentation License.


Giant Panda

Mercedes Car
James Bond Guide
This site monitored by SitePinger.net