Brinkman number
The Brinkman number (Br) is a dimensionless number related to heat conduction from a wall to a flowing viscous fluid, commonly used in polymer processing. There are several definitions; one is
where
- μ is the dynamic viscosity;
- u is the flow velocity;
- κ is the thermal conductivity;
- T0 is the bulk fluid temperature;
- Tw is the wall temperature;
- Pr is the Prandtl number
- Ec is the Eckert number[1]
It is the ratio between heat produced by viscous dissipation and heat transported by molecular conduction. i.e., the ratio of viscous heat generation to external heating. The higher its value, the slower the conduction of heat produced by viscous dissipation and hence the larger the temperature rise.[2][3]
In, for example, a screw extruder, the energy supplied to the polymer melt comes primarily from two sources:
- viscous heat generated by shear between elements of the flowing liquid moving at different velocities;
- direct heat conduction from the wall of the extruder.
The former is supplied by the motor turning the screw, the latter by heaters. The Brinkman number is a measure of the ratio of the two.
References
- ↑ Michael M. Khonsari; E. Richard Booser (28 July 2008). Applied Tribology: Bearing Design and Lubrication. John Wiley & Sons. p. 125. ISBN 978-0-470-05944-9. Retrieved 19 July 2012.
- ↑ Robert S. Brodkey; Harry C. Hershey (1988). Transport Phenomena: A Unified Approach. Brodkey Publishing. p. 333. ISBN 978-0-9726635-9-5. Retrieved 19 July 2012.
- ↑ José Pontes. COMPUTATIONAL HEAT AND MASS TRANSFER – CHMT 2001-. Editora E-papers. pp. 113–. ISBN 978-85-87922-44-1. Retrieved 19 July 2012.
- J. D. Huba. NRL Plasma Formulary. Naval Research Laboratory, 1994.
- Carl W. Hall. Laws and Models: Science, Engineering and Technology. — CRC Press, Boca Raton, 2000. ISBN 978-0-8493-2018-7.
- Stephen M. Richardson. Fluid mechanics.
- L. P. Yarin, A. Mosyak, Gad Hetsroni. Fluid flow, heat transfer and boiling in micro-channels.
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