A singular perturbation analysis and Green’s second theorem are used in order to obtain a general expression for the heat transfer from a particle at low Peclet numbers, when advection and conduction are heat transfer modes of comparable magnitude. The particle may have arbitrary shape, and its motion in the fluid is not constrained to be Stokesian. In the ensuring analysis, the governing equations for the temperature fields at short and long times are derived. The expressions are combined to yield a general equation for the temperature field and for the total rate of heat transfer. The final results for the rate of heat transfer demonstrate the existence of a history integral, whose kernel decays faster than the typical history integrals of the purely conduction regime. As applications of the general results, analytical expressions for the Nusselt number are derived in the case of a sphere undergoing a step temperature change.
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Transient Heat Transfer From a Particle With Arbitrary Shape and Motion
Zhi-Gang Feng,
Zhi-Gang Feng
Department of Mechanical Engineering, Tulane University, New Orleans, LA 70118
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E. E. Michaelides
E. E. Michaelides
Department of Mechanical Engineering, Tulane University, New Orleans, LA 70118
e-mail: emichael@mailhost.tcs.tulane.edu
Search for other works by this author on:
Zhi-Gang Feng
Department of Mechanical Engineering, Tulane University, New Orleans, LA 70118
E. E. Michaelides
Department of Mechanical Engineering, Tulane University, New Orleans, LA 70118
e-mail: emichael@mailhost.tcs.tulane.edu
J. Heat Transfer. Aug 1998, 120(3): 674-681 (8 pages)
Published Online: August 1, 1998
Article history
Received:
August 16, 1996
Revised:
March 24, 1998
Online:
December 5, 2007
Citation
Feng, Z., and Michaelides, E. E. (August 1, 1998). "Transient Heat Transfer From a Particle With Arbitrary Shape and Motion." ASME. J. Heat Transfer. August 1998; 120(3): 674–681. https://doi.org/10.1115/1.2824336
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