Summary
From the assumption that the heat flux (mass flux with respect to the mass-average velocity) vector is an isotropic function of the temperature (mass-fraction) gradient, it is shown that, wherek(D) is a function of the absolute value of the temperature (mass-fraction) gradient.
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Abbreviations
- C v :
-
Heat capacity at constant volume per unit mass of system
- D :
-
the diffusion coefficient
- G :
-
another symbol for
- g1,g2,g3,g4:
-
the principal values ofG (diagonal elements of the matrixḠ)
- I :
-
the identity matrix,\(I_{ij} = \left\{ \begin{array}{l} 1 if i = j \\ 0 if i \ne j \\ \end{array} \right.\)
- j A :
-
mass flux vector with respect to the mass average velocity
- k :
-
thermal conductivity
- p :
-
pressure
- q :
-
heat flux vector with respect to the mass-average velocity
- q1,q2,q3,q4:
-
Principal values ofq (diagonal elements of the matrix\(\bar q\))
- \(\bar q_{ij} \) :
-
elements of the matrix\(\bar q\)
- r A :
-
rate at which mass of componentA is formed in system of unit volume by chemical reaction
- S :
-
orthogonal transformation matrix
- t :
-
time
- T :
-
temperature
- gu :
-
velocity vector
- ρ :
-
density
- τ :
-
stress deviation tensor
- ω A :
-
mass fraction of componentA
- :
-
the “del” operator, in rectangular co-ordinates it equals
$$\frac{\partial }{{\partial x}}i + \frac{\partial }{{\partial y}}j + \frac{\partial }{{\partial z}}k$$ - τ :v:
-
rate at which energy is dissipated due to viscous effects per unit volume=τ i j υ′ j i overline the corresponding diagonal matrix
References
Bird, R. B., W. E. Stewart and E. N. Lightfoot, Transport Phenomena, John Wiley, New York, 1960.
Birkhoff, G. and S. MacLane, A Survey of Modern Algebra, Macmillan, New York, 1953.
McConnel, A. J., Applications of Tensor Analysis, Dover, New York, 1957.
Serrin, J., Handbuch der Physik, Band VIII/1, ed. by S. Flügge, Springer, Berlin, 1959.
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Slattery, J.C. Quasi-linear heat and mass transfer. Appl. sci. Res. 12, 51–56 (1964). https://doi.org/10.1007/BF03184747
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DOI: https://doi.org/10.1007/BF03184747