846 Appendix B Fluxes and the Equations of Change
5B.3 FICK'S (FIRST) LAW OF BINARY DIFFUSIONa
[jA = -P%ABVWAI
Cartesian coordinates (x, y, z):
Cylindrical coordinates tr, 8 , ~ ) :
Spherical coordinates tr, 8 , 4 ) :
" To get the molar fluxes with respect to the molar average velocity, replace j,, p, and w, by J:, c, and x,.
5B.4 THE EQUATION OF CONTINUITYa
[ d p / d t + (V .pv) = 01
Cartesian coordinates (x, y, z):
Cylindrical coordinates (r, 8 , ~ ) :
Spherical coordinates (r, 8, 4):
3 + --
1 d (p?ur) +
dt y2 dr
--
r sin 8 d8
(pv, sin 8) + -- (pv+)= 0
r sin 8 dr$
" When the fluid is assumed to have constant mass density p, the equation simplifies to (V .v) = 0.
850 Appendix B Fluxes and the Equations of Change
sB.9 THE EQUATION OF ENERGY FOR PURE NEWTONIAN
FLUIDS WITH CONSTANTap AND k
Cartesian coordinates ( x , y, z):
Cylindrical coordinates (r, 0 , ~ ) :
Spherical coordinates (r, 8,4):
" This form of the energy equation is also valid under the less stringent assumptions k = constant and (d In p / d In T),,Dp/Dt = 0. The
assumption p = constant is given in the table heading because it is the assumption more often made.
The function @,, is given in sB.7. The term p @ ,is usually negligible, except in systems with large velocity gradients.
sB.10 THE EQUATION OF CONTINUITY FOR SPECIES a
IN TERMSaOF ja
[pDo,/Dt = -(V .j,) + r,]
Cartesian coordinafes ( x , y, z):
Cylindrical coordinafes (r, 8, z):
-- -
Spherical coordinates (r, 8,+):
do, dw, us d o , 1 d .
[La
Urn
dt fur-+--+---
dr Y r sm 8 a+ =
r2dr (r2j,r) + r sin 0 - ('"' sin 0) + Y sln 0 -
aia'i.m]+r,
d+ (8.10-3)
" To obtain the corresponding equations in terms of J,* make the following replacements:
Replace P v
sB.11 The Equation of Continuity for Species A in Terms of w, for Constant p%,, 851
gB.11 THE EQUATION OF CONTINUITY FOR SPECIES A
IN TERMS OF oAFOR CONSTANTapBAB
- -
Cartesian coordinates (x,y, 2):
Cylindrical coordinates (r, 19, z):
Spherical coordinates (r, O,+):
1
r2 sin 0 d o
(B.11-3)
" To obtain the corresponding equations in terms of x,, make the following replacements:
Replace P 0, v re
N
by c X, V* R, - x, 1 Rp
p=1