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Fick’s Law of Diffusion
 Molecular diffusion or molecular transport can be defined as the
transfer or movement of individual molecules through a fluid by
mean of the random, individual movements of the molecules.
 If there are greater number of A molecules near point (1) than at
(2), then since molecules diffuse randomly in both direction,
more A molecules will diffuse from (1) to (2) than from (2) to (1).
 The net diffusion of A is from high to low concentration regions.
B
B
B
B
B
B
B
B
B
B
B
A
A
Figure 3: Schematic diagram of molecular diffusion process
(2)
(1)
 The two modes of mass transfer:
- Molecular diffusion
- Convective mass transfer
Molecular diffusion
The diffusion of molecules when the whole
bulk fluid is not moving but stationary.
Diffusion of molecules is due to a
concentration gradient.
The general Fick’s Law Equation for binary mixture of A and B
dz
dx
cD
J A
AB
AZ 

*
c = total concentration of A and B [kgmol (A + B)/m3
]
xA= mole fraction of A in the mixture of A and B
Example
A mixture of He and N2 gas is contained in a
pipe at 298 K and 1 atm total pressure
which is constant throughout. At one end of
the pipe at point 1 the partial pressure pA1
of He is 0.6 atm and at the other end 0.2 m
pA2 = 0.2 atm. Calculate the flux of He at
steady state if DAB of the He-N2 mixture is
0.687 x 10-4
m2
/s.
Solution
 Since a total pressure P is constant, the c is constant, where
c is as follows for a gas according to the perfect gas law:
 Where n is kg mol A plus B, V is volume in m3
, T is
temperature in K, R is 8314.3 m3
.Pa/kg mol.K or R is 82.057 x
10-3
cm3
. atm/g. mol. K, and c is kg mol A plus B/m3.
 For steady state the flux J*Az in Eq.(6.1-3) is constant. Also DAB
for gas is constant. Rearranging Eq. (6.1-3) and integrating.
(6.1-11)
 Also, from the perfect gas law, pAV=nART, and
 Substituting Eq. (6.1-12) into (6.1-11),
 This is the final equation to use, which is in a form eqsily
used for gases. Partial pressures are pA1 = 0.6 atm = 0.6 x
1.01325 x 105
= 6.04 x 104
Pa and pA2 = 0.2 atm = 0.2 x
1.01325 x 105
= 2.027 x 104
Pa. Then, using SI units,
(6.1-13)
 If pressures in atm are used with SI unit,
 Other driving forces (besides concentration
differences) for diffusion also occur
because of temperature, pressure,
electrical potential, and other gradients.
Convection Mass Transfer
 When a fluid flowing outside a solid surface in forced convection motion,
rate of convective mass transfer is given by:
kc - mass transfer coefficient (m/s)
cL1 - bulk fluid conc.
cLi - conc of fluid near the solid surface
 Kc depend on:
1. system geometry
2. Fluid properties
3. Flow velocity
)
( 1 Li
L
c
A c
c
k
N 

Principles of Mass
Transfer
Molecular Diffusion in Gases
Molecular Diffusion in Gases
CONTENTS
Mass Transfer
Molecular Diffusion Convective Mass Transfer
Gases Liquid Solid
35236lect 1Introduction to Masالثالث  الثالث مقسم1s Transfer.ppt
Molecular Diffusion in Gases
 Equimolar Counterdiffussion in Gases
35236lect 1Introduction to Masالثالث  الثالث مقسم1s Transfer.ppt
35236lect 1Introduction to Masالثالث  الثالث مقسم1s Transfer.ppt
 For a binary gas mixture of A and B,
the diffusivity coefficient DAB=DBA

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35236lect 1Introduction to Masالثالث الثالث مقسم1s Transfer.ppt

  • 1. Fick’s Law of Diffusion  Molecular diffusion or molecular transport can be defined as the transfer or movement of individual molecules through a fluid by mean of the random, individual movements of the molecules.  If there are greater number of A molecules near point (1) than at (2), then since molecules diffuse randomly in both direction, more A molecules will diffuse from (1) to (2) than from (2) to (1).  The net diffusion of A is from high to low concentration regions. B B B B B B B B B B B A A Figure 3: Schematic diagram of molecular diffusion process (2) (1)
  • 2.  The two modes of mass transfer: - Molecular diffusion - Convective mass transfer
  • 3. Molecular diffusion The diffusion of molecules when the whole bulk fluid is not moving but stationary. Diffusion of molecules is due to a concentration gradient. The general Fick’s Law Equation for binary mixture of A and B dz dx cD J A AB AZ   * c = total concentration of A and B [kgmol (A + B)/m3 ] xA= mole fraction of A in the mixture of A and B
  • 4. Example A mixture of He and N2 gas is contained in a pipe at 298 K and 1 atm total pressure which is constant throughout. At one end of the pipe at point 1 the partial pressure pA1 of He is 0.6 atm and at the other end 0.2 m pA2 = 0.2 atm. Calculate the flux of He at steady state if DAB of the He-N2 mixture is 0.687 x 10-4 m2 /s.
  • 5. Solution  Since a total pressure P is constant, the c is constant, where c is as follows for a gas according to the perfect gas law:  Where n is kg mol A plus B, V is volume in m3 , T is temperature in K, R is 8314.3 m3 .Pa/kg mol.K or R is 82.057 x 10-3 cm3 . atm/g. mol. K, and c is kg mol A plus B/m3.  For steady state the flux J*Az in Eq.(6.1-3) is constant. Also DAB for gas is constant. Rearranging Eq. (6.1-3) and integrating. (6.1-11)
  • 6.  Also, from the perfect gas law, pAV=nART, and  Substituting Eq. (6.1-12) into (6.1-11),  This is the final equation to use, which is in a form eqsily used for gases. Partial pressures are pA1 = 0.6 atm = 0.6 x 1.01325 x 105 = 6.04 x 104 Pa and pA2 = 0.2 atm = 0.2 x 1.01325 x 105 = 2.027 x 104 Pa. Then, using SI units, (6.1-13)
  • 7.  If pressures in atm are used with SI unit,  Other driving forces (besides concentration differences) for diffusion also occur because of temperature, pressure, electrical potential, and other gradients.
  • 8. Convection Mass Transfer  When a fluid flowing outside a solid surface in forced convection motion, rate of convective mass transfer is given by: kc - mass transfer coefficient (m/s) cL1 - bulk fluid conc. cLi - conc of fluid near the solid surface  Kc depend on: 1. system geometry 2. Fluid properties 3. Flow velocity ) ( 1 Li L c A c c k N  
  • 9. Principles of Mass Transfer Molecular Diffusion in Gases Molecular Diffusion in Gases
  • 10. CONTENTS Mass Transfer Molecular Diffusion Convective Mass Transfer Gases Liquid Solid
  • 12. Molecular Diffusion in Gases  Equimolar Counterdiffussion in Gases
  • 15.  For a binary gas mixture of A and B, the diffusivity coefficient DAB=DBA