1. Chapter 7

2. 7.2

3. Dilute systems with convection…

4. 7.3

5. Figure 7.1 Schematic of components of solute flux.
What does this mean?

6. Conservation of mass…

7. Conservation of mass…
What if we divided everything by volume?…

8. Conservation of mass…
What if we divided everything by volume?…

9. Conservation of mass…
What is this?

10. Conservation of mass…
What is this?

11. Conservation of mass…
What is this?
What is this?

12. Conservation of mass…
What is this?
What is this?

13. Conservation of mass…
What is this?
What is this?

14. Conservation of mass…
What is this?
What is this?
What is this?

15. Conservation of mass…
What is this?
What is this?
What is this?

16. Conservation of mass… What is this? What is this? What is this?
What about everything?

17. Conservation of mass… What is this? What is this? What is this?
What about everything?

18. Conservation of mass… ? What is this? What is this? What is this?
What about everything?

19. Conservation of mass… What is this? What is this? What is this?
What is this?
What about everything?

20. Conservation of mass… ? What is this? What is this? What is this?
What is this?
What about everything?

21. Conservation of mass… ρVel What is this? What is this? What is this?
What is this?
What about everything?

22. Conservation of mass… ρVel What is this? What is this? What is this?
What is this?
What about everything?
Also…

23. So…

25. ?

26. Fick’s 2nd
+ ?

27. Fick’s 2nd
+ convection

28. Example 7.1

29. Figure 7.2 Schematic of transport across a membrane with convection.

30. Figure 7.2 Schematic of transport across a membrane with convection.
C(Z=0)=ΦCo
C(Z=L)=ΦCL
Where to start?
What coordinates are we using?

31. Figure 7.2 Schematic of transport across a membrane with convection.
C(Z=0)=ΦCo
C(Z=L)=ΦCL
Where to start?
What coordinates are we using?
Fick’s 2nd + Convection… Yay!

32. Figure 7.2 Schematic of transport across a membrane with convection.
C(Z=0)=ΦCo
C(Z=L)=ΦCL
Where to start?
What coordinates are we using?
Fick’s 2nd + Convection… Yay!

33. Figure 7.2 Schematic of transport across a membrane with convection.
C(Z=0)=ΦCo
C(Z=L)=ΦCL
Where to start?
What coordinates are we using?
Fick’s 2nd + Convection… Yay!

34. Figure 7.2 Schematic of transport across a membrane with convection.
C(Z=0)=ΦCo
C(Z=L)=ΦCL
Where to start?
What coordinates are we using?
Fick’s 2nd + Convection… Yay! ?

35. Figure 7.2 Schematic of transport across a membrane with convection.
C(Z=0)=ΦCo
C(Z=L)=ΦCL
Where to start?
What coordinates are we using?
Fick’s 2nd + Convection… Yay!
S.S ?

36. Figure 7.2 Schematic of transport across a membrane with convection.
C(Z=0)=ΦCo
C(Z=L)=ΦCL
Where to start?
What coordinates are we using?
Fick’s 2nd + Convection… Yay!
S.S
N/A ?

37. Figure 7.2 Schematic of transport across a membrane with convection.
C(Z=0)=ΦCo
C(Z=L)=ΦCL
Where to start?
What coordinates are we using?
Fick’s 2nd + Convection… Yay!
S.S
N/A
N/A ?

38. Figure 7.2 Schematic of transport across a membrane with convection.
C(Z=0)=ΦCo
C(Z=L)=ΦCL
Where to start?
What coordinates are we using?
Fick’s 2nd + Convection… Yay!
S.S
N/A
N/A f ?

39. Figure 7.2 Schematic of transport across a membrane with convection.
C(Z=0)=ΦCo
C(Z=L)=ΦCL
Where to start?
What coordinates are we using?
Fick’s 2nd + Convection… Yay!
S.S
N/A
N/A f
Deff ?

40. Figure 7.2 Schematic of transport across a membrane with convection.
C(Z=0)=ΦCo
C(Z=L)=ΦCL
Where to start?
What coordinates are we using?
Fick’s 2nd + Convection… Yay!
S.S
N/A
N/A f
Deff
N/A ?

41. Figure 7.2 Schematic of transport across a membrane with convection.
C(Z=0)=ΦCo
C(Z=L)=ΦCL
Where to start?
What coordinates are we using?
Fick’s 2nd + Convection… Yay!
S.S
N/A
N/A f
Deff
N/A
N/A ?

42. Figure 7.2 Schematic of transport across a membrane with convection.
C(Z=0)=ΦCo
C(Z=L)=ΦCL
Where to start?
What coordinates are we using?
Fick’s 2nd + Convection… Yay!
S.S
N/A
N/A f
Deff
N/A
N/A
Need ?

43. Figure 7.2 Schematic of transport across a membrane with convection.
C(Z=0)=ΦCo
C(Z=L)=ΦCL
Where to start?
What coordinates are we using?
Fick’s 2nd + Convection… Yay!
S.S
N/A
N/A f
Deff
N/A
N/A
Need
N/A

44. Figure 7.2 Schematic of transport across a membrane with convection.
C(Z=0)=ΦCo
C(Z=L)=ΦCL
Fick’s 2nd + Convection… Yay!
S.S
N/A
N/A f
Deff
N/A
N/A
Need
N/A

45. Figure 7.2 Schematic of transport across a membrane with convection.
C(Z=0)=ΦCo
C(Z=L)=ΦCL
How do we solve this for Ci?

46. Figure 7.2 Schematic of transport across a membrane with convection.
C(Z=0)=ΦCo
C(Z=L)=ΦCL
How do we solve this for Ci?

48. 7.4

49. Table 7.3

50. Laplace Equation

51. What if it is at steady state and without a reaction?
If the Pe# is approximately zero then what does that mean about the velocity?
Laplace equation (has nothing to do with Laplace Transformations which we will do later in the semester):
If you take Fick’s second law and pass 5 tau units the concentration is no longer changing (much) in time. Thus dC/dt = 0 = D gradient^2(C), thus 0 = gradient^2(C). This is known as the Laplace equation.

52. What if it is at steady state and without a reaction?
If the Pe# is approximately zero then what does that mean about the velocity?
Close to zero…
Laplace equation…
Laplace equation (has nothing to do with Laplace Transformations which we will do later in the semester):
If you take Fick’s second law and pass 5 tau units the concentration is no longer changing (much) in time. Thus dC/dt = 0 = D gradient^2(C), thus 0 = gradient^2(C). This is known as the Laplace equation.

53. Nernst Plank Equation

54. Nernst Plank Equation…
TANGENT ?
Nernst Plank Equation…
F = Faraday’s Constant = 1.602e-19 Coloumbs*Avogadro’s # (C/mol of ion)
R = J/(mol*Kelvin)
RT = J/mol
z = charge of ion
Note: current density i = NF

55. Figure (a) Schematic of electrical potential difference ∆Ψ applied to a solution of the 1:1 electrolyte M+X-.
Note that electrons react with M+ only and not X- so
Current density = F*N of + or current density = F for cation
And N = 0 for anion
z=0
cathode
B.C.: C = C0 at z=0 and C=CL at z=L; ∆ѱ= ?; i = ? z
z=L
anode
B.C.: C = C0 at z=0 and C=CL at z=L; ∆ѱ= ?

56. Figure (a) Schematic of electrical potential difference ∆Ψ applied to a solution of the 1:1 electrolyte M+X-.
Note that electrons react with M+ only and not X- so
Current density = F*N of + or current density = F for cation
And N = 0 for anion
z=0
cathode
B.C.: C = C0 at z=0 and C=CL at z=L; ∆ѱ= ?; i = ? z
z=L
anode
B.C.: C = C0 at z=0 and C=CL at z=L; ∆ѱ= ?
Counter-current assumption;
Analogous to mass-countering…

57. Figure (a) Schematic of electrical potential difference ∆Ψ applied to a solution of the 1:1 electrolyte M+X-.
Note that electrons react with M+ only and not X- so
Current density = F*N of + or current density = F for cation
And N = 0 for anion
z=0
cathode
B.C.: C = C0 at z=0 and C=CL at z=L; ∆ѱ= ?; i = ? z
z=L
anode
B.C.: C = C0 at z=0 and C=CL at z=L; ∆ѱ= ?
Hint: solve for the differential of potential with respect to z in the N- equation and plug in to the N+ flux and solve for i.

58. Figure 7.5

59. Figure 7. 5 Potential difference across a charged cellular membrane
Figure Potential difference across a charged cellular membrane. The transmembrane potential Vm equals the potential inside the cell minus the potential outside the cell, Ψi - Ψ0 or Vm
3 Assumptions:
The electric potential varies linearly across the membrane = constant field assumption
Each ion because independently
Membrane properties are uniform across

60. 7.5.20b
7.5.20a (pg. 362)

61. Figure 7. 5 Potential difference across a charged cellular membrane
Figure Potential difference across a charged cellular membrane. The transmembrane potential Vm equals the potential inside the cell minus the potential outside the cell, Ψi - Ψ0 or Vm
Counter –current assumption…
What does this mean
About different Ds of
Ions and the voltage?
= diffusion potential
Net current across = 0 so… z + N+ = z-N- and solve for the differential of potential (respect to space)
B.C.: C = C0 at z=0 and C=CL at z=L; ∆ѱ= ?
∆ѱ= ?

62. Nernst-Planck Equation + Conserv. Relation
Algebra will be “prettier” if multiply both
Sides by a negative…
Solve for Ci (equation a) and remember fick’s first law to get N=-Dgrad(C) b)
Assume counter current or sum of the fluxes = 0 (do this for potassium, sodium, and chloride) and calculate Vm
B.C.
At z=0, Ci = ΦiCo
At z=L, Ci= ΦiCL
1-D (use z)
(Make prettier with permeabilities (= ΦD/L))

63. Example 7.4 The book references 7.3.9a dC/dt = gradient(N)+Ri
No reaction and it is at steady state so 0=dN/dz.
We assume (sum of zN=0) applies here so…

65. Poisson Equation:
Charge distribution
Debye length and what is the relationship with Zeta Potential? Distance the voltage drops by 1/e…
Represents the characteristic distance over which counterion concentration is elevated around the central ion…
ε= permittivity (units are Farads/m)
What’s a Farad
Permittivity = # of coulombs to cause 1 volt in 1 m
F = Faraday’s constant = coloumbs/mol
How units cancel to be distance
A special thank you to Wikipedia.