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Module 3 Lecture II 3/1/2021
1
CM3120: Module 3
Β© Faith A. Morrison, Michigan Tech U.1
Diffusion and Mass Transfer I
I. Introduction to diffusion/mass transferII. Classic diffusion and mass transferβQuick Start a): 1D EvaporationIII. Classic diffusion and mass transferβQuick Start b): 1D Radial dropletIV. Cycle back: Fickβs mass transport lawV. Microscopic species A mass balanceVI. Classic diffusion and mass transferβc): 1D Mass transfer with
chemical reaction
CM3120: Module 3
Β© Faith A. Morrison, Michigan Tech U.2
Professor Faith A. Morrison
Department of Chemical EngineeringMichigan Technological University
www.chem.mtu.edu/~fmorriso/cm3120/cm3120.html
Module 3 Lecture II
Quick Start 1:1D Evaporation
Module 3 Lecture II 3/1/2021
2
Β© Faith A. Morrison, Michigan Tech U.3
Microscopic species A mass balanceβFive forms
ππππ΄ππ‘
π£ β βππ΄ β β ποΏ½Μ²οΏ½ ππ΄
ππ· π» π π
πππ₯π΄ππ‘
π£β β βπ₯π΄ β β οΏ½Μ²οΏ½π΄β π₯π΅π π΄ π₯π΄π π΅
ππ·π΄π΅β2π₯π΄ π₯π΅π π΄ π₯π΄π π΅
πππ΄ππ‘
β β ππ΄ π π΄
In terms of mass flux and mass
concentrations
In terms of molar flux and molar
concentrations
In terms of combined molar flux and molar
concentrations
Weβll do a βQuick Startβ and get into some examples and return to the βwhyβ of it all a
bit later.
It turns out that there are many interesting and applicable problems we can address readily with thisform of the species mass balance.
Letβs jump in!
Microscopic species mass balance in terms of
combined molar flux π΅π¨
Diffusion and Mass Transfer
QUICK START
(to problem solving)
Microscopic species A mass balanceβFive forms
ππππ΄ππ‘
π£ β βππ΄ β β ποΏ½Μ²οΏ½ ππ΄
ππ· π» π π
πππ₯π΄ππ‘
π£β β βπ₯π΄ β β οΏ½Μ²οΏ½π΄β π₯π΅π π΄ π₯π΄π π΅
ππ·π΄π΅β2π₯π΄ π₯π΅π π΄ π₯π΄π π΅
πππ΄ππ‘
β β ππ΄ π π΄
In terms of mass flux and mass
concentrations
In terms of molar flux and molar
concentrations
In terms of combined molar flux and molar
concentrations
Β© Faith A. Morrison, Michigan Tech U.4
Weβll do a βQuick Startβ and get into some examples and return to the βwhyβ of it all a
bit later.
It turns out that there are many interesting and applicable problems we can address readily with thisform of the species mass balance.
Letβs jump in!
Microscopic species mass balance in terms of
combined molar flux π΅π¨
Module 3 Lecture II 3/1/2021
3
5
Diffusion and Mass Transfer QUICK START
Β© Faith A. Morrison, Michigan Tech U.
π» β π π
Using the microscopic species mass balance in terms of combined molar flux and molar concentrations
π
π₯ π the concentration of π΄ in the mixture
π
β combined molar flux of π΄ (both diffusion and
convection) relative to stationary coordinates
π
β rate of production of π΄ by reaction per unit
volume mixture
π
molar density of the mixture (for ideal gases π
QUICK START
6
Diffusion and Mass Transfer QUICK START
Β© Faith A. Morrison, Michigan Tech U.
ππ ,
π ,
π ,
Combined molar flux:
ππππππ π΄
ππππ β π‘πππ
combined molar flux of π΄
(due to both diffusion and convection)
QUICK START
Flux of moles of species A, both magnitude and
direction, in the mixture
Module 3 Lecture II 3/1/2021
4
7
Diffusion and Mass Transfer QUICK START
Β© Faith A. Morrison, Michigan Tech U.
π π₯ π π ππ· π»π₯
Using Fickβs law of diffusion in terms of the same combined molar flux:
π
β combined molar flux of π΄ (both diffusion and
convection) relative to stationary coordinates
π₯
mole fraction of π΄
π· diffusion coefficient (diffusivity) of π΄ in π΅
π
molar density of the mixture (for ideal gases π
QUICK START
8
Diffusion and Mass Transfer QUICK START
Β© F
aith A. M
orrison, Michigan Tech U
.
https://pages.mtu.edu/~fmorriso/cm3120/species_mass_bal_3_combinedmolarflux.pdf
Using worksheets to learn the common modeling assumptions QUICK START
Module 3 Lecture II 3/1/2021
5
Microscopic Species Mass Balance
Β© Faith A. Morrison, Michigan Tech U.9
Note: this handout is on the web
pages.mtu.edu/~fmorriso/cm3120/Homeworks_Readings.html
QUICK START
Fickβs Law of Diffusion in terms of Combined Molar Flux π
Β© Faith A. Morrison, Michigan Tech U.10
Note: this handout is on the web
pages.mtu.edu/~fmorriso/cm3120/Homeworks_Readings.html
QUICK START
Module 3 Lecture II 3/1/2021
6
Handy reminder of definitions and relationships among mixture quantities
Β© Faith A. Morrison, Michigan Tech U.11
Note: this handout is on the web
pages.mtu.edu/~fmorriso/cm3120/Homeworks_Readings.html
QUICK START
Β© Faith A. Morrison, Michigan Tech U.
Example 1: Water (40 πΆ, 1.0 ππ‘π) slowly and steadily evaporates into nitrogen (40 πΆ, 1.0 ππ‘π) from the bottom of a cylindrical tank as shown in the figure below. A stream of dry nitrogen flows slowly past the open tank. The mole fraction of water in the gas at the top opening of the tank is 0.02. The geometry is as shown in the figure. What is the rate of water evaporation?
π§
π§ π§ 0.3π
π§ π§ 1.0π
2π
π
π» π
0.25π
π§ 0
BSL2, p547 12
QUICK START1D Evaporation from tank
Module 3 Lecture II 3/1/2021
7
Example: Water (40 πΆ, 1.0 ππ‘π) slowly and steadily evaporates into nitrogen (40 πΆ, 1.0 ππ‘π) from the bottom of a cylindrical tank as shown in the figure below. A stream of dry nitrogen flows slowly past the open tank. The mole fraction of water in the gas at the top opening of the tank is 0.02. What is the rate of water evaporation?
π§
π§ π§ 0.3π
π§ π§ 1.0π
2π
π
π» π
0.25π
π§ 0
QUICK START
Β© Faith A. Morrison, Michigan Tech U.BSL2, p547 13
Why does the water evaporate?
What limits the rate of evaporation?
What could be done to accelerate the evaporation?
What could be done to slow down the evaporation?
Interrogating the problem:
What is the driving physics?
Β© Faith A. Morrison, Michigan Tech U.
Example 1: Water (40 πΆ, 1.0 ππ‘π) slowly and steadily evaporates into nitrogen (40 πΆ, 1.0 ππ‘π) from the bottom of a cylindrical tank as shown in the figure below. A stream of dry nitrogen flows slowly past the open tank. The mole fraction of water in the gas at the top opening of the tank is 0.02. The geometry is as shown in the figure. What is water mole fraction as a function of vertical position in the tank? You may assume ideal gas properties. What is the rate of water evaporation?
π§
π§ π§ 0.3π
π§ π§ 1.0π
2π
π
π» π
0.25π
π§ 0
BSL2, p547 14
QUICK START1D Evaporation from tank
Module 3 Lecture II 3/1/2021
8
Β© F
aith
A. M
orris
on, M
ichi
gan
Tech
U.
BSL2, p547 15
Example: Water (40 πΆ, 1.0 ππ‘π) slowly and steadily evaporates into nitrogen (40 πΆ , 1.0 ππ‘π) from the bottom of a cylindrical tank as shown in the figure below. A stream of dry nitrogen flows slowly past the open tank. The mole fraction of water in the gas at the top opening of the tank is 0.02. What is the rate of water evaporation?
π§
π§ π§ 0.3π
π§ π§ 1.0π
2π
π
π» π
0.25π
π§ 0
QUICK START
Solve.
1D Evaporation from tank
Β© F
aith
A. M
orris
on, M
ichi
gan
Tech
U.
16
Raoultβs LawReference: Felder and Rousseau, 3rd Edition, Section 6.3, Gas-Liquid Systems, One Condensable Component
βA law that describes the behavior of gas-liquid systems over a wide range of conditions provides the desired relationship [between π,π, and π¦ ]. If a gas at temperature π and pressure π contains a saturated vapor whose mole fraction is π¦ (mole vapor/mol total gas), and if this vapor is the only species that would condense if the temperature were slightly lowered, then the partial pressure of the vapor in the gas equals the pure-component vapor pressure πβ π at the system temperature, [which we look up from tables or data correlations].
π π¦ π πβ πRaoultβs Law
(single condensable component)
Module 3 Lecture II 3/1/2021
9
Β© Faith A. Morrison, Michigan Tech U.
17
Revisiting and using important concepts/physics
Pre-reqs
Β© F
aith
A. M
orris
on, M
ichi
gan
Tech
U.
18
Raoultβs LawReference: Felder and Rousseau, 3rd Edition, Section 6.3, Gas-Liquid Systems, One Condensable Component
βA law that describes the behavior of gas-liquid systems over a wide range of conditions provides the desired relationship [between π,π, and π¦ ]. If a gas at temperature π and pressure π contains a saturated vapor whose mole fraction is π¦ (mole vapor/mol total gas), and if this vapor is the only species that would condense if the temperature were slightly lowered, then the partial pressure of the vapor in the gas equals the pure-component vapor pressure πβ π at the system temperature, [which we look up from tables or data correlations].
π π¦ π πβ πRaoultβs Law
(single condensable component)
Where do we get the vapor pressure, ππ¨
β π» ?
1. Tables (water, Felder and Rousseau, Table B.3)2. Clausius-Clapeyron equation (constant Ξπ» , FR Table B.1)
ln πβΞπ»π π
π΅
3. Antoine equation (FR Table B.4)
log πβ π΄π΅
π πΆ
Module 3 Lecture II 3/1/2021
10
BSL2, p547 19
Solution:
1 π₯1 π₯
1 π₯1 π₯
Or:
π₯ 1 1 π₯1 π₯1 π₯
Flux of water:
π ππππ§ π§
ln1 π₯1 π₯
8.0 10 πππ/π π
Rate of evaporation:π΄ π 3.9 10 πππ/π
1D Evaporation from tank
Example: Water (40 πΆ, 1.0 ππ‘π) slowly and steadily evaporates into nitrogen (40 πΆ , 1.0 ππ‘π) from the bottom of a cylindrical tank as shown in the figure below. A stream of dry nitrogen flows slowly past the open tank. The mole fraction of water in the gas at the top opening of the tank is 0.02. What is the rate of water evaporation?
π§
π§ π§ 0.3π
π§ π§ 1.0π
2π
π
π» π
0.25π
π§ 0
QUICK START
Β© Faith A. Morrison, Michigan Tech U.
Note:
πππ
ππ π
0.000
0.010
0.020
0.030
0.040
0.050
0.060
0.070
0.080
0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0
water mole fraction in vapor
distance from tank bottom, m
Evaporation in Cylindrical Tank
Β© F
aith
A. M
orris
on, M
ichi
gan
Tech
U.
20
π§
π§π§
0.3π
π§π§
1.0π
2π
π
π»π
π§0
1D Evaporation from tank
What does the solution look like?π₯ 0.073π₯ 0.02π§ 0.3ππ§ 1.0π
π₯ 1 1 π₯1 π₯1 π₯
π₯ 0.073
π₯ 0.02
Dilute regime:
Module 3 Lecture II 3/1/2021
11
Β© F
aith
A. M
orris
on, M
ichi
gan
Tech
U.
21
π§
π§π§
0.3π
π§π§
1.0π
2π
π
π»π
π§0π₯ 1 1 π₯
1 π₯1 π₯
0.0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1.0
0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0 1.1
mole fraction A
z, meters
0.999
0.975
0.900
0.800
0.650
0.500
0.350
0.250
0.100
What does the solution look like?
All concentrations:π₯
1D Evaporation from tank
Β© Faith A. Morrison, Michigan Tech U.22
π§
π§ π§ 0.3π
π§ π§ 1.0π
2π
π
π» ππ§ 0
Summary1D Evaporation from tank
Model:β’ 1D diffusion through stagnant layer
of B π 0β’ Steady, no reactionβ’ Concentration boundary conditionsβ’ Constant π , π
Results: Constant flux π Profile depends strongly on BC Linear profile (like1D rectangular
heat transfer) for dilute systems Nonlinear profile for non-dilute
systems
1D Evaporation from tank
0.0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1.0
0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0 1.1
mole fraction A
z, meters
0.999
0.975
0.900
0.800
0.650
0.500
0.350
0.250
0.100
Module 3 Lecture II 3/1/2021
12
Β© Faith A. Morrison, Michigan Tech U.
Example 1 Redo: Water (40 πΆ, 1.0 ππ‘π) slowly and steadily evaporates into nitrogen (40 πΆ, 1.0 ππ‘π) from the bottom of a cylindrical tank as shown in the figure below. A stream of dry nitrogen flows slowly past the open tank. The mole fraction of water in the gas at the top opening of the tank is 0.02. The geometry is as shown in the figure. What is water mole fraction as a function of vertical position in the tank? You may assume ideal gas properties andthat the concentration is dilute in water. What is the rate of water evaporation?
π§
π§ π§ 0.3π
π§ π§ 1.0π
2π
π
π» π
0.25π
π§ 0
BSL2, p547 23
QUICK START1D Evaporation from tank
Example 1 Redo: Water ( ) slowly and steadily evaporates into nitrogen ( ) from the bottom of a cylindrical tank as shown in the figure below. A stream of dry nitrogen flows slowly past the open tank. The mole fraction of water in the gas at the top opening of the tank is The geometry is as shown in the figure. What is water mole fraction as a function of vertical position in the tank? You may assume ideal gas properties andthat the concentration is dilute in water. What is the rate of water evaporation?
QUICK START1D Evaporation from tank
Β© F
aith
A. M
orris
on, M
ichi
gan
Tech
U.
BSL2, p547 24
Solve.
1D Evaporation from tank
Answer:π₯ π₯π₯ π₯
π§ π§π§ π§
or
π₯ π₯ π₯ π₯π§ π§π§ π§ linear
Module 3 Lecture II 3/1/2021
13
25Β© Faith A. Morrison, Michigan Tech U.
CM3120: Module 3
Module 3 Lecture IIb
Quick Start 2:1D Radial Diffusion, Reaction
Example: A water mist forms in an industrial printing operation. Spherical water droplets slowly and steadily evaporate into the air (mostly nitrogen). What is the rate of evaporation and how does the water concentration vary in the gas?