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Chapter 5 - 1
ISSUES TO ADDRESS...
• How does diffusion occur?
• Why is it an important part of processing?
• How can the rate of diffusion be predicted for
some simple cases?
• How does diffusion depend on structure
and temperature?
Chapter 5: Diffusion
Chapter 5 - 2
Diffusion
Diffusion - Mass transport by atomic motion
Mechanisms
• Gases & Liquids – random (Brownian) motion
• Solids – vacancy diffusion or interstitial diffusion
Chapter 5 - 3
• Interdiffusion: In an alloy, atoms tend to migrate
from regions of high conc. to regions of low conc.
Initially
Adapted from
Figs. 5.1 and
5.2, Callister &
Rethwisch 8e.
Diffusion
After some time
Chapter 5 - 4
• Self-diffusion: In an elemental solid, atoms
also migrate.
Label some atoms
Diffusion
A
B
C
D
After some time
A
B
C
D
Chapter 5 - 5
Diffusion Mechanisms
Vacancy Diffusion:
• atoms exchange with vacancies
• applies to substitutional impurities atoms
• rate depends on:
-- number of vacancies
-- activation energy to exchange.
increasing elapsed time
Chapter 5 - 6
• Simulation of
interdiffusion
across an interface:
• Rate of substitutional
diffusion depends on:
-- vacancy concentration
-- frequency of jumping.
(Courtesy P.M. Anderson)
Diffusion Simulation
This slide contains an animation that requires Quicktime
and a Cinepak decompressor. Click on the message or
image below to activate the animation.
Chapter 5 - 7
Diffusion Mechanisms
• Interstitial diffusion – smaller atoms can
diffuse between atoms.
More rapid than vacancy diffusion
Adapted from Fig. 5.3(b), Callister & Rethwisch 8e.
Chapter 5 - 8
Adapted from
chapter-opening
photograph,
Chapter 5,
Callister &
Rethwisch 8e.
(Courtesy of
Surface Division,
Midland-Ross.)
• Case Hardening:
-- Diffuse carbon atoms
into the host iron atoms
at the surface.
-- Example of interstitial
diffusion is a case
hardened gear.
• Result: The presence of C
atoms makes iron (steel) harder.
Processing Using Diffusion
Chapter 5 - 9
• Doping silicon with phosphorus for n-type semiconductors:
• Process:
3. Result: Doped
semiconductor
regions.
silicon
Processing Using Diffusion
magnified image of a computer chip
0.5mm
light regions: Si atoms
light regions: Al atoms
2. Heat it.
1. Deposit P rich
layers on surface.
silicon
Adapted from Figure 18.27, Callister &
Rethwisch 8e.
Chapter 5 - 10
Diffusion
• How do we quantify the amount or rate of diffusion?
   s
m
kg
or
s
cm
mol
time
area
surface
diffusing
mass)
(or
moles
Flux
2
2



J
J  slope
dt
dM
A
l
At
M
J 

M =
mass
diffused
time
• Measured empirically
– Make thin film (membrane) of known surface area
– Impose concentration gradient
– Measure how fast atoms or molecules diffuse through the
membrane
Chapter 5 - 11
Steady-State Diffusion
dx
dC
D
J 

Fick’s first law of diffusion
C1
C2
x
C1
C2
x1 x2
D  diffusion coefficient
Rate of diffusion independent of time
Flux proportional to concentration gradient =
dx
dC
1
2
1
2
linear
if
x
x
C
C
x
C
dx
dC






Chapter 5 - 12
Example: Chemical Protective
Clothing (CPC)
• Methylene chloride is a common ingredient of paint
removers. Besides being an irritant, it also may be
absorbed through skin. When using this paint
remover, protective gloves should be worn.
• If butyl rubber gloves (0.04 cm thick) are used, what
is the diffusive flux of methylene chloride through the
glove?
• Data:
– diffusion coefficient in butyl rubber:
D = 110x10-8 cm2/s
– surface concentrations:
C2 = 0.02 g/cm3
C1 = 0.44 g/cm3
Chapter 5 - 13
s
cm
g
10
x
16
.
1
cm)
04
.
0
(
)
g/cm
44
.
0
g/cm
02
.
0
(
/s)
cm
10
x
110
(
2
5
-
3
3
2
8
-




J
Example (cont).
1
2
1
2
-
x
x
C
C
D
dx
dC
D
J





D
tb
6
2


glove
C1
C2
skin
paint
remover
x1 x2
• Solution – assuming linear conc. gradient
D = 110x10-8 cm2/s
C2 = 0.02 g/cm3
C1 = 0.44 g/cm3
x2 – x1 = 0.04 cm
Data:
Chapter 5 - 14
Diffusion and Temperature
• Diffusion coefficient increases with increasing T.
D  Do exp







Qd
RT
= pre-exponential [m2/s]
= diffusion coefficient [m2/s]
= activation energy [J/mol or eV/atom]
= gas constant [8.314 J/mol-K]
= absolute temperature [K]
D
Do
Qd
R
T
Chapter 5 - 15
Diffusion and Temperature
Adapted from Fig. 5.7, Callister & Rethwisch 8e. (Date for Fig. 5.7
taken from E.A. Brandes and G.B. Brook (Ed.) Smithells Metals
Reference Book, 7th ed., Butterworth-Heinemann, Oxford, 1992.)
D has exponential dependence on T
Dinterstitial >> Dsubstitutional
C in a-Fe
C in g-Fe
Al in Al
Fe in a-Fe
Fe in g-Fe
1000K/T
D (m2/s)
0.5 1.0 1.5
10-20
10-14
10-8
T(C)
1500
1000
600
300
Chapter 5 - 16
Example: At 300ºC the diffusion coefficient and
activation energy for Cu in Si are
D(300ºC) = 7.8 x 10-11 m2/s
Qd = 41.5 kJ/mol
What is the diffusion coefficient at 350ºC?




















1
0
1
2
0
2
1
ln
ln
and
1
ln
ln
T
R
Q
D
D
T
R
Q
D
D d
d














1
2
1
2
1
2
1
1
ln
ln
ln
T
T
R
Q
D
D
D
D d
transform
data
D
Temp = T
ln D
1/T
Chapter 5 - 17
Example (cont.)














 
K
573
1
K
623
1
K
-
J/mol
314
.
8
J/mol
500
,
41
exp
/s)
m
10
x
8
.
7
( 2
11
2
D

















1
2
1
2
1
1
exp
T
T
R
Q
D
D d
T1 = 273 + 300 = 573K
T2 = 273 + 350 = 623K
D2 = 15.7 x 10-11 m2/s
Chapter 5 - 18
Non-steady State Diffusion
• The concentration of diffusing species is a function of
both time and position C = C(x,t)
• In this case Fick’s Second Law is used
2
2
x
C
D
t
C





Fick’s Second Law
Chapter 5 -
VMSE: Student Companion Site
Diffusion Computations & Data Plots
19
Chapter 5 - 20
Non-steady State Diffusion
Adapted from
Fig. 5.5,
Callister &
Rethwisch 8e.
B.C. at t = 0, C = Co for 0  x  
at t > 0, C = CS for x = 0 (constant surface conc.)
C = Co for x = 
• Copper diffuses into a bar of aluminum.
pre-existing conc., Co of copper atoms
Surface conc.,
C of Cu atoms bar
s
Cs
Chapter 5 - 21
Solution:
C(x,t) = Conc. at point x at
time t
erf (z) = error function
erf(z) values are given in
Table 5.1
CS
Co
C(x,t)
 










Dt
x
C
C
C
t
,
x
C
o
s
o
2
erf
1
dy
e y
z 2
0
2 



Adapted from Fig. 5.5,
Callister & Rethwisch 8e.
Chapter 5 - 22
Non-steady State Diffusion
• Sample Problem: An FCC iron-carbon alloy initially
containing 0.20 wt% C is carburized at an elevated
temperature and in an atmosphere that gives a
surface carbon concentration constant at 1.0 wt%. If
after 49.5 h the concentration of carbon is 0.35 wt%
at a position 4.0 mm below the surface, determine
the temperature at which the treatment was carried
out.
• Solution: use Eqn. 5.5 









Dt
x
C
C
C
t
x
C
o
s
o
2
erf
1
)
,
(
Chapter 5 - 23
Solution (cont.):
– t = 49.5 h x = 4 x 10-3 m
– Cx = 0.35 wt% Cs = 1.0 wt%
– Co = 0.20 wt%










Dt
x
C
C
C
)
t
,
x
(
C
o
s
o
2
erf
1
)
(
erf
1
2
erf
1
20
.
0
0
.
1
20
.
0
35
.
0
)
,
(
z
Dt
x
C
C
C
t
x
C
o
s
o 














 erf(z) = 0.8125
Chapter 5 - 24
Solution (cont.):
We must now determine from Table 5.1 the value of z for which the
error function is 0.8125. An interpolation is necessary as follows
z erf(z)
0.90 0.7970
z 0.8125
0.95 0.8209
7970
.
0
8209
.
0
7970
.
0
8125
.
0
90
.
0
95
.
0
90
.
0





z
z  0.93
Now solve for D
Dt
x
z
2

t
z
x
D
2
2
4

/s
m
10
x
6
.
2
s
3600
h
1
h)
5
.
49
(
)
93
.
0
(
)
4
(
m)
10
x
4
(
4
2
11
2
2
3
2
2














t
z
x
D
Chapter 5 - 25
• To solve for the temperature at
which D has the above value,
we use a rearranged form of
Equation (5.9a);
)
ln
ln
( D
D
R
Q
T
o
d


from Table 5.2, for diffusion of C in FCC Fe
Do = 2.3 x 10-5 m2/s Qd = 148,000 J/mol
/s)
m
10
x
6
.
2
ln
/s
m
10
x
3
.
2
K)(ln
-
J/mol
314
.
8
(
J/mol
000
,
148
2
11
2
5 



T

Solution (cont.):
T = 1300 K = 1027ºC
Chapter 5 - 26
Example: Chemical Protective
Clothing (CPC)
• Methylene chloride is a common ingredient of paint removers.
Besides being an irritant, it also may be absorbed through skin.
When using this paint remover, protective gloves should be
worn.
• If butyl rubber gloves (0.04 cm thick) are used, what is the
breakthrough time (tb), i.e., how long could the gloves be used
before methylene chloride reaches the hand?
• Data
– diffusion coefficient in butyl rubber:
D = 110x10-8 cm2/s
Chapter 5 - 27
CPC Example (cont.)
Time required for breakthrough ca. 4 min
glove
C1
C2
skin
paint
remover
x1 x2
• Solution – assuming linear conc. gradient
D
tb
6
2


Equation from online CPC
Case Study 5 at the Student
Companion Site for Callister &
Rethwisch 8e (www.wiley.com/
college/callister)
cm
0.04
1
2 

 x
x

D = 110x10-8 cm2/s
min
4
s
240
/s)
cm
10
x
110
)(
6
(
cm)
04
.
0
(
2
8
-
2



b
t
Breakthrough time = tb
Chapter 5 - 28
Diffusion FASTER for...
• open crystal structures
• materials w/secondary
bonding
• smaller diffusing atoms
• lower density materials
Diffusion SLOWER for...
• close-packed structures
• materials w/covalent
bonding
• larger diffusing atoms
• higher density materials
Summary
Chapter 5 - 29
Core Problems:
Self-help Problems:
ANNOUNCEMENTS
Reading:

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ch05_.pdf.pdf

  • 1. Chapter 5 - 1 ISSUES TO ADDRESS... • How does diffusion occur? • Why is it an important part of processing? • How can the rate of diffusion be predicted for some simple cases? • How does diffusion depend on structure and temperature? Chapter 5: Diffusion
  • 2. Chapter 5 - 2 Diffusion Diffusion - Mass transport by atomic motion Mechanisms • Gases & Liquids – random (Brownian) motion • Solids – vacancy diffusion or interstitial diffusion
  • 3. Chapter 5 - 3 • Interdiffusion: In an alloy, atoms tend to migrate from regions of high conc. to regions of low conc. Initially Adapted from Figs. 5.1 and 5.2, Callister & Rethwisch 8e. Diffusion After some time
  • 4. Chapter 5 - 4 • Self-diffusion: In an elemental solid, atoms also migrate. Label some atoms Diffusion A B C D After some time A B C D
  • 5. Chapter 5 - 5 Diffusion Mechanisms Vacancy Diffusion: • atoms exchange with vacancies • applies to substitutional impurities atoms • rate depends on: -- number of vacancies -- activation energy to exchange. increasing elapsed time
  • 6. Chapter 5 - 6 • Simulation of interdiffusion across an interface: • Rate of substitutional diffusion depends on: -- vacancy concentration -- frequency of jumping. (Courtesy P.M. Anderson) Diffusion Simulation This slide contains an animation that requires Quicktime and a Cinepak decompressor. Click on the message or image below to activate the animation.
  • 7. Chapter 5 - 7 Diffusion Mechanisms • Interstitial diffusion – smaller atoms can diffuse between atoms. More rapid than vacancy diffusion Adapted from Fig. 5.3(b), Callister & Rethwisch 8e.
  • 8. Chapter 5 - 8 Adapted from chapter-opening photograph, Chapter 5, Callister & Rethwisch 8e. (Courtesy of Surface Division, Midland-Ross.) • Case Hardening: -- Diffuse carbon atoms into the host iron atoms at the surface. -- Example of interstitial diffusion is a case hardened gear. • Result: The presence of C atoms makes iron (steel) harder. Processing Using Diffusion
  • 9. Chapter 5 - 9 • Doping silicon with phosphorus for n-type semiconductors: • Process: 3. Result: Doped semiconductor regions. silicon Processing Using Diffusion magnified image of a computer chip 0.5mm light regions: Si atoms light regions: Al atoms 2. Heat it. 1. Deposit P rich layers on surface. silicon Adapted from Figure 18.27, Callister & Rethwisch 8e.
  • 10. Chapter 5 - 10 Diffusion • How do we quantify the amount or rate of diffusion?    s m kg or s cm mol time area surface diffusing mass) (or moles Flux 2 2    J J  slope dt dM A l At M J   M = mass diffused time • Measured empirically – Make thin film (membrane) of known surface area – Impose concentration gradient – Measure how fast atoms or molecules diffuse through the membrane
  • 11. Chapter 5 - 11 Steady-State Diffusion dx dC D J   Fick’s first law of diffusion C1 C2 x C1 C2 x1 x2 D  diffusion coefficient Rate of diffusion independent of time Flux proportional to concentration gradient = dx dC 1 2 1 2 linear if x x C C x C dx dC      
  • 12. Chapter 5 - 12 Example: Chemical Protective Clothing (CPC) • Methylene chloride is a common ingredient of paint removers. Besides being an irritant, it also may be absorbed through skin. When using this paint remover, protective gloves should be worn. • If butyl rubber gloves (0.04 cm thick) are used, what is the diffusive flux of methylene chloride through the glove? • Data: – diffusion coefficient in butyl rubber: D = 110x10-8 cm2/s – surface concentrations: C2 = 0.02 g/cm3 C1 = 0.44 g/cm3
  • 13. Chapter 5 - 13 s cm g 10 x 16 . 1 cm) 04 . 0 ( ) g/cm 44 . 0 g/cm 02 . 0 ( /s) cm 10 x 110 ( 2 5 - 3 3 2 8 -     J Example (cont). 1 2 1 2 - x x C C D dx dC D J      D tb 6 2   glove C1 C2 skin paint remover x1 x2 • Solution – assuming linear conc. gradient D = 110x10-8 cm2/s C2 = 0.02 g/cm3 C1 = 0.44 g/cm3 x2 – x1 = 0.04 cm Data:
  • 14. Chapter 5 - 14 Diffusion and Temperature • Diffusion coefficient increases with increasing T. D  Do exp        Qd RT = pre-exponential [m2/s] = diffusion coefficient [m2/s] = activation energy [J/mol or eV/atom] = gas constant [8.314 J/mol-K] = absolute temperature [K] D Do Qd R T
  • 15. Chapter 5 - 15 Diffusion and Temperature Adapted from Fig. 5.7, Callister & Rethwisch 8e. (Date for Fig. 5.7 taken from E.A. Brandes and G.B. Brook (Ed.) Smithells Metals Reference Book, 7th ed., Butterworth-Heinemann, Oxford, 1992.) D has exponential dependence on T Dinterstitial >> Dsubstitutional C in a-Fe C in g-Fe Al in Al Fe in a-Fe Fe in g-Fe 1000K/T D (m2/s) 0.5 1.0 1.5 10-20 10-14 10-8 T(C) 1500 1000 600 300
  • 16. Chapter 5 - 16 Example: At 300ºC the diffusion coefficient and activation energy for Cu in Si are D(300ºC) = 7.8 x 10-11 m2/s Qd = 41.5 kJ/mol What is the diffusion coefficient at 350ºC?                     1 0 1 2 0 2 1 ln ln and 1 ln ln T R Q D D T R Q D D d d               1 2 1 2 1 2 1 1 ln ln ln T T R Q D D D D d transform data D Temp = T ln D 1/T
  • 17. Chapter 5 - 17 Example (cont.)                 K 573 1 K 623 1 K - J/mol 314 . 8 J/mol 500 , 41 exp /s) m 10 x 8 . 7 ( 2 11 2 D                  1 2 1 2 1 1 exp T T R Q D D d T1 = 273 + 300 = 573K T2 = 273 + 350 = 623K D2 = 15.7 x 10-11 m2/s
  • 18. Chapter 5 - 18 Non-steady State Diffusion • The concentration of diffusing species is a function of both time and position C = C(x,t) • In this case Fick’s Second Law is used 2 2 x C D t C      Fick’s Second Law
  • 19. Chapter 5 - VMSE: Student Companion Site Diffusion Computations & Data Plots 19
  • 20. Chapter 5 - 20 Non-steady State Diffusion Adapted from Fig. 5.5, Callister & Rethwisch 8e. B.C. at t = 0, C = Co for 0  x   at t > 0, C = CS for x = 0 (constant surface conc.) C = Co for x =  • Copper diffuses into a bar of aluminum. pre-existing conc., Co of copper atoms Surface conc., C of Cu atoms bar s Cs
  • 21. Chapter 5 - 21 Solution: C(x,t) = Conc. at point x at time t erf (z) = error function erf(z) values are given in Table 5.1 CS Co C(x,t)             Dt x C C C t , x C o s o 2 erf 1 dy e y z 2 0 2     Adapted from Fig. 5.5, Callister & Rethwisch 8e.
  • 22. Chapter 5 - 22 Non-steady State Diffusion • Sample Problem: An FCC iron-carbon alloy initially containing 0.20 wt% C is carburized at an elevated temperature and in an atmosphere that gives a surface carbon concentration constant at 1.0 wt%. If after 49.5 h the concentration of carbon is 0.35 wt% at a position 4.0 mm below the surface, determine the temperature at which the treatment was carried out. • Solution: use Eqn. 5.5           Dt x C C C t x C o s o 2 erf 1 ) , (
  • 23. Chapter 5 - 23 Solution (cont.): – t = 49.5 h x = 4 x 10-3 m – Cx = 0.35 wt% Cs = 1.0 wt% – Co = 0.20 wt%           Dt x C C C ) t , x ( C o s o 2 erf 1 ) ( erf 1 2 erf 1 20 . 0 0 . 1 20 . 0 35 . 0 ) , ( z Dt x C C C t x C o s o                 erf(z) = 0.8125
  • 24. Chapter 5 - 24 Solution (cont.): We must now determine from Table 5.1 the value of z for which the error function is 0.8125. An interpolation is necessary as follows z erf(z) 0.90 0.7970 z 0.8125 0.95 0.8209 7970 . 0 8209 . 0 7970 . 0 8125 . 0 90 . 0 95 . 0 90 . 0      z z  0.93 Now solve for D Dt x z 2  t z x D 2 2 4  /s m 10 x 6 . 2 s 3600 h 1 h) 5 . 49 ( ) 93 . 0 ( ) 4 ( m) 10 x 4 ( 4 2 11 2 2 3 2 2               t z x D
  • 25. Chapter 5 - 25 • To solve for the temperature at which D has the above value, we use a rearranged form of Equation (5.9a); ) ln ln ( D D R Q T o d   from Table 5.2, for diffusion of C in FCC Fe Do = 2.3 x 10-5 m2/s Qd = 148,000 J/mol /s) m 10 x 6 . 2 ln /s m 10 x 3 . 2 K)(ln - J/mol 314 . 8 ( J/mol 000 , 148 2 11 2 5     T  Solution (cont.): T = 1300 K = 1027ºC
  • 26. Chapter 5 - 26 Example: Chemical Protective Clothing (CPC) • Methylene chloride is a common ingredient of paint removers. Besides being an irritant, it also may be absorbed through skin. When using this paint remover, protective gloves should be worn. • If butyl rubber gloves (0.04 cm thick) are used, what is the breakthrough time (tb), i.e., how long could the gloves be used before methylene chloride reaches the hand? • Data – diffusion coefficient in butyl rubber: D = 110x10-8 cm2/s
  • 27. Chapter 5 - 27 CPC Example (cont.) Time required for breakthrough ca. 4 min glove C1 C2 skin paint remover x1 x2 • Solution – assuming linear conc. gradient D tb 6 2   Equation from online CPC Case Study 5 at the Student Companion Site for Callister & Rethwisch 8e (www.wiley.com/ college/callister) cm 0.04 1 2    x x  D = 110x10-8 cm2/s min 4 s 240 /s) cm 10 x 110 )( 6 ( cm) 04 . 0 ( 2 8 - 2    b t Breakthrough time = tb
  • 28. Chapter 5 - 28 Diffusion FASTER for... • open crystal structures • materials w/secondary bonding • smaller diffusing atoms • lower density materials Diffusion SLOWER for... • close-packed structures • materials w/covalent bonding • larger diffusing atoms • higher density materials Summary
  • 29. Chapter 5 - 29 Core Problems: Self-help Problems: ANNOUNCEMENTS Reading: