issues to address · 2018. 12. 13. · chapter 5 - 13 example problem (2) • problem: the...
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![Page 1: ISSUES TO ADDRESS · 2018. 12. 13. · Chapter 5 - 13 Example Problem (2) • Problem: The diffusion coefficient for copper in Al at 500 and 600 oC -are 4.8x10 14 2and 5.3x10-13 m](https://reader035.vdocuments.site/reader035/viewer/2022081621/6120d73aac76cc71db69b3e2/html5/thumbnails/1.jpg)
Chapter 5 - 1
ISSUES TO ADDRESS...
• Non-steady state diffusion and Fick’s 2nd Law
• How does diffusion depend on structure?
Chapter 5: Diffusion (2)
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Chapter 5 -
Class Exercise (1)
• Put a sugar cube inside a cup of pure
water, roughly draw the sugar
concentration profile inside the water for i)
time is zero (i.e., right after the sugar cube
was placed in water), ii) after a short time
(e.g., 30 sec) and iii) after very long time
2
t = 0
t is small t is long
C
x
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Chapter 5 -
Class Exercise (2)
• Given Fick’s 1st Law in 1D,
1) Explain the physical meaning for each of
the terms in the equation and their unit
2) if both flux J and diffusion coefficient D
are constants, prove the concentration
change linearly with position
3
dx
dCDJ
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Chapter 5 -
Class Exercise (3)
• If diffusion coefficient at different
temperatures (i.e., D1 at T1, D2 at T2, D3 at T3,
D4 at T4) are measured, describe how to
mathematically determine diffusion
activation energy Qd
4
RT
QDD dexp0
TR
QDD d 1
lnln 0
1/T
lnD
lnD0
Slope = R
Qd
1
1
T 2
1
T3
1
T 4
1
T
1ln D
2ln D
3ln D
4ln D
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Chapter 5 - 5
Non-Steady State Diffusion
• General case: The concentration of diffusing species is a function of position, time, and, maybe, concentration C = C(x, t, c)
• Fick’s Second Law
• If D is a constant (i.e., does not change with concentration)
x
CD
xt
C
2
2
x
CD
t
C
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Chapter 5 - 6
Special Example for Non-steady
State Diffusion
Adapted from
Fig. 5.5,
Callister &
Rethwisch 8e.
Boundary conditions
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
C s
2
2
x
CD
t
C
Fick’s 2nd law C(x, t)?
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Chapter 5 - 7
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
CC
Ct,xC
os
o
2 erf1
dye yz 2
0
2
Adapted from Fig. 5.5,
Callister & Rethwisch 8e.
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Chapter 5 - 8
Example of a Special Case for
Non-steady State Diffusion • 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 diffusion coefficient. Knowing concentration at
time t and position x satisfy the following relationship:
Dt
x
CC
CtxC
os
o
2erf1
),(
t = 49.5 h x = 4 x 10-3 m
Cx = 0.35 wt% Cs = 1.0 wt%
Co = 0.20 wt%
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Chapter 5 - 9
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
CC
C)t,x(C
os
o
2erf1
)(erf12
erf120.00.1
20.035.0),(z
Dt
x
CC
CtxC
os
o
erf(z) = 0.8125
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Chapter 5 - 10
Solution (cont.): We must now determine the value of z for which the error function
is 0.8125. If as in Table 5.1 in textbook, tabulated data are given,
an interpolation can be used to obtain the approximate value
z erf(z)
0.90 0.7970
z 0.8125
0.95 0.8209
7970.08209.0
7970.08125.0
90.095.0
90.0
z
z 0.93
Now solve for D
Dt
xz
2
tz
xD
2
2
4
/sm 10 x 6.2s 3600
h 1
h) 5.49()93.0()4(
m)10 x 4(
4
211
2
23
2
2
tz
xD
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Chapter 5 -
Diffusion Length
• When
• Diffusion (characteristic) length
11
5.02
erf1
Dt
x
CC
CC
os
o
5.0
os
o
CC
CC
2
0 sCCC
5.02
erf
Dt
x
5.02
z Dt
x
Dtx
x
C
0
C0
CS
t1 t2 t3
2
0CCS
x1 x2 x3
Dt
x
CC
Ct,xC
os
o
2 erf1
The depth (length) within which significant
diffusion has happened
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Chapter 5 -
Class Exercise • Knowing diffusion length
Diffusion coefficient for P and Cu in Si at 1000C is
1x10-14 cm2/sec and 5.3x10-6 cm2/sec, respectively. If
putting Cu and P on surface of Si, please estimate the
depth within silicon that is impacted by P and Cu
diffusion after 30 min at 1000C, respectively
12
Dtx
nmcm
cmDtxP
42102.4
sec1800sec/10
6
214
mcm
cmDtxCu
90009.0
sec1800sec/103.5 26
•At the same temperature for same
time, Cu would diffuse
(penetrate) much deeper than P
into Si!
•As Cu is detrimental to Si
devices, people have to apply a
“diffusion barrier” (e.g., Ru or
TaN) in the semiconductor
industry when using Cu as metal
conductor for Si micro-chips
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Chapter 5 - 13
Example Problem (2)
• Problem: The diffusion coefficient for copper in Al at 500
and 600 oC are 4.8x10-14 and 5.3x10-13 m2/s, respectively.
Determine the approximate time at 500 oC that will produce
the same diffusion result (i.e., diffusion length) as a 10 hour
heat treatment at 600 oC. Note that diffusion length
• Same diffusion result, therefore, same diffusion length, i.e.,
In this case,
D1 (600oC) =5.3x10-13 m2/s,
D2 (500oC) = 4.8x10-14 m2/s
t1 (600oC) = 10 h
Dtx
222111 xtDtDx
htD
DCt o 4.110)500( 1
2
12
It would need a much longer time
at lower temperature to produce
the same (diffusion) result as that
obtained at a higher temperature
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Chapter 5 - 14
Diffusion FASTER for...
• More open crystal structures
• Materials w/secondary
bonding
• Smaller diffusing atoms
• Lower density materials
Diffusion SLOWER for...
• Close-packed structures
• Materials with all covalent
bonding
• Larger diffusing atoms
• Higher density materials
Structure Effects on Diffusion
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Chapter 5 -
Homework
• Read chapter 5 of Calister 8ed and give an
honor statement confirming you finished
the required reading
• Callister 8ed, 5.1, 5.3(a), 5.6, 5.11, 5.16,
5.22
15
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Chapter 5 -
• Calister 8ed, 5.1
5.1 Briefly explain the difference between self-
diffusion and interdiffusion.
• Calister 8ed, 5.3(a)
5.3 (a) Compare interstitial and vacancy
atomic mechanisms for diffusion.
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Chapter 5 -
Calister 8ed, 5.6
The purification of hydrogen gas by diffusion
through a palladium sheet was discussed in
Section 5.3. Compute the number of kilograms
of hydrogen that pass per hour through a
5-mm-thick sheet of palladium having an area
of 0.20 m2 at 500C. Assume a diffusion
coefficient of 1.0 10-8 m2/s, that the
concentrations at the high- and low-pressure
sides of the plate are 2.4 and 0.6 kg of
hydrogen per cubic meter of palladium, and
that steady-state conditions have been
attained.
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Chapter 5 -
• Calister 8ed, 5.11
5.11 Determine the carburizing time necessary
to achieve a carbon concentration of 0.45
wt% at a position 2 mm into an iron–carbon
alloy that initially contains 0.20 wt% C. The
surface concentration is to be maintained at
1.30 wt% C, and the treatment is to be
conducted at 1000C. Use the diffusion data
for γ-Fe in Table 5.2
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Chapter 5 -
• Calister 8ed, 5.16
5.16 Cite the values of the diffusion
coefficients for the interdiffusion of carbon in
both α-iron (BCC) and γ-iron (FCC) at 900°C
(from Table 5.2). Which is larger? Explain
why this is the case.
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Chapter 5 -
• Calister 8ed, 5.22
5.22 The diffusion coefficients for silver in
copper are given at two temperatures:
(a) Determine the values of D0 and Qd.
(b) What is the magnitude of D at 875°C?
T (°C) D (m2/s)
650 5.5 × 10–16
900 1.3 × 10–13