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Question 5.7: Design of a Carburizing Treatment The surface of a 0.1% C st......

Design of a Carburizing Treatment
The surface of a 0.1% C steel gear is to be hardened by carburizing. In gas carburizing, the steel gears are placed in an atmosphere that provides 1.2% C at the surface of the steel at a high temperature (Figure 5-1). Carbon then diffuses from the surface into the steel. For optimum properties, the steel must contain 0.45% C at a depth of 0.2 cm below the surface. Design a carburizing heat treatment that will produce these optimum properties. Assume that the temperature is high enough (at least 900 °C) so that the iron has the FCC structure.

5.1
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Since the boundary conditions for which Equation 5-7 was derived are assumed to be valid, we can use this equation:
\frac{c_{s} \ – \ c_{x}}{c_{s} \ – \ c_{0}}= erf ( \frac{x}{2\sqrt{Dt}})
We know that c_{s} = 1.2% C, c_{0} = 0.1% C, c_{x} = 0.45% C, and x = 0.2 cm. From Fick’s second law:
\frac{c_{s} \ – \ c_{x}}{c_{s} \ – \ c_{0}}=  \frac{1.2 \% \ C \ – \ 0.45 \% \ C}{1.2 \% \ C \ – \ 0.1 \% \ C} =0.68 =erf ( \frac{0.2 \ cm}{2\sqrt{Dt}}) = erf ( \frac{0.1 \ cm}{\sqrt{Dt}})
From Table 5-3, we find that
\frac{0.1 \ cm}{\sqrt{Dt}} = 0.71 or Dt =( \frac{0.1}{0.71})^2 = 0.0198 cm^2
Any combination of D and t with a product of 0.0198 cm² will work. For carbon diffusing in FCC iron, the diffusion coefficient is related to temperature by Equation 5-4:
D = D_{0} \exp(\frac{-Q}{RT})
From Table 5-1:
D = 0.23 \exp[\frac{-32,900 \ cal/mol}{(1.987 \ \frac{cal}{mol  ⋅  K})T} ] = 0.23 \exp(\frac{-16,558}{T})
Therefore, the temperature and time of the heat treatment are related by
t = \frac{0.0198 \ cm^2}{D} =\frac{0.0198 \ cm^2}{0.23 \exp(-16,558/T)} =\frac{0.0861}{\exp (-16,558/T)}
Some typical combinations of temperatures and times are
If T = 900 °C = 1173 K, then t = 116,273 s = 32.3 h
If T = 1000 °C = 1273 K, then t = 38,362 s = 10.7 h
If T = 1100 °C = 1373 K, then t = 14,876 s = 4.13 h
If T = 1200 °C = 1473 K, then t = 6,560 s = 1.82 h
The exact combination of temperature and time will depend on the maximum temperature that the heat treating furnace can reach, the rate at which parts must be produced, and the economics of the tradeoffs between higher temperatures versus longer times. Another factor to consider is changes in microstructure that occur in the rest of the material. For example, while carbon is diffusing into the surface, the rest of the microstructure can begin to experience grain growth or other changes.

Table 5-3 Error function values for Fick’s second law
Argument of the Error Function \frac{x}{ 2 \sqrt{Dt}} Value of the Error Function erf \frac{x}{ 2 \sqrt{Dt}}
0 0
0.10 0.1125
0.20 0.2227
0.30 0.3286
0.40 0.4284
0.50 0.5205
0.60 0.6039
0.70 0.6778
0.80 0.7421
0.90 0.7969
1.00 0.8427
1.50 0.9661
2.00 0.9953

Note that error function values are available in many software packages.

Table 5-1 Diffusion data for selected materials
Diffusion Couple Q (cal/mol) D_{0}  (cm^2/s)
Interstitial diffusion:
C in FCC iron 32,900 0.23
C in BCC iron 20,900 0.011
N in FCC iron 34,600 0.0034
N in BCC iron 18,300 0.0047
H in FCC iron 10,300 0.0063
H in BCC iron 3,600 0.0012
Self-diffusion (vacancy diffusion):
Pb in FCC Pb 25,900 1.27
Al in FCC Al 32,200 0.10
Cu in FCC Cu 49,300 0.36
Fe in FCC Fe 66,700 0.65
Zn in HCP Zn 21,800 0.1
Mg in HCP Mg 32,200 1.0
Fe in BCC Fe 58,900 4.1
W in BCC W 143,300 1.88
Si in Si (covalent) 110,000 1800.0
C in C (covalent) 163,000 5.0
Heterogeneous diffusion (vacancy diffusion):
Ni in Cu 57,900 2.3
Cu in Ni 61,500 0.65
Zn in Cu 43,900 0.78
Ni in FCC iron 64,000 4.1
Au in Ag 45,500 0.26
Ag in Au 40,200 0.072
Al in Cu 39,500 0.045
Al in Al_{2}O_{3} 114,000 28.0
O in Al_{2}O_{3} 152,000 1900.0
Mg in MgO 79,000 0.249
O in MgO 82,100 0.000043

Based on several sources, including Adda, Y. and Philibert, J., La Diffusion dans les Solides, Vol. 2, 1966.

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