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.
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.