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Callister - An introduction - 8th edition

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5.4 Nonsteady-State Diffusion • 129<br />

Solution to Fick’s<br />

second law for the<br />

condition of constant<br />

surface concentration<br />

(for a semiinfinite<br />

solid)<br />

Comprehensive collections of these are given by Crank, and Carslaw and Jaeger<br />

(see References).<br />

One practically important solution is for a semi-infinite solid 2 in which the surface<br />

concentration is held constant. Frequently, the source of the diffusing species<br />

is a gas phase, the partial pressure of which is maintained at a constant value. Furthermore,<br />

the following assumptions are made:<br />

1. Before diffusion, any of the diffusing solute atoms in the solid are uniformly<br />

distributed with concentration of C 0 .<br />

2. The value of x at the surface is zero and increases with distance into the solid.<br />

3. The time is taken to be zero the instant before the diffusion process begins.<br />

These boundary conditions are simply stated as<br />

For t 0, C C 0 at 0 x <br />

For t 0, C C s (the constant surface concentration) at x 0<br />

C C 0 at x <br />

Application of these boundary conditions to Equation 5.4b yields the solution<br />

C x C 0<br />

x<br />

1 erf a<br />

C s C 0 21Dt b<br />

(5.5)<br />

where C x represents the concentration at depth x after time t. The expression<br />

erf1x/21Dt2 is the Gaussian error function, 3 values of which are given in mathematical<br />

tables for various x/21Dt values; a partial listing is given in Table 5.1. The<br />

Table 5.1<br />

Tabulation of Error Function Values<br />

z erf(z) z erf(z) z erf(z)<br />

0 0 0.55 0.5633 1.3 0.9340<br />

0.025 0.0282 0.60 0.6039 1.4 0.9523<br />

0.05 0.0564 0.65 0.6420 1.5 0.9661<br />

0.10 0.1125 0.70 0.6778 1.6 0.9763<br />

0.15 0.1680 0.75 0.7112 1.7 0.9838<br />

0.20 0.2227 0.80 0.7421 1.8 0.9891<br />

0.25 0.2763 0.85 0.7707 1.9 0.9928<br />

0.30 0.3286 0.90 0.7970 2.0 0.9953<br />

0.35 0.3794 0.95 0.8209 2.2 0.9981<br />

0.40 0.4284 1.0 0.8427 2.4 0.9993<br />

0.45 0.4755 1.1 0.8802 2.6 0.9998<br />

0.50 0.5205 1.2 0.9103 2.8 0.9999<br />

2 A bar of solid is considered to be semi-infinite if none of the diffusing atoms reaches the<br />

bar end during the time over which diffusion takes place. A bar of length l is considered to<br />

be semi-infinite when l 7 102Dt.<br />

3 This Gaussian error function is defined by<br />

erf 1z2 <br />

1p 2 z<br />

e y2 dy<br />

where x/21Dt has been replaced by the variable z.<br />

0

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