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21-Mat-A4 Deformation Behaviour and Properties of Materials · December 2013

Question 6 of 8: Diffusion (20 marks)

Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)

Notes on this paper

Paper format. National Exams, December 2013 — Met-A4, Structure of Materials. Three hours, closed book, one approved calculator (Casio or Sharp). Eight questions of 20 marks each; the rubric asks for any five, and only the first five in the answer book are marked. All eight are solved here. All necessary equations and constants are provided in the exam's own appendix (reproduced where used below).

The printed exam header reads Met-A4, Structure of Materials. Only two of the eight questions (VI and VII) are genuinely diffusion/mechanical-properties content; the paper as a whole is a broad introductory materials-science survey — bonding, crystal defects, crystallography, XRD and phase diagrams — and is answered as such below.

Reference texts. The answers below are keyed to the works normally recommended for this syllabus code:


Question VI — Diffusion (20 marks)

Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.

Given. Non-steady-state (Fickian) carburizing: bulk composition $C_0=0.2\%\text{C}$, surface composition (held fixed) $C_s=1.0\%\text{C}$, depth $x=0.3\ \text{mm}=0.03\ \text{cm}$, time $t_1=10\ \text{h}=36{,}000\ \text{s}$, $D=0.298\times10^{-6}\ \text{cm}^2/\text{s}$ (constant, single temperature — matches published $D$ for C in $\gamma$-Fe near 1000°C, so no anomaly flag is needed here).

Find. (i) $C(x{=}0.3\ \text{mm},\,t{=}10\ \text{h})$; (ii) the time $t_2$ for $C(0.3\ \text{mm})$ to reach 0.6%C.

Approach. Apply the standard semi-infinite-solid solution to Fick's second law, $\dfrac{C_s-C_x}{C_s-C_0}=\text{erf}\!\left(\dfrac{x}{2\sqrt{Dt}}\right)$ (appendix), reading/interpolating the appendix erf table.

  1. Part (i) — compute the erf argument. $$\sqrt{Dt_1} = \sqrt{(0.298\times10^{-6})(36{,}000)} = \sqrt{0.010728} = 0.10358\ \text{cm}$$ $$z_1 = \frac{x}{2\sqrt{Dt_1}} = \frac{0.03}{2(0.10358)} = 0.1448$$
  2. Read/interpolate erf$(z_1)$. From the appendix table, $\text{erf}(0.10)=0.1125$ and $\text{erf}(0.15)=0.1680$; interpolating at $z_1=0.1448$ (fraction 0.897 of the way from 0.10 to 0.15): $$\text{erf}(0.1448) \approx 0.1125+0.897(0.1680-0.1125) = 0.1623$$
  3. Solve for $C_x$. $$\frac{1.0-C_x}{1.0-0.2} = 0.1623 \ \Rightarrow\ 1.0-C_x = 0.1623(0.8) = 0.1298$$ $$C_x = \boxed{0.870\ \%\text{C}}$$
  4. Part (ii) — set up for $C_x=0.6\%$ at the same depth. $$\frac{C_s-C_x}{C_s-C_0} = \frac{1.0-0.6}{1.0-0.2} = 0.500 = \text{erf}(z_2)$$ From the appendix table, $\text{erf}(0.45)=0.4755$ and $\text{erf}(0.50)=0.5205$; interpolating for $\text{erf}(z_2)=0.500$ (fraction 0.544): $$z_2 \approx 0.45+0.544(0.05) = 0.477$$
  5. Solve for $t_2$. Re-arranging $z_2=x/(2\sqrt{Dt_2})$: $$\sqrt{Dt_2} = \frac{x}{2z_2} = \frac{0.03}{2(0.477)} = 0.03145\ \text{cm} \ \Rightarrow\ Dt_2 = 9.89\times10^{-4}\ \text{cm}^2$$ $$t_2 = \frac{9.89\times10^{-4}}{0.298\times10^{-6}} = 3319\ \text{s} = \boxed{0.922\ \text{h}\ (\approx 55.3\ \text{min})}$$

Part (ii)'s answer being less than the 10 h of part (i) is the expected direction: 0.6%C is a smaller carbon pickup than the 0.87%C already reached after 10 h at that depth, so the shallower target is met sooner.

Question VI — final results
QuantityValue
$C$ at 0.3 mm after 10 h0.870 %C
Time for $C=0.6\%$ at 0.3 mm3319 s = 0.922 h (≈55.3 min)