17-Phys-B7 Structure of Materials · May 2013
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Paper format. 98-Phys-B7 Structure of Materials, National Examination May 2013 — a closed-book examination (Casio or Sharp approved calculators only; all necessary equations, constants and diagrams supplied in the paper's own appendix). Candidates attempt any five of the eight questions, each worth 20 marks; every question is nonetheless answered in full below so the paper remains a complete study resource.
Reference texts. W. D. Callister Jr. & D. G. Rethwisch, Materials Science and Engineering: An Introduction, 10th ed. (atomic bonding, crystal structure and packing, point defects, diffusion, dislocations and slip, mechanical properties, phase diagrams and the lever rule, precipitation hardening, X-ray diffraction); D. J. Griffiths, Introduction to Quantum Mechanics, 3rd ed. (de Broglie wavelength, Heisenberg uncertainty).
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.
Part 1 — Given. Al-Si eutectic phase diagram (from the exam appendix): eutectic at 577°C, 12.6 wt% Si; maximum solubility of Si in $\alpha$ (Al-rich solid solution) at the eutectic temperature, 1.65 wt% Si; $\beta$ (Si-rich solid solution) essentially pure, solidus at 99.8 wt% Si; alloy composition 50 wt% Si, cooled slowly from 1200°C.
Find. (a) first-solid temperature, (b) first-solid composition, (c) last-liquid composition, (d) last-liquid solidification temperature.
Approach. The 50 wt% Si alloy is Si-rich of the eutectic (12.6 wt%), so on cooling from an all-liquid state it enters the $\beta+L$ two-phase field first; the liquidus temperature at 50 wt% Si (read from the printed curve, calibrated against the diagram's own labelled points) fixes (a), and the tie-line end-points there and at the eutectic isotherm answer (b)–(d) directly from the printed diagram values.
[Figure not reproduced: Al-Si eutectic phase diagram, redrawn from the exam figure, with the tie-line construction for the 50 wt% Si alloy at its liquidus (blue) and the eutectic isotherm (red) marked. See the official exam paper.]
Part 2(a) — Given. The Al-rich $\alpha$ solvus meets the eutectic isotherm at 1.65 wt% Si (577°C), and the solubility of Si in $\alpha$ falls with decreasing temperature (the solvus line drawn sloping toward the Al axis).
Find. The maximum Si content for which an Al-Si alloy is age-hardenable.
Precipitation (age) hardening needs a solvus whose solubility decreases with falling temperature, so that a composition solutionized as single-phase $\alpha$ at high temperature can be quenched into a supersaturated solid solution and then aged to precipitate a fine, hardening dispersion of $\beta$. That mechanism is only available up to the composition where the alloy is still single-phase $\alpha$ just below the eutectic temperature — i.e. up to the maximum solid solubility itself, $$\boxed{1.65\ \text{wt\%\ Si}}.$$ Beyond this composition, the alloy enters the $\alpha+\beta$ two-phase field immediately below the eutectic isotherm with no single-phase $\alpha$ solutionizing window available.
Part 2(b). Choosing an Al–1.0 wt%Si alloy (comfortably inside the 1.65 wt% age-hardenable limit) as a concrete example, a standard three-stage schedule is: (i) solutionize at a temperature just below the solvus/eutectic line, e.g. ≈550–560°C, held long enough (several hours) to dissolve all $\beta$ into a homogeneous single-phase $\alpha$; (ii) quench rapidly (water quench) to room temperature, suppressing diffusion so the alloy is trapped as a supersaturated solid solution (SSSS) — still single-phase $\alpha$, but now carrying far more Si than room-temperature equilibrium solubility allows; (iii) age (reheat) at an intermediate temperature, e.g. ≈170–180°C for several hours, to let fine $\beta$ (Si-rich) precipitates nucleate and grow throughout the $\alpha$ matrix, which is what produces the hardening — overaging past the optimum time coarsens the precipitates and softens the alloy again.
Part 2(c). The three microstructures below correspond to the same three stages: solutionized (uniform single-phase $\alpha$ grains, no visible second phase); quenched (still visually single-phase $\alpha$ — the supersaturation is not resolvable optically, only by the elevated hardness/lattice strain it carries); reheated/aged (a fine, dispersed population of $\beta$ precipitates throughout each $\alpha$ grain, which is what pins dislocations and raises the strength).
Part 3. Following the same Liquid $\leftrightarrow$ Solid 1 + Solid 2 pattern given for the eutectic reaction, the three related invariant reactions are written:
| Reaction | General form |
|---|---|
| Eutectic (given) | $L\leftrightarrow S_1+S_2$ |
| Eutectoid | $S_1\leftrightarrow S_2+S_3$ |
| Peritectic | $L+S_1\leftrightarrow S_2$ |
| Monotectic | $L_1\leftrightarrow S_1+L_2$ |
The eutectoid reaction is the solid-state analogue of the eutectic: one solid phase transforms isothermally, on cooling, into two different solid phases (e.g. the classic $\gamma\leftrightarrow\alpha+\text{Fe}_3\text{C}$ reaction in the Fe-C system). The peritectic reaction runs the eutectic pattern with one fewer degree of freedom on the liquid side: an existing solid combines with the remaining liquid, on cooling, to form a single new solid phase. The monotectic reaction is the odd one out, involving two liquids: one liquid phase separates, on cooling, into a solid phase and a second, compositionally distinct liquid phase.
| Quantity | Value |
|---|---|
| First-solid temperature (50 wt% Si) | ≈971°C |
| First-solid composition | ≈99.8 wt% Si ($\beta$) |
| Last-liquid composition | 12.6 wt% Si |
| Last-liquid solidification temperature | 577°C |
| Max. age-hardenable composition | 1.65 wt% Si |