21-Mat-A4 Deformation Behaviour and Properties of Materials · May 2016
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Paper format. National Exams, May 2016 — 10-Met-A4, Structure of Materials. Three hours, closed book, one approved calculator (Casio or Sharp). Eight questions of 20 marks each (Roman numerals I–VIII); the rubric asks for any five, with only the first five in the answer book marked. All eight are solved here, because this set is a study resource rather than an exam script. All necessary equations, constants and an error-function table are provided in the exam's own appendix (reproduced where used below).
Note on the exam title. The printed exam header reads 10-Met-A4, Structure of Materials. Only Question VIII (mechanical deformation) is genuinely deformation/mechanical-properties content; the paper as a whole is a broad introductory materials-science survey — bonding, crystal structure, crystallographic directions/planes, imperfections, phase diagrams, XRD and diffusion — and is answered as such below.
Reference texts. The answers below are keyed to the works normally recommended for this syllabus code:
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.
In the standard perovskite setting, Ba²⁺ occupies the 8 cube corners (each shared 1/8, giving 1 Ba/cell), Ti⁴⁺ occupies the body centre (coordination 6, octahedrally surrounded by O²⁻, giving 1 Ti/cell), and O²⁻ occupies the 6 face centres (each shared 1/2, giving 3 O/cell). Formula check: Ba₁Ti₁O₃ — matches BaTiO₃. The O²⁻ face-centre positions alone do form an FCC sub-lattice, as stated in the question; adding the corner Ba²⁺ and body-centre Ti⁴⁺ on top of that FCC anion array is exactly the perovskite structure.
Given. $A_{Ba}=137$, $A_{Ti}=48$, $A_O=16$ g/mol; $\rho=6\ \text{g/cm}^3$; $Z=1$ formula unit per cell.
Find. Lattice parameter $a$.
Approach. $\rho=ZM/(a^3N_A)$, so $a=\left(ZM/(\rho N_A)\right)^{1/3}$, with $M$ the BaTiO₃ formula weight.
0.401 nm is close to the accepted room-temperature (cubic, above the 130°C Curie point) BaTiO₃ lattice parameter of 0.403 nm — a sound check on the given density.
Approach. Shifting the coordinate origin by $(\tfrac12,\tfrac12,\tfrac12)$ (i.e. re-choosing which lattice point is labelled "corner") moves every ion by that same vector, mod 1, without changing the physical crystal at all.
| Quantity | Value |
|---|---|
| Formula weight, $M$ | 233 g/mol |
| Lattice parameter, $a$ | 0.401 nm |
| Alt. origin: Ti positions | 8 cube corners |
| Alt. origin: O positions | 12 edge centres |