17-Phys-B7 Structure of Materials · December 2016
Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)
Paper format. 98-Phys-B7 Structure of Materials, National Examination December 2016 — a closed-book examination (Casio or Sharp approved calculators only; all necessary equations, constants, the error-function table and the Cu–Ag phase diagram are supplied in the paper's own appendix). Candidates attempt any five of the seven questions, each worth 20 marks; every question is nonetheless answered in full below so the paper remains a complete study resource. This sitting numbers its questions with Roman numerals (Question I–VII) while sub-items inside each question use Arabic numerals (1., 2., 3.).
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, X-ray diffraction); D. J. Griffiths, Introduction to Quantum Mechanics, 3rd ed. (Bohr model, 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. Three organizing principles for how electrons fill the atomic energy levels of a many-electron atom:
a. Aufbau principle. Electrons fill the available orbitals starting from the lowest energy orbital upward, so the ground-state configuration is built one electron at a time into the lowest still-vacant state. Example: carbon ($Z=6$) fills $1s^2\,2s^2\,2p^2$—$1s$ and $2s$ are completely filled before any electron enters $2p$.
b. Pauli's exclusion principle. No two electrons in the same atom may share an identical set of all four quantum numbers ($n,\ell,m_\ell,m_s$); an orbital (fixed $n,\ell,m_\ell$) therefore holds at most two electrons, and only if their spins are opposite. Example: the $1s$ orbital of helium holds exactly two electrons, $1s^2$, with $m_s=+1/2$ and $m_s=-1/2$—a third electron cannot enter $1s$.
c. Electronegativity. A relative measure of how strongly an atom attracts the shared electron pair of a covalent bond toward itself. Example: in H–F, fluorine ($\chi\approx 4.0$) is far more electronegative than hydrogen ($\chi\approx 2.1$), so the bonding electron density is pulled toward F, giving the molecule a permanent dipole (polar covalent bond).
Part 2 — Given. Hydrogen atom, transition $n_i=4\to n_f=3$, Bohr energy levels $E_n=-13.6\,\text{eV}/n^2$.
Find. $\Delta E$ for the transition, and whether the photon is absorbed or emitted.
Part 3(a) — Given. Radiation frequency $f=1\ \text{Hz}$ (as printed on the exam), $h=6.63\times10^{-34}\ \text{J}\cdot\text{s}$, $c=3.00\times10^{8}\ \text{m/s}$.
Find. The energy of a single quantum, and its wavelength.
Part 3(b) — Given. Electron speed $v=c/6$; position uncertainty $\Delta x=1\%$ of the electron's own de Broglie wavelength $\lambda_{dB}$ (the only length scale the sub-part establishes, via the de Broglie question asked immediately before it).
Find. What de Broglie's hypothesis states, and the minimum uncertainty in the electron's speed, $\Delta v_{\min}$.
de Broglie's hypothesis: every moving particle has an associated wave of wavelength $\lambda=h/p$, where $p=mv$ is its momentum—matter, not just light, exhibits wave–particle duality.
| Quantity | Value |
|---|---|
| $\Delta E$ ($n=4\to3$) | $-0.661$ eV (emitted) |
| Quantum energy, $f=1$ Hz | $6.63\times10^{-34}$ J |
| Wavelength, $f=1$ Hz | $3.00\times10^{8}$ m |
| $\lambda_{dB}$ (electron, $v=c/6$) | $1.456\times10^{-11}$ m |
| $\Delta v_{\min}$ | $3.98\times10^{8}$ m/s |