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17-Phys-B7 Structure of Materials · December 2016

Question 1 of 7: Electron Structure

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

Notes on this paper

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 I: Electron Structure (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.

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.

  1. Level energies. $E_4=-13.6/4^2=-0.850\ \text{eV}$, $E_3=-13.6/3^2=-1.511\ \text{eV}$.
  2. Energy change. $$\Delta E=E_3-E_4=-1.511-(-0.850)=\boxed{-0.661\ \text{eV}}.$$ The negative sign means the atom loses energy: the electron drops from the higher energy level ($n=4$) to the lower energy level ($n=3$), so a photon of energy $0.661$ eV is emitted, not absorbed.

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.

Check: the printed frequency for this illustrative "tungsten filament" quantum is literally $f=1\ \text{Hz}$, many orders of magnitude below the thermal/visible frequencies a real heated filament radiates at ($\sim10^{14}\ \text{Hz}$). The sub-part is read as a direct formula-application exercise (Planck's relation $E=hf$ and $c=\lambda f$), exactly as printed, per the paper's own instruction to state any assumption when a value looks unusual.
  1. Quantum energy. $$E=hf=6.63\times10^{-34}\times1=\boxed{6.63\times10^{-34}\ \text{J}}.$$
  2. Wavelength. $$\lambda=\frac{c}{f}=\frac{3.00\times10^{8}}{1} =\boxed{3.00\times10^{8}\ \text{m}}.$$ (For scale, this "wavelength" is comparable to the Earth–Moon distance—a direct consequence of using an everyday, non-thermal frequency in the formula.)

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.

  1. de Broglie wavelength. $v=c/6=5.00\times10^{7}\ \text{m/s}$, $p=m_ev=9.11\times10^{-31}\times5.00\times10^{7}=4.555\times10^{-23}\ \text{kg}\cdot\text{m/s}$. $$\lambda_{dB}=\frac{h}{p}=\frac{6.63\times10^{-34}}{4.555\times10^{-23}} =\boxed{1.456\times10^{-11}\ \text{m}=14.56\ \text{pm}}.$$
  2. Position uncertainty. $\Delta x=0.01\times1.456\times10^{-11} =1.456\times10^{-13}\ \text{m}$.
  3. Minimum speed uncertainty. Using $\Delta x\,\Delta p\ge h/(4\pi)$, $$\Delta p_{\min}=\frac{h}{4\pi\,\Delta x}=\frac{6.63\times10^{-34}}{4\pi\times1.456\times10^{-13}} =3.62\times10^{-22}\ \text{kg}\cdot\text{m/s},$$ $$\Delta v_{\min}=\frac{\Delta p_{\min}}{m_e}=\boxed{3.98\times10^{8}\ \text{m/s}}.$$
Check: $\Delta v_{\min}\approx1.33\,c$—the non-relativistic Heisenberg calculation formally exceeds the speed of light. This is the point the sub-part is testing: confining an electron to $1\%$ of its own (already sub-atomic, $14.6$ pm) de Broglie wavelength demands a momentum uncertainty so large that the resulting speed uncertainty is unphysical, illustrating just how tightly the uncertainty principle constrains simultaneous knowledge of an electron's position and speed at atomic length scales.
Final results — Question I
QuantityValue
$\Delta E$ ($n=4\to3$)$-0.661$ 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
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