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Atomic Structure and Atomic Theory — Diagnostic Tests

Unit Tests

UT-1: Electron Configuration Exceptions

Question: Write the ground-state electron configurations for chromium (Z=24Z = 24) and copper (Z=29Z = 29). Explain why neither follows the expected aufbau filling order, referring to the relative stability of half-filled and fully filled dd-subshells.

Solution: Chromium: expected [Ar]4s23d4[Ar]\, 4s^2\, 3d^4, actual [Ar]4s13d5[Ar]\, 4s^1\, 3d^5. Copper: expected [Ar]4s23d9[Ar]\, 4s^2\, 3d^9, actual [Ar]4s13d10[Ar]\, 4s^1\, 3d^{10}.

The 4s4s orbital is filled before 3d3d according to aufbau, but once electrons occupy the 3d3d subshell, the 3d3d orbital drops in energy below 4s4s. A half-filled dd-subshell (d5d^5) has extra exchange energy (five unpaired electrons, each with parallel spin), which lowers the total energy. A fully filled d10d^{10} subshell has a symmetric spherically averaged charge distribution that minimises electron-electron repulsion. In Cr, promoting one 4s4s electron to 3d3d gives d5d^5 (half-filled) for a net energy gain. In Cu, promoting one 4s4s electron to 3d3d gives d10d^{10} (fully filled) for a net energy gain.


UT-2: Quantum Numbers and Orbital Maximums

Question: State the four quantum numbers (nn, \ell, mm_\ell, msm_s) for each electron in a 2p42p^4 configuration. How many electrons maximum can occupy the n=3n = 3 shell, and why?

Solution: The 2p2p subshell has n=2n = 2, =1\ell = 1, m{1,0,+1}m_\ell \in \{-1, 0, +1\}, ms=±12m_s = \pm \tfrac{1}{2}. With four electrons, applying Hund's rule (maximum multiplicity first):

Electronnn\ellmm_\ellmsm_s
121+1+12+\tfrac{1}{2}
2210+12+\tfrac{1}{2}
321-1+12+\tfrac{1}{2}
421+112-\tfrac{1}{2}

The n=3n = 3 shell has subshells 3s3s (=0\ell = 0, 2 electrons), 3p3p (=1\ell = 1, 6 electrons), and 3d3d (=2\ell = 2, 10 electrons). Maximum capacity: 2+6+10=182 + 6 + 10 = 18 electrons.


UT-3: Isotopic Abundance and Relative Atomic Mass

Question: Naturally occurring chlorine has two stable isotopes: 35Cl^{35}\text{Cl} (34.969 u) and 37Cl^{37}\text{Cl} (36.966 u). The relative atomic mass of chlorine is 35.453 u. Calculate the percentage abundance of each isotope to three significant figures.

Solution: Let xx be the fraction of 35Cl^{35}\text{Cl}. Then 1x1 - x is the fraction of 37Cl^{37}\text{Cl}.

34.969x+36.966(1x)=35.45334.969x + 36.966(1 - x) = 35.453

34.969x+36.96636.966x=35.45334.969x + 36.966 - 36.966x = 35.453

1.997x=35.45336.966=1.513-1.997x = 35.453 - 36.966 = -1.513

x=1.5131.997=0.7576x = \frac{1.513}{1.997} = 0.7576

35Cl^{35}\text{Cl}: 75.8%75.8\%, 37Cl^{37}\text{Cl}: 24.2%24.2\%.

Integration Tests

Question: Explain why the first ionisation energy of aluminium (1090 kJ mol11090\ \text{kJ mol}^{-1}) is lower than that of magnesium (1097 kJ mol11097\ \text{kJ mol}^{-1}), even though aluminium has a greater nuclear charge. Then explain why the first ionisation energy of sulfur (1000 kJ mol11000\ \text{kJ mol}^{-1}) is lower than that of phosphorus (1012 kJ mol11012\ \text{kJ mol}^{-1}).

Solution: Both anomalies arise from the stability of half-filled and fully filled subshells.

Magnesium has the configuration [Ne]3s2[Ne]\, 3s^2 -- the 3s3s subshell is fully filled, which is a relatively stable arrangement. Aluminium has [Ne]3s23p1[Ne]\, 3s^2\, 3p^1; the 3p3p electron is in a higher-energy subshell that is also more effectively shielded (penetration effect of s>ps \gt p). Despite the extra proton in Al, the electron being removed is from a higher-energy pp orbital with greater average distance from the nucleus, so less energy is required.

Phosphorus has [Ne]3s23p3[Ne]\, 3s^2\, 3p^3: three unpaired electrons in three separate pp orbitals (Hund's rule), giving a half-filled pp-subshell with extra exchange stability. Sulfur has [Ne]3s23p4[Ne]\, 3s^2\, 3p^4: the fourth pp electron must pair with another electron in one of the pp orbitals. The pairing introduces additional electron-electron repulsion, making this electron easier to remove.


IT-2: Emission Spectra and Energy Levels (with Measurement and Data Processing)

Question: A hydrogen emission line has a wavelength of 434.0 nm434.0\ \text{nm}. Calculate the energy of one photon of this light, determine the transition responsible (express your answer as ninfn_i \to n_f), and calculate the uncertainty in the energy if the wavelength measurement has an uncertainty of ±0.5 nm\pm 0.5\ \text{nm}.

Solution:

Energy: E=hcλ=(6.626×1034)(2.998×108)434.0×109=4.576×1019 JE = \frac{hc}{\lambda} = \frac{(6.626 \times 10^{-34})(2.998 \times 10^8)}{434.0 \times 10^{-9}} = 4.576 \times 10^{-19}\ \text{J}.

Converting to eV: E=4.576×10191.602×1019=2.857 eVE = \frac{4.576 \times 10^{-19}}{1.602 \times 10^{-19}} = 2.857\ \text{eV}.

The Balmer series has nf=2n_f = 2. The energy of level nn is En=13.6/n2 eVE_n = -13.6/n^2\ \text{eV}.

E2=13.6/4=3.40 eVE_2 = -13.6/4 = -3.40\ \text{eV}. The photon energy corresponds to ΔE=2.857 eV\Delta E = 2.857\ \text{eV}.

Ei=Ef+ΔE=3.40+2.857=0.543 eVE_i = E_f + \Delta E = -3.40 + 2.857 = -0.543\ \text{eV}.

ni=13.6/0.543=25.045n_i = \sqrt{13.6/0.543} = \sqrt{25.04} \approx 5. The transition is n=5n=2n = 5 \to n = 2.

Uncertainty: ΔEE=Δλλ\frac{\Delta E}{E} = \frac{\Delta\lambda}{\lambda} (from E1/λE \propto 1/\lambda, so ΔE=hcΔλλ2\Delta E = \frac{hc\,\Delta\lambda}{\lambda^2}).

ΔE=hc×0.5×109(434.0×109)2=9.936×10341.884×1013=5.27×1021 J0.033 eV\Delta E = \frac{hc \times 0.5 \times 10^{-9}}{(434.0 \times 10^{-9})^2} = \frac{9.936 \times 10^{-34}}{1.884 \times 10^{-13}} = 5.27 \times 10^{-21}\ \text{J} \approx 0.033\ \text{eV}.


IT-3: Electron Configuration and Chemical Properties (with Chemical Bonding)

Question: Sodium (Z=11Z = 11) readily forms Na+\text{Na}^+, whereas neon (Z=10Z = 10) is chemically inert. Use electron configuration and ionisation energy data to explain this difference. The first three ionisation energies of sodium are 496496, 45624562, and 6912 kJ mol16912\ \text{kJ mol}^{-1}. What do these values reveal about the stability of the Na+\text{Na}^+ ion?

Solution: Na: [Ne]3s1[Ne]\, 3s^1. Ne: 1s22s22p6=[Ne]1s^2\, 2s^2\, 2p^6 = [Ne].

Neon has a complete octet in the n=2n = 2 shell -- all subshells are fully filled. Removing an electron from a filled 2p2p orbital requires breaking into a stable noble gas configuration, resulting in a very high first ionisation energy (2081 kJ mol12081\ \text{kJ mol}^{-1}). Neon therefore has no tendency to lose or gain electrons under normal conditions.

Sodium has a single 3s3s electron outside a filled [Ne][Ne] core. This valence electron is far from the nucleus and well-shielded by the inner 10 electrons. The first ionisation energy (496 kJ mol1496\ \text{kJ mol}^{-1}) is relatively low, so Na readily loses this electron to form Na+\text{Na}^+, achieving the stable [Ne][Ne] configuration.

The huge jump between the first (496496) and second (45624562) ionisation energies confirms that removing the first electron is easy but removing a second electron requires breaking into the stable [Ne][Ne] core. The ratio 4562/4969.24562/496 \approx 9.2 shows that Na+\text{Na}^+ is highly stable -- it is extremely energetically unfavourable to form Na2+\text{Na}^{2+}.