Standard difficulty · 20 questions · 40 marks
Show your working for Sections B and C. Answers are on the last page — try every question first!
Structure of Atom · AW-11C-SOA-2026-V1 · For parents — fold back or tear off before handing the sheet to your child.
| Q | Answer | Working |
|---|---|---|
| 1 | (d) J. J. Thomson | — |
| 2 | (a) 10 | Z = 12, A = 24: protons 12, neutrons 24 − 12 = 12, electrons 12 − 2 = 10 |
| 3 | (d) 4.97 × 10−19 J | E = hc/λ, with λ in metres |
| 4 | (a) n = 1, l = 2, mₗ = +1, mₛ = +½ | l must be less than n (here l = 2, n = 1) |
| 5 | (a) Balmer series (visible) | the series is named by the lower level, n = 2 |
| 6 | (c) 0 | total nodes = n − 1 |
| 7 | (a) [Ar] 3d10 4s2 4p5 | fill by the (n + l) rule: 1s 2s 2p 3s 3p 4s 3d 4p |
| 8 | (d) A is false, but R is true. | A is false: [Ar] 3d10 4s1: 1 unpaired. R is true. |
| 9 | Electrons enter the orbitals of a subshell singly, with parallel spins, before any pairing begins. | — |
| 10 | ν = 6.00 × 1014 Hz; ν̄ = 2.00 × 106 m−1 | ν = c/λ; ν̄ = 1/λ (λ in metres) |
| 11 | 2.04 × 10−18 J | ΔE = 2.18 × 10−18 (1/12 − 1/42) |
| 12 | ν̄ = 15,232.92 cm−1; λ = 656.47 nm (Balmer series) | ν̄ = R(1/22 − 1/32); λ = 1/ν̄ (1 cm = 107 nm) |
| 13 | 8.28 × 10−35 m | λ = h/(mv), with m in kg; far too small to observe |
| 14 | 6.54 × 1019 | number = total energy ÷ hc/λ |
| 15 | n = 4, l = 3; mₗ = −3, −2, −1, 0, +1, +2, +3; 7 orbitals; 14 electrons | l = 3 for f; mₗ from −l to +l |
| 16 | W0 = 3.313 × 10−19 J; KE = 5.301 × 10−19 J | W0 = hν0; KE = h(ν − ν0) |
| 17 | A thin gold foil was bombarded with α-particles. Most passed straight through, a few were deflected through small angles, and very few (about 1 in 20,000) bounced back. So most of the atom is empty space, with its positive charge and almost all its mass in a tiny nucleus; electrons move around it. Drawback: an electron moving in a circle should radiate energy and spiral into the nucleus, so the model cannot explain the stability of the atom (or line spectra). | — |
| 18 | (a) 3.03 × 10−19 J; (b) 656.52 nm; (c) Balmer series, visible | ΔE = 2.18 × 10−18 (1/n12 − 1/n22); λ = hc/ΔE |
| 19 | (a) 1s2 2s2 2p6 3s2 3p6 3d10 4s2 4p4; (b) 2; (c) 16; (d) 18; (e) 4p | Aufbau order; Hund’s rule for unpaired electrons |
| 20 | (a) electrons 36, protons 35, neutrons 44; (b) bromine: 7935Br− | if electrons = x, neutrons = x(1 + 22.22/100) and protons = x − 1; protons + neutrons = 79 |