Bohr's Atomic Model & Energy Levels
Limitations of Rutherford's Model
Rutherford's nuclear model could not explain why electrons don't radiate energy and spiral into the nucleus, nor why atoms emit light only at specific wavelengths. Niels Bohr (1913) proposed a modified model to address these issues.
Bohr's Postulates
- Electrons orbit the nucleus in fixed circular paths called shells (energy levels), labelled n = 1, 2, 3, 4…
- While in an allowed orbit, an electron does not radiate energy — it stays at constant energy.
- Each shell has a fixed energy. Higher n = higher energy = further from nucleus.
- An electron moves between shells by absorbing or emitting a photon of energy exactly equal to the energy difference: ΔE = hf.
Section 2.1 — Shells & Subshells
10 QuestionsThe maximum number of electrons in the second shell (n=2) is:
The subshell with l=1 is:
Maximum electrons in the 3d subshell:
The Aufbau principle states electrons:
Hund's rule states that in degenerate orbitals, electrons:
The Pauli exclusion principle states:
Electron configuration of Na (Z=11):
Why does 4s fill before 3d?
Electron configuration of Cl (Z=17):
Number of unpaired electrons in carbon (Z=6):
Hydrogen Spectrum & Spectral Lines
Emission Spectrum of Hydrogen
When hydrogen is excited (electrical discharge or heat), electrons are promoted to higher levels. As they fall back, they emit photons of specific frequencies producing a line emission spectrum — bright coloured lines on a dark background. Each line corresponds to electrons falling from n₂ to n₁.
| Series | Transition | Region |
|---|---|---|
| Lyman | n ≥ 2 → n=1 | Ultraviolet (UV) |
| Balmer | n ≥ 3 → n=2 | Visible light |
| Paschen | n ≥ 4 → n=3 | Infrared (IR) |
| Brackett | n ≥ 5 → n=4 | Infrared (IR) |
Convergence and Ionisation Energy
As n increases, energy levels get closer together — spectral lines converge. At the convergence limit (n → ∞), the electron is completely removed. The frequency at convergence gives the ionisation energy directly:
Section 2.2 — Electronic Configurations & The Periodic Table
10 QuestionsElements in the same group have the same:
Cr (Z=24) has configuration [Ar]3d⁵4s¹ rather than [Ar]3d⁴4s². Why?
Which block of the periodic table contains elements with outermost electrons in d orbitals?
The electron configuration [Ar]3d⁶4s² belongs to:
How many electrons does a 4p subshell hold?
The ground state of Cu (Z=29) is:
In which period would an element with configuration 1s²2s²2p⁶3s²3p⁶4s² be placed?
How many orbitals in the 3d subshell?
An element has config 1s²2s²2p⁶3s²3p⁶3d¹⁰4s²4p⁵. It is in Group:
When transition metal atoms form ions, which electrons are removed first?
Atomic Spectra
Evidence for Quantised Energy Levels
Discrete spectral lines (not a continuous spectrum) are direct evidence that electrons can only exist at specific, quantised energy levels. If energy were continuous, a continuous spectrum would result. Only certain wavelengths being emitted proves energy levels are discrete.
Orbitals & Quantum Numbers
Quantum Mechanical Model
Bohr's circular orbits were replaced by the quantum mechanical model. Electrons do not follow defined paths — instead we describe regions of space where there is high probability of finding an electron: atomic orbitals. Each orbital holds a maximum of 2 electrons (opposite spins).
| Quantum Number | Symbol | Describes | Values |
|---|---|---|---|
| Principal | n | Shell (energy level), distance from nucleus | 1, 2, 3, 4… |
| Angular momentum | l | Subshell (orbital shape) | 0 to (n−1) |
| Magnetic | mₗ | Orbital orientation in space | −l to +l |
| Spin | mₛ | Electron spin direction | +½ or −½ |
| l value | Subshell | Shape | Orbitals | Max e⁻ |
|---|---|---|---|---|
| 0 | s | Spherical | 1 | 2 |
| 1 | p | Dumbbell (3 orientations) | 3 | 6 |
| 2 | d | Double dumbbell (5 orientations) | 5 | 10 |
| 3 | f | Complex (7 orientations) | 7 | 14 |
| Shell (n) | Subshells | Total orbitals | Max electrons (2n²) |
|---|---|---|---|
| n=1 | 1s | 1 | 2 |
| n=2 | 2s, 2p | 4 | 8 |
| n=3 | 3s, 3p, 3d | 9 | 18 |
| n=4 | 4s, 4p, 4d, 4f | 16 | 32 |
Three Rules for Filling Orbitals
1. Aufbau Principle — fill in order of increasing energy:
2. Pauli Exclusion Principle — no two electrons in the same atom can have identical quantum numbers. Each orbital holds max 2 electrons with opposite spins (↑↓).
3. Hund's Rule — electrons fill degenerate orbitals singly with parallel spins before any pairing occurs. Minimises repulsion.
Electronic Configuration of Atoms & Ions
Writing Electron Configurations
List each subshell and its electron count: e.g., 1s²2s²2p⁶. Shorthand uses the previous noble gas: Na = [Ne]3s¹.
| Element | Z | Configuration | Shorthand |
|---|---|---|---|
| H | 1 | 1s¹ | — |
| He | 2 | 1s² | — |
| Li | 3 | 1s²2s¹ | [He]2s¹ |
| C | 6 | 1s²2s²2p² | [He]2s²2p² |
| N | 7 | 1s²2s²2p³ | [He]2s²2p³ |
| O | 8 | 1s²2s²2p⁴ | [He]2s²2p⁴ |
| Ne | 10 | 1s²2s²2p⁶ | — |
| Na | 11 | 1s²2s²2p⁶3s¹ | [Ne]3s¹ |
| Mg | 12 | 1s²2s²2p⁶3s² | [Ne]3s² |
| Al | 13 | 1s²2s²2p⁶3s²3p¹ | [Ne]3s²3p¹ |
| P | 15 | 1s²2s²2p⁶3s²3p³ | [Ne]3s²3p³ |
| S | 16 | 1s²2s²2p⁶3s²3p⁴ | [Ne]3s²3p⁴ |
| Ar | 18 | 1s²2s²2p⁶3s²3p⁶ | — |
| K | 19 | …3p⁶4s¹ | [Ar]4s¹ |
| Ca | 20 | …3p⁶4s² | [Ar]4s² |
| Fe | 26 | …3d⁶4s² | [Ar]3d⁶4s² |
| Cr* | 24 | …3d⁵4s¹ | [Ar]3d⁵4s¹ |
| Cu* | 29 | …3d¹⁰4s¹ | [Ar]3d¹⁰4s¹ |
| Zn | 30 | …3d¹⁰4s² | [Ar]3d¹⁰4s² |
Ion Electron Configurations
Cations: remove electrons from the highest energy subshell first. For transition metals, remove 4s before 3d.
Anions: add electrons to the next available subshell.
Ion Configurations
Fe²⁺: remove 2×4s → [Ar]3d⁶
Fe³⁺: remove 2×4s + 1×3d → [Ar]3d⁵
O²⁻: add 2e⁻ to 2p → 1s²2s²2p⁶ (isoelectronic with Ne)
Cu²⁺: remove 4s¹ + one 3d → [Ar]3d⁹
Box Notation (Orbital Diagrams)
Arrows (↑ = spin up, ↓ = spin down) in boxes represent electrons in orbitals. Demonstrates Hund's rule clearly.
Ionisation Energy, Energy Levels & Influencing Factors
X(g) → X⁺(g) + e⁻ ΔH = IE₁ (always positive — endothermic)
| Factor | Effect | Explanation |
|---|---|---|
| Nuclear charge (Z) | ↑Z → ↑IE | More protons attract electrons more strongly. |
| Distance from nucleus | ↑distance → ↓IE | Outer electrons further away feel weaker attraction. |
| Shielding | ↑shielding → ↓IE | Inner electrons reduce effective nuclear charge felt by outer electrons. |
| Paired electron repulsion | Paired → ↓IE | Electrons paired in the same orbital repel each other — easier to remove one. |
Trends in First Ionisation Energy
Across a period (left → right): IE₁ generally increases — Z increases while shielding stays roughly constant → greater effective nuclear charge → stronger hold on outer electrons.
Anomalous dips across Period 2/3:
- Group 2 → Group 13 dip (Be→B, Mg→Al): Group 13 outer electron is in a higher-energy p subshell, shielded by the s electrons → easier to remove despite higher Z.
- Group 15 → Group 16 dip (N→O, P→S): Group 16 has a paired p electron; repulsion between paired electrons makes it easier to remove one → IE₁(O) < IE₁(N).
Down a group: IE₁ decreases — each new period adds a shell, increasing distance and shielding → outer electron easier to remove.
Successive IEs and Shell Structure
A plot of log(IE) vs ionisation number shows large jumps when removal crosses into an inner shell. These jumps confirm the number of electrons in each shell.
Sodium (Na, Z=11, config 2,8,1):
Identifying an Element from Successive IEs
Section 2.3 — Ionisation Energies
10 QuestionsFirst ionisation energy is defined as:
Down Group 1, first ionisation energy:
The large jump between 2nd and 3rd ionisation energies of Na indicates:
Across Period 3, the general trend in first ionisation energy is:
Why is IE₁(Mg) > IE₁(Al)?
Successive ionisation energies always:
Which element has successive IEs of 786, 1577, 3232, 4356 kJ/mol? (Big jump between 2nd and 3rd)
Effective nuclear charge (Zeff) is:
Why does shielding by electrons in the same shell provide less shielding than inner shell electrons?
An element has successive IEs (kJ/mol): 1000, 2260, 3390, 4540, 6950... Big jump between 4th and 5th. The element is in Group:
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Exercises
- State Bohr's three postulates about electron behaviour. What evidence from atomic spectra supports quantised energy levels?
(1) Electrons orbit in fixed shells (n=1,2,3…) without radiating energy. (2) Each shell has a fixed energy; higher n = higher energy. (3) Electrons move between levels by absorbing/emitting photons of energy ΔE=hf. Evidence: Only specific wavelengths are observed (line spectrum, not continuous). This proves electrons occupy discrete energy levels — only certain transitions are possible, each producing one specific photon frequency.
- Write the full electron configurations for: (a) S (Z=16), (b) Fe (Z=26), (c) Br (Z=35).
(a) S: 1s²2s²2p⁶3s²3p⁴
(b) Fe: 1s²2s²2p⁶3s²3p⁶3d⁶4s²
(c) Br: 1s²2s²2p⁶3s²3p⁶3d¹⁰4s²4p⁵ - Write the electron configurations for: (a) Fe²⁺, (b) Fe³⁺, (c) Cl⁻, (d) Cu²⁺.
(a) Fe²⁺: [Ar]3d⁶ (b) Fe³⁺: [Ar]3d⁵
(c) Cl⁻: 1s²2s²2p⁶3s²3p⁶ (isoelectronic with Ar)
(d) Cu²⁺: [Ar]3d⁹ - State and explain why IE₁(B) < IE₁(Be) and IE₁(O) < IE₁(N).
B < Be: B has its outer electron in 2p (higher energy, shielded by 2s electrons). Be's outer electron is in 2s. The 2p electron is easier to remove despite higher Z. O < N: O (2p⁴) has one doubly-occupied 2p orbital. Electron-electron repulsion in the paired orbital makes it easier to remove one electron, lowering IE₁ below N (2p³, all singly occupied, no such repulsion).
- The successive IEs (kJ mol⁻¹) of element Y are: 578, 1817, 2745, 11578, 14831, 18378. Determine Y's group and suggest its identity.
Large jump between IE₃ (2745) and IE₄ (11578). Three outer electrons → Group 13. IE₁ = 578 kJ mol⁻¹ → Aluminium (Al, Z=13).
- Draw the orbital (box) diagrams for (a) carbon and (b) phosphorus, showing Hund's rule.
(a) C (1s²2s²2p²): 1s[↑↓] 2s[↑↓] 2p[↑][↑][ ] — two unpaired electrons in separate 2p orbitals.
(b) P (1s²2s²2p⁶3s²3p³): …3s[↑↓] 3p[↑][↑][↑] — all three 3p orbitals singly occupied, all spins parallel.
Multiple Choice Quiz — 25 Questions
Unit 2 Quiz
Select one answer per questionUnit Test — 50 Marks
Section A — Short Answer
20 marksState the three rules used to determine the electron configuration of an atom. Name each rule and state what it requires, with one example. [4]
Write electron configurations for: (a) Cl⁻ [1]; (b) Mn (Z=25) [1]; (c) Mn²⁺ [1]; (d) Zn²⁺ (Z=30) [1].
Explain why: (a) IE₁(B) < IE₁(Be) [2]; (b) IE₁(S) < IE₁(P) [2].
Successive IEs (kJ mol⁻¹) of element Z: 590, 1145, 4912, 6474, 8144, 10496, 12270… (a) How many outer shell electrons does Z have? [1] (b) State Z's group. [1] (c) Suggest the identity of Z. [1] (d) Explain why successive IEs always increase. [1]
Describe the Lyman, Balmer, and Paschen series of the hydrogen emission spectrum (transitions + spectral regions) [3]. Explain how the Lyman convergence limit gives the ionisation energy of hydrogen. [1]
Section B — Extended Answer
30 marksExplain what is meant by an emission spectrum. Using Bohr's model, explain how the line emission spectrum of hydrogen is produced. Why does the spectrum provide evidence for quantised energy levels? Describe the Balmer series including why lines converge. [8]
Hydrogen emission by Bohr model [3]: At ground state, H’s electron is in n=1. When energy is supplied (electrical discharge), the electron is promoted to n=2,3,4… (excited state). The excited state is unstable — the electron rapidly falls to a lower level, emitting a photon of energy ΔE = E_upper − E_lower = hf. Since only specific energy levels are allowed, only specific photon frequencies are emitted → line spectrum.
Evidence for quantisation [2]: A continuous range of energies would give a continuous spectrum (rainbow). Only discrete wavelengths are observed → electrons can only exist at specific, discrete energy levels. Each line proves one specific transition — direct evidence for quantised energy levels.
Balmer series [2]: Transitions n≥3 → n=2; produces 4 visible lines (red n=3→2, blue-green n=4→2, violet n=5→2, etc.). Lines converge at shorter wavelengths/higher frequencies because energy levels get closer together as n increases — the energy gap between consecutive levels decreases, so photons emitted become more similar in energy/frequency until they merge at the convergence limit (n=∞→n=2).
Define quantum number and describe all four quantum numbers. Explain Aufbau, Pauli, and Hund's principles. Write full orbital box diagrams for (a) oxygen and (b) silicon. [8]
Three principles [3]: Aufbau: fill orbitals starting from lowest energy (1s→2s→2p→3s→3p→4s→3d…). Pauli: no two electrons share all four quantum numbers; max 2 per orbital with opposite spins. Hund: fill degenerate orbitals singly with parallel spins before pairing to minimise electron repulsion.
Orbital diagrams [3]:
(a) O (Z=8, 1s²2s²2p⁴):
1s[↑↓] 2s[↑↓] 2p[↑↓][↑][↑] — first two 2p electrons fill separately (Hund), then third 2p must pair up because all three orbitals are singly filled. [1.5]
(b) Si (Z=14, 1s²2s²2p⁶3s²3p²):
1s[↑↓] 2s[↑↓] 2p[↑↓][↑↓][↑↓] 3s[↑↓] 3p[↑][↑][ ] — two 3p electrons fill separately (Hund's rule). [1.5]
Define first ionisation energy. State the four main factors that influence IE. Use these to explain the general increase in IE₁ across Period 3 and the two anomalous dips. [6]
Four factors [2]: (1) Nuclear charge Z: higher Z → greater attraction → higher IE. (2) Distance/shell: outer electrons in higher shells → weaker attraction → lower IE. (3) Shielding: inner electrons reduce effective nuclear charge felt by outer electrons; more inner electrons = more shielding = lower IE. (4) Paired electron repulsion: electrons paired in the same orbital repel each other, making one easier to remove → lower IE than expected.
General increase across Period 3 [2]: From Na to Ar, Z increases by 1 each step. All outer electrons are added to the same shell (n=3), so distance and shielding change only slightly. Increasing Z provides greater effective nuclear charge → stronger nuclear attraction on outer electrons → IE₁ generally increases.
Two dips [1]: Mg→Al: Al’s outer electron is in 3p (higher energy, shielded by 3s), while Mg’s is in 3s → easier to remove despite higher Z. P→S: S has a paired 3p electron causing repulsion → one electron is easier to remove; P (3p³) has no paired 3p electrons.
Successive IEs (kJ mol⁻¹) of Q: 738, 1451, 7733, 10540, 13630, 17995, 21703, 25656. (a) Identify Q's group and element. [2] (b) Sketch a log(IE) vs ionisation number graph, marking the large jump. [2] (c) Explain what successive IEs reveal about Q's electronic structure. [2] (d) Write equations for the first three IEs of Q. [2]
(b) x-axis: ionisation number 1–8; y-axis: log(IE). Two low points (IE₁, IE₂) at left, large upward step between points 2 and 3 marked clearly, then gradually rising plateau for IE₃–IE₁⁰ (n=2 shell), then another very large jump at IE₁₁/IE₁₂ (n=1 shell). [2]
(c) IE₁–IE₂ relatively low and close: 2 electrons in n=3 outer shell (3s²) — well-shielded, far from nucleus. IE₃–IE₁⁰ much higher, rise gradually: 8 electrons in n=2 shell (closer to nucleus, stronger attraction). IE₁₁–IE₁₂ extremely high: 2 electrons in n=1 (maximum attraction, no shielding). The two jumps confirm Mg’s electron structure: 2,8,2 across shells n=1,2,3. [2]
(d) Mg(g) → Mg⁺(g) + e⁻ ΔH = +738 kJ mol⁻¹ [1]
Mg⁺(g) → Mg²⁺(g) + e⁻ ΔH = +1451 kJ mol⁻¹ [0.5]
Mg²⁺(g) → Mg³⁺(g) + e⁻ ΔH = +7733 kJ mol⁻¹ [0.5]