The big idea: You can pull electrons off an atom one at a time. The energy to remove each one is a successive ionization energy — the 1st IE, 2nd IE, 3rd IE, and so on.
Every successive IE is larger than the one before it. Once you have removed an electron the particle is a positive ion, and the next electron is held by an ion with one fewer electron and the same nuclear charge — so the pull on it is stronger and it costs more energy to remove.
The pattern of those rising energies is a fingerprint of how the atom's electrons are arranged.
The vocabulary: - 1st ionization energy — energy to remove one mole of electrons from one mole of gaseous atoms: X(g) → X⁺(g) + e⁻. - 2nd ionization energy — energy for X⁺(g) → X²⁺(g) + e⁻, and so on. - Successive IEs — the whole sequence (1st, 2nd, 3rd …), always measured for the gaseous species. - Each one is bigger than the last because the electron leaves an increasingly positive ion — more protons pulling on fewer electrons.
Why each step costs more: Two reasons the energy rises with every electron removed:
1. Greater effective nuclear pull — the same number of protons now holds fewer electrons, so each remaining electron feels a stronger net attraction. 2. Less electron–electron repulsion — fewer electrons means the survivors are pulled in tighter.
Both make the next electron harder to remove. The interesting part is how much harder — that is what tells us about shells.
Most successive IEs rise gently. But every so often there is a sudden large jump — the next electron costs several times more than the last. That jump is the key piece of evidence in this topic.
A big jump = a new, inner shell: A large rise in successive IE happens when the next electron must be pulled from a new, inner (lower) main energy level — a shell closer to the nucleus.
Electrons in an inner shell are:
- closer to the nucleus (stronger attraction), and - less shielded by other electrons.
So breaking into a new inner shell costs a large jump of energy. The existence of these jumps is direct evidence that electrons are arranged in shells at different distances from the nucleus.
Sodium (2, 8, 1): the lone outer electron leaves easily (low 1st IE). Removing the next electron means breaking into the full n = 2 shell — a big jump in IE. The pattern 1 | 8 | 2 mirrors the three shells.
Interactive diagram
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| Ionization | Electron removed from | IE / kJ mol⁻¹ | Jump? |
|---|---|---|---|
| 1st | n = 3 (outer) | 496 | — |
| 2nd | n = 2 | 4 562 | × ~9 — BIG JUMP |
| 3rd | n = 2 | 6 910 | small rise |
| 4th | n = 2 | 9 543 | small rise |
| … | … | … | … |
| 9th | n = 2 | 104 000 | small rise |
| 10th | n = 2 | 124 400 | small rise |
| 11th | n = 1 (innermost) | 159 100 | BIG JUMP |
Reading sodium's pattern: Sodium is 2, 8, 1. Look at the jumps in its successive IEs:
- The 1st electron (the lone n = 3 electron) leaves easily — 496 kJ mol⁻¹. - The 2nd electron must come from the full n = 2 shell → a huge jump to 4 562 kJ mol⁻¹ (about nine times larger). - Electrons 2nd → 10th all come from n = 2 and rise only gently. - The 11th electron comes from the innermost n = 1 shell → another big jump.
Two big jumps → three shells → 2, 8, 1. The pattern is the electron arrangement.
Big jumps vs small rises: - A BIG jump (several-fold) = the next electron comes from a new inner main shell → evidence for shells. - A small extra rise (within a shell) can mark a change of sub-shell (e.g. moving from a p to an s sub-shell) → finer evidence for sub-shells.
For deducing the group you only need the big jumps; the small rises are the subtler sub-shell evidence.
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The rule that wins marks: For a main-group element, count the electrons removed before the first big jump.
Number of electrons before the first big jump = number of outer-shell electrons = the GROUP number.
- 1 electron, then a big jump → Group 1. - 2 electrons, then a big jump → Group 2. - 3 electrons, then a big jump → Group 13 (3 outer electrons).
The outer electrons leave relatively easily; the first big jump marks the point where you start breaking into the full inner shell.
Magnesium (2, 8, 2): two outer electrons leave fairly easily, then the big jump comes at the 3rd electron (into the full n = 2 shell). Two electrons before the first big jump → Group 2.
Interactive diagram
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IB-style question — deduce the group
The first five successive ionization energies of an element X (in kJ mol⁻¹) are: 738, 1 451, 7 733, 10 540, 13 630. Deduce the group of X in the periodic table, and explain your reasoning. [2]
How to score the marks
- Mark 1 — locate the first big jump. The rise from the 1st (738) to the 2nd (1 451) IE is gentle, but the 2nd → 3rd IE jumps from 1 451 to 7 733 (about 5×). So the big jump is between the 2nd and 3rd electron — meaning two electrons are easy to remove before the inner shell is reached.
- Mark 2 — state the group. Two outer electrons leave before the big jump, so X has 2 outer-shell electrons → Group 2. (The data are for magnesium.)
Final answer
Group 2. There are two outer electrons that leave relatively easily (738, 1 451 kJ mol⁻¹); the large jump at the 3rd IE shows the 3rd electron comes from a new inner shell.
Watch the position of the jump, not its size: It is where the first big jump falls (after how many electrons), not how big it is, that gives the group.
A Group 1 element has its big jump after 1 electron; a Group 13 element after 3 electrons. Count carefully: the jump is the step into the next-lower shell, so the outer electrons are the ones removed before it.
How this is tested: Successive IEs are a favourite HL Paper 2 data question.
- Paper 1A (MCQ): pick the element / group that matches a short list of successive IEs, or spot which jump is the big one. - Paper 2: you are given a table or a log-scale graph of successive IEs and asked to deduce the group, identify the element, or explain a particular jump in terms of shells.
Graphs are usually plotted as log₁₀(IE) against electron number so that all the values fit on one axis — the big jumps then show up as clear steps.
Why the graph is logarithmic: Successive IEs span a huge range (hundreds to hundreds of thousands of kJ mol⁻¹). Plotting log₁₀(IE) compresses that range so the whole sequence fits on one graph.
On a log plot, electrons from the same shell sit on a roughly flat step; a step up to a higher level marks a new inner shell. The number of points on the first (lowest) step = the number of outer electrons = the group.
Successive ionization energies of magnesium (2, 8, 2) on a log scale. The two big jumps — after the 2nd electron and after the 10th — split the points into three flat steps: 2 | 8 | 2, the three shells. The first (lowest) step holds 2 points → 2 outer electrons → Group 2.
Interactive diagram
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Reading the graph above for magnesium (2, 8, 2): the curve climbs in three flat steps with a sharp jump between each. The lowest step has 2 points (the two outer n = 3 electrons), the middle step has 8 (the n = 2 shell), and the top step has 2 more (the n = 1 shell). Counting the points on the first step gives 2 → Group 2. The same numbers are laid out in the table below.
| Electron # | IE / kJ mol⁻¹ | log₁₀(IE) | Shell (step) |
|---|---|---|---|
| 1 | 738 | 2.87 | n = 3 — bottom step (1st of 2 points) |
| 2 | 1 451 | 3.16 | n = 3 — bottom step (2nd point) |
| 3 | 7 733 | 3.89 | n = 2 — middle step jumps up here |
| … | … | … | n = 2 (8 points on this step) |
| 10 | 169 996 | 5.23 | n = 2 |
| 11 | 189 371 | 5.28 | n = 1 — top step jumps up again (1st of 2) |
| 12 | 265 924 | 5.42 | n = 1 — top step (2nd point) |
IB-style question — identify the element
An element Y has the following successive ionization energies (kJ mol⁻¹): 578, 1 817, 2 745, 11 580, 14 840. Deduce the group of Y, and hence identify Y given that it is in Period 3. [2]
How to score the marks
- Mark 1 — find the first big jump and the group. The first three IEs rise modestly (578 → 1 817 → 2 745); the 3rd → 4th jumps to 11 580 (about 4×). Three electrons leave before the big jump → 3 outer electrons → Group 13.
- Mark 2 — identify Y. A Group 13, Period 3 element is aluminium, Al. (Its three outer electrons are 3s² 3p¹; the 4th electron comes from the full n = 2 shell, hence the big jump.)
Final answer
Group 13; Y is aluminium, Al. Three electrons (the 3s² 3p¹ outer electrons) leave before the big jump at the 4th IE, which is into the full n = 2 shell.