Ionisation Energy Across a Period
Increasing attraction with subshell and pairing exceptions
Lesson 985 of 4,500 · Periodic Classification and Trends
Learning objectives
- Explain the broad increase in first ionisation energy across a period
- Identify why a trend graph has local exceptions
Introduction
First ionisation energy generally rises from the left toward the right of a main-group period. Increasing proton number and similar inner shielding pull valence electrons more strongly. The plot is not a perfect staircase: boron lies below beryllium, and oxygen below nitrogen in the second period. Their configurations explain why.
Core explanation
Across period two, neutral atoms add protons and electrons while the main inner 1s core stays broadly similar. The outer electrons occupy n = 2 states. Rising nuclear charge generally produces stronger effective attraction, making it harder to remove an electron from a gaseous neutral atom. The first ionisation energies tend to rise overall from lithium toward neon. The same broad argument applies to sodium through argon with an [Ne] core and outer n = 3 states.
This directional explanation is not a mathematical rule that IE₁ at Z + 1 must exceed IE₁ at Z. The electron removed can come from a different subshell, and electron pairing can change repulsion. In period two, beryllium is [He]2s², while boron is [He]2s²2p¹. Boron's first electron is removed from a 2p state, which is generally higher in energy and less penetrating than the 2s state removed from beryllium. As a result, boron's first ionisation energy is lower than beryllium's despite boron having one more proton.
Nitrogen and oxygen give a second familiar exception. Nitrogen is [He]2s²2p³, with one electron in each of three p orbitals in the simple Hund arrangement. Oxygen is [He]2s²2p⁴, so one p orbital contains a pair. Repulsion within that paired occupancy can make one oxygen p electron easier to remove than one of nitrogen's unpaired p electrons. Oxygen's first ionisation energy is therefore slightly lower than nitrogen's in measured data, interrupting the overall rise.
Similar classes of exception can appear in later main-group periods when filling changes from s to p or when pairing begins. Do not assert exact values from configurations alone. Measured ionisation energy includes the energies of both the initial atom and the relaxed positive ion, with electron interactions throughout. The subshell and pairing explanations are physically motivated qualitative accounts of observed data.
The general trend connects to other periodic patterns but is not identical to them. Atomic radius generally shrinks across a period under compatible definitions, consistent with tighter electron attraction. Metallic character broadly decreases as electron loss becomes harder. However, a single element's reaction rate, conductivity or compound type is not specified by IE₁ alone. Whole chemistry involves multiple steps and structures.
Graphs must be read carefully. Check that the y-axis shows first ionisation energy, not electron affinity or an average of successive ionisations. Check units such as kJ mol⁻¹, and compare gaseous ground-state atoms as defined. Mark the broad rise and then name the local exceptions instead of fitting a straight line through them or calling the whole trend false.
For an exam explanation, state the controlled across-period factors first: increasing Z, similar core shielding and same outer principal shell. Then, if a neighbouring pair is specified, write their configurations and examine the orbital being removed. The detailed configuration can override the simple arrow for a local comparison.
Step-by-step reasoning
1. Confirm the data are first ionisation energies of gaseous neutral atoms. 2. Explain the broad increase by rising Z and similar core shielding. 3. For a local reversal, compare the subshell and pairing of removed electrons. 4. Distinguish a local exception from rejection of the overall trend.
Visual explanation
Sketch a rising period-two IE₁ graph with small dips at B and O. Below, draw Be 2s [↑↓] versus B 2s [↑↓] 2p [↑], then N 2p [↑][↑][↑] versus O 2p [↑↓][↑][↑]. Connect each dip to the changed occupancy.
Real-world analogy
A hill generally climbs toward a summit but can contain small downhill steps. The overall elevation trend remains upward, while local terrain explains each dip. Ionisation data similarly combine broad nuclear attraction with orbital-specific details.
Real-world example
The second-period plot of measured first ionisation energies rises strongly from lithium to neon overall, yet boron and oxygen are lower than the immediately preceding elements. The exceptions make configuration analysis more useful than memorising a smooth arrow.
Why?
Why can oxygen's first ionisation energy be lower than nitrogen's? Oxygen's extra 2p electron creates a paired occupancy with additional repulsion, making one electron somewhat easier to remove.
Common misconception
“One decrease between neighbours disproves the across-period trend.” A trend is a general pattern, not a promise of strict increase at every point. Subshell and pairing effects account for local deviations.
Worked example
Compare Be and B. Be is [He]2s²; B is [He]2s²2p¹. Across the period, B has higher Z, which tends to strengthen attraction. But its first removed electron is the higher-energy 2p electron rather than a 2s electron. The observed IE₁ of B is lower than that of Be. State both competing factors to explain the exception.
Quick check
1. Which second-period element has a lower first ionisation energy than nitrogen despite following it? Answer: Oxygen, because its paired 2p occupancy makes one electron easier to remove.
Exam focus
Use “generally rises across a period,” then explain Be/B and N/O with configurations. Include gas-phase, first-electron conditions. Do not confuse this trend with electron affinity or whole reaction energetics.
Advanced insight
Electron removal also changes how the remaining electrons relax. Quantum calculations compare total energies of the neutral atom and cation, not just a single orbital label. The standard exceptions demonstrate why a one-electron picture has limits.
Summary
First ionisation energy broadly increases across a main-group period as effective nuclear attraction rises. The Be-to-B and N-to-O drops arise from subshell and pairing differences. Local exceptions refine the model rather than erase the overall pattern.
Practice questions
1. Why does IE₁ generally rise from Na toward Ar? Answer: Z rises while major inner-core shielding is broadly similar, holding valence electrons more strongly. 2. Why is boron's IE₁ lower than beryllium's? Answer: Boron's removed electron is in a higher-energy 2p state rather than Be's 2s state. 3. What 2p occupancy difference separates N and O? Answer: Nitrogen has three singly occupied p orbitals; oxygen has one paired p orbital. 4. Is a lower IE₁ enough to prove a faster water reaction? Answer: No; the whole reaction has other energetic and kinetic steps.