IB Chemistry HL Topic 1 — Electronic Configurations HL only Core skill ~12 min read

Ionisation Energy from an Emission Spectrum

The convergence limit is the point where an atom’s emission lines run together and stop. Run that transition backwards and you have the energy needed to tear the electron off completely — which means a spectrum can be used to measure ionisation energy directly.

📚 What you need to know

What ionisation energy means

First ionisation energy X(g) → X+(g) + e

Notice the state symbols. Ionisation energies are defined for gaseous atoms, because otherwise you would also be paying the energy cost of separating the atoms from each other, and the number would no longer be a property of the atom alone.

THE SAME GAP, MEASURED TWO WAYSn = 1n = 23, 4, 5n = ∞ionisationenergy inconvergence limitphoton emittedelectron freeof the atomthe energy to remove the electron equals the energy released when it returnsso measuring the emitted photon measures the ionisation energy
Only the Lyman convergence limit gives the first ionisation energy, because only the Lyman series ends at n = 1, the ground state.

The calculation route

Every question of this type follows the same four steps. Learn the route rather than individual examples and none of them can surprise you.

FOUR STEPS, ALWAYS THE SAME FOURFREQUENCYENERGY PER ATOMPER MOLEINTO kJf = c ÷ λE = h f× 6.02 × 10²³÷ 1000convert nm to mjoules, one atomjoules per molekJ mol⁻¹firstif you are given the frequency instead, start at step twosteps three and four are where nearly all the marks are lostan answer around 10⁻¹⁹ means you forgot Avogadro’s constant
A useful sense check: first ionisation energies for real elements land between about 400 and 2400 kJ mol−1. Anything wildly outside that range means a step was skipped.
The reason step three exists is a definition, not a piece of physics. E = hf gives you the energy to ionise one atom, but ionisation energy is always quoted per mole. Multiplying by 6.02 × 1023 is simply converting from one atom to a mole of them. Miss it and your answer is out by twenty-three orders of magnitude, which is at least easy to spot.
WORKED EXAMPLE

The convergence limit in the emission spectrum of lithium occurs at a wavelength of 230 nm. Calculate the first ionisation energy of lithium in kJ mol−1.

Step 1: convert and find the frequency λ = 230 × 10−9 = 2.30 × 10−7 m f = c ÷ λ = 3.00 × 108 ÷ 2.30 × 10−7 = 1.30 × 1015 s−1 Step 2: energy for one atom E = hf = 6.63 × 10−34 × 1.30 × 1015 = 8.65 × 10−19 J Step 3: scale up to one mole 8.65 × 10−19 × 6.02 × 1023 = 5.21 × 105 J mol−1 Step 4: convert to kJ mol−1 5.21 × 105 ÷ 1000 = 521 IE1(Li) = 521 kJ mol−1 The data booklet gives 520 kJ mol−1, so the method checks out.
WORKED EXAMPLE

The convergence limit for potassium occurs at a frequency of 1.05 × 1015 s−1. Calculate its first ionisation energy in kJ mol−1.

Frequency is given, so skip straight to E = hf E = 6.63 × 10−34 × 1.05 × 1015 = 6.96 × 10−19 J There is no wavelength to convert, so there is no c = fλ step at all. Per mole 6.96 × 10−19 × 6.02 × 1023 = 4.19 × 105 J mol−1 Into kJ IE1(K) = 419 kJ mol−1 Sense check against lithium Potassium is below lithium in Group 1, so its outer electron is further from the nucleus and better shielded. A lower ionisation energy than lithium’s 521 is exactly what you would expect.
WORKED EXAMPLE

The first ionisation energy of magnesium is 738 kJ mol−1. Calculate the wavelength of its convergence limit, in nm.

Run the route backwards, starting per atom 738 × 1000 = 7.38 × 105 J mol−1 E = 7.38 × 105 ÷ 6.02 × 1023 = 1.23 × 10−18 J per atom Rearrange E = hf for frequency f = E ÷ h = 1.23 × 10−18 ÷ 6.63 × 10−34 = 1.85 × 1015 s−1 Then c = fλ for wavelength λ = c ÷ f = 3.00 × 108 ÷ 1.85 × 1015 = 1.62 × 10−7 m λ = 162 nm Does that make sense? 162 nm is well into the ultraviolet, which is right: convergence limits for ionisation always fall in the UV, since ionisation is a large energy jump.

💡 Exam tip

⚠️ Common mix-up

Up next: Successive Ionisation Energies — you have removed one electron. The next page keeps going, and shows how the pattern of what happens next reveals an element’s group without being told what it is.

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