Emission spectra and photon energy
Emission spectrum forms when excited electrons fall to lower energy levels and emit photons.
Continuous spectrum = all wavelengths present; line spectrum = only specific wavelengths present.
Across the electromagnetic spectrum: longer wavelength leftarrow lower frequency and lower energy; shorter wavelength leftarrow higher frequency and higher energy.
Key relationships: and .
For visible light: red = longer wavelength, lower frequency, lower energy; violet = shorter wavelength, higher frequency, higher energy.
Each element has a unique line spectrum, so spectra can be used to identify elements.

This image shows the visible hydrogen emission lines as distinct coloured lines rather than a continuous rainbow. It is useful for remembering that hydrogen produces a line spectrum because electrons can only move between discrete energy levels. Source
Hydrogen line spectrum: evidence for discrete energy levels
The hydrogen emission spectrum proves electrons occupy discrete energy levels, not any energy value.
Spectral lines converge at higher energies because the energy levels get closer together as increases.
You must relate spectral lines to electron transitions to the first, second and third energy levels.
Transitions to release the highest-energy photons; transitions to release less energy; transitions to release even less.
Bigger energy drop rightarrow higher frequency, shorter wavelength photon.
The series names do not need to be memorized.

This diagram shows visible hydrogen transitions ending at the same lower level, with labelled wavelengths such as 656 nm, 486 nm and 433 nm. It helps connect electron transitions to the colours and wavelengths seen in the line spectrum. Source
Main energy levels, sublevels and orbitals
The main energy level is labelled by the integer .
Maximum electrons in a main energy level = .
So the first four levels can hold: , , , electrons.
A more detailed model divides main energy levels into sublevels: s, p, d, f in order of increasing energy.
Sublevels contain fixed numbers of orbitals:
s has 1 orbital
p has 3 orbitals
d has 5 orbitals
f has 7 orbitals
Each orbital can hold a maximum of 2 electrons with opposite spin.
Therefore maximum electrons per sublevel are: s = 2, p = 6, d = 10, f = 14.
s orbital is spherical. The three p orbitals are oriented at right angles to each other: , , .

This diagram shows the shape of the s orbital and the three p orbitals with different orientations. It is ideal for revising that s is spherical while p orbitals have the same shape but point in different directions. Source
Writing electron configurations
Use atomic number, to find the number of electrons in a neutral atom.
For ions: cations have lost electrons; anions have gained electrons.
Electron configurations up to must be deduced using:
Aufbau principle = electrons fill lowest-energy orbitals first
Hund’s rule = electrons occupy equal-energy orbitals singly first before pairing
Pauli exclusion principle = an orbital holds at most 2 electrons with opposite spin
Standard filling order up to krypton:
1s, 2s, 2p, 3s, 3p, 4s, 3d, 4p
Both full electron configurations and condensed configurations using a noble gas core are required.
Example: Cl = 1s² 2s² 2p⁶ 3s² 3p⁵ = [Ne] 3s² 3p⁵.
Example: Ca = [Ar] 4s².
Example: Br = [Ar] 4s² 3d¹⁰ 4p⁵.
For transition-metal ions, electrons are removed from the highest main energy level first (so 4s electrons are removed before 3d).

This diagram shows the Aufbau filling order of orbitals, helping you remember why 4s fills before 3d. It is useful when building both full and noble-gas shorthand electron configurations. Source
Orbital diagrams and key exceptions
Orbital diagrams (arrow-in-box diagrams) show both filling order and electron spin.
In a p sublevel, place one electron in each orbital before pairing: ↑ ↑ ↑ then ↑↓ ↑↓ ↑↓.
Watch the two key exceptions:
Cr = [Ar] 4s¹ 3d⁵ (not [Ar] 4s² 3d⁴)
Cu = [Ar] 4s¹ 3d¹⁰ (not [Ar] 4s² 3d⁹)
These exceptions occur because a half-filled or filled d sublevel gives a lower-energy arrangement.
In exam questions, always check whether the element is Cr or Cu before finalizing the configuration.

This image shows how individual orbitals sit within each sublevel, which is helpful for drawing orbital box diagrams correctly. It reinforces how many orbitals are present in s, p, d, and f sublevels and where electrons pair. Source
HL only: convergence limit and first ionization energy
In an emission spectrum, the convergence limit at the highest frequency corresponds to ionization.
At this point, the electron is removed completely from the atom: .
If given the wavelength or frequency of the convergence limit, calculate the first ionization energy using:
Combine them when needed: .
Be careful with units: convert nm to m before substitution.
The result from the formula is the energy for one atom; convert appropriately if the question asks for per mole.
HL only: trends in first ionization energy
First ionization energy = energy required to remove one electron from one mole of gaseous atoms.
Across a period, first IE generally increases because nuclear charge increases and electrons are held more strongly.
Down a group, first IE generally decreases because the outer electron is farther from the nucleus and experiences more shielding.
Important discontinuities across a period:
Group 2 to 13 drop: electron removed from a higher-energy p sublevel, so it is easier to remove.
Group 15 to 16 drop: repulsion between paired electrons in one p orbital makes removal easier.
Explanations must be based on the energy of the electron removed, distance from nucleus, shielding, and sublevel structure.

This graph shows the overall increase across periods, the decrease down groups, and the small dips/discontinuities that IB loves to test. Use it to spot where changes in sublevel energy and electron pairing explain exceptions to the trend. Source
HL only: successive ionization energies
Successive ionization energies always increase because electrons are removed from an increasingly positive ion.
A very large jump shows that the next electron would be removed from an inner shell.
Use the position of the big jump to deduce the number of valence electrons.
Example idea: if the large jump is after the 3rd electron, the atom has 3 valence electrons and is in Group 13.
This is a common data-analysis question: look for the first dramatic increase, then infer the group.
Checklist: can you do this?
Explain why hydrogen gives a line spectrum and relate line position to energy level transitions.
Write full, condensed and orbital diagram electron configurations for atoms and ions up to .
Apply the Aufbau principle, Hund’s rule and Pauli exclusion principle, including the Cr/Cu exceptions.
Calculate photon energy or first ionization energy from given wavelength/frequency data.
Interpret successive ionization energy data to deduce an element’s group.
Exam traps to avoid
Do not confuse energy levels, sublevels and orbitals.
Do not say a line spectrum is produced by electrons absorbing energy; for emission, electrons drop down and emit photons.
Do not forget that each orbital holds only 2 electrons.
Do not pair electrons in p orbitals too early; apply Hund’s rule first.
Do not miss the Cr and Cu exceptions.
Do not remove 3d electrons before 4s when forming many transition-metal ions.
In HL calculations, do not forget unit conversions, especially nm to m and per atom to per mole.

Shubhi is a seasoned educational specialist with a sharp focus on IB, A-level, GCSE, AP, and MCAT sciences. With 6+ years of expertise, she excels in advanced curriculum guidance and creating precise educational resources, ensuring expert instruction and deep student comprehension of complex science concepts.
Shubhi is a seasoned educational specialist with a sharp focus on IB, A-level, GCSE, AP, and MCAT sciences. With 6+ years of expertise, she excels in advanced curriculum guidance and creating precise educational resources, ensuring expert instruction and deep student comprehension of complex science concepts.