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ChemistryCBSE Class 11 · Chapter 2

Structure of Atom Class 11: Atomic Models, Quantum Numbers and Solved Numericals

Updated 15 October 2026 · Fact-checked

Structure of Atom is Unit 2 of CBSE Class 11 Chemistry and carries 9 of the 70 theory marks. It covers electrons, protons and neutrons, the Thomson and Rutherford models, photons and the photoelectric effect, Bohr's model and the hydrogen spectrum, de Broglie waves, the uncertainty principle, quantum numbers, orbitals and electronic configurations.

What Structure of Atom is about

This chapter tells the story of how chemists worked out what is inside an atom, and why the simple picture of electrons going round the nucleus like planets had to be replaced.

It starts with the discovery of the electron in cathode ray tubes, its charge-to-mass ratio (Thomson) and its charge (Millikan), followed by the proton and the neutron. Thomson's 'plum pudding' model failed when Rutherford's alpha particles bounced back from gold foil, revealing a tiny, dense, positive nucleus. Atomic number, mass number, isotopes and isobars follow from this.

Rutherford's model, however, could not explain why atoms are stable or why they give line spectra. The answer came from light. Light behaves as a wave (wavelength, frequency, wavenumber) and also as a stream of particles called photons with energy . This particle picture explains black-body radiation and the photoelectric effect.

Bohr combined the nucleus with quantised energy levels. His model gives the energy and radius of each orbit of hydrogen and explains its line spectrum: Lyman, Balmer, Paschen, Brackett and Pfund series. But it fails for atoms with more than one electron.

The quantum mechanical model fixes this. de Broglie showed that electrons have wave properties (), and Heisenberg showed that position and momentum cannot both be known exactly. So we speak of orbitals (regions of probability) labelled by four quantum numbers: n, l, mₗ and mₛ. The chapter ends with the shapes and energies of orbitals and the rules for filling them: the aufbau principle, Pauli's exclusion principle and Hund's rule, including the extra stability of half-filled and completely filled subshells (Cr and Cu).

Expect 1-mark questions on quantum numbers and configurations, 2- and 3-mark numericals on photons, Bohr energies and de Broglie wavelengths, and descriptive questions on Rutherford's experiment and the limits of Bohr's model.

Weightage: This chapter is Unit II, Structure of Atom, which the syllabus gives 9 of the 70 theory marks in the school annual exam.Source: CBSE Chemistry (043) syllabus 2026-27, Class XI course structure, Unit II Structure of Atom

Key concepts

Discovery of sub-atomic particles
NCERT section 2.1 Discovery of Sub-atomic Particles (2.1.1 to 2.1.4)

Electron: When a high voltage is applied across a gas at very low pressure in a discharge tube, rays travel from the cathode to the anode. These cathode rays travel in straight lines, cast shadows, are deflected towards the positive plate in an electric field (so they are negatively charged), and their properties do not depend on the gas or the electrode material. They are streams of electrons.

J. J. Thomson measured the charge-to-mass ratio of the electron by balancing electric and magnetic deflections: C kg⁻¹. The deflection is larger when the particle's charge is larger, its mass smaller, or the field stronger.

R. A. Millikan's oil drop experiment gave the charge: C. Combining the two gives the mass of the electron, kg.

Proton: Using a perforated cathode, Goldstein observed canal rays (anode rays) moving the other way. They are positive ions; their charge-to-mass ratio depends on the gas, and the lightest one, from hydrogen, is the proton (charge +1.602 × 10⁻¹⁹ C, mass 1.672 × 10⁻²⁷ kg, about 1836 times the electron).

Neutron: In 1932 Chadwick bombarded beryllium with alpha particles and found electrically neutral particles slightly heavier than protons: neutrons (mass 1.675 × 10⁻²⁷ kg).

Worked example

Use C kg⁻¹ and C to calculate the mass of an electron. Then explain why the charge-to-mass ratio of canal rays changes with the gas in the tube but that of cathode rays does not. (3 marks)

Try it first, then show the solutionSolution
  1. kg. (1)
  2. Cathode rays are electrons, which are the same in every atom, so their e/m is fixed. (1)
  3. Canal rays are positive ions formed from whatever gas is in the tube; different gases give ions of different masses, so e/m changes. (1)

Answer: m_e ≈ 9.1 × 10⁻³¹ kg; electrons are identical in all atoms, but canal-ray ions depend on the gas.

Thomson and Rutherford models; atomic number, mass number, isotopes and isobars
NCERT section 2.2 Atomic Models (2.2.1 to 2.2.5)

Thomson's model pictured the atom as a sphere of uniformly spread positive charge with electrons embedded in it, like seeds in a watermelon. It explained overall neutrality but not later experiments.

Rutherford's alpha-particle scattering experiment: a thin gold foil (about 100 nm thick) was bombarded with fast alpha particles (He²⁺), and a zinc sulphide screen recorded flashes. Observations:
1. Most alpha particles passed straight through.
2. A small fraction were deflected by small angles.
3. A very few (about 1 in 20 000) bounced right back.

Conclusions: most of the atom is empty space; the positive charge and almost all the mass are packed into a tiny central nucleus (radius about 10⁻¹⁵ m against 10⁻¹⁰ m for the atom); electrons move around the nucleus in circular paths called orbits, held by electrostatic attraction.

  • Atomic number (Z) = number of protons = number of electrons in a neutral atom.
  • Mass number (A) = protons + neutrons (nucleons). Number of neutrons = A − Z. The symbol is written .
  • Isotopes: same Z, different A (¹H protium, ²H deuterium, ³H tritium). Chemical properties are decided by electrons, so isotopes behave alike chemically.
  • Isobars: same A, different Z (¹⁴C and ¹⁴N).

Drawbacks of Rutherford's model: an electron moving in a circle is accelerating, and by classical electromagnetic theory it should radiate energy and spiral into the nucleus, so the atom would not be stable. The model also says nothing about how electrons are arranged or their energies, and cannot explain line spectra.

Worked example

A species has 24 electrons, 26 protons and 30 neutrons. (a) Find its atomic number and mass number. (b) Write its symbol with charge. (c) Give the symbol of an isobar of ⁵⁶Fe with Z = 27. (2 marks)

Try it first, then show the solutionSolution
  1. (a) Z = protons = 26 (iron); A = 26 + 30 = 56. (½ + ½)
  2. (b) Electrons are two fewer than protons, so the charge is +2: . (½)
  3. (c) An isobar has the same A and different Z: . (½)

Answer: Z = 26, A = 56; ⁵⁶₂₆Fe²⁺; isobar ⁵⁶₂₇Co

Wave nature of electromagnetic radiation
NCERT section 2.3.1 Wave Nature of Electromagnetic Radiation

James Maxwell showed that light is an electromagnetic wave: oscillating electric and magnetic fields at right angles to each other and to the direction of travel. Such waves need no medium and travel in vacuum at m s⁻¹.

The quantities used to describe a wave:

  • Wavelength (λ): distance between two crests, in m, nm (10⁻⁹ m) or pm (10⁻¹² m).
  • Frequency (ν): number of waves passing a point per second, in hertz (Hz = s⁻¹).
  • **Wavenumber ()**: number of wavelengths per unit length, , in m⁻¹ or cm⁻¹.
  • They are linked by .

The electromagnetic spectrum, in order of increasing frequency (decreasing wavelength): radio waves, microwaves, infrared, visible, ultraviolet, X-rays, gamma rays (cosmic rays have the highest frequencies). Visible light runs from about 400 nm (violet) to 750 nm (red); our eyes see only this small part.

Worked example

An FM radio station broadcasts at 98.3 MHz. Calculate the wavelength of the radio waves and their wavenumber. ( m s⁻¹) (2 marks)

Try it first, then show the solutionSolution
  1. m. (1)
  2. m⁻¹. (1)

Answer: λ ≈ 3.05 m; wavenumber ≈ 0.33 m⁻¹

Particle nature of radiation: Planck's quantum theory and the photoelectric effect
NCERT section 2.3.2 Particle Nature of Electromagnetic Radiation: Planck's Quantum Theory

Some observations cannot be explained by waves:

  • Black-body radiation: a perfect absorber and emitter (a black body) emits radiation whose intensity–wavelength curve depends only on temperature. As a body is heated it glows dull red, then orange-yellow, then white-blue: the peak moves to shorter wavelength as temperature rises.
  • Photoelectric effect: when light of suitable frequency falls on a metal such as potassium or caesium, electrons are emitted immediately.

Planck's quantum theory: energy is emitted or absorbed not continuously but in small packets called quanta. The energy of one quantum is
, where Planck's constant J s.
Einstein called a quantum of light a photon.

Photoelectric effect explained (Einstein):
1. Electrons are ejected only if the light has at least a minimum frequency, the threshold frequency , specific to each metal. Below it, no electrons come out, however bright the light.
2. Above , one photon gives all its energy to one electron. Part of it (, the work function ) frees the electron; the rest becomes kinetic energy: .
3. The number of electrons depends on the intensity (number of photons), but their kinetic energy depends only on the frequency.

So radiation has a dual nature: it acts as a wave in interference and diffraction, and as particles when it exchanges energy with matter.

Worked example

The work function of potassium is 2.25 eV. Light of wavelength 400 nm falls on it. (a) Calculate the energy of one photon in eV. (b) Find the maximum kinetic energy of the emitted electrons. (c) What is the threshold wavelength? ( J s, m s⁻¹, 1 eV = 1.602 × 10⁻¹⁹ J) (3 marks)

Try it first, then show the solutionSolution
  1. (a) J = 4.97 × 10⁻¹⁹ ÷ 1.602 × 10⁻¹⁹ = 3.10 eV. (1)
  2. (b) KE = 3.10 − 2.25 = 0.85 eV (= 1.36 × 10⁻¹⁹ J). (1)
  3. (c) m = 551 nm. (1)

Answer: (a) 3.10 eV (b) 0.85 eV (c) about 551 nm

Atomic spectra and Bohr's model of the hydrogen atom
NCERT section 2.3.3 Evidence for Quantized Electronic Energy Levels: Atomic Spectra; 2.4 Bohr's Model for Hydrogen Atom (2.4.1, 2.4.2)

White light passed through a prism gives a continuous spectrum. Atoms excited by heat or electricity emit light only at certain wavelengths, giving a line spectrum (emission spectrum); the same atoms absorb exactly those wavelengths from white light (absorption spectrum). Each element has its own line spectrum, like a fingerprint; rubidium, caesium, thallium, indium, gallium and scandium were discovered this way.

The lines of hydrogen fall into series given by the Rydberg equation:
cm⁻¹, with .
Lyman ( = 1, ultraviolet), Balmer ( = 2, visible), Paschen ( = 3), Brackett ( = 4) and Pfund ( = 5) (all three infrared).

Bohr's postulates (1913):
1. The electron moves round the nucleus in fixed circular orbits (stationary states) without losing energy.
2. Each orbit has a fixed energy; energy increases outwards.
3. Energy is absorbed or emitted only when the electron jumps between orbits: (Bohr's frequency rule).
4. Angular momentum is quantised: .

Results for hydrogen (and hydrogen-like ions such as He⁺, Li²⁺ with atomic number Z):

  • Radius: pm.
  • Energy: J.

The energy is negative because the bound electron has less energy than a free electron at rest (taken as zero at ). The ground state ( = 1) is the most stable.

For a jump from a higher level n_i to a lower level n_f, the energy given out is J for . The number of lines possible when an electron falls from level n to the ground state is .

Limitations: Bohr's model fails for atoms with more than one electron, cannot explain the fine structure of lines or the splitting of lines in electric (Stark) and magnetic (Zeeman) fields, cannot explain chemical bonding, and contradicts de Broglie's waves and the uncertainty principle.

Worked example

Calculate the energy and wavelength of the photon emitted when the electron in a hydrogen atom drops from n = 6 to n = 2. To which series and region does the line belong? ( J s, m s⁻¹) (3 marks)

Try it first, then show the solutionSolution
  1. J. (1)
  2. m = 410 nm. (1)
  3. The lower level is n = 2, so it is a Balmer line, at the violet end of the visible region. (1)

Answer: ΔE ≈ 4.84 × 10⁻¹⁹ J; λ ≈ 410 nm; Balmer series, visible (violet) region

Dual behaviour of matter and Heisenberg's uncertainty principle
NCERT section 2.5 Towards Quantum Mechanical Model of the Atom (2.5.1, 2.5.2)

de Broglie (1924) proposed that matter, like radiation, has both particle and wave properties. A particle of mass m moving with velocity v has a wavelength

where p is the momentum. This was confirmed when electron beams were found to be diffracted by crystals; the electron microscope uses the wave nature of electrons to magnify about 15 million times.

For everyday objects the wavelength is so tiny that it cannot be detected; the wave nature matters only for very light particles such as electrons.

Using the kinetic energy: gives , then .

Heisenberg's uncertainty principle (1927): it is impossible to find both the exact position and the exact momentum (or velocity) of an electron at the same time:
, or .
To locate an electron precisely we must hit it with light of very short wavelength, whose high-energy photons change its momentum.

Significance: the idea of a definite path (orbit) for an electron has no meaning. We can talk only of the probability of finding the electron in a region. For large objects the uncertainty is negligible, so classical mechanics works for them. This is why Bohr's model, with fixed circular orbits, had to be replaced.

Worked example

(a) Calculate the de Broglie wavelength of an electron moving at 1.0 × 10⁶ m s⁻¹. (b) If the position of this electron is known to within 40 pm, find the minimum uncertainty in its velocity, and comment. ( J s, kg) (3 marks)

Try it first, then show the solutionSolution
  1. (a) m = 727 pm. (1)
  2. (b) m s⁻¹. (1)
  3. The uncertainty in velocity is larger than the velocity itself, so an exact path for the electron cannot be defined. (1)

Answer: (a) ≈ 727 pm (b) Δv ≈ 1.45 × 10⁶ m s⁻¹, larger than v itself

Quantum mechanical model: orbitals, quantum numbers and shapes
NCERT section 2.6 Quantum Mechanical Model of Atom (2.6.1 Orbitals and Quantum Numbers; 2.6.2 Shapes of Atomic Orbitals)

In 1926 Schrödinger wrote an equation whose solutions, wave functions (ψ), describe electrons in atoms. ψ itself has no physical meaning, but ψ² gives the probability density of finding the electron at a point. An orbital is the region where the probability of finding the electron is high, described by one wave function. Each orbital holds at most two electrons.

Four quantum numbers describe an electron:

  • Principal (n) = 1, 2, 3 …: the shell; decides size and (for hydrogen) energy. Shell n has n² orbitals and holds 2n² electrons.
  • Azimuthal or subsidiary (l) = 0 to (n − 1): the subshell and the shape. l = 0, 1, 2, 3 are s, p, d, f.
  • Magnetic (mₗ) = −l to +l, giving (2l + 1) orbitals per subshell: one s, three p, five d, seven f. It gives the orientation in space.
  • Spin (mₛ) = +½ or −½: the two spin orientations of an electron.

Shapes:

  • s orbitals are spherical. The 1s orbital has no node; ns has (n − 1) radial nodes.
  • p orbitals are dumb-bell shaped, with two lobes along an axis (pₓ, p_y, p_z) and a nodal plane through the nucleus.
  • d orbitals: four have four lobes (d_xy, d_yz, d_xz, d_x²−y²) and d_z² has two lobes along z with a doughnut ring.

Nodes: radial nodes = n − l − 1; angular nodes = l; total nodes = n − 1.

Worked example

(a) Give the designation of the orbital with n = 4, l = 2, and list its possible mₗ values. (b) How many radial and angular nodes does a 3p orbital have? (c) How many electrons in an atom can have n = 3? (3 marks)

Try it first, then show the solutionSolution
  1. (a) l = 2 is d, so the orbital is 4d; mₗ = −2, −1, 0, +1, +2 (five 4d orbitals). (1)
  2. (b) 3p: n = 3, l = 1. Radial nodes = 3 − 1 − 1 = 1; angular nodes = l = 1. (1)
  3. (c) Shell n = 3 has n² = 9 orbitals, each holding 2 electrons: 18 electrons. (1)

Answer: (a) 4d; mₗ = −2 to +2 (b) one radial and one angular node (c) 18

Energies of orbitals, filling rules and electronic configuration
NCERT section 2.6.3 to 2.6.6 Energies of Orbitals, Filling of Orbitals, Electronic Configuration, Stability of Half-filled and Completely Filled Orbitals

In hydrogen, the energy depends only on n: 1s < 2s = 2p < 3s = 3p = 3d …. Orbitals of the same energy are degenerate.

In atoms with many electrons, energy depends on both n and l because inner electrons shield the outer ones from the nucleus. The attraction actually felt is the effective nuclear charge. s electrons penetrate closer to the nucleus than p, p closer than d, so for the same n: s < p < d < f.

(n + l) rule: the lower the value of (n + l), the lower the energy; if two orbitals have the same (n + l), the one with lower n has lower energy. This gives the filling order:
1s, 2s, 2p, 3s, 3p, then 4s before 3d, then 4p, 5s, 4d and so on (6s comes before 4f and 5d)

Three filling rules:
1. Aufbau principle: fill orbitals in order of increasing energy.
2. Pauli exclusion principle: an atom cannot contain two electrons whose four quantum numbers are all identical, so an orbital holds at most two electrons with opposite spins.
3. Hund's rule of maximum multiplicity: in degenerate orbitals (p, d, f), electrons first occupy each orbital singly with parallel spins; pairing starts only when each orbital has one electron.

Examples: N = 1s² 2s² 2p³ (three unpaired electrons); Fe = [Ar] 3d⁶ 4s².

Exceptions: chromium and copper. Cr is [Ar] 3d⁵ 4s¹, not 3d⁴ 4s², and Cu is [Ar] 3d¹⁰ 4s¹, not 3d⁹ 4s². Half-filled and completely filled subshells are extra stable because (a) their electron distribution is symmetrical, so shielding is smaller and the electrons are held more tightly, and (b) they have the maximum exchange energy: electrons of parallel spin in degenerate orbitals can exchange positions, and each exchange releases energy.

Worked example

Write the electronic configurations of (a) Cr (Z = 24) and (b) Fe³⁺ (Z of Fe = 26), and give the number of unpaired electrons in each. Explain the configuration of Cr. (3 marks)

Try it first, then show the solutionSolution
  1. (a) Cr: 1s² 2s² 2p⁶ 3s² 3p⁶ 3d⁵ 4s¹; six unpaired electrons (five 3d and one 4s). (1)
  2. (b) Fe is [Ar] 3d⁶ 4s². Electrons are removed first from 4s (the outermost shell), then 3d: Fe³⁺ = [Ar] 3d⁵; five unpaired electrons. (1)
  3. Cr takes 3d⁵ 4s¹ because a half-filled d subshell has symmetrical distribution and maximum exchange energy, which makes it more stable than 3d⁴ 4s². (1)

Answer: (a) Cr [Ar] 3d⁵ 4s¹, 6 unpaired (b) Fe³⁺ [Ar] 3d⁵, 5 unpaired

Chemistry in real life: Structure of Atom

Each concept, met in an everyday situation. Read the situation, try the problem, then check the solution. The one-line hook is what to remember.

Particle nature of radiation: Planck's quantum theory and the photoelectric effect

Suppose an automatic door at a shopping mall uses a photocell: a beam of light falls on a metal surface and the emitted electrons keep a current flowing. When someone blocks the beam, the current stops and the door opens.

The metal has a threshold frequency of 5.0 × 10¹⁴ Hz. Will (a) red light of 700 nm or (b) blue light of 450 nm work in this photocell? Would making the red lamp brighter help?

Try it first, then show the solutionSolution
  1. Frequency = c/λ. Red: 3.0 × 10⁸ ÷ 700 × 10⁻⁹ = 4.29 × 10¹⁴ Hz. Blue: 3.0 × 10⁸ ÷ 450 × 10⁻⁹ = 6.67 × 10¹⁴ Hz.
  2. Only frequencies above the threshold 5.0 × 10¹⁴ Hz can eject electrons, so blue works and red does not.
  3. Brightness only increases the number of photons, not the energy of each, so a brighter red lamp still ejects no electrons.

Answer: Blue light works; red light does not, however bright, because its frequency is below the threshold.

Memory hook: Frequency opens the door; intensity only counts the people.

Atomic spectra and Bohr's model of the hydrogen atom

Imagine you see the crimson-red glow of a hydrogen discharge lamp in the physics lab. A spectroscope shows the red line at 656 nm.

Show that this line comes from the electron falling from n = 3 to n = 2 in hydrogen. ( J s)

Try it first, then show the solutionSolution
  1. ΔE = 2.18 × 10⁻¹⁸ (1/4 − 1/9) = 2.18 × 10⁻¹⁸ × 0.1389 = 3.03 × 10⁻¹⁹ J.
  2. λ = hc/ΔE = (6.626 × 10⁻³⁴ × 3.0 × 10⁸) ÷ 3.03 × 10⁻¹⁹ = 6.56 × 10⁻⁷ m = 656 nm.
  3. The lower level is 2, so it is the first line of the Balmer series.

Answer: The 3 → 2 transition gives 656 nm, the red Balmer line.

Memory hook: Balmer lands on 2 and glows in the visible.

Dual behaviour of matter and Heisenberg's uncertainty principle

Suppose a cricket ball of mass 0.16 kg is bowled at 40 m s⁻¹, and a friend asks why it does not bend round the stumps like a wave.

Calculate its de Broglie wavelength and explain why its wave nature is never noticed. ( J s)

Try it first, then show the solutionSolution
  1. λ = h/mv = 6.626 × 10⁻³⁴ ÷ (0.16 × 40) = 1.04 × 10⁻³⁴ m.
  2. This is far smaller than even a nucleus (about 10⁻¹⁵ m), so no object or gap can diffract it.
  3. Only very light particles such as electrons have wavelengths comparable to atomic spacings.

Answer: About 1.0 × 10⁻³⁴ m, far too small to detect, so the ball behaves as an ordinary particle.

Memory hook: Heavy and fast means a wavelength too small to matter.

Thomson and Rutherford models; atomic number, mass number, isotopes and isobars

Suppose an archaeologist dates a wooden tool using carbon-14, while ordinary carbon in the wood is mostly carbon-12.

How many protons, neutrons and electrons are in each atom, and why do both behave alike in chemical reactions?

Try it first, then show the solutionSolution
  1. Both have Z = 6, so 6 protons and 6 electrons.
  2. Neutrons: ¹²C has 12 − 6 = 6; ¹⁴C has 14 − 6 = 8.
  3. Chemical behaviour depends on electrons, which are the same, so the isotopes react alike.

Answer: ¹²C: 6p, 6n, 6e; ¹⁴C: 6p, 8n, 6e. They are isotopes with the same chemistry.

Memory hook: Same protons, same chemistry; neutrons just add weight.

Energies of orbitals, filling rules and electronic configuration

Imagine a chemist explaining why copper wires are used in electric cables and why copper forms Cu⁺ and Cu²⁺ ions.

Write the configuration of Cu (Z = 29), and of Cu⁺ and Cu²⁺. Which ion has a completely filled d subshell?

Try it first, then show the solutionSolution
  1. Cu: [Ar] 3d¹⁰ 4s¹ (completely filled 3d is extra stable).
  2. Cu⁺: remove the 4s electron, giving [Ar] 3d¹⁰.
  3. Cu²⁺: remove one 3d electron as well, giving [Ar] 3d⁹.

Answer: Cu [Ar] 3d¹⁰ 4s¹; Cu⁺ [Ar] 3d¹⁰ (completely filled); Cu²⁺ [Ar] 3d⁹.

Memory hook: Copper and chromium cheat to fill or half-fill d.

Topics in this chapter

Structure of Atom formula sheet

Mass number and neutrons
Z = protons; for an ion, electrons = Z − charge.
Wave relations
c = 3.0 × 10⁸ m s⁻¹.
Energy of a photon
h = 6.626 × 10⁻³⁴ J s. Multiply by for one mole of photons.
Photoelectric equation
is the work function .
Bohr energy and radius (hydrogen-like)
Z = 1 for H, 2 for He⁺, 3 for Li²⁺.
Energy of a transition
Positive for emission written this way ().
Rydberg equation
= 1, 2, 3, 4, 5 for Lyman, Balmer, Paschen, Brackett, Pfund.
Number of spectral lines
From level n down to the ground state.
de Broglie wavelength
Use SI units: m in kg, v in m s⁻¹.
Uncertainty principle
h/4π = 5.27 × 10⁻³⁵ J s.
Orbitals, electrons and nodes
A subshell has 2l + 1 orbitals.

Structure of Atom: diagrams to practise

Practise each one on paper: draw it from the checklist, then tick off every label.

Rutherford's alpha-particle scattering experiment

Draw a labelled diagram of the gold foil experiment or of the paths of alpha particles near a nucleus.

Draw

  1. A lead block on the left with a narrow slit, emitting a beam of alpha particles.
  2. A thin gold foil in the centre.
  3. A circular zinc sulphide screen around the foil.
  4. Arrows: most going straight through, some bent by small angles, one bouncing back.

Label

  • Source of α-particles (in lead block)
  • Beam of α-particles
  • Gold foil
  • ZnS screen
  • Undeflected
  • Deflected
  • Rebounding particle

Watch out: In the close-up, draw the nucleus as a tiny dot; only paths passing very near it are strongly bent.

Shapes of s and p orbitals

Draw the boundary surface diagrams of 1s, 2s and the three 2p orbitals.

Draw

  1. A sphere for 1s and a larger sphere for 2s, each centred on the nucleus.
  2. Three sets of x, y, z axes.
  3. On each set, two lobes along one axis (x, y or z) meeting at the nucleus.

Label

  • 1s
  • 2s
  • 2pₓ
  • 2p_y
  • 2p_z
  • Nucleus
  • Nodal plane

Watch out: The lobes of a p orbital meet at the nucleus with a node there; label the axis on each.

Energy levels of hydrogen and the spectral series

Show the transitions that give the Lyman, Balmer and Paschen series.

Draw

  1. Horizontal lines for n = 1 to 6 and ∞, getting closer together upwards.
  2. Downward arrows ending on n = 1 (Lyman), n = 2 (Balmer) and n = 3 (Paschen).

Label

  • n = 1
  • n = 2
  • n = 3
  • n = ∞
  • Lyman (UV)
  • Balmer (visible)
  • Paschen (IR)

Watch out: Arrows point down for emission. Space the levels closer as n increases.

How the school exam asks Structure of Atom

The question patterns to expect, and the method that works for each.

Question typeHow it is askedMethod
1-mark MCQs on quantum numbers and configurationsPick the impossible set of quantum numbers, the number of orbitals in a shell, or the configuration of Cr, Cu or an ion.Check l < n and |mₗ| ≤ l. For ions of transition metals remove 4s electrons before 3d.
Assertion-reasonStatements on the photoelectric effect, Bohr's model, half-filled subshells or the uncertainty principle.Test A and R separately; for photoelectric items remember intensity changes the number, frequency changes the energy.
Photon and photoelectric numericals (2-3 marks)Energy of a photon or a mole of photons, photons emitted by a bulb, threshold frequency, KE of photoelectrons.Convert nm to m, use E = hc/λ, and keep J and eV apart (1 eV = 1.602 × 10⁻¹⁹ J).
Bohr model numericals (2-3 marks)Energy of an orbit, ionisation energy, wavelength of a line, radius for He⁺ or Li²⁺, number of lines.Write the formula with Z² and n², then substitute; name the series from the lower level.
de Broglie and Heisenberg numericalsWavelength of an electron or ball, uncertainty in velocity or position.Write λ = h/mv or Δv = h/(4πmΔx) before substituting; mass in kg.
Descriptive (3-5 marks)Rutherford's experiment with observations and conclusions, drawbacks of Rutherford or Bohr models, filling rules with examples, shapes of orbitals.Use numbered points: observation → conclusion. Draw a diagram where one is asked.

Tricks to remember Structure of Atom

Short memory aids. Say each one aloud once, then use it on a question the same day.

  • Raging Martians Invaded Venus Using X-ray Guns

    Radio, Microwave, Infrared, Visible, Ultraviolet, X-rays, Gamma: increasing frequency and energy.

    Use it when: Ordering the electromagnetic spectrum.

  • Lazy Boys Play Basketball Peacefully

    Lyman (1), Balmer (2), Paschen (3), Brackett (4), Pfund (5): the number is the lower level n₁.

    Use it when: Naming the series of a hydrogen line.

  • Bus seat rule (Hund)

    On a bus, people sit alone on each double seat before sharing. Electrons fill degenerate orbitals singly first, with parallel spins.

    Use it when: Writing orbital diagrams and counting unpaired electrons.

  • Diagonal arrows for filling order

    Write 1s; 2s 2p; 3s 3p 3d; 4s 4p 4d 4f … in rows and draw diagonal arrows from top right to bottom left: 1s, 2s, 2p, 3s, 3p, 4s, 3d, 4p, 5s …

    Use it when: Aufbau order without memorising a list.

  • n − l − 1 for radial nodes

    Radial = n − l − 1, angular = l, total = n − 1. 'Total is one less than the shell.'

    Use it when: Node questions.

Structure of Atom: exam-level solved questions

Ordered from exam level to HOTS. Cover the solution, write your own, then compare step by step.

Example 1: Impossible quantum numbers · 1 mark · MCQExam level

Which set of quantum numbers is not possible?
(a) n = 3, l = 2, mₗ = −2 (b) n = 2, l = 2, mₗ = 0 (c) n = 4, l = 0, mₗ = 0 (d) n = 3, l = 1, mₗ = +1

Try it first, then show the solutionSolution
  1. l must be less than n.
  2. In (b) l = n = 2, which is not allowed.

Answer: (b)

Example 2: Photoelectric effect and intensity · 1 mark · Assertion-reasonExam level

Assertion (A): Increasing the intensity of light above the threshold frequency increases the kinetic energy of the emitted electrons.
Reason (R): Each photon gives all its energy to a single electron.
(a) Both A and R are true and R is the correct explanation of A.
(b) Both A and R are true but R is not the correct explanation of A.
(c) A is false but R is true.
(d) Both A and R are false.

Try it first, then show the solutionSolution
  1. Intensity increases the number of photons, so more electrons are emitted, but each electron's kinetic energy depends on frequency only. A is false.
  2. R is a correct statement of Einstein's explanation.

Answer: (c) A is false but R is true.

Example 3: Energy of a mole of photons · 2 marks · Very short answerExam level

Calculate the energy of one mole of photons of wavelength 500 nm. ( J s, mol⁻¹) (2 marks)

Try it first, then show the solutionSolution
  1. E (one photon) = hc/λ = 6.626 × 10⁻³⁴ × 3.0 × 10⁸ ÷ 500 × 10⁻⁹ = 3.98 × 10⁻¹⁹ J. (1)
  2. E (one mole) = 3.98 × 10⁻¹⁹ × 6.022 × 10²³ = 2.39 × 10⁵ J = 239 kJ mol⁻¹. (1)

Answer: About 239 kJ mol⁻¹

Example 4: Ionisation from an excited state · 3 marks · Short answerHarder exam level

How much energy is needed to ionise a hydrogen atom whose electron is in the n = 3 level? What wavelength of light would just do this? (3 marks)

Try it first, then show the solutionSolution
  1. E₃ = −2.18 × 10⁻¹⁸ ÷ 9 = −2.42 × 10⁻¹⁹ J. (1)
  2. Ionisation energy = 0 − E₃ = 2.42 × 10⁻¹⁹ J. (1)
  3. λ = hc/E = 1.988 × 10⁻²⁵ ÷ 2.42 × 10⁻¹⁹ = 8.21 × 10⁻⁷ m = 821 nm (infrared). (1)

Answer: 2.42 × 10⁻¹⁹ J; λ ≈ 821 nm

Example 5: Wavelength of He⁺ transition · 3 marks · Short answerHarder exam level

Calculate the wavelength of light emitted when the electron in He⁺ falls from n = 2 to n = 1. In which region does it lie? (3 marks)

Try it first, then show the solutionSolution
  1. ΔE = 2.18 × 10⁻¹⁸ × Z² (1/1² − 1/2²) = 2.18 × 10⁻¹⁸ × 4 × 0.75 = 6.54 × 10⁻¹⁸ J. (1)
  2. λ = hc/ΔE = 1.988 × 10⁻²⁵ ÷ 6.54 × 10⁻¹⁸ = 3.04 × 10⁻⁸ m = 30.4 nm. (1)
  3. Far ultraviolet. (1)

Answer: About 30.4 nm, in the ultraviolet

Example 6: de Broglie wavelength from kinetic energy · 3 marks · Short answerHarder exam level

An electron has a kinetic energy of 2.0 × 10⁻¹⁷ J. Calculate its de Broglie wavelength. ( kg, J s) (3 marks)

Try it first, then show the solutionSolution
  1. v = √(2KE/m) = √(2 × 2.0 × 10⁻¹⁷ ÷ 9.11 × 10⁻³¹) = √(4.39 × 10¹³) = 6.63 × 10⁶ m s⁻¹. (1)
  2. λ = h/mv = 6.626 × 10⁻³⁴ ÷ (9.11 × 10⁻³¹ × 6.63 × 10⁶) (1)
  3. = 1.10 × 10⁻¹⁰ m = 110 pm. (1)

Answer: About 1.1 × 10⁻¹⁰ m (110 pm)

Example 7: Lines, series and limits · 5 marks · Long answerHOTS / competency

Electrons in a sample of hydrogen atoms are excited to n = 5. (a) What is the maximum number of different lines in the emission spectrum? (b) How many of these lie in the Balmer series? (c) Find the shortest wavelength in the Lyman series. (5 marks)

Try it first, then show the solutionSolution
  1. (a) Lines = n(n − 1)/2 = 5 × 4 ÷ 2 = 10. (1)
  2. (b) Balmer lines end on n = 2: from n = 5, 4 and 3, so 3 lines. (1)
  3. (c) The shortest Lyman wavelength is from n = ∞ to n = 1: ΔE = 2.18 × 10⁻¹⁸ J. (1)
  4. λ = hc/ΔE = 1.988 × 10⁻²⁵ ÷ 2.18 × 10⁻¹⁸ = 9.12 × 10⁻⁸ m = 91.2 nm. (1)
  5. In this sample the electrons start at n = 5, so the shortest line actually seen is 5 → 1: ΔE = 2.18 × 10⁻¹⁸ × 24/25 = 2.09 × 10⁻¹⁸ J, λ = 95.0 nm. (1)

Answer: (a) 10 (b) 3 (c) series limit 91.2 nm; shortest line from n = 5 is about 95 nm

Example 8: Uncertainty for a ball and an electron · 3 marks · Short answerHOTS / competency

Calculate the uncertainty in position for (a) a 40 g ball moving at 30 m s⁻¹ measured to 1% accuracy and (b) an electron moving at 3.0 × 10⁶ m s⁻¹ measured to 1%. Use the results to explain why the uncertainty principle matters only for tiny particles. ( J s, kg) (3 marks)

Try it first, then show the solutionSolution
  1. (a) Δv = 0.30 m s⁻¹; Δx = 5.27 × 10⁻³⁵ ÷ (0.040 × 0.30) = 4.4 × 10⁻³³ m. (1)
  2. (b) Δv = 3.0 × 10⁴ m s⁻¹; Δx = 5.27 × 10⁻³⁵ ÷ (9.11 × 10⁻³¹ × 3.0 × 10⁴) = 1.93 × 10⁻⁹ m. (1)
  3. The ball's uncertainty is unmeasurably small, but the electron's (about 2 nm) is about ten times the size of an atom, so its position inside the atom is truly uncertain. (1)

Answer: (a) ≈ 4.4 × 10⁻³³ m (b) ≈ 1.9 × 10⁻⁹ m; significant only for the electron

Case-study practice (Section E style)

Read the situation, then answer every part. In a school exam set on the board pattern this is a 4-mark question split into 1 + 1 + 2 marks.

Fireworks and flame colours

Suppose a fireworks maker explains that strontium salts give red, sodium salts yellow and copper salts blue-green. In the flame, electrons in the metal atoms absorb energy and jump to higher levels, then fall back and emit light of particular wavelengths. Sodium's yellow light has a wavelength of 589 nm.

  1. (i) · 1 mark

    What type of spectrum does each metal produce: continuous or line?

    Answer

    Answer: A line (emission) spectrum.

    Atoms emit only certain wavelengths, corresponding to jumps between fixed energy levels.

  2. (ii) · 1 mark

    Calculate the energy of one photon of sodium's yellow light.

    Answer

    Answer: 3.38 × 10⁻¹⁹ J

    E = hc/λ = 6.626 × 10⁻³⁴ × 3.0 × 10⁸ ÷ 589 × 10⁻⁹ = 3.38 × 10⁻¹⁹ J.

  3. (iii) · 2 marks

    Why do different metals give different colours, and why can this be used to identify elements?

    Answer

    Answer: Each element has its own set of energy levels, so its line spectrum is unique.

    The gaps between energy levels differ for each element, so the photons emitted have different energies and wavelengths (1). This unique set of lines acts like a fingerprint for identifying an element (1).

Seeing with electrons

Suppose a biology lab uses an electron microscope to view a virus about 100 nm across, which is too small for an ordinary light microscope. A microscope can resolve details roughly as small as the wavelength it uses. The electrons are accelerated to a speed of 7.27 × 10⁶ m s⁻¹. ( J s, kg)

  1. (i) · 1 mark

    Which idea about electrons makes an electron microscope possible?

    Answer

    Answer: The wave nature of electrons (de Broglie).

    Moving electrons behave as waves with λ = h/mv, so they can form images like light.

  2. (ii) · 1 mark

    Calculate the de Broglie wavelength of the electrons.

    Answer

    Answer: 1.0 × 10⁻¹⁰ m (100 pm)

    λ = 6.626 × 10⁻³⁴ ÷ (9.11 × 10⁻³¹ × 7.27 × 10⁶) = 1.0 × 10⁻¹⁰ m.

  3. (iii) · 2 marks

    Visible light has wavelengths of 400-750 nm. Explain why the electron microscope can show details of the virus while a light microscope cannot.

    Answer

    Answer: The electron wavelength is thousands of times smaller than visible light, so far finer detail is resolved.

    Visible light (≥ 400 nm) is larger than the whole virus, so its details blur (1). Electron waves of about 0.1 nm can resolve features far smaller than 100 nm (1).

Where the marks are

How a typical answer is split into step marks. Show every step: a right final answer alone rarely earns full marks.

State Hund's rule of maximum multiplicity and use it to find the number of unpaired electrons in an oxygen atom (Z = 8). (2 marks) (2 marks)

StepMarks
In orbitals of equal energy (such as the three p orbitals), electrons pair up only after each orbital has received one electron, and the single electrons have parallel spins.1
O: 1s² 2s² 2p⁴; the 2p electrons fill as ↑↓, ↑, ↑, giving 2 unpaired electrons.1

Calculate (a) the energy of the electron in the first Bohr orbit of Li²⁺ and (b) the radius of that orbit. (c) What energy is needed to remove this electron completely? (3 marks) (3 marks)

StepMarks
E₁ = −2.18 × 10⁻¹⁸ × Z²/n² = −2.18 × 10⁻¹⁸ × 9 = −1.96 × 10⁻¹⁷ J.1
r₁ = 52.9 × n²/Z = 52.9 ÷ 3 = 17.6 pm.1
Ionisation energy = E∞ − E₁ = 0 − (−1.96 × 10⁻¹⁷) = 1.96 × 10⁻¹⁷ J.1

(a) Describe Rutherford's alpha-particle scattering experiment, giving three observations and the conclusion drawn from each. (b) Give two drawbacks of Rutherford's model. (5 marks) (5 marks)

StepMarks
Set-up: a beam of high-energy alpha particles directed at a very thin gold foil, surrounded by a circular zinc sulphide screen that flashes where particles strike.1
Most particles passed undeflected → most of the atom is empty space.1
A few were deflected by small angles → the positive charge is concentrated in a small region.0.5
Very few (about 1 in 20 000) bounced back → there is a tiny, dense, positively charged nucleus holding nearly all the mass.1.5
Drawbacks: an orbiting (accelerating) electron should radiate energy and spiral into the nucleus, so the model cannot explain stability; it does not describe the distribution or energies of electrons (or line spectra).1

Where students lose marks in Structure of Atom

The slips examiners see most often, and what to write instead.

  • Mistake: Removing 3d electrons before 4s when forming ions

    Students reverse the filling order.

    Wrong working

    Fe²⁺ = [Ar] 3d⁴ 4s²

    Right working

    Fe²⁺ = [Ar] 3d⁶ (the 4s electrons leave first)

    Do this: Electrons leave from the highest n first.

    Usually costs: 1 mark.

  • Mistake: Not converting nm or Å to metres

    Students substitute 400 for 400 nm.

    Wrong working

    E = 6.626 × 10⁻³⁴ × 3 × 10⁸ ÷ 400

    Right working

    E = 6.626 × 10⁻³⁴ × 3 × 10⁸ ÷ (400 × 10⁻⁹) = 4.97 × 10⁻¹⁹ J

    Do this: Write every quantity in SI units before substituting.

    Usually costs: The answer mark.

  • Mistake: Writing Cr as 3d⁴ 4s²

    Students apply the aufbau order blindly.

    Do this: Learn Cr (3d⁵ 4s¹) and Cu (3d¹⁰ 4s¹) with the two reasons: symmetry and exchange energy.

    Usually costs: 1 mark.

  • Mistake: Saying brighter light gives faster photoelectrons

    Intensity and frequency are confused.

    Do this: Intensity → number of electrons; frequency → kinetic energy of each.

    Usually costs: 1 mark in MCQ or assertion-reason.

  • Mistake: Forgetting Z² for He⁺ and Li²⁺

    The hydrogen formula is used unchanged.

    Wrong working

    E₁(He⁺) = −2.18 × 10⁻¹⁸ J

    Right working

    E₁(He⁺) = −2.18 × 10⁻¹⁸ × 2² = −8.72 × 10⁻¹⁸ J

    Do this: Write Z²/n² in the formula every time.

    Usually costs: 1-2 marks.

  • Mistake: Giving mass of the electron in grams in λ = h/mv

    Units are mixed.

    Do this: h is in J s = kg m² s⁻¹, so mass must be in kg and velocity in m s⁻¹.

    Usually costs: The answer mark.

NCERT exercise guide: Structure of Atom

What each exercise in the NCERT chapter tests, how to approach it, and a question of the same kind solved step by step. Questions here are written in our own words.

Exercises 2.1-2.4, 2.22-2.23 and 2.26-2.27 (particles, atomic number and mass number)

What it tests: Electrons in a mass of substance, protons and neutrons in nuclei, symbols of atoms and ions, isoelectronic species.

How to approach it: Electrons per molecule × moles × ; neutrons = A − Z; electrons in an ion = Z − charge.

Same kind as Exercise 2.22

Which of these are isoelectronic: Na⁺, Mg²⁺, F⁻, Ne, Ca²⁺?

Show the solutionSolution
  1. Electrons: Na⁺ 11 − 1 = 10; Mg²⁺ 12 − 2 = 10; F⁻ 9 + 1 = 10; Ne 10; Ca²⁺ 20 − 2 = 18.
  2. The species with 10 electrons are isoelectronic.

Answer: Na⁺, Mg²⁺, F⁻ and Ne (10 electrons each); Ca²⁺ has 18.

Exercises 2.5-2.21 (radiation, photons, Bohr model, de Broglie)

What it tests: λ, ν and wavenumber, photon energy, photons per second from a bulb, photoelectric effect, hydrogen transitions, ionisation energy, de Broglie wavelength.

How to approach it: SI units first; E = hν = hc/λ; for Bohr use ΔE = 2.18 × 10⁻¹⁸ Z²(1/n_f² − 1/n_i²) J; for matter waves λ = h/mv.

Same kind as Exercise 2.11

A 60 W lamp emits light of wavelength 600 nm. How many photons does it emit each second? ( J s)

Show the solutionSolution
  1. Energy of one photon = hc/λ = 6.626 × 10⁻³⁴ × 3.0 × 10⁸ ÷ 600 × 10⁻⁹ = 3.31 × 10⁻¹⁹ J.
  2. Energy emitted per second = 60 J.
  3. Photons per second = 60 ÷ 3.31 × 10⁻¹⁹ = 1.81 × 10²⁰.

Answer: About 1.8 × 10²⁰ photons per second

Exercises 2.24-2.25 and 2.28-2.67 (quantum numbers and configurations)

What it tests: Allowed quantum numbers, orbital names, number of electrons and orbitals, configurations and unpaired electrons.

How to approach it: Use the rules l = 0 … n − 1 and mₗ = −l … +l; fill by (n + l), Pauli and Hund; remember Cr and Cu.

Same kind as Exercise 2.25

An electron is in a 4f orbital. Give the possible values of n, l and mₗ.

Show the solutionSolution
  1. 4f means n = 4 and l = 3.
  2. mₗ runs from −3 to +3.

Answer: n = 4, l = 3, mₗ = −3, −2, −1, 0, +1, +2, +3

Practice questions on Structure of Atom

Write each answer on paper first. Open the hint only if you are stuck, and the answer only when you have finished.

  1. Q1 · 1 mark · MCQExam level

    The number of radial nodes in a 3s orbital is:
    (a) 0 (b) 1 (c) 2 (d) 3

    Hint

    n − l − 1.

    Answer

    (c) 2

  2. Q2 · 1 mark · MCQExam level

    Which of the following has the electronic configuration [Ar] 3d⁵?
    (a) Mn²⁺ (b) Fe²⁺ (c) Cr (d) Co³⁺

    Hint

    Count electrons after removing 4s first.

    Answer

    (a) Mn²⁺ (Mn is [Ar] 3d⁵ 4s²; losing 4s² gives 3d⁵). Fe³⁺ would also be 3d⁵, but Fe²⁺ is 3d⁶.

  3. Q3 · 2 marks · Very short answerExam level

    Give two differences between an orbit and an orbital. (2 marks)

    Hint

    Path versus probability.

    Answer

    An orbit is a definite circular path (Bohr) while an orbital is a 3-D region of high probability of finding an electron (1). An orbit is two-dimensional and violates the uncertainty principle; an orbital can hold at most two electrons and has a shape (s, p, d) (1).

  4. Q4 · 2 marks · Very short answerExam level

    Calculate the frequency and wavenumber of radiation of wavelength 600 nm. (2 marks)

    Hint

    c = νλ.

    Answer

    ν = 3.0 × 10⁸ ÷ 600 × 10⁻⁹ = 5.0 × 10¹⁴ Hz (1); wavenumber = 1/λ = 1.67 × 10⁶ m⁻¹ (1).

  5. Q5 · 3 marks · Short answerHarder exam level

    The threshold wavelength of a metal is 540 nm. Ultraviolet light of wavelength 360 nm falls on it. Calculate (a) the threshold frequency, (b) the kinetic energy of the fastest emitted electrons and (c) their speed. ( J s, m s⁻¹, kg) (3 marks)

    Hint

    KE = hc(1/λ − 1/λ₀).

    Answer

    (a) ν₀ = c/λ₀ = 3.0 × 10⁸ ÷ 540 × 10⁻⁹ = 5.56 × 10¹⁴ Hz (1). (b) KE = 1.988 × 10⁻²⁵ × (1/360 × 10⁻⁹ − 1/540 × 10⁻⁹) = 1.988 × 10⁻²⁵ × 9.26 × 10⁵ = 1.84 × 10⁻¹⁹ J (1). (c) v = √(2 × 1.84 × 10⁻¹⁹ ÷ 9.11 × 10⁻³¹) = √(4.04 × 10¹¹) = 6.36 × 10⁵ m s⁻¹ (1).

  6. Q6 · 2 marks · Very short answerHarder exam level

    What is the radius of the third Bohr orbit of He⁺, and how does it compare with the first orbit of hydrogen? (2 marks)

    Hint

    r = 52.9 n²/Z pm.

    Answer

    r = 52.9 × 9 ÷ 2 = 238 pm (1); this is 4.5 times the first orbit of hydrogen (52.9 pm) (1).

  7. Q7 · 2 marks · Very short answerHarder exam level

    Arrange the following orbitals in increasing order of energy in a multi-electron atom, giving the (n + l) value for each: 4s, 3d, 4p, 5s, 4d. (2 marks)

    Hint

    Lower n + l first; ties go to lower n.

    Answer

    (n + l): 4s = 4, 3d = 5, 4p = 5, 5s = 5, 4d = 6 (1). Order: 4s < 3d < 4p < 5s < 4d (1).

  8. Q8 · 3 marks · Short answerHarder exam level

    Suppose a student shines ultraviolet light of wavelength 250 nm on a metal and finds that the fastest electrons have a kinetic energy of 2.0 eV. (a) Find the work function in eV. (b) What would happen with light of 600 nm? (1 eV = 1.602 × 10⁻¹⁹ J) (3 marks)

    Hint

    Find the photon energy in eV first.

    Answer

    (a) E = 1.988 × 10⁻²⁵ ÷ 250 × 10⁻⁹ = 7.95 × 10⁻¹⁹ J = 4.96 eV (1); W₀ = 4.96 − 2.0 = 2.96 eV (1). (b) A 600 nm photon has 2.07 eV, less than 2.96 eV, so no electrons are emitted (1).

  9. Q9 · 3 marks · Short answerHarder exam level

    Write the four quantum numbers for the last electron of sodium (Z = 11), and explain why two electrons in the same orbital must differ in spin. (3 marks)

    Hint

    Na = [Ne] 3s¹.

    Answer

    n = 3, l = 0, mₗ = 0, mₛ = +½ (or −½) (2). Two electrons in one orbital already share n, l and mₗ; by Pauli's principle they must differ in mₛ (1).

  10. Q10 · 3 marks · Short answerHarder exam level

    Why is Bohr's model said to contradict the uncertainty principle? Give two other limitations of the model. (3 marks)

    Hint

    A fixed orbit means exact position and momentum.

    Answer

    A fixed circular orbit of definite radius means the electron's position and velocity are known exactly at every instant, which Heisenberg's principle forbids (1). Limitations (any two): fails for multi-electron atoms; cannot explain fine structure of lines; cannot explain Zeeman and Stark effects; cannot explain chemical bonding (2).

  11. Q11 · 3 marks · Short answerHOTS / competency

    Suppose a teacher says: 'In chromium, one 4s electron moves into 3d because 3d⁵ 4s¹ has more exchange energy.' Count the exchange pairs in the 3d subshell for 3d⁴ (four parallel spins) and 3d⁵ (five parallel spins), and use the result to support her statement. Also give the second reason for the stability of half-filled subshells. (3 marks)

    Hint

    Number of pairs from k electrons = k(k − 1)/2.

    Answer

    3d⁴: 4 × 3 ÷ 2 = 6 exchange pairs; 3d⁵: 5 × 4 ÷ 2 = 10 exchange pairs (1). More exchanges release more exchange energy, so 3d⁵ 4s¹ is lower in energy than 3d⁴ 4s² (1). Second reason: the symmetrical distribution of electrons in a half-filled subshell reduces shielding, so electrons are held more strongly (1).

  12. Q12 · 5 marks · Long answerHOTS / competency

    A hydrogen atom in its ground state absorbs a photon of wavelength 97.3 nm. (a) To which level is the electron raised? (b) When it returns, list the possible emitted lines that fall in the visible region. ( J m) (5 marks)

    Hint

    Set 2.18 × 10⁻¹⁸ (1 − 1/n²) equal to the photon energy.

    Answer

    (a) Photon energy = 1.988 × 10⁻²⁵ ÷ 97.3 × 10⁻⁹ = 2.043 × 10⁻¹⁸ J (1). 1 − 1/n² = 2.043 ÷ 2.18 = 0.937, so 1/n² = 0.063 and n² ≈ 16, n = 4 (2). (b) Visible lines are Balmer lines ending on n = 2 from n ≤ 4: 4 → 2 (486 nm) and 3 → 2 (656 nm) (2).

Test your recall

Answer in your head or on paper first, then open the card. Pulling an answer out of memory makes it stick far better than re-reading.

  1. 1.Who measured the charge on the electron and how?Show answer

    R. A. Millikan, by the oil drop experiment.

  2. 2.What did the few alpha particles that bounced back show?Show answer

    That the positive charge and nearly all the mass are concentrated in a tiny nucleus.

  3. 3.Define isobars with an example.Show answer

    Atoms with the same mass number but different atomic numbers, e.g. ¹⁴C and ¹⁴N.

  4. 4.What is the threshold frequency?Show answer

    The minimum frequency of light that can eject an electron from a given metal surface.

  5. 5.In which region of the spectrum is the Lyman series?Show answer

    Ultraviolet.

  6. 6.Write Bohr's quantisation condition.Show answer

    Angular momentum mₑvr = nh/2π.

  7. 7.State Pauli's exclusion principle.Show answer

    An atom cannot contain two electrons with all four quantum numbers identical.

  8. 8.How many orbitals are there in the n = 4 shell?Show answer

    16 (n²).

  9. 9.What is the shape of a p orbital?Show answer

    Dumb-bell, with two lobes and a nodal plane through the nucleus.

  10. 10.Give the configuration of copper.Show answer

    [Ar] 3d¹⁰ 4s¹.

Best order to study it

  1. Learn the discovery of the three particles and the facts about each.
  2. Study Rutherford's experiment (observations, conclusions, drawbacks) with Z, A, isotopes and isobars.
  3. Practise wave relations and photon energies, then the photoelectric effect.
  4. Master Bohr's postulates, the energy and radius formulas, and the hydrogen series with numericals.
  5. Finish with de Broglie, Heisenberg, quantum numbers, orbital shapes and electronic configurations including Cr and Cu.

Quick revision checklist

The night before the exam: can you do each of these without looking?

  • Can you list the observations and conclusions of the gold foil experiment?
  • Can you convert between λ, ν and wavenumber?
  • Can you find the KE of a photoelectron from λ and the work function?
  • Can you calculate the energy and radius of any Bohr orbit for H, He⁺ or Li²⁺?
  • Can you find the wavelength of a hydrogen line and name its series?
  • Can you calculate a de Broglie wavelength from velocity or kinetic energy?
  • Can you spot an impossible set of quantum numbers?
  • Can you write configurations of Z = 1 to 30, including Cr, Cu and common ions?

Structure of Atom: frequently asked questions

How many marks does Structure of Atom carry in Class 11 (2026-27)?

The CBSE 2026-27 syllabus gives Unit 2 9 of the 70 theory marks in the school annual exam, one of the highest shares among the Class 11 Chemistry units.

Do I need to derive Bohr's energy formula?

No. NCERT states the radius and energy expressions without a full derivation; you need to know Bohr's postulates, use the formulas and explain their meaning, including why the energy is negative.

Why is the energy of an electron in an atom negative?

The zero of energy is taken as a free electron at rest at infinite distance. A bound electron is more stable than that, so its energy is lower than zero, that is, negative.

Why are 4s electrons removed before 3d when ions form?

Once the 3d orbitals contain electrons they lie lower in energy than 4s, and the 4s electrons are in the outermost shell (n = 4), so they are lost first.

What is the difference between an orbit and an orbital?

An orbit is Bohr's fixed circular path with a definite radius. An orbital is a three-dimensional region around the nucleus where the probability of finding an electron is high; it has no fixed path, as the uncertainty principle requires.

Based on: CBSE Chemistry (043) syllabus 2026-27 (Classes XI-XII); NCERT Chemistry Part I, Textbook for Class XI, Unit 2 (Reprint 2026-27)