Nuclear structure and nuclides

Key idea: A reviewed, static H2 Physics learning chain for all official Nuclear Physics outcomes, from Rutherford evidence to fusion and fission.

  • GCE A-Level H2 Physics 2027

Learn the idea

Big question: What does nuclide notation reveal about a nucleus?

A nucleus contains protons and neutrons: proton number Z identifies the element and nucleon number A counts both, so neutron number is A − Z. Isotopes share Z but differ in neutron number. Scattering evidence shows positive charge and most atomic mass concentrated in a tiny nucleus.

Turn each scattering observation into an inference

Most alpha particles crossed thin foil with little or no deflection, showing that most atomic volume is empty. Some deflected because positive alpha particles were repelled by positive charge.

A very small fraction turned through large angles. A strong force in a rare close encounter requires positive charge and most atomic mass to be concentrated in a tiny nucleus.

Check your understanding: Why does the rarity of backward scattering show that the nucleus is small?

Only particles passing very close to the concentrated repelling region turn back, and very few do so.

Read nuclide notation without mixing the two numbers

In ᴬ_ZX, Z is the proton number and identifies the element. A is the nucleon number, so neutron number is A − Z. A neutral atom has Z electrons, but electrons are not counted in A.

Isotopes share the same Z and therefore belong to one element, but have different neutron numbers and A values.

Check your understanding: How many neutrons are in ³⁷₁₇Cl?

37 − 17 = 20 neutrons.

Rutherford scattering observations and inferencesA beam of alpha particles crosses a thin foil. Most paths remain nearly straight, while a few bend through large angles near a small positive nucleus.α sourcethin metal foil+most: little deflectionrare: large-angle scatteringatom mostlyempty spacetiny nucleus:positiveand massive
Scroll diagram horizontally to read all labels.
Most alpha particles pass through with little deflection, but rare large-angle events require a tiny region containing concentrated positive charge and most of the atom’s mass.

Key ideas to keep

  • Changing neutron number makes an isotope, not a different element.
  • Nucleon number is not the same as relative atomic mass.
  • Nuclear size is far smaller than atomic size.

Worked example

Use scattering evidence and nuclide notation together

Question: A foil experiment records 99.3% of alpha particles within 1° of their original direction and 0.02% beyond 90°. Explain both observations. Then interpret ⁶⁰₂₇Co.

  1. Step 1: Interpret the common result

    Why: The dominant path describes most of the atom's volume.

    Working: Almost all particles pass through, so most atomic volume is empty.

  2. Step 2: Interpret the rare strong result

    Why: A turn beyond 90° requires a strong repulsive interaction.

    Working: Positive charge and most mass are concentrated in a very small nucleus encountered only rarely.

  3. Step 3: Read the nuclide

    Why: Z and A count different nuclear properties.

    Working: Cobalt-60 has 27 protons and 60 − 27 = 33 neutrons.

Answer: The atom is mostly empty with a tiny positive massive nucleus; cobalt-60 contains 27 protons and 33 neutrons.

Check: The proton count matches cobalt's Z, while protons plus neutrons return A = 60.

Question

Connect the frequency of Rutherford deflections to nuclear size and charge.

Check the worked solution

Most alpha particles see little concentrated charge; rare close approaches experience strong repulsion and large deflection. Rarity bounds the positive region to a tiny fraction of atomic volume.

Practise with support

Try this

For ³⁷₁₇Cl, state proton and neutron numbers.

Hint: Neutrons equal A − Z.

Check your answer

17 protons and 20 neutrons.

Practise independently

Your turn

Explain Rutherford evidence and distinguish nucleon number, proton number and isotopes.

Check your answer

Scattering supports a tiny positive nucleus and mostly empty atom. A counts protons plus neutrons; Z counts protons and identifies the element. Isotopes share Z but differ in neutron number and A.

Common mistakes

Common mistake

Isotopes have different proton numbers.

What is wrong with this reasoning?

Show better thinking

Isotopes share proton number and differ in neutron number.

Exam guidance

Check that nucleon and charge numbers balance whenever you write a nuclide symbol.

Exam-style practice [7 marks]

Explain how Rutherford scattering supports a nuclear atom, then distinguish the nuclides ³⁵₁₇Cl and ³⁷₁₇Cl.

Plan before you answer

  • Match each scattering observation to an inference.
  • Use the alpha particle's positive charge.
  • Compare Z and A for the nuclides.
Mark your answer and compare the model

Marking points

Tick each point only if your answer states it clearly.

Model answer

Most alpha particles pass straight through, so most of the atom is empty. Positive alpha particles are repelled, and the rare large-angle turns require a strong force from positive charge concentrated in a very small nucleus that also contains most of the mass. Both chlorine nuclides have Z = 17, so each has 17 protons. They have 18 and 20 neutrons respectively and are isotopes of the same element.

Check what stayed with you

Recall question 1

What does Z represent?

Check the answer

Proton number.

Recall question 2

What does A − Z give?

Check the answer

Neutron number.

Recall question 3

What observation supports a tiny nucleus?

Check the answer

The very small fraction of alpha particles scattered through large angles or backwards.

Try this next

Continue to the next lesson in this topic.

Random decay, radiation, activity and half-life

Syllabus and review details

This lesson covers the listed H2 Physics 9478 outcomes. Topic 20 excludes knowledge of positron emission in 20(g) and detailed knowledge of the antineutrino and particle zoo in 20(o). Nuclide equations conserve nucleon number, charge, mass-energy and momentum. Count data require background correction before population-law inference. Applications must relate half-life, penetration and ionisation to benefit and hazard. The binding-energy-per-nucleon curve, not a claim that mass disappears, explains fusion and fission energy release.

  • GCE A-Level H2 PhysicsTopic 20(a) / Topic 20(b) / Topic 20(c) · 2027Checked against the syllabus · partial topic coverageOfficial 9478 syllabus
Course and syllabus information
Course
GCE A-Level H2 Physics
Edition
GCE A-Level H2 Physics 2027