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The nuclear atom and alpha scatteringEdexcel A-Level Physics: Revision notes

Section 1

Nuclear structure

The atom has a small, dense, positively charged nucleus containing protons and neutrons (together called nucleons), surrounded by electrons.

  • Proton number ZZ: the number of protons in the nucleus. It defines the element.
  • Nucleon number AA: the total number of protons and neutrons.
  • Neutron number: N=A−ZN = A - Z.

A nuclide is written ZAX{}^{A}_{Z}\text{X}. For 2963Cu{}^{63}_{29}\text{Cu} there are 29 protons, 63−29=3463 - 29 = 34 neutrons and, in a neutral atom, 29 electrons.

Atoms of the same element with different numbers of neutrons (same ZZ, different AA) are isotopes. Copper-65 has 29 protons and 36 neutrons.

Key termsnucleonproton numbernucleon number
Common mistake

Taking the nucleon number as the number of neutrons. Neutrons = A − Z; electrons in a neutral atom = Z.

Section 2

The plum pudding model

After the discovery of the electron in 1897, J. J. Thomson proposed the plum pudding model: an atom is a sphere of positive charge spread evenly through its volume, with negatively charged electrons embedded in it, so the whole atom is neutral.

In this model the positive charge is spread out, so the electric force on a charged particle passing through is weak everywhere. A fast alpha particle should pass through with at most a small deflection.

Key termsplum pudding model

Section 3

The alpha-scattering experiment

In 1909 Geiger and Marsden, working with Rutherford, fired a narrow beam of alpha particles (positively charged) at a very thin gold foil in an evacuated chamber, and counted the scattered particles at different angles.

  • The chamber is evacuated because alpha particles have a short range in air and would be absorbed or scattered by air molecules.
  • The foil is very thin so that each large deflection is due to one interaction with one nucleus, not several.

Observations:

  1. Most alpha particles passed straight through, or with little deflection.
  2. A small fraction (about 1 in 8000) was deflected through more than 90°.
  3. A few were scattered almost straight back.
Key termsalpha particle

Section 4

Conclusions: the nuclear model

Rutherford explained the results with the nuclear model (1911):

  • Most alpha particles pass through undeflected, so most of the atom is empty space.
  • Some are deflected through large angles, so there is a strong repulsive force, and the nucleus is positively charged (like charges repel).
  • Very few are scattered back, so the nucleus is very small compared with the atom, and the charge is concentrated in a tiny region.
  • Alpha particles rebounding almost straight back must have hit something far more massive, so most of the mass is in the nucleus.

Electrons are too light to deflect alpha particles significantly.

Key termsnuclear model

Section 5

How atomic models changed

Models change when new evidence cannot be explained:

  • Dalton: atoms as tiny, solid, indivisible spheres.
  • Thomson: the electron's discovery showed that atoms have structure, giving the plum pudding model.
  • Rutherford: the alpha-scattering results contradicted the plum pudding model, giving the nuclear atom.
  • Later refinements: for example the discovery of the neutron explained the mass of the nucleus, and Bohr added energy levels for electrons.

A model is accepted when it explains the evidence and its predictions are tested by repeatable experiments checked by other scientists, and it stays provisional.

Key termsprovisional model

Must know

  • AA = nucleon number, ZZ = proton number, neutrons = A−ZA - Z
  • Plum pudding: positive charge spread through the atom
  • Alpha scattering: most pass through, a few deflected by more than 90°, very few back
  • Conclusion: tiny, positive, massive nucleus; atom mostly empty space
  • Thin foil and a vacuum are needed
  • Models are changed by new evidence

That's the notes covered.

Carry on to the next subtopic.

Exam questions on The nuclear atom and alpha scattering

  1. A neutral atom of copper-63 is written ⁶³₂₉Cu.
    Another isotope of copper has a nucleon number of 65. State the number of protons and the number of neutrons in its nucleus, and explain why it is still copper.2 marks
  2. In the Geiger–Marsden experiment a narrow beam of alpha particles in an evacuated chamber was directed at a very thin gold foil. A detector that could be moved round the foil counted the alpha particles scattered at different angles. Most alpha particles passed through the foil with little or no deflection, but a very small number were deflected through large angles.
    Explain why the gold foil had to be very thin.2 marks
  3. In one run of an alpha-scattering experiment with a thin gold foil, a total of 4.0 × 10⁵ alpha particles were counted. About 1 in 8000 of them was scattered through an angle of more than 90°.
    Calculate the number of alpha particles scattered through more than 90°, and state what such a small fraction shows about the nucleus.3 marks
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Written by the Exaim team, led by Shaun Daswani (Head of Upper Secondary, Improve ME Institute; MSc Financial Mathematics, Imperial College London; BSc, UCL) and Jason Daswani (operational lead, Improve ME Institute; LSE).