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IB · E · extended response

The rare deflections that changed the atomic model

Nuclear and quantum physics · Original GioPhysics question with a detailed, mark-by-mark answer guide.

Demand
discriminating
Marks
6
Topics
1
Answer
Complete
Explore the question data

Illustrative alpha-scattering observations

Supplied question data. Read the labelled axes and use the observations to test the physical model.

Vertical axis (y): Counts per minute

Illustrative alpha-scattering observationsSupplied question data. Read the labelled axes and use the observations to test the physical model. Horizontal axis: Scattering angle / °. Vertical axis: Counts per minute. Exact values are available in the data table below.02.50e45.00e47.50e41.00e5037.575112.5150xy

Horizontal axis (x): Scattering angle / °

Reading 1Scattering angle / °: 10Counts per minute: 1.00e5
Read the exact data as a table
Illustrative alpha-scattering observations — supplied values
Scattering angle / °Counts per minute
10100000
3010000
601000
90100
15010

These are the supplied values, not a worked answer. No fitted trend is drawn.

extended response6 marks

A narrow alpha-particle beam strikes a very thin gold foil. Detectors covering equal solid angles record the supplied count rates; values are illustrative rather than a full scattering-law fit. Most alpha particles pass close to the forward direction. Gold-197 has atomic number 79, and an alpha particle is a helium-4 nucleus of charge +2e. Supplied data (Scattering angle / °; Counts per minute): (10, 100000), (30, 10000), (60, 1000), (90, 100), (150, 10).

  1. (a)

    Explain what the common small deflections and rare large deflections imply, and compare them with a model of diffuse positive charge.

    3 marks
  2. (b)

    Determine proton, neutron and electron numbers in neutral gold-197 and in a gold-197 ion of charge +3e. Describe an isotope and balance alpha emission from a parent with A = 201, Z = 81.

    3 marks
Ready to self-mark?Reveal the detailed answer guide
Answer overview(a) Most atomic volume is sparsely occupied; positive charge and most mass are concentrated in a small nucleus. (b) Neutral Au-197: 79 p, 118 n, 79 e; Au³⁺ has 76 e. Alpha daughter: A = 197, Z = 79.
01

(a)

3 marks

Explain what the common small deflections and rare large deflections imply, and compare them with a model of diffuse positive charge.

How to approach it

Build a chain of claim, evidence and physics reasoning. Address more than one relevant factor, identify a limitation or assumption, and finish with a conclusion that is conditional on the evidence rather than absolute.

  1. 1

    Most projectiles cross the foil with little change in direction, so atoms are not solid dense obstacles across their full dimensions.

  2. 2

    A rare close encounter with concentrated positive nuclear charge can strongly repel an alpha particle. Very large deflections require a strong local interaction and a sufficiently massive scattering centre.

  3. 3

    A diffuse positive-charge model would spread the repulsion over the atomic volume and struggles to explain the observed rare strong deflections. The evidence supports a compact nucleus, while this count table alone does not determine an exact nuclear radius.

02

(b)

3 marks

Determine proton, neutron and electron numbers in neutral gold-197 and in a gold-197 ion of charge +3e. Describe an isotope and balance alpha emission from a parent with A = 201, Z = 81.

How to approach it

Build a chain of claim, evidence and physics reasoning. Address more than one relevant factor, identify a limitation or assumption, and finish with a conclusion that is conditional on the evidence rather than absolute.

  1. 1

    Atomic number gives 79 protons. Neutrons are A−Z = 197−79 = 118; neutrality requires 79 electrons.

  2. 2

    A +3e ion has lost three electrons and has 76; its nucleus is unchanged. An isotope has the same proton number but a different neutron number.

  3. 3

    Alpha emission removes A = 4 and Z = 2: ²⁰¹₈₁X → ¹⁹⁷₇₉Au + ⁴₂He. Both nucleon and charge numbers balance.

Complete marking guidance

Use these worked steps alongside the part-by-part answers. They explain the method and mark allocation; they do not add extra marks.

  1. Most projectiles cross the foil with little change in direction, so atoms are not solid dense obstacles across their full dimensions.
  2. A rare close encounter with concentrated positive nuclear charge can strongly repel an alpha particle. Very large deflections require a strong local interaction and a sufficiently massive scattering centre.
  3. A diffuse positive-charge model would spread the repulsion over the atomic volume and struggles to explain the observed rare strong deflections. The evidence supports a compact nucleus, while this count table alone does not determine an exact nuclear radius.
  4. Atomic number gives 79 protons. Neutrons are A−Z = 197−79 = 118; neutrality requires 79 electrons.
  5. A +3e ion has lost three electrons and has 76; its nucleus is unchanged. An isotope has the same proton number but a different neutron number.
  6. Alpha emission removes A = 4 and Z = 2: ²⁰¹₈₁X → ¹⁹⁷₇₉Au + ⁴₂He. Both nucleon and charge numbers balance.

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