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IB · E · extended response

A fusion power estimate and a star's fuel lifetime

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

Fusion energy release

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

Vertical axis (y): Energy / 10²⁶ J

Fusion energy releaseSupplied question data. Read the labelled axes and use the observations to test the physical model. Horizontal axis: Completed cycles / 10³⁸. Vertical axis: Energy / 10²⁶ J. Exact values are available in the data table below.03.2046.4089.61212.8200.751.52.253xy

Horizontal axis (x): Completed cycles / 10³⁸

Reading 1Completed cycles / 10³⁸: 0Energy / 10²⁶ J: 0
Read the exact data as a table
Fusion energy release — supplied values
Completed cycles / 10³⁸Energy / 10²⁶ J
00
14.272
28.544
312.816

These are the supplied values, not a worked answer. Lines join the supplied values; they are not a fitted model.

extended response6 marks

In an idealised net stellar fusion cycle, four hydrogen nuclei ultimately produce one helium-4 nucleus plus other particles and radiation, releasing 26.7 MeV per completed cycle. Use 1 MeV = 1.60×10⁻¹³ J and c = 3.0×10⁸ m s⁻¹. The supplied graph gives cumulative energy from completed cycles. A star emits 4.0×10²⁶ W and has 2.0×10²⁹ kg of available hydrogen fuel; take four hydrogen nuclei as 6.68×10⁻²⁷ kg. Supplied data (Completed cycles / 10³⁸; Energy / 10²⁶ J): (0, 0), (1, 4.272), (2, 8.544), (3, 12.816).

  1. (a)

    Find energy per cycle, mass defect per cycle and the cycle rate supplying the stated luminosity.

    3 marks
  2. (b)

    Estimate the fuel-consumption rate and idealised lifetime, taking 1 yr = 3.16×10⁷ s. Explain two limits of this estimate.

    3 marks
Ready to self-mark?Reveal the detailed answer guide
Answer overview(a) Energy = 4.272×10⁻¹² J; mass defect≈4.75×10⁻²⁹ kg; rate≈9.36×10³⁷ cycles s⁻¹. (b) Fuel consumption≈6.25×10¹¹ kg s⁻¹; idealised lifetime≈1.01×10¹⁰ years.
01

(a)

3 marks

Find energy per cycle, mass defect per cycle and the cycle rate supplying the stated luminosity.

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

    Convert 26.7 MeV to joules: E = 26.7(1.60×10⁻¹³) = 4.272×10⁻¹² J.

  2. 2

    The decrease in total rest mass is Δm = E/c² = 4.272×10⁻¹²/(9.0×10¹⁶)≈4.75×10⁻²⁹ kg per net cycle.

  3. 3

    Cycle rate is L/E = 4.0×10²⁶/(4.272×10⁻¹²)≈9.36×10³⁷ s⁻¹. Nuclear binding-energy differences, rather than chemical combustion, power this process.

02

(b)

3 marks

Estimate the fuel-consumption rate and idealised lifetime, taking 1 yr = 3.16×10⁷ s. Explain two limits of this estimate.

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

    Each cycle uses about 6.68×10⁻²⁷ kg of hydrogen, so consumption is (9.36×10³⁷)(6.68×10⁻²⁷)≈6.25×10¹¹ kg s⁻¹.

  2. 2

    Time is available fuel divided by its consumption rate: 2.0×10²⁹/(6.25×10¹¹)≈3.20×10¹⁷ s≈1.01×10¹⁰ yr.

  3. 3

    Luminosity changes as the star evolves, only part of its hydrogen is accessible to core fusion, and some fusion energy can escape in neutrinos. A full stellar model must account for structure, composition and evolving reactions.

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. Convert 26.7 MeV to joules: E = 26.7(1.60×10⁻¹³) = 4.272×10⁻¹² J.
  2. The decrease in total rest mass is Δm = E/c² = 4.272×10⁻¹²/(9.0×10¹⁶)≈4.75×10⁻²⁹ kg per net cycle.
  3. Cycle rate is L/E = 4.0×10²⁶/(4.272×10⁻¹²)≈9.36×10³⁷ s⁻¹. Nuclear binding-energy differences, rather than chemical combustion, power this process.
  4. Each cycle uses about 6.68×10⁻²⁷ kg of hydrogen, so consumption is (9.36×10³⁷)(6.68×10⁻²⁷)≈6.25×10¹¹ kg s⁻¹.
  5. Time is available fuel divided by its consumption rate: 2.0×10²⁹/(6.25×10¹¹)≈3.20×10¹⁷ s≈1.01×10¹⁰ yr.
  6. Luminosity changes as the star evolves, only part of its hydrogen is accessible to core fusion, and some fusion energy can escape in neutrinos. A full stellar model must account for structure, composition and evolving reactions.

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