CAIE A-Level Physics 23 Nuclear Physics
Practise using mass defect, binding energy, nuclear equations and decay laws to calculate energy release, compare reactions and interpret radioactive data.
- Syllabus
- 2028–2030
- Course
- Physics 9702
- Level
- A2
Practise using mass defect, binding energy, nuclear equations and decay laws to calculate energy release, compare reactions and interpret radioactive data.
Use data from (b) to calculate the mass that is converted into energy every second in the Sun.
mass = kg
m=c2E=3.00×10823.83×1026=4.26×109 kg
A1
A radiation detector is placed close to a radioactive source. The detector does not surround the source.
Radiation is emitted in all directions and, as a result, the activity of the source and the measured count rate are different.
Suggest two other reasons why the activity and the measured count rate may be different.
1.
2.
emission from radioactive daughter products
- self-absorption in source
- absorption in air before reaching detector
- detector not sensitive to all radiations
- window of detector may absorb some radiation
- dead-time of counter
- background radiation
Any two points.
B2
The variation with time t of the measured count rate in (a) is shown in Fig. 12.1.

Fig. 12.1
State the feature of Fig. 12.1 that indicates the random nature of radioactive decay.
curve is not smooth
or
curve fluctuates/curve is jagged
B1
Use Fig. 12.1 to determine the half-life of the radioactive isotope in the source.
half-life = hours
clear evidence of allowance for background
B1
half-life determined at least twice
B1
half-life = 1.5 hours
(1 mark if in range 1.7-2.0; 2 marks if in range 1.4-1.6)
A2
The readings in (b) were obtained at room temperature.
A second sample of this isotope is heated to a temperature of 500∘C.
The initial count rate at time t=0 is the same as that in (b).
The variation with time t of the measured count rate from the heated source is determined.
State, with a reason, the difference, if any, in
1. the half-life,
2. the measured count rate for any specific time.
1. half-life: no change
M1
because decay is spontaneous/independent of environment
A1
2. count rate (likely to be or could be) different/is random/cannot be predicted
B1
State what is meant by nuclear fusion and nuclear fission.
nuclear fusion:
nuclear fission:
fusion: two nuclei combine to form a (single) nucleus
B1
fission: a (single) large nucleus divides to form (smaller) nuclei
B1
Any one from:
- fusion is initiated by (very) high temperatures
- fission is initiated by neutron bombardment
- resulting nuclei in fission are of similar size
- (both processes) release energy
- binding energy per nucleon increases
- total binding energy increases
- fission involves release of neutrons
B1
A nuclear reaction which may, in the future, be used for the generation of electrical energy is
Name the particle x .
neutron
B1
Data for the binding energy per nucleon EB of some nuclei are given in Fig. 12.1.

Fig. 12.1
1. State the binding energy per nucleon of x .
2. Calculate the energy change that takes place in this reaction.
1. zero
A1
2. (4×11.3290×10−13)−(2×1.7813×10−13)−(3×4.5285×10−13)
C1
energy change =45.316×10−13−17.148×10−13=2.82×10−12 J
A1
Use your answer in (ii) part 2 to determine the energy release when 2.0 g of deuterium (12H) reacts with 3.0 g of tritium (13H).
1.0 mol or NA nuclei of each
energy =2.817×10−12×6.02×1023=1.7×1012 J
A1