5.1.7
Radioactive Decay
Radioactive Decay
Radioactive Decay
When an object is radioactive it releases radioactive particles but as time passes the rate of particles decreases. This is called decay.
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Random decay
Random decay
- The decay of a radioactive substance is random and unpredictable.
- To measure decay, we must look at the count rate over a long time to see if it decreases.
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Probability
Probability
- The probability that a given nucleus will decay in a given time is proportional to the number of nuclei. The equation for calculating the rate of decay is:
- The rate of decay of nuclei = decay constant x the number of nuclei
- is the decay constant.
- is the number of nuclei.
The Exponential Law
The Exponential Law
The reduction in the rate of decay decreases according to an exponential pattern.


Exponential decay
Exponential decay
- From the equation for the rate of decay, we can find an exponential relationship between the number of nuclei and time.
- The equation for the rate of decay of nuclei is:
- The exponential relationship corresponding to this is:
- is the initial number of nuclei.


Activity
Activity
- The activity of a sample can be found by using the decay constant and the number of nuclei. The equation for activity is:
- Activity = decay constant x number of nuclei
- The exponential relationship corresponding to the activity is:
Half-Life
Half-Life
Although each nuclear decay is random, with a large collection of nuclei, we can statistically predict how many will decay after a certain time.
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Time taken to halve
Time taken to halve
- Half-life, T1/2, is the time taken:
- For the number of radioactive nuclei in a sample to halve.
- For the activity (the number of decays per second) to halve.


Activity
Activity
- The activity of a sample is directly proportional to the number of nuclei remaining:
- Activity = decay constant, λ x number of nuclei remaining.
- Activity is related to the half life:


Activity 2
Activity 2
- By knowing the activity, we can infer how many nuclei are remaining.
- Knowing the atomic mass of an isotope and the mass of a sample of isotope enables the number of nuclei and so the activity to be found.


Example
Example
- Find the half-life of a sample of plutonium-239, which has a mass of 1200 g and an activity of 2.8 × 1012 Bq:
- Number of moles of Pu-239 = 1200 ÷ 239 = 5.021.
- Number of nuclei = number of moles × Avogadro’s constant = 3.02 × 1024.
- λ = activity ÷ number of nuclei = 9.26 × 10-13.
- So, half-life T1/2 = ln(2) ÷ λ = 7.5 × 1010 s.
1Space, Time & Motion
1.1Motion
1.2Forces
1.3Momentum & Impulse
2The Particulate Nature of Matter
2.1Thermal Concepts
3Wave Behaviour
3.1Oscillations
3.2Travelling Waves
3.3Wave Characteristics
3.4Wave Behaviour
3.5Standing Waves
3.6Simple Harmonic Motion
3.7Single Slit Diffraction
3.8Interference
3.9Doppler Effect
4Fields
4.1Circular Motion
4.2Newton's Law of Gravitation
4.3Fields
4.4Fields at Work
4.5Electric Fields
4.6Magnetic Effect of Electric Currents
4.7Heating Effect of Currents
4.8Electromagnetic Induction
4.9Power Generation & Transmission
5Nuclear & Quantum Physics
5.1Discrete Energy & Radioactivity
5.2Nuclear Reactions
5.3The Interaction of Matter with Radiation
6Measurements
6.1Measurements & Errors
6.2Uncertainties & Errors
6.3Vectors & Scalars
Jump to other topics
1Space, Time & Motion
1.1Motion
1.2Forces
1.3Momentum & Impulse
2The Particulate Nature of Matter
2.1Thermal Concepts
3Wave Behaviour
3.1Oscillations
3.2Travelling Waves
3.3Wave Characteristics
3.4Wave Behaviour
3.5Standing Waves
3.6Simple Harmonic Motion
3.7Single Slit Diffraction
3.8Interference
3.9Doppler Effect
4Fields
4.1Circular Motion
4.2Newton's Law of Gravitation
4.3Fields
4.4Fields at Work
4.5Electric Fields
4.6Magnetic Effect of Electric Currents
4.7Heating Effect of Currents
4.8Electromagnetic Induction
4.9Power Generation & Transmission
5Nuclear & Quantum Physics
5.1Discrete Energy & Radioactivity
5.2Nuclear Reactions
5.3The Interaction of Matter with Radiation
6Measurements
6.1Measurements & Errors
6.2Uncertainties & Errors
6.3Vectors & Scalars
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