Radioactive Decay

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Radioactive Decay

We have looked at the properties of alpha, beta and gamma decay. Each of these may be emitted as part of radioactive decay. 

What is Radioactive Decay?

Radioactive decay is the random and spontaneous decay of the nucleus of an atom to become more stable, resulting in the emission of alpha, beta or gamma radiation

When looking closely at a radioactive source, it is impossible to predict which nucleus will decay and when it will decay. This is because the process is completely random. It is also important to remember that no changes in the conditions surrounding a source will affect its rate of decay. 

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Activity

The activity (A) of a radioactive source is the average number of nuclei that decay per unit of time. Notice two things from this definition:

  • Average – as radioactive decay is random, the number of nuclei that decay per unit of time varies. We can however state the average number of decaying nuclei per unit of time.
  • The definition states per unit of time. This unit of time can vary depending upon which isotope is being observed and how quickly they decay. 

A radioactive source that is described as highly radioactive has a high activity. This is measured in Becquerels (Bq)text{(Bq)} where 1 Bq=1bold{1} text{ Bq}= bold{1} decaying nuclei per second

The equation used to calculate activity is as follows:

A=ΔNΔtA=dfrac{Delta N}{Delta t}

  • A=A= the activity in becquerels (Bq)text{(Bq)}
  • ΔN=Delta N= the number of decayed nuclei 
  • Δt=Delta t= the change in time in seconds (s)text{(s)}

Example: Over a period of one hour, a GM counter detects 25,00025,000 counts of radiation. What is the activity of the source? The background radiation has been measured at 11 count per second.

[3 marks]

Substitute the given values into the activity equation:

A=ΔNΔt=25,00060×60= 6.9 Bqbegin{aligned} bold{A} &= bold{dfrac{Delta N}{Delta t}} &= dfrac{textcolor{f43364}{25, 000}}{textcolor{10a6f3}{60 times 60}} &=  bold{6.9} text{ Bq} end{aligned}

Subtract the background radiation:

6.91=5.9 Bq6.9 – textcolor{00d865}{1} = bold{5.9} textbf{ Bq}

We can also use the decay constant (λ)(lambda) to describe how radioactive a source is. The decay constant is the probability that a nuclei will decay per second. Decay constant is related to activity using the following equation:

A=λNA= lambda N

  • A=A= the activity in becquerels (Bq)text{(Bq)}
  • λ=lambda = the decay constant per second (s1)text{(s}^{-1}text{)}
  • N=N= the number of nuclei in a sample

Example: A source contains 6×10246 times 10^{24} undecayed nuclei. If the decay constant is 2.1×106 s12.1 times 10^{-6} text{ s}^{-1}, calculate the activity of the source.

[2 marks]

Substitute the values into the equation linking activity and decay constant:

A=λN=2.1×106×6×1024=1.3×1019 Bqbegin{aligned} bold{A} &= bold{lambda N} &= textcolor{f95d27}{2.1 times 10^{-6}} times textcolor{ffad05}{6 times 10^{24}} &= bold{1.3 times 10^{19}} textbf{ Bq} end{aligned}

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Exponential Decay

It’s common to see radioactive decay graphs like the one below. This graph shows how the number of undecayed nuclei (N)text{(N)} varies with time (t)text{(t)}

This type of decay curve is an exponential decay curve. The number of nuclei begins to decay from N0 (initial number of nuclei) rapidly but the rate of decay slows over time until almost reaching zero. 

The steeper slope, represented above in black, shows a decay with a higher decay constant compared to the shallower red line. 

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Radioactive Decay Equations

Because of the nature of exponential decay, it can be difficult to predict how many nuclei would be remaining in a sample after a certain amount of time. A calculation can be completed to calculate this number:

N=N0eλtN=N_0e^{-lambda t}

  • N=N= the number of undecayed nuclei 
  • N0=N_0= the initial number of undecayed nuclei
  • λ=lambda = the decay constant per second (s1)text{(s}^{-1}text{)}
  • t=t= the time in seconds (s)text{(s)}

As the activity of a source and the count rate also decays exponentially, the equation may also be written as:

A=A0eλtA=A_0 e^{- lambda t}

  • A=A= the activity at a given time (t) in becquerels (Bq)text{(Bq)}
  • A0A_0 the initial activity in becquerels (Bq)text{(Bq)}
  • λ=lambda= the decay constant per second (s1)text{(s}^{-1}text{)}
  • t=t= the time in seconds (s)text{(s)}

C=C0eλtC=C_0 e^{-lambda t}

  • C=C= the count rate at a given time (t) (s1, min1 or hour1 etc)(text{s}^{-1}text{, min}^{-1}text{ or hour}^{-1} text{ etc})
  • C0=C_0= the initial count rate (s1, min1 or hour1 etc)(text{s}^{-1}text{, min}^{-1}text{ or hour}^{-1} text{ etc})
  • λ=lambda = the decay constant per second (s1)text{(s}^{-1}text{)}
  • t=t= time in seconds (s)text{(s)}

Example: A source contains 6×10246 times 10^{24}. If the decay constant of 2.1×106 s12.1 times 10^{-6} text{ s}^{-1}, calculate the activity of the source after 11 year.

[4 marks]

Convert 11 year to seconds:

t=1 year=1×365×24×60×60=31536000 st= textcolor{ffad05}{1 text{ year}} = 1 times 365 times 24 times 60 times 60 = textcolor{f95d27}{bold{31 , 536 , 000} textbf{ s} }

Calculate the initial activity:

A=λNA0=2.1×106×6×1024)=1.26×1019 Bqbegin{aligned} A &= lambda N A_0 &= textcolor{00bfa8}{2.1 times 10^{-6}} times textcolor{d11149}{6 times 10^{24}}) &= textcolor{aa57ff}{bold{1.26 times 10^{19}}} textbf{ Bq} end{aligned}

Substitute values into the equation for decay in activity:

A=A0eλt=1.26×1019×e(2.1×106×31536000)=2.25×1010 Bqbegin{aligned} bold{A} &= bold{A_0 e^{-lambda t}} &= textcolor{aa57ff}{1.26 times 10^{19}} times e^{-(textcolor{00bfa8}{2.1 times 10^{-6}} times textcolor{f95d27}{31 , 536 , 000}}) &= bold{2.25 times 10^{-10}} textbf{ Bq} end{aligned}

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Half-life

The half-life of a sample is the time taken for the number of radioactive nuclei to halve. Therefore, it could also be defined as the time taken for the activity or count rate to halve. The half-life of a sample can be calculated using the equation:

t12=ln(2)λt_{dfrac{1}{2}}= dfrac{ln(2)}{lambda}

  • t12=t_{dfrac{1}{2}}= the half-life in seconds, minutes, hours, days or years
  • λ=lambda= the decay constant per second (s1)text{(s}^{-1}text{)}

Example: A source of radiation has a decay constant of 0.04 s10.04 text{ s}^{-1}. What is its half life? 

Substitute into the equation for half-life:

t12=ln(2)λ=ln(2)0.04=17.3 sbegin{aligned} bold{t_{dfrac{1}{2}}} &= bold{dfrac{ln(2)}{lambda}} &= dfrac{ln(2)}{textcolor{00d865}{0.04}} &= bold{17.3} textbf{ s} end{aligned}

Alternatively, half-life can be calculated graphically. By taking two values for activity (one exactly half of the other) and their corresponding times, the half-life can be found.

Example: Use the graph to calculate the half-life of this radioactive source. 

[2 marks]

Choose two values for activity from the graph, one half the othet:

A0=290 Bq and A1=145 BqA_0=290 text{ Bq and } A_1=145 text{ Bq} 

Read off the corresponding times: = 0 s and 9.5 s

t0=0 s and t1=9.5 st_0= 0 text{ s and }t_1=9.5 text{ s}

Therefore:

half-life=9.5 stext{half-life}= bold{9.5} textbf{ s}

Knowledge of half-life can have some practical applications. For example, carbon14-14 is a radioactive isotope with a half-life of 54005400 years. By measuring the amount of carbon14-14 in an artefact, the artefact can be dated. This is known as carbon dating

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Radioactive Decay Example Questions

Question 1: Over a period of one day, a GM counter detects 6×1066times 10^6 counts of radiation. What is the activity of the source?

[2 marks]

A Level AQA

1 day =24×60×60=86400 sA=ΔNΔt=6×10686400=69.4 Bq1 text{ day}  = 24 times 60 times 60 = 86400 text{ s} begin{aligned} bold{A} &= bold{dfrac{Delta N}{Delta t}} &= dfrac{6 times 10^6}{86400} &= bold{69.4} textbf{ Bq}end{aligned}

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Question 2: State what is meant by the half-life of a radioactive sample? 

[1 mark]

A Level AQA

The time taken for the number of nuclei/activity/count rate to decrease by half.

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Question 3: A radioactive source has a half-life of 20 s20 text{ s}. Calculate its decay constant. 

[2 marks]

A Level AQA

t12=ln(2)λλ=ln(2)t12=ln(2)20=0.035 s1begin{aligned} bold{t_{dfrac{1}{2}}} &= bold{dfrac{ln(2)}{lambda} } lambda &= dfrac{ln(2)}{t_{dfrac{1}{2}}} &= dfrac{ln(2)}{20} &= bold{0.035} textbf{ s}bold{^{-1}} end{aligned}

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Specification Points Covered

AQA A-level:

  • 3.8.1.3 Radioactive decay (A-level only)