In this module, we explore the properties of radiation. We discover the potential hazards of radiation and how these can be managed to safely use radiation in a range of applications. We delve into some of the maths of radioactive decay and have a go at modelling it in an edible experiment using sweets!
2.1: Radiation Dosages (Questions)
2.2: Modelling the interactions between radiation and matter (Online Simulation)
2.3: Properties of Radiation (Questions)
2.4: Skittlium - Modelling radioactive decay with Skittles (Experiment)
2.5: Radiocarbon Dating and Half Lives (Questions)
In the video below, nuclear physicist Dr Liam Gaffney from the University of Liverpool explains how we measure radioactivity and the effects that different types of radiation can have. Find out about the banana equivalent scale and why radiation is around us all the time.
As Liam explained in the video above, small amounts of radiation are around us all the time and are harmless. This is called background radiation, and it comes from both natural and artificial sources.
Natural radiation is given out by rocks and soil, cosmic rays (coming from the Sun and stars), and all living things – even us! A more dangerous source is the radioactive gas, radon. You can check to see if this is a risk in your area on the UK Radon Map.
Artificial sources of radiation also contribute to this background level. However, our highest dosage comes from medical uses - both imaging and treatments. We will learn more about this in Module 4. Other man-made sources include the fallout from nuclear weapons testing and nuclear accidents.
A person's radiation dose from this background radiation will vary depending on many factors, such as their job and where they live. Dosage is measured in sieverts (Sv). Bananas, which are very good for us, are a natural source of potassium – an isotope of which is radioactive. Eating one banana gives us a dose of 0.1µSv. We can use this as a way to measure radiation dose: it’s called the banana equivalent dose (BED).
Check out some examples of the banana equivalent dose:
Have a look at the fascinating XKCD Radiation Dose Chart below. This lists lots of everyday sources of radiation, as well as explaining what radiation doses would be fatal.
The reason radiation can cause harm is that it is ionising.
Normally, in an atom, there are an equal number of protons and electrons. This makes the atom electrically neutral. If an atom gains or loses electrons, this creates an ion. A positive ion is where an atom has lost electrons, and a negative ion is where an atom has gained electrons.
Ionising radiation, such as alpha, beta, and gamma radiation, can cause ionisation by stripping an atom of one or more of its electrons, turning the atom into a positive ion. Since the atom becomes charged, it is more likely to take part in chemical reactions. This can be dangerous if it happens inside the body. For example, if your DNA becomes damaged, this can cause cancer.
The more massive and charged the radiation is, the more ionising it is and the less it is able to penetrate. This is summarised for alpha particles (24⍺), beta particles (-10ꞵ), and gamma rays (00𝛾) in the table below.
Figure 1: The types of ionising radiation and their penetration power.
Log in to Isaac Physics and answer the questions:
Radiation Dosage
Radiation Dosages and the Effects of Radioactivity
Don't forget to log in to Isaac Physics!
As well as conducting experiments, advanced software can simulate how different types of radiation (such as alpha, beta, and gamma) interact with different materials - everything from air, to lead and concrete, to body tissue and bones. This allows accurate predictions to be made before technical equipment is built, or medical treatments are given, for example.
Figure 2: Visualisation of GEANT4 simulation of a proton in air.
Simulations such as this not only provide images, like that above, of what would happen in a particular experiment, but they also output lots of data. In the next activity, you will use the data output from a piece of software called Geant 4 in order to investigate the properties of different types of radiation.
We can pull meaningful data out from these simulations by putting them into different software which analyses the data. These software packages look at the data and allow us to see how the energy deposition changes with depth into the material and the divergence from the beam line for different particles. This analysis takes files that are over 80 gigabytes in size (each!) and turns them into graphs which are a couple of megabytes - far easier to store!
We have used these GEANT4 simulations to create a web application that allows you to simulate these ground-breaking treatment methods, as well as explore other properties of radiation, in real time. The app is simple to use, requiring only a couple of inputs to generate real data.
Figure 3: Annotated screenshot from the simulation showing parameters that can be controlled
There are three different outputs from the simulation. Figure 4 (below) shows the 'Energy Deposition vs Depth' option. The radiation will deposit energy when it is absorbed into the material. This means that it does not travel any further.
Figure 4: Annotated screenshot from the simulation showing a graph of Energy Deposition vs Depth
You will only need this graph option to answer the questions in Activity 2.3. However, you may also want to explore the two other outputs. The first of these shows the energy deposited (using colour coding) both in terms of depth into the material (as in the graph above), but also in terms of the distance from the beam (on the y-axis). The second shows the particle tracks, which are generated from the data each time the simulation is run.
Try investigating different types of radiation, different energies, different materials, and different thicknesses of material. What patterns do you notice? Once you have experimented with this simulation, have a go at the Questions in Activity 2.3 (below).
Access the radiation and matter interaction simulation
Figure 3 (above) shows the different parameters you can control within the simulation. You can choose between different types of radiation (remember that beta radiation is an electron) and also select the energy of the particle. The units of energy used here are MeV (mega electron volts). These are the most common unit used in particle physics. One electron volt (eV) is the energy gained by an electron when accelerated by a potential difference of one volt, or 1eV = 1.6 x 10-19 J.
You can also select the material that the radiation is travelling through (water, paper, concrete etc), and the thickness of the material. Note that 'soft tissue' refers to tissue in the body such as muscle, fat or blood vessels, and not the type of tissue you sneeze into!
Log into Isaac Physics and answer questions:
Properties of Radiation: Simulation Questions
You will need to use the simulation above to generate "Energy Deposition vs Depth" figures to answer these questions!
Don't forget to log in to Isaac Physics!
Radiation is usually invisible to us. However, one way that we can actually see the paths of these particles is with a cloud chamber. Find out all about how these were invented and how they work in the video below, produced by post-graduate researcher Alexander Backis from the University of Glasgow.
Cloud chambers give us a very visual representation of the particles. However, they are not portable, and they do not provide much data beyond the type of particle.
A more common device for detecting radiation is a Geiger Counter, also known as a Geiger-Müller tube. This registers a click every time it encounters a particle of ionising radiation. This measures the count rate of a source, (number of decays recorded a second).
From this, we can calculate the activity. The activity is the rate at which a source of radioactive/unstable nuclei decays, measured in decays per second. The unit of activity is the becquerel (Bq) where 1 Bq = 1 decay per second.
Even the Geiger Counter is limited in what it can do. In the video below, nuclear physicist Dr Jamie Brown from the University of York talks about a new type of detector that is so small that it can be carried in a pocket (it's about the same size as a mobile phone). It can also identify the isotope that is the source of the radiation!
Matylda Sękpl.wiki: Cygaretkacommons: Cygaretka, CC BY-SA 3.0, via Wikimedia Commons
Radioactive decay is a random process. In a sample of radioactive material, there are lots and lots of nuclei. We can't predict which nucleus will decay next, or when any particular nucleus will decay, and not all nuclei will decay at the same time. Instead, we know that a certain number of nuclei will decay in a certain time. The time taken for half the unstable nuclei in a sample to decay is called the half life, (t1/2).
There are two important definitions of half life:
The time it takes for the number of radioactive nuclei in a sample to decrease by 50%.
The time it takes for the activity/count rate of a radioactive source to decrease by 50%.
We cannot affect the half life of an isotope - changing the temperature or pressure, for example, make no difference. Some isotopes have very short half lives of only a few seconds, whilst others can be thousands of years.
Just like radioactive decay, tossing a coin is also a random process because we don't know whether a particular coin will be heads or tails. We can therefore use coins, or anything else that has two different sides (such as Skittles!) to model radioactive decay.
To do this experiment, you will need a small bag of Skittles (or at least 20 objects that have two distinct sides - coins work well, but you can just use scraps of paper with an X on one side)
Count the number of sweets (or objects) that you start with - these are your unstable nuclei. Record this number in a table for time = 0
Place the sweets in a cup and shake them
Pour the sweets onto the table
Count any sweets with an ‘s’ facing up. These represent nuclei that haven’t decayed yet. Record this number in your table for time = 1 and put these sweets back into the cup (You can eat any Skittles that land 's' side down!)
Shake and throw the sweets again, keeping and recording any sweets that land 's' up (and eating the rest)
Repeat until all your skittles have decayed!
Now plot a graph of the time along the x-axis and the number of radioactive nuclei on the y-axis.
Find the half life of your sweets (or other objects) by reading off the time when half of your sweets have 'decayed' (see graph below).
To improve the accuracy of the half life, take another two points on your graph where the number of unstable nuclei have halved and take an average of your two half lives.
One application of half lives is Radiocarbon Dating. This is the process of determining the age of a previously living object by measuring the ratio of carbon-14 to carbon-12 present, (carbon-14 is unstable, and decays to nitrogen-14, whereas carbon-12 is stable). This is explained by Archaeologist Dr Penny Bickle from the Universityisty of York in the video below.
Log in to Isaac Physics and answer the questions:
Carbon Dating
Definition of Half Life
Decay Fractions
Half-Life 1 to Half-Life 5
Don't forget to log in to Isaac Physics!
ISIS Neutron and Muon Source is a world-leading centre for research at the STFC Rutherford Appleton Laboratory. Their neutron and muon instruments give unique insights into the properties of materials on the atomic scale.
Find out why neutrons make excellent probes for materials here; or take a 360 degree tour here; or why not see some of the exciting jobs at ISIS in the staff profiles here.
Boulby Underground Laboratory is the UK’s deep underground science facility, located 1.1km below ground in Boulby mine, a working potash, polyhalite and salt mine in the North East of England.
Find out more about this amazing facility in this short video.
Watch a video of Boulby's Emma Meehan, explaining her amazing career path - from cleaner, to the Institute of Physics' Technician Award winner in 2019, to her current role as Facility Manager.
CERN is most well known for the Large Hadron Collider - the largest and most powerful particle accelerator in the world. With a 27km ring of superconducting magnets accelerating two beams of particles to almost the speed of light in opposite directions, UK membership of CERN gives physicists and engineers access to some of the world’s biggest and most complex scientific instruments to study the basic building blocks of matter.
CERN has lots of interesting reading and engaging content on their website. We particularly like this virtual tour of the Large Hadron Collider.