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RADIOACTIVITY!
Introduction:
Hey everyone! Today we’ll study about radioactive substances and the characteristics of the radiations they emit.
Radioactivity:
There are certain elements such as Radium which emit radiations. Such elements are called radioactive elements
and this phenomenon is called radioactivity. These radiations that these substances emit are of three types known as
alpha (α) particles, beta (β) particles and gamma (γ) rays.
Detection of Radioactivity:
There are several methods to detect the radioactivity, but the one that we’ll study is that using the Geiger-Muller tube
(G-M tube). It is the most sensitive detection device.
Now to coming to how it is used, here is how it actually looks like:
GM tube is basically a cylinder filled with a gas at low pressure. When alpha, beta or gamma radiations enter the
tube, they produce ions in the gas. The ions created in the gas enable the tube to conduct. A current is produced in
the tube for a short time. The current produces a voltage pulse. Each voltage pulse corresponds to one ionising
radiation entering the GM tube. The voltage pulse is amplified and counted. As shown, the tube is connected to the
counting circuit (rate meter) which counts this voltage pulse.
Now if you remove the radioactive source, the GM tube will still register a count of about 20 to 50 per minute. Why is
this? It’s due to the background radiations which are always present. This is called the background count. It is
subtracted from the final measurements if the emission rate form the radioactive source is low but if the rate is high, it
may be ignored without affecting the accuracy.
Characteristics of Alpha, Beta and Gamma:
1. Nature
What are these particles, actually? Okay. Alpha is the helium nucleus, not the helium atom itself, but the nucleus
only. We know that a nucleus carries positive charge, so alpha is a positively charged helium nucleus containing two
protons and two neutrons.
Beta particles are high-energy electrons and we know electrons carry negative charge.
Gamma rays, which we know are a part of electromagnetic spectrum, are those with the highest frequency in the
spectrum. Or we can say, rays with very short wavelength.
2. Ionizing effect
When fast moving alpha or beta particles collide with an atom, the atom becomes charged as an electron may be
ejected from it. Alpha particles have a very high ionizing power while beta particles have a small amount of it.
Gamma rays hardly ionize as they carry no charge.
3. Penetration
In the diagram above, you can see that an alpha particle cannot pass through paper. This is because it is a heavy
particle (a helium nucleus). Beta particles (electrons) can easily pass through paper while they are stopped by a 5mm
thick aluminium sheet. Gamma rays, on the other hand, are highly penetrating as they can pass easily through both
paper and aluminium. A 2cm thick lead can stop gamma rays.
4. Deflection
If these particles are placed in a magnetic field, they will be deflected. We have already studied in the tutorial on
Electromagnetism of how positive and negative charges are deflected in magnetic field. In this case, the same is
going to happen. The alpha particle will behave like a positive charge while a beta particle will behave like a negative
charge. The gamma rays are uncharged, hence they will be undeflected. The diagram makes it clearer:
Do you notice that the deflection of beta particles is much higher than alpha particles? Why is that? It’s due to their
masses. Electron has a mass nothing compared to the helium nucleus.
5. Speed
The speed of gamma rays will be that of the waves in electromagnetic spectrum i.e. 3 x 108
m/s.
The speed of beta particles is just less than that of gamma rays. While alpha particles have a lower speed compared
to both as it is a heavier particle. It’s speed is 107
m/s.
Half-Life:
Emission of these radiations occur randomly over time as a result of radioactive decay. Radioactive decay is a
process when a group of unstable nuclei decay to form stable nuclei. Half life of a sample of radioactive element is
the time taken for half of the unstable nuclei to decay.
The rate of decay at different times is called activity. Different elements have different half lives. It can be as much as
hundreds of years or as little as few hours. It depends. The activity (rate of decay) can be found using a GM tube
along with a counter.
The diagram shows how. The detector is the GM tube.
The count rate is measured at several intervals of time. Then a graph is plotted of count rate against time as shown:
Now initially, the count is 80. We have to calculate the half life of this certain element. Half life is the time taken for
half the particles to decay. That means time taken for 40, right? Now you should know how to read the graph, for 40 it
takes 6 days. Now 6 days is One half life. Two half lives means time taken for half of the first half particles, as in
further half, which is 20. It takes 12 days. For 10, 18 days. And so on..
The same graph with half-lives is shown.
Model of atom:
Rutherford, a scientist, performed an experiment where he aimed a source emitting a beam of alpha particles at a
thin piece of gold foil. Most of these passed straight through the gold-foil while a very small fraction of alpha particles
bounced back towards the source.
The diagram shows how this happens.
To see it closely for one atom, take a look at this diagram:
A strong repulsive force between alpha particles (which carry positive charge, we know) and gold nucleus (which
carries positive charge as well).
Nuclear Reactions:
Radioactive decay can be shown using nuclear equations. The parent nuclide X which is unstable is changed into Y,
which is more stable, with the emission of an alpha particle, a beta particle or gamma rays. Lets learn these three
different types of equations.
1. Alpha Decay
This is the general equation for alpha decay:
Q here is the energy released.
Consider the decay of Polonium as an example.
Energy (not shown) is also released.
2. Beta Decay
The general equation for beta decay:
Now take carbon as an example, this will be the equation for its decay.
3. Gamma decay
This is the general equation for gamma decay:
The * indicates unstable form or excited state of X. At this moment, gamma rays are emitted.
Nuclear Fission:
Uranium-236 is an isotope of uranium and is unstable, so it breaks down into two nearly equal nuclei. The equation
for this is:
As you can see that in nuclear fission a larger particle is broken down into smaller ones. Now coming to fusion, it’s
opposite.
Nuclear Fusion:
In fusion, however, smaller particles ‘fuse’ together, as the name indicates, and form a larger one. Energy is released
in this process.In both situations, energy is released due to loss in mass.
As you can see that in nuclear fission a larger particle is broken down into smaller ones. Now coming to fusion, it’s
opposite.
Nuclear Fusion:
In fusion, however, smaller particles ‘fuse’ together, as the name indicates, and form a larger one. Energy is released
in this process.In both situations, energy is released due to loss in mass.

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Radioactivity

  • 1. RADIOACTIVITY! Introduction: Hey everyone! Today we’ll study about radioactive substances and the characteristics of the radiations they emit. Radioactivity: There are certain elements such as Radium which emit radiations. Such elements are called radioactive elements and this phenomenon is called radioactivity. These radiations that these substances emit are of three types known as alpha (α) particles, beta (β) particles and gamma (γ) rays. Detection of Radioactivity: There are several methods to detect the radioactivity, but the one that we’ll study is that using the Geiger-Muller tube (G-M tube). It is the most sensitive detection device. Now to coming to how it is used, here is how it actually looks like: GM tube is basically a cylinder filled with a gas at low pressure. When alpha, beta or gamma radiations enter the tube, they produce ions in the gas. The ions created in the gas enable the tube to conduct. A current is produced in the tube for a short time. The current produces a voltage pulse. Each voltage pulse corresponds to one ionising radiation entering the GM tube. The voltage pulse is amplified and counted. As shown, the tube is connected to the counting circuit (rate meter) which counts this voltage pulse. Now if you remove the radioactive source, the GM tube will still register a count of about 20 to 50 per minute. Why is this? It’s due to the background radiations which are always present. This is called the background count. It is subtracted from the final measurements if the emission rate form the radioactive source is low but if the rate is high, it may be ignored without affecting the accuracy. Characteristics of Alpha, Beta and Gamma: 1. Nature What are these particles, actually? Okay. Alpha is the helium nucleus, not the helium atom itself, but the nucleus only. We know that a nucleus carries positive charge, so alpha is a positively charged helium nucleus containing two protons and two neutrons. Beta particles are high-energy electrons and we know electrons carry negative charge. Gamma rays, which we know are a part of electromagnetic spectrum, are those with the highest frequency in the spectrum. Or we can say, rays with very short wavelength. 2. Ionizing effect
  • 2. When fast moving alpha or beta particles collide with an atom, the atom becomes charged as an electron may be ejected from it. Alpha particles have a very high ionizing power while beta particles have a small amount of it. Gamma rays hardly ionize as they carry no charge. 3. Penetration In the diagram above, you can see that an alpha particle cannot pass through paper. This is because it is a heavy particle (a helium nucleus). Beta particles (electrons) can easily pass through paper while they are stopped by a 5mm thick aluminium sheet. Gamma rays, on the other hand, are highly penetrating as they can pass easily through both paper and aluminium. A 2cm thick lead can stop gamma rays. 4. Deflection If these particles are placed in a magnetic field, they will be deflected. We have already studied in the tutorial on Electromagnetism of how positive and negative charges are deflected in magnetic field. In this case, the same is going to happen. The alpha particle will behave like a positive charge while a beta particle will behave like a negative charge. The gamma rays are uncharged, hence they will be undeflected. The diagram makes it clearer: Do you notice that the deflection of beta particles is much higher than alpha particles? Why is that? It’s due to their masses. Electron has a mass nothing compared to the helium nucleus. 5. Speed The speed of gamma rays will be that of the waves in electromagnetic spectrum i.e. 3 x 108 m/s.
  • 3. The speed of beta particles is just less than that of gamma rays. While alpha particles have a lower speed compared to both as it is a heavier particle. It’s speed is 107 m/s. Half-Life: Emission of these radiations occur randomly over time as a result of radioactive decay. Radioactive decay is a process when a group of unstable nuclei decay to form stable nuclei. Half life of a sample of radioactive element is the time taken for half of the unstable nuclei to decay. The rate of decay at different times is called activity. Different elements have different half lives. It can be as much as hundreds of years or as little as few hours. It depends. The activity (rate of decay) can be found using a GM tube along with a counter. The diagram shows how. The detector is the GM tube. The count rate is measured at several intervals of time. Then a graph is plotted of count rate against time as shown: Now initially, the count is 80. We have to calculate the half life of this certain element. Half life is the time taken for half the particles to decay. That means time taken for 40, right? Now you should know how to read the graph, for 40 it takes 6 days. Now 6 days is One half life. Two half lives means time taken for half of the first half particles, as in further half, which is 20. It takes 12 days. For 10, 18 days. And so on..
  • 4. The same graph with half-lives is shown. Model of atom: Rutherford, a scientist, performed an experiment where he aimed a source emitting a beam of alpha particles at a thin piece of gold foil. Most of these passed straight through the gold-foil while a very small fraction of alpha particles bounced back towards the source. The diagram shows how this happens. To see it closely for one atom, take a look at this diagram:
  • 5. A strong repulsive force between alpha particles (which carry positive charge, we know) and gold nucleus (which carries positive charge as well). Nuclear Reactions: Radioactive decay can be shown using nuclear equations. The parent nuclide X which is unstable is changed into Y, which is more stable, with the emission of an alpha particle, a beta particle or gamma rays. Lets learn these three different types of equations. 1. Alpha Decay This is the general equation for alpha decay: Q here is the energy released. Consider the decay of Polonium as an example. Energy (not shown) is also released. 2. Beta Decay The general equation for beta decay: Now take carbon as an example, this will be the equation for its decay. 3. Gamma decay This is the general equation for gamma decay: The * indicates unstable form or excited state of X. At this moment, gamma rays are emitted. Nuclear Fission: Uranium-236 is an isotope of uranium and is unstable, so it breaks down into two nearly equal nuclei. The equation for this is:
  • 6. As you can see that in nuclear fission a larger particle is broken down into smaller ones. Now coming to fusion, it’s opposite. Nuclear Fusion: In fusion, however, smaller particles ‘fuse’ together, as the name indicates, and form a larger one. Energy is released in this process.In both situations, energy is released due to loss in mass.
  • 7. As you can see that in nuclear fission a larger particle is broken down into smaller ones. Now coming to fusion, it’s opposite. Nuclear Fusion: In fusion, however, smaller particles ‘fuse’ together, as the name indicates, and form a larger one. Energy is released in this process.In both situations, energy is released due to loss in mass.