Radioactivity Flashcards
Who proposed the first nuclear model of the atom?
Ernest Rutherford
Describe Rutherford’s experiment
A thin beam of alpha particles (all with the same kinetic energy) from a source in an evacuated metal container, aimed at a thin metal foil. A microscope with a fluorescent screen at the end rotating round the metal container from 0-almost 180 degrees. He measured the number of alpha particles reaching the detector per minute for different angles
Describe the results for Rutherford’s experiment
- Most alpha particles passed straight through the foil with little or no deflection; about 1 in 2000 were deflected
- A small percentage of alpha particles (about 1 in 10000) were deflected through angles greater than 90 degrees
Give 3 conditions Rutherford had to have in his experiment and why
1) The alpha particles must have had the same speed (otherwise slow particles would be deflected more than fast particles on the initial path)
2) The container must be evacuated (otherwise alpha particles would be stopped by air molecules)
3) The source of the alpha particles must have a long half life (otherwise later readings would be lower than earlier readings due to radioactive decay of the source)
Describe the deflection of alpha, beta and gamma radiation for a magnetic field into the page in Rutherford’s investigation of radioactivity where the beam of radioactive particles enter the field from the left
Alpha particles move up the page (because the current moves in the same way as they do - due to their +ve charge)
Beta particles move down the page (because the current moves in the opposite way as they do - due to their -ve charge)
Gamma radiation remains unchanged (due to it being uncharged)
Describe and explain an experiment to investigate the ionising effect of each type of radiation.
A radioactive source is held over an ionisation chamber full of air at atmospheric pressure and a central electrode connected to a picoammeter, a battery supply and a wall electrode. Ions created in the chamber are attracted to the oppositely charged electrode where they are discharged. Electrons move through the picoammeter as a result of ionisation and thus the current is proportional to the number of ions per second created in the chamber.
Describe the ionising effect of each type of radiation in an ionisation chamber
- Alpha radiation: causes strong ionisation but ionisation ceases beyond a certain distance if the source is moved away (about 1cm). This is because the particles ionise air molecules.
- Beta radiation: has a weaker ionising effect than alpha radiation but its range in air varies up to a metre or more.
- Gamma radiation: has a much weaker ionising effect than both alpha or beta radiation. This is because the photons carry no charge.
Explain how cloud chambers work within radioactivity experiments
The cloud chamber contains air saturated with a vapour at a very low temperature. Because the air is supersaturated, when an ion (caused by ionising particles) passes through the vapour, the ions trigger the formation of droplets in a vapour trail.
Describe the 2 different signals that indicate both alpha and beta particles in a cloud chamber.
- Alpha particles - produce straight tracks which radiate from the source and are easily visible. The tracks from the same isotope are all of the same length
- Beta particles - produce wispy tracks that are easily deflected as a result of collision with air molecules. The tracks are less easily seen because they Beta particles are less ionising than alpha particles.
Describe the equipment involved in a test to measure the absorption of radiation for different materials.
A source in a sealed container whose radioactive emissions pass through an absorber and into a Geiger tube, which measures the count rate (counts / time)
Describe the process of how the radioactive absorption for different materials would be measured.
A source would be set up in front of the material and a Geiger tube. The count rate would be measured without the source or an absorber present to record the background radiation. The background count rate would then be subtracted from the recorded count rate with the source to give the corrected/true count rate from the source.
The count rate would then be measured with the absorber in a fixed position and the count rates would be compared for varying thicknesses of material.
Describe a Geiger tube and explain how it works
The Geiger tube is a sealed metal tube that contains gaseous Argon at low pressure. The thin mica window at the end of the tube allows alpha and beta particles to enter (gamma can enter through the wall).
A thin metal rod down through the tube has a positive potential whilst the tube wall is connected to the negative terminal of the power supply and is earthed. This circuit is connected to a pulse counter.
When an ionising particle enters the tube, it ionises gas particles it collides with, which accelerate towards the oppositely charged terminal, ionising more air particles on the way. The discharge of these ions at the terminals creates a pulse of charge which is detected by the pulse counter.
Explain what the dead time of a Geiger tube is and explain why the count rate should never exceed about 5000s^(-1)
The dead time is the time taken for the tube to regain its non-conducting state after ionising particles enter it.
It is typically of the order 0.2ms, therefore the count rate should not exceed 5000s^(-1) (1/0.2ms)
Describe the charge and makeup of an alpha particle
The nucleus of a Helium atom and is positively charged
Describe the set-up and explain how Rutherford devised the structure of alpha particles
He filled a tube ,fitted with two electrodes, with gaseous alpha particles. He applied a voltage, the gas conducted electricity and emitted light.
Using a spectrometer, he proved that the spectrum of light from the tube was the same as that from a tube filled with helium gas.
Describe how Beta radiation was proved to be fast moving electrons
A beam of Beta particles were deflected in electric and magnetic fields. The measurements of deflection were used to calculate the specific charge of the beta particles, which was the same as the specific charge of a electron.
Give the equation for the intensity (I) of gamma radiation at distance r from the source in terms of k and give the value of k if the source emits n number of photons per second
I = k / r^(2)
k = nhf / 4π
For an alpha particle, give:
i) the structure
ii) the range in air
iii) deflection in a magnetic field
iv) absorption
v) ionisation
vi) energy of each particle
i) 2 protons + 2 neutrons
ii) fixed range, depends on energy, can be up to 100mm
iii) easily deflected
iv) stopped by paper
v) about 10^(4) ions per mm in air at STP
vi) constant for a given source