Radioactivity

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52 Terms

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Some isotopes are unstable because of their _____

large size or because they have too many or too few neutrons

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Unstable nuclei can emit ____ to become more stable + in what form?

radiation

  • Radiation can be in the form of a high energy particle or wave

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How does this make it more stable?

  • As the radiation moves away from the nucleus, it takes some energy with it

    • This reduces the overall energy of the nucleus

    • This makes the nucleus more stable

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What is this called?

radioactive decay

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What does random decay mean?

  • This means it is not possible to know exactly when a particular nucleus will decay

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Radioactive decay is defined as:

The spontaneous disintegration of a nucleus to form a more stable nucleus, resulting in the emission of an alpha, beta or gamma particle

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Radioactive decay is a random process, which means that:

  • There is an equal probability of any nucleus decaying

  • It cannot be known which particular nucleus will decay next

  • It cannot be known at what time a particular nucleus will decay

  • The rate of decay is unaffected by the surrounding conditions

  • It is only possible to estimate the proportion of nuclei decaying in a given time period

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Radioactive decay is a spontaneous process, which means that: 

  • The decay of nuclei is not affected by the presence of other nuclei in the sample

  • External factors such as pressure do not have an effect on the decay

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Radioactivity Fluctuations, downloadable AS & A Level Physics revision notes

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What are alpha particles made up of?

Alpha (α) particles are high energy particles made up of 2 protons and 2 neutrons (the same as a helium nucleus)

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alpha particles are usually emitted when __

nuclei that are too large

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  • Alpha is a ___ penetrating type of radiation

    • Alpha particles have a range of ____

low

a few cm in air

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What are beta particles?

Beta (β) particles are high energy electrons emitted from the nucleus

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When are beta particles emitted?

  • β particles are emitted by nuclei that have too many neutrons

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Beta is a _______ ionising type of radiation

moderately

  • This is due to it having a charge of +1e

  • This means it is able to do some slight damage to cells (less than alpha but more than gamma)

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  • Beta is a _______ penetrating type of radiation

    • Beta particles have a range of around __ cm - _ m in air, depending on their energy

moderaletly

20 -3

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Beta can be stopped by a ________

few millimetres of aluminium foil

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Gamma (γ) rays are ______

high energy electromagnetic waves

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They are emitted by ____ that need to lose some energy

nuclei

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Gamma particle, downloadable AS & A Level Physics revision notes

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  • Gamma is a ____ penetrating type of radiation

    • Gamma particles have a range of around _ - __cm in lead or several metres in concrete

highly

1-10

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  • If these particles hit other atoms, they can knock out electrons, ionising the atom

  • This can cause chemical changes in materials and can damage or kill living cells

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  • aim of this experiment is to investigate the penetration powers of different types of radiation using either radioactive sources or simulations

  • Independent variable = Absorber material

  • Dependent variable = Count rate

  • Control variables:

    • Radioactive source

    • Distance of GM tube to source

    • Location / background radiation

  1. Connect the Geiger-Müller tube to the counter and, without any sources present, measure background radiation over a one minute period

  2. Repeat this three times, and take an average

  3. Now place a radioactive source a fixed distance of 3 cm away from the tube and take another reading over a one minute interval

  4. Now take a set of absorbers: some paper, several different thicknesses of aluminium (increasing in 0.5mm intervals) and different thickness of lead

  5. One at a time, place these absorbers between the source and the tube and take another reading over a one minute interval

  6. Repeat the above experiment for other radioactive sources

Results

  • Alpha radiation will be absorbed by the paper

  • Beta radiation will be absorbed by the aluminium foil

  • Some gamma radiation will be absorbed by the thick lead

<ul><li><p><span style="color: var(--emphasis-color,#323232)"><strong>Independent variable</strong></span> = Absorber material</p></li><li><p><span style="color: var(--emphasis-color,#323232)"><strong>Dependent variable</strong></span> = Count rate</p></li><li><p>Control variables:</p><ul><li><p>Radioactive source</p></li><li><p>Distance of GM tube to source</p></li><li><p>Location / background radiation</p></li></ul></li></ul><p></p><ol><li><p>Connect the <strong>Geiger-Müller tube</strong> to the <strong>counter</strong> and, without any sources present, <strong>measure background radiation</strong> over a one minute period</p></li><li><p>Repeat this three times, and take an average</p></li><li><p>Now place a radioactive source&nbsp;<strong>a fixed distance</strong> of 3 cm away from the tube and take another reading over a one minute interval</p></li><li><p>Now take a set of <strong>absorbers</strong>: some paper, several different thicknesses of aluminium (increasing in 0.5mm intervals) and different thickness of lead</p></li><li><p>One at a time, place these absorbers between the source and the tube and take another reading over a one minute interval</p></li><li><p>Repeat the above experiment for other radioactive sources</p></li></ol><p>Results</p><ul><li><p><strong>Alpha radiation</strong> will be <strong>absorbed</strong> by the <strong>paper</strong></p></li><li><p><strong>Beta radiation</strong> will be <strong>absorbed</strong> by the <strong>aluminium foil</strong></p></li><li><p>Some <strong>gamma radiation</strong> will be <strong>absorbed</strong> by the <strong>thick lead</strong></p></li></ul><p></p>
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Safety Considerations

  • When not using a source, keep it in a lead lined container

  • When in use, try and keep a good distance (a metre or so) between yourself and the source

  • When handling the source, do so using tweezers (or tongs) and point the source away from you

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Alpha Decay

  • During alpha decay an alpha particle is emitted from an unstable nucleus

  • A completely new element is formed in the process

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Beta Decay

  • During beta decay, a neutron changes into a proton and an electron

    • The electron is emitted and the proton remains in the nuclei

  • A completely new element is formed because the atomic number changes

Beta minus decay GCSE, downloadable IGCSE & GCSE Physics revision notes

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The decay constant λ is defined as:

The probability, per second, that a given nucleus will decay

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  • When a sample is highly radioactive, this means the number of decays per unit time is very high

    • This suggests it has a high level of activity

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Activity, or the number of decays per unit time can be calculated using:

A = activity of the sample (Bq)

ΔN = number of decayed nuclei

Δt = time interval (s)

λ = decay constant (s-1)

N = number of nuclei remaining in a sample

<p>A = activity of the sample (Bq)</p><p>ΔN = number of decayed nuclei</p><p>Δt = time interval (s)</p><p>λ = decay constant (s-1)</p><p>N = number of nuclei remaining in a sample</p>
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The activity of a sample is measured in ________

Becquerels (Bq)

  • An activity of 1 Bq is equal to one decay per second, or 1 s-1

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This equation shows:

  • The greater the decay constant, the greater the activity of the sample

  • The activity depends on the number of undecayed nuclei remaining in the sample

  • The minus sign indicates that the number of nuclei remaining decreases with time - however, for calculations it can be omitted

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Half life is defined as:

The time taken for the initial number of nuclei to reduce by half

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this means when a time equal to the half-life has passed, the activity of the sample will ___ + why?

half

  • This is because activity is proportional to the number of undecayed nuclei, A ∝ N

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  • To find an expression for half-life, start with the equation for exponential decay:

N = N0e–λt

  • N = number of nuclei remaining in a sample

  • N0 = the initial number of undecayed nuclei (when t = 0)

  • λ = decay constant (s-1)

  • t = time interval (s)

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  • When time t is equal to the half-life t½, the activity N of the sample will be half of its original value, so N = ½ N0

knowt flashcard image
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what does this show:

This equation shows that half-life t½ and the radioactive decay rate constant λ are inversely proportional

Therefore, the shorter the half-life, the larger the decay constant and the faster the decay

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graph of number of undecayed nuclei against time

  • The steeper the slope, the larger the decay constant λ (and vice versa)

  • The decay curves always start on the y-axis at the initial number of undecayed nuclei (N0)

<ul><li><p>The steeper the slope, the larger the decay constant λ (and vice versa)</p></li><li><p>The decay curves always start on the y-axis at the initial number of undecayed nuclei (N<sub>0</sub>)</p></li></ul><p></p>
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The received count rate C is related to the activity of the sample, hence it can also be represented in exponential form by the equation:

C = C0 e–λt

  • C = count rate at a certain time t (counts per minute or cpm)

  • C0 = initial count rate (counts per minute or cpm)

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spreadsheet to model the exponential decay of nuclei:

  1. Start with a given number of undecayed nuclei, N in the sample

  • N= 1000 is a logical number to start with

       2. Choose a very small interval of time, Δt 

  • This should be significantly shorter than the half-life of the isotope chosen

       3. Calculate the number of nuclei decaying, ΔN during the time period

  • ∆N∆t = -λN

  • So, ΔN = (λΔt) x N

     4. Calculate the number of undecayed nuclei, N now left at the end of the time period, Δt 

  • N- ΔN N

     5. Repeat this process by iterating your value for as your new N for many values of Δt 

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The isotope ______ is commonly used in radioactive dating

carbon-14

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how is it formed:

It forms as a result of cosmic rays knocking out neutrons from nuclei, which then collide with nitrogen nuclei in the air:

1n + 14N → 14C + 1p

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How does carbon-14 get it stuff?

  • Plants take in carbon dioxide from the atmosphere for photosynthesis, including the radioactive isotope carbon-14

  • Animals and humans take in carbon-14 by eating the plants

    • Therefore, all living organisms absorb carbon-14, but after they die they do not absorb any more

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is amount constant?

  • The proportion of carbon-14 is constant in living organisms as carbon is constantly being replaced during the period they are alive

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  • When they die, the activity of carbon-14 in the organic matter starts to fall, with a half-life of around __ years

5730

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how does it work ?

  • Samples of living material can be tested by comparing the current amount of carbon-14 in them and compared to the initial amount (which is based on the current ratio of carbon-14 to carbon-12), and hence they can be dated

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problems:

  • Carbon dating is a highly reliable ageing method for samples ranging from around 1000 years old up to a limit of around 40 000 years old

    • Therefore, for very young, or very old samples, carbon dating is not the most reliable method to use

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This can be explained by looking at the decay curve of carbon-14:

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If the sample is less than 1000 years old:

  • The activity of the sample will be too high

  • So, it is difficult to accurately measure the small change in activity

  • Therefore, the ratio of carbon-14 to carbon-12 will be too high to determine an accurate age

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If the sample is more than 40 000 years old:

  • The activity will be too small and have a count rate similar to that of background radiation

  • So, there will be very few carbon-14 atoms remaining, hence very few decays will occur

  • Therefore, the ratio of carbon-14 to carbon-12 will be too small to determine an accurate age

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other prob:

  • Carbon dating uses the currently known ratio of carbon-14 to carbon-12, however, scientists cannot know the level of carbon-14 in the biosphere thousands of years ago

  • Therefore, this makes it difficult to age samples which are very old