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Radiation in Medicine
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A = λN = λN0e(-λt) = A0e(-λt)
Activity Activity is the number of disintegrations per second. The effect it has largely depends on how ionising the radiation is. A = λN = λN0e(-λt) = A0e(-λt)
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Dosimetry The exposure to radiation can be measured in 3 ways:
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Exposure (X) This measures the amount of ionising radiation you would be exposed to in a particular environment. Exposure (X) = Q/m Q = Total charge of + ions produced m = Mass of air in the room Units = C.kg-1
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Exposure (X) Exposure X = Q/m
It is only used for X-rays and gamma rays as alpha and beta have a small range in air and anyone standing a few metres away in the same room will not be exposed to them.
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Absorbed dose (D) This is the energy absorbed per unit mass of actual tissue Absorbed dose (D) = E/m E = Total energy absorbed m = mass of tissue Unit = J.kg-1 (called a gray, Gy)
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Dose equivalent (H) H = QD
This is an attempt to measure the actual damage that occurs in tissues Dose equivalent = Quality factor x absorbed dose H = QD Units = J.kg-1, but this time called a sievert (Sv) Alpha particles will have a higher quality factor than gamma rays etc.
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Quality factor Particle/wave Quality factor X-ray 1 Gamma ray
Beta particle (electron) Alpha particle 20
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Sievert To distinguish between absorbed dose and dose equivalent the Sievert is used. Since Q = 1 for X-rays, the absorbed dose and dose equivalent of X-rays is the same. For other radiations, the dose equivalent gives the amount of X-radiation that would give the same harm.
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Dose equivalents Source Dose equivalent /mSv Background dose in 1 year
3 Ankle X-ray 0.02 CT scan of the head 2.0 Barium meal 8.0
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Dose effects Dose/mSv Effect 1000 Nausea. vomiting 2000
Loss of body hair 4000 Bleeding in the mouth 10 000 Death after 14 days 50 000 Death within 48 hours
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Firemen at Chernobyl mSv
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Biological effects of radiation
Ionisation could cause damage directly to DNA or RNA Metabolic pathways could be interfered with (the complex chemical reactions that take place in the body)
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Biological effects of radiation
Damage to a cell could cause it to divide at a rate faster than cells die. The malignant cells could continue to grow until they interfere with the normal workings of the organ/tissue. Death is the result. This is called cancer.
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Radiation safety Intensity decreases with distance
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Radiation safety Dose received is proportional to time exposed
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Radiation safety Shielding – alpha is stopped by paper, beta by a sheet of aluminium, gamma by a few cm of lead.
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Monitoring Film badge – photographic film is a cheap and effective way of monitoring absorbed dose
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Monitoring Ionising particle causes chemical change in one of the grains that cover the film. When processed the grain turns black. Different areas of the badge can have different filters in front of the film The badge is processed about once a month.
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Balanced risk Risk Benefit Ankle X-ray (0.02 nSv)
Ankle gets repaired correctly Radiation emitted from a smoke detector Detector might detect a fire and save lives CT scan of an unborn baby to find out if it is a boy or girl (2 mSv) Know whether to paint nursery blue or pink
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Questions
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Radiation therapy
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External radiation to kill cancerous cells
Gamma rays It will also affect healthy cells Cancerous cells do not function correctly so are unable to repair themselves as well as normal cells
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External radiation to kill cancerous cells
Gamma fired from different directions to intersect at tumour which gets the highest dose
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Internal radiation Placing a solid radiactive source next to the tumour (brachytherapy) or injecting/ingesting a fluid containing a radiactive isotope.
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Choice of isotope Energy – High energy will be mnore damaging to cancer cells , but also may pass through the cancer into neighbouring healthy cells
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Choice of isotope Type – Alpha is the most damaging but not very penetrating so needs to be placed close to cancer cells. Beta and gamma sources need longer exposure time and have more effect on surrounding tissue
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Choice of isotope Chemical properties – Some elements collect in certain organs – iodine in the thyroid for example.
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Choice of isotope Half-life – If solid and can be retrieved – does not matter, although a long half-life means it can be re-used If ingested, needs to be shorter so it doesn’t stay in the body too long.
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Different half lives Due to normal radioactive decay (physical half-life) Amount of material time Physical half-life (Tρ)
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Different half lives Due to biological processes (excretion respiration etc.) Amount of material time Biological half-life (TB)
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Effective half-life TE
The effective half-life (TE) is the time it takes for the actual number of nuclei in the body to reduce. It obviously depends both on the physical half life (Tρ) and the biological half-life (TB) TE is a combination of both processes
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Effective half-life TE
1/TE = 1/Tρ + 1/TB
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Example Iodine is a gamma emitter with a half-life of 8 days. It accumulates in the thyroid gland. The biological half-life is 80 days. Effective half-life? 1/TE = 1/8 + 1/80 TE = 7.3 days
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Radioactive tracers Small amount of a radioactive isotope is injected into the blood. Since activity is proportional the amount present (A = -λN) it is possible to find how much isotope is present in any part of the body simply by measuring the activity.
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Measuring blood volume
Small amount of isotope is put into a known amount of blood and its activity measured. Blood re-injected into body and allowed to “mix” New sample taken and “diluted” activity measured Original activity/Diluted activity = total volume/sample volume
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Thyroid activity Thyroid uses iodine to make hormones so iodine collects in the thyroid. By using a tracer the flow of iodine in and out of the thyroid can be monitored
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Calcium build-up in the heart
Build-up of calcium is an indication of a damaged heart muscle. Radioactive technetium takes the place of calcium in the heart muscle giving an indication of the amount of calcium build-up.
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Imaging using tracers The radiation emitted from a radioactive tracer can be used to produce an image of an organ.
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Positron Emission Tomography
PET Scans Positron Emission Tomography
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PET This uses an isotope of carbon, carbon-11, as a tracer
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PET A small amount of carbon monoxide (CO) containing some C-11 is inhaled and is taken up by red blood cells and circulated around the body.
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PET When the carbon-11 decays, it decays by positive beta decay (positron emission). 11C +1β + 11B
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PET When the positron meets an electron they annihilate each other to produce 2 gamma rays +1β + -1β 2γ
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PET The two gamma rays emitted travel in opposite directions γ γ
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PET The two gamma rays can be detected and the position of their origin calculated with great accuracy Detector surrounding patient γ γ
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PET This is used especially to image a functioning brain (when given specific tasks to do).
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Medical Physics That’s it!
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