RT2 - Dosimetry equipment Flashcards
1
Q
3 ways to measure energy deposited from ionising radiation:
A
- Ionisation - collect ion pairs produced in air
- Calorimetry - ionising particle shares energy with many others, ions recombine, energy ends up as heat
- Chemical effects - free radicals produced by ionising particals can cause chemical effects
2
Q
Define exposure
A
- Charge liberated per unit mass [C/Kg]
- total chartge of ions in dry air when all electrons liberated in mass dm of air are completely utilised
- Need to collect all ions produced by electrons originating in mass dm
- Electrons are produced both inside and outside of dm
3
Q
Define Electronic Equilibrium
A
- Ions produced by electrons travelling into dm is equal to ions leaving dm.
- I.e. collecting as many electrons from outside as you are not collecting the ones that leave
- Exposure is only measurable under electronic equilibrium
- Minmum dimension between boundaries of dm and surrounding interacting homegenous medium > range of electrons
4
Q
Operation of Free-Air ion chamber
A
- Photon beam passes between paralell plates (high voltage)
- X-rays produce electrons which cause ionisation
- Ions are collected and measured electronically
- V needs to be high enough to separate as many =ve ans -ve ions before they recombine
5
Q
What is a primary standard?
A
- Absolute measurement against which secondary standards and reference instruments are calibrated
- Measurement from first principles
- NPL
- Free-air ion chamber (kV photons)
- Graphite calorimeters (MV photons & electrons)
6
Q
How does NPLs free air ion chamber calibrate a KV beam?
A
- Free air ion chamber
- Kerma = Dose (to air) = energy required to create ion pair * number of ion pairs produced/unit mass
- Collect all the ions, know the energy needed to create a pair, work back to dose
- User puts thimble ion chamber in same beam conditions, and you get a calibration factor
7
Q
How do you convert air kerma to absorbed dose in water?
A
- Dose to water = dose to air * ration of mass energy absorption coefficents (water/air) averaged over photon spectrum in air
- Dose on surface of water phantom requires backscatter factor, which you measure with TLD (fixed SSD one on surface of water, other in air)
8
Q
Thimble Ion chamber
A
- Needed for high energies where free air chambers would be too large
- Used for clinical measurements, measure exposure (proportional to dose)
- Free-air chamber - small air cavity dm + surrounding air volume (dimensions > R)
- Thimble chamber - small air cavity dm + surrounding air-equivelent wall of graphite (dimensions > R)
9
Q
Farmer chamber
A
- Thimble-type ion chambe enclosing small volume of air in conducting graphite cap with insulated axial collecting electrode
- Walls have z similar to air
- Wall thickness > R in wall (1mm wall = 1m air)
- Dose is proportional to exposure, calibrated against primary dosimetry standards
10
Q
Operation of thimble chamber
A
- Hiigh polarising voltage between wall and central electrode (200Vcm-1)
- Ions produced in cavity move to one wall or other
- Collected charge is measured with electrometer
- Volume typically 0.6ml
11
Q
Ion chamber sizes
A
Large
- Sensitive & low spat res
- used for environmental monitoring
Small
- good spat res, small singal
- fine resolution scanning
12
Q
Paralell plate chamber
A
- Used to measure high dose gradient fields (e.g. electrons)
- Need a small chamber so that you son’t get contribution from other parts of high gradient field
- Thin = better res
- Detecting volume still large enough for good signal
13
Q
Principle of Calorimetry
A
- Absorbed dose = energy/mass
- E = mc dT
- Dose = specific heat capacity * temp rise
Direct measurement of absorbed dose. Difficult to sue water due to effects of purity, NPL uses graphite and converts to water by comparing ratio of electron densities.
14
Q
NPL Graphite Calorimeter method
Why do you use graphite?
How do you measure temp rise?
A
- Inner graphite core surrounded by two jackets
- Core thermally isolated from outer jackets by vacuum
- Temperature rise in core measured with sensitive thermistors
- Use graphite because 1Gy produces temp rise of 1.5mK in graphite, but only 0.24mK in water. Lower specific heat = more temp to measure, better precision
- More accurate to measure by keeping the temperature constant (peltier element) and recording the power in the heating circuit, Dose to graphite = change in power * time beam is on / mass of core
15
Q
Secondary standard
A
- High quality dose meter owned by hospital
- sent to NPL to be calibrated against primary reference (calibrated against primary)
- Correction factor
- Transferred to field instruments by cross-calibration