chapter 27 - medical physics Flashcards
X-ray properties
- short wavelenght
- EM waves
- can be polarised and diffracted
- high intensity can be harmful to living cells
production of X-rays in an X-ray tube
- use can evacuated tube containing 2 electrodes
- large pd between electrodes
- cathode is a heater which produces electrons by thermionic emissions
- electrons are accelerated towards the anode (target metal) eg tungsten - high mtp
- X-rays produced when electrons decelerate by hitting anode
- anode is shaped so rays are emitted in the desired direction
how to prevent X-ray tubes heating up too much
- cooling fins help dissipate heat from the tube
- water and oil cooling systems
- target is rotated
shortest wavlentg of X-rays produced in an X-ray tube
eV = hf
eV = hc/λ
λ = hc/eV
so λ prop to 1/V
increasing current just increases intensity (as more electrons emitted)
X- ray spectra
- range of decelerations of electrons inside the x-ray tube result in Bremsstrahlung (overall curve)
- narrow intense lines (K-lines) are due to incident electrons removing electrons from the atom and these are filled by electrons dropping down energy levels and releasing photons of specific energies
how x-ray spectra is effected by increasing pd
intensity increases - graph shifts up and lowest wavelength shifts left (decreases)
attenuation
gradual decrease in intensity of the x-ray beam as it travels through a medium - bone attenuates more than soft tissue
energy range of x-rays used to diagnose bones
100eV - 100keV
4 attenuation mechanisms
- simple scatter
- photoelectric effect
- compton scattering
- pair production
simple scatter
1-20keV
- photon changes direction
- energy unchanged
photoelectric effect
<100keV
- X-ray photon absorbed
- electron emitted
- used in X-ray imaging
compton scattering
0.5-5MeV
- in high energy x-rays (radiotherapy) - used to kill cancerous cells
- elastic scattering of X-rays by orbital electron
- X-ray incident - low energy photon + electron released
pair production
1.02MeV
- X-ray photon -> electron-positron pair
attenuation coefficient
- μ
- interaction of x-ray photons with matter reduces intensity of the beam
- transmitted intensity of x-rays depends on energy of photons + thickness/ type of substance
I = I0 e^-μx
contrast medium
- soft tissue have low absorption coefficients but adding a contrast medium allows visibility (larger absorption coefficient)
- eg iodine and barium - have large atomic number which is related to absorption
CAT scan
- patient lies on table that can slide in and out of large vertical ring
- x-ray tube on one side and an array of detectors on the other
- x-ray tube and detectors rotate
- x-ray tube produces a then beam of x-rays which are attenuated by different amounts by different tissues
- each time the tube rotates a 2D slice is formed - slices are turned into a 3D image by computer
+ CAT
- 3D image
- more detailed
- can distinguish between soft tissues of similar attenuation coefficients
- CAT
- takes longer
- patients receive a higher dose of ionising radiation vs an x-ray
- have to lay still
medical tracers used
- need to target desired tissures
- radioisotopes combined with elements to achieve this