Chapter 27 - Medical Physics Flashcards
X-ray wavelengths
10^-13 –> 10^-8 m
Producing x-rays
Eject electrons from a cathode in thermionic emission with a p.d. of 50 to 200kV
They are attracted to an anode (tungsten), reducing the kinetic energy of electrons and converting to photons
Bremsstrahlung
A continuous spectrum of energies of x-rays emitted as electrons lose kinetic energy
Characteristic x-rays
Emitted from the anode as electrons move between energy levels in the anode
Shortest wavelength of x-rays
λ = hc/eV
Hard and soft x-rays
Hard (0.10 to 0.01nm) are more penetrative than soft (10 to 0.1nm)
An aluminium sheet is used to filter out ionising but less useful soft x-rays
Collimated x-rays
A parallel beam
μ
The linear attenuation coefficient (the percentage reduction in intensity per unit length)
Attenuation
The decrease in intensity of EM radiation
X-ray intensity formula
I = I0 e^-μx
Simple scattering
X-rays <20keV cannot remove electrons from atoms so they are scattered and intensity is reduced
Soft x-rays are filtered so not significant in radiography
Photoelectric effect
If hf > Φ, electrons absorb a photon and are emitted, meaning the intensity is reduced as photons are lost
Compton effect
0.5 to 50 MeV energy
A photon with momentum collides with an electron, knocking it out of the nucleus, reducing its own momentum
The energy is reduced and likely no longer an x-ray photon
Pair production
Energy >= 1.02 MeV
A photon exchanges its energy for mass, producing an electron-positron pair
Contrast media
Compounds with high atomic numbers create scattering in soft tissue
μ ∝ Z^3
e.g. barium
Used to detect the boundaries between media