Medical Physics Flashcards
Larmor frequency
The frequency of precession of nuclei in an external magnetic field
Define acoustic impedance
The property of a material that determines the intensity of ultrasound refracted at a boundary with another material
Z = pc (measured in kg m^-2 s^-1)
How are X-rays produced?
Bombarding tungsten with high energy particles
What is the wavelength of X-rays?
10^-13 to 10^-8
What is the typical frequency of ultrasound used in medicine?
1-15MHz
What is the name of the frequency at which the protons precess?
Larmor Frequence
After the pulses of radio waves has ceased the nuclei relax and emmit what kind of wave?
Radio
Gamma Cameras are used with what?
Radioactive tracers
Describe X-ray production
A tungsten cathode is heated so that it releases electrons
These electrons are fired across a vacuum by a voltage generated by the mains
These electrons hit the negative anode and some of their energy (about 1%) is converted into X-ray photons
These X-ray photons can only exit through a window in the casing and there may be sheets of metal either side of the window to absorb X-rays not travelling straight, forming a collimated beam
The rest of the energy of the electron is gained by the anode as heat, so it rotates very fast to get rid of excess heat
The energy of one X-ray photon is virtually the same as the K.E. of the electrons, as the work function is negligible
The energy of an electron is eV and the energy of an X-ray photon is hf. Therefore…
hf = eV
And as λ = v/f, λ = c/ (eV/h), λ = hc/ eV
Describe X-ray absorption, with reference to the photoelectric effect
As with light rays, X-rays are also capable of producing photoelectrons
Energy of incoming photon = work function + KE of photoelectron
hf = ϕ + 1/2 mv^2
The work function is the energy required to break the bonds holding an electron in place
Because the energy of X-rays is so high, the work function is considered negligible
Therefore the photoelectron s produced have virtually the same energy as the X-ray photons that caused them
This is the main way that low energy X-rays are absorbed
Describe Compton Scattering
Occurs for higher energy X-rays (0.5-5MeV)
Instead of giving all their energy to an electron, the X-ray photon only loses a small amount of energy when it hits one
The ‘Compton Electron’ is knocked off its orbit and moves of in a different direction, ionising the atom
The X-ray photon now has slightly less energy, so a smaller frequency (E=hf) and hence a longer wavelength (λ = v/f) and is also deflected
Describe pair production with X-rays
Pair production occurs when an X-ray photon with energy above 1.02 MeV spontaneously splits into a positron and an electron when entering the electric field around the nucleus of an atom
The energy of the X-ray photon is converted into the mass of the electron and positron as E = mc^2 applies
The positron is soon annihilated when it collides with an electron, producing two gamma-ray photons that move off in opposite directions to each other
Describe film intensifiers
To intensify the image produced from a traditional film X-ray, intensifier sheets are used
These sheets are of material that contain a phosphor – a substance that emits visible light photons when an X-ray photon hits it
The film is placed behind an intensifier screen and many light photons produced by the screen blacken the film
This dramatically reduces the energy of the X-rays that needs to be used, so reducing the risk to the patient
Describe digital intensifiers
Incoming X-rays strike a phosphor screen which releases thousands of visible light photons for each X-ray photon that hits it
These then hit a photocathode, which releases an electron for each light photon, via the photoelectric effect
These electrons are then focused onto a screen which is another phosphor that gives out visible light
Image intensifies are used to reduce the length of time the patient has to be exposed to X-rays, and so that a lower intensity can be used
Describe contrast media
Used to show up a certain tissue that has a similar attenuation coefficient to other tissues in the body, which would normally not show up well on an ordinary X-ray scan
The medium used has to be a good absorber of X-rays, so has to have lots of electrons and hence a high atomic number (Z)
The medium, often barium, is injected into the tissue of interest, causing the tissue to become a better absorber of X-rays, so it’s edges are more clearly defined on the final image