X-ray interaction 1 Flashcards
X-ray Photon Interactions cases
Case 1: X-ray photon passes straight through the matter without interacting
- Pass through object but might absorb it.
- Other reaction it can be stopped x-ray detector.
- It can be scattered diverged from its original path and not be able to detect it.
Some materials absorb more x-ray material than others, such as bone will absorb more than soft tissues.
Case 2: X-ray photon is completely absorbed by the matter
Case 3: X-ray photon is scattered from its original path because of interacting with the matter
What are X-ray Photon Interactions
Any one of these aforementioned processes is not guaranteed for individual X-ray photons – there is only a probability that one of the processes may occur.
X-ray photon interactions are random statistical processes
On average however when considering many X-ray photon interactions some interactions have a higher probability which is dependent on a number of factors
For example
it is more likely that a thicker object will absorb more X-ray photons than a thinner object made of the same material
it is more likely that a dense object will absorb more X-ray photons than a less dense object
What are the 5 processes whereby an X-ray photon can interact with matter?
Photoelectric absorption
Compton scattering
Coherent (Rayleigh) scattering
Pair production
Photodisintegration
Photoelectric Absorption
Absorption definition
Dependence on
Atomic Number
Density
X-ray photon energy
Image quality
Radiation dose
What is Absorption?
The transfer of energy from the X-ray beam to the medium
Photoelectric Absorption
An X-ray photon, with sufficient energy, interacts with a bound electron from the inner shell of an atom in an object.
The X-ray photon must have an energy greater than the binding energy of the inner shell electron to take part in photoelectric absorption
Photoelectric absorption: Where does all of the energy of the photon transfer to?
All of the energy of the photon is transferred to the electron
The electron then has enough energy to be freed as a photoelectron and leaves a ‘hole’ or ‘vacancy’ in the shell.
Photoelectric Absorption: What energy does it have?
The photoelectron will have a kinetic energy equal to the difference of the incident X-ray photon energy and the binding energy of an inner shell electron.
The photoelectron will only travel a short distance and deposit its energy into the surrounding mater
Photoelectric Absorption: Describe the vacancy in the inner shell
The vacancy in the inner shell is filled by electrons from higher shells of the atom.
This produces a photon (characteristic radiation) of usually low energy – so it is not an X-ray photon
The emitted photon is usually absorbed close to the site where it was produced—this deposition of energy contributes to patient dose
The atom is left with a net positive charge as a result of losing an electron
The vacancy in the higher shell is filled by electrons in higher shells
With each transition characteristic radiation is produced further contributing to patient dose
All of the energy of the incident X-ray photon is deposited in the patient and thus contributes to dose
The probability of photoelectric effect depends on: (give equation)
E - energy of the x-ray photon
Z - atomic number of the material
p - mass density of the material
𝑃𝐸𝑝𝑟𝑜𝑏 ∝ 𝜌𝑍^3/𝐸^3
Photoelectric Absorption: Energy of the X-ray photon
Probability of photoelectric interactions is highest when the X-ray photons energy is slightly above the electron binding energy
If the X-ray photon energy is too low in cannot free the bound electron
If the energy is too high the probability significantly decreases due to the inverse relationship with the cube of the energy (see previous slide)
Photoelectric Absorption & Image Quality
Photoelectric effect produces excellent images because it enhances natural tissue contrast and does not produce scatter
X-ray image contrast depends on some tissues absorbing more X-ray photons than other tissues
Contrast is greatest when the difference in absorption between adjacent tissues is greatest
Because the number of photoelectric reactions depends on the third power of the atomic number, the photoelectric effect magnifies the difference in tissues composed of different elements such as bone and soft tissue
Photoelectric Absorption & Patient Dose
The photoelectric effect results in patients receiving more radiation dose than from any other type of interaction
All the energy of an incident photon is absorbed by the patient
Effect of photoelectric interaction can be reduced using high-energy (kVp) techniques
Photoelectric Absorption: Key Points
Dominates at low photon energy
Produces excellent radiographic contrast
Responsible for majority of patient dose
Photoelectric absorption & contrast media
K-edge absorption
Iodine & barium contrast media
As the photon energy increases, there are values where there is a sudden jump in attenuation (absorption increases)
For example, at energies just below the k-edge the X-ray photons don’t have enough energy to free the k-shell electrons
K-edge Absorption & Contrast Media: What happens as the energy increases and the probability of the x-ray photon?
As the energy increases to just over the required energy, a much larger number of bound electrons in the object become available for photoelectric absorption
Therefore, the probability of the X-ray photon being attenuated by a photoelectric interaction significantly increases—overall absorption increase significantly
K-edge Absorption & Contrast Media: What is it useful for some materials in radiography?
This is particularly useful for some materials used in radiography such as iodine and barium
These materials have k-edge absorption energies within the diagnostic energy range and therefore standout really well on images—they produce excellent contrast.
Iodine contrast agent is often injected into blood vessels to make their structures visible on X-ray images—they would be otherwise invisible.
Barium contrast agent is often administered orally to make gastrointestinal structures visible of X-ray images—they would otherwise be invisible
K-edge: Iodine: 33.2 keV, Barium: 37.4 keV
X-ray Interactions with Matter
: Compton Scattering
Scattering
Dependence on
Density
X-ray beam energy
Consequence of Compton scatter on
Patient & staff dose
Image quality
Proportion of Compton scattering compared with photoelectric absorption
What is scattering?
A change in the direction of an X-ray photon due to interaction