interactions of xray with matter and exposure factors Flashcards
types of interaction
scattering (x-ray photon goes off in a different direction)
absorption (x-ray photon lost)
no interaction (passes thru without any interaction)
attenuation coefficient
value to show how good an element attenuates the beam
attenuation processes
coherent - S
compton - S
photoelectric - A
pair production - A
photodisintegration - A
coherent scattering
If the energy of a photon is considerably less than binding energies of orbiting electrons of an atom the photon may be deflected from its path with NO loss in energy
- photon interacts with e- in atom of medium = causes raise in energy
- energy rise not sufficient for e- to become ionised
- e- then returns to og energy level and emits a photon with same energy as incident photon
- emitted photon has different direction to incident therefore scattered
- no energy has been permanently transferred to material
- coherent scattering only significant at energies lower than those normally encountered
photoelectric absorption
- x-ray photon involved with interacting with an orbiting e-
- photon gives up all energy and therefore disappears (absorbed)
- e- ejected from atom
- can only take place of photon energy is =/> the e- binding energy
- vacancy created in inner most shell
- filled by e- in next shell
- quantum jumps produces characteristic radiation
- energy of characteristic photon is = to energy difference between shells
photoelectric effect
causes both attenuation and absorption
- individual photons are removed from beam is attenuation
- energy is imparted to the absorbing medium is absorption
ENERGY ABSORBED:
- kinetic energy of ejected e-
- energy of recoil of absorbing atom
- energy of characteristic radiation
compton scattering
INTERACTION BETWEEN FREE E- AN PHOTON
- when a photon collides with an e-, if the photon energy is > than the e- binding energy, the e- may be considered a free e-
- photon may be scattered in any direction
- partial absorption of photon energy (outgoing photon has lower energy than incoming)
- e- can only travel forward relative to incident photon
- radiation scattered in all directions although with higher energies scattered more forwards
pair production
formation of 2 charged particles- an e- + positron pair- from a single high- energy photon
- process converts energy into mass, and can only occur for photon energies greater than 1.02 Mev
- only significant for high energies and materials with high atomic number
- Photon interacts with electric field of nucleus
- Photon energy is converted into mass
- Any remaining photon energy is passed to particles as kinetic energy
- Absorption, not scattering
photodisintegration
Very high-energy photons (>10MeV) can escape interaction with electrons and nuclear electric field, and reach the nucleus.
- The stability of the nucleus may be disrupted by absorption of the photon energy
- Absorption
exposure factors
mAs (milliampere seconds)
kVp (kilovoltage peak)
mAs
product of current (flowing from cathode filament to anode target) and time (current allowed to flow to anode)
- Correlates with the current applied across the cathode filament circuitry
- Indicative of the quantity of photons in the x-ray beam
Effects Intensity (amount)
“Total energy per second flowing through a unit area”
- Does not effect x-ray quality (penetration)
exposure time (s)
- length of time current is allowed to flo to anode target (facilitate x-ray production
- ideally kept as short as possible to minimise blue from patient motion
- REDUCED TIME= INCREASED mA
mAs proportion
mAs is directly proportional to the number of photons produced
short time and high mA may increase tube loading
kVp
- refers to max voltage applied between the cathode ad anode at exposure
- effects the speed and energy with which e-s cross from cathode to anode
- directly related to the max energy of x-ray photons produced
changing kVp
- affects the quality of photons and quantity of photons produced
the MORE ENERGETIC e- will produce HIGHER ENERGYphotons (QUALITY)
a higher kVp will apply a greater potential difference across cathode and anode
therefore e- will be ACCELERATED FASTER towards anode and can be involved in multiple interactions at the anode= producing MORE PHOTONS