Ch. 3-4 Flashcards
What does kVp control
QUALITY, or penetrating power
Name 3 ways X-Rays interact with human tissue
- Interact with the atoms of the patient and become ABSORBED
- Intersect with the atoms of the patient and become SCATTERED
- Pass through the patient WITHOUT interaction
More Absorption =
Greater possibility of biological damage
Primary Radiation
What exits the tube
Anode
Target
Reasons tungsten/rhenium are used as target materials
High melting points
High atomic numbers
Inherent Filtration
Built-In
Added Filtration
A certain thickness of added ALUMINUM to “harden” the beam within the collimator
Combo of X-Ray tube glass wall and added aluminum placed within the collimator may be called
Permanent Inherent Filtration
Primary Radiation happens (before/after) it has gone through filtration
AFTER
SINGLE PHASE
100% voltage ripple
3 phase (6 pulse)
13% voltage ripple
3 phase (12 pulse)
4% voltage ripple
High Frequency
1% voltage ripple
Do all photons in a X-Ray beam have the same energy
No
The energy of the average photon is about 1/3 of the energy of the most energetic photon
Example:
100 kVp beam contains photons having energies of 100 KeV or less, with an average energy of approximately 33 KeV
100 divided by 1/3=33
Can the most energetic X-Ray photon have more energy than the set kVp
No, the photons can have no more energy than the set kVp
Photons that travel through the patient without interacting & reach the image receptor
Direct Transmission
(Possible/Impossible) to predict with certainty what will happen to a single photon when it enters human tissue
IMPOSSIBLE
(Possible/Impossible) to predict what will happen on the average when a large number of photons enter the human body
POSSIBLE
Absorbed Dose
D
Coherent Scattering
Occurs with low-energy photons, less than 10 KeV (kVp’s 1-50)
Wavelengths of incident and scattered are the same, so no new energy is absorbed by the atom, because no kinetic energy is lost
Small angle scatter
May result in small amounts of fog
Photoelectric Absorption
Interaction of a X-Ray PHOTON and an INNER SHELL ELECTRON
Involves ejection of an inner shell electron
Vacancy of inner shell is filled by an outer orbital shell electron
A difference in binding energies between the two electron shells forms a second photon
Photoelectron created ^
IMPORTANT MODE OF INTERACTION FOR PRODUCING USEFUL IMAGES
PHOTOELECTRIC ABSORPTION/Auger Effect
When an inner electron is removed (inner-shell vacancy) the energy given off by another electron filling his void can go on to eject another electron in the same atom
Instead of filling the “hole” , it ejects another electron
Probability of photoelectric absorption depends on
Energy (E) of the incident photons
Atomic number (Z) of the atoms comprising the body part
Energy of the incident photon decreases as
kVp decreases
Bone Atomic #
13.8
Soft Tissue Atomic #
7.4
Air Atomic #
7.6
Absorption vs kVp
As kVp decreases
Absorption increases
The whiter areas on radiographs
The higher the absorption
(Bone, Lead, Medal, Barium, ETC)
(Darker/Whiter) Less attenuation by the body part
Darker
(Darker/Whiter) More attenuation by the body part
Whiter
Ex: Knee replacements show up really bright because they absorb more
Increase window level =
Brighter, white, increased brightness
Decreased window level =
Darker, black, decreased brightness
Use of positive contrast medium- Iodine/Barium
Appears lighter because it increases photoelectric effect
Use of negative contrast medium-Air
Appears darker
Compton Scattering
Interaction with a loosely bound outer shell electron
X-Ray photon dislodges the electron from its outer shell, ionizing the atom
The freed electron is able to ionize other atoms and bounces around unit it finds an atom in need of another electron
The incident X-Ray photon that kicked out the electron continues on its way but in a new direction
Very Bad- Degrades image ‼️