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filtration
process of eliminating undesirable low-energy x-ray photons by insertion of absorbing materials into primary beam
allows radiographer to shape emission spectrum
reduces quantity and increases quality of the primary beam
low energy photons cannot penetrate the part
only contribute to patient dose
filter
any material designed to selectively absorb photons from the x-ray beam
aluminum
most common and standard filtering material other than glass, oil, copper, tin
expressed as Al/Eq
hardening of the beam
removes low energy “soft” photons
increases average beam energy
soft tissue penetration
requires approximately 30-40 kiloelectronvolt (keV) photons
half-value layer (HVL)
filtration needed to reduce beam to one half its original intensity
for the purpose of quality control of x-ray beam
types of filtration
inherent filtration, added filtration, compound filtration, compensation filtration, total filtration
inherent filtration
glass envelope
dielectric oil bath (also cools/insulates tube)
glass window of housing
about 0.5 to 1 mm Al/Eq
tube aging increases this type of filtration
vaporized tungsten coats tube window
HNL testing important
added filtration
any filtration outside tube and housing
collimator
typically provides 1 mm Al/Eq due to silver on collimator mirror
other
additional added aluminum
compound filtration
K-edge filters
two or more materials
each layer absorbs characteristic photons created in previous layer
Tin, copper, aluminum in Thoraeus filter
characteristic photons produced by aluminum are 1.5 keV
these are absorbed by air between filter and patient
thoraeus filter in radiation therapy
compensation filter
evens radiographic density with parts that have uneven tissue thickness or densities
e.g. wedge for foot or T-spine, trough for CXR
Al, lead-plastic etc.
total filtration
inherent + added
does not take into account any compound or compensating filtration
effect on patient dose
ideally, filtration would only remove low-energy photons
some high energy photons are removed
results in decrease in radiographic density that must be compensated for with increase in technique
overall, patient dose reduction
exposure
radiation intensity in air
measured in Roengtens (R) — traditional unit
SI unit: coulomb/kilogram (C/kg)
dose
amount of radiation absorbed
measured in rad
entrance skin exposure (ESE)
patient receives the highest exposure at the entrance of skin
maximum exposure to body
calculated at minimum SOD
better to overestimate exposure rather than underestimate
requires a calculation of mR/mAs
we measure exposure for patient dose estimation
varies between x-ray machines and x-ray tubes
diagnostic radiography mR/mAs charts
tube output in mR divided by mAs at particular SID
typically calculated at 40’’ SID (100cm)
varies based upon kVp
higher kVp’s produce a higher mR/mAs
how to estimate ESE
apply inverse square law
derive mR1 from mR/mAs chart
derive SOD from SID and object to receptor distance (OID)
select the correct kVp to identify mR/mAs based upon kVp
fluoroscopic R/min charts
ESE for fluoroscopic equipment
measured in R/min
FDA limits fluoroscopic exposure rates
standard fluoroscopy
11.5 R/min (10cGy/min)
high level control fluoroscopy
23 R/min (20cGy/min)
reducing patient dose with communication
radiographers must appear confident to gain a patient’s confidence
earning a patient’s confidence results in more cooperation
demonstrates competence and professionalism
reducing patient dose with positioning
radiographic projection
different projections of body part can yield differing ESE and absorbed dose values
AP female pelvis versus PA female pelvis
lower ovarian exposure
PA skull versus AP skull
lower exposure to lens of eye
immobilization
immobilization
elimination of movement essential to reducing patient dose
reduces retakes due to motion artifacts
improves image quality and visible spatial resolution
reducing patient dose with technical factors
interrelationship with prime factors: kilovoltage range, milliamperage time, distance, focal spot size, filtration
field size, gonad shielding, subject part density, grids
digital image receptor system, film/screen receptor systems, film processing
interrelationship of prime factors
all factors influence total dose
(mAs)(kVp)2 / d2
kilovoltage range
increase in kVp without compensation in mAs
increase patient dose
increase in kVp with compensation in mAs
decrease patient dose
best kVp and mAs combination if image quality is good
high kVp, low mAs
milliamperage and time
increase in mAs without compensation from other technical factors
increases patient dose
mAs at lowest level possible will reduce patient dose
distance
SID of SOD increases
results in ESE decrease
decrease in OID will increase SOD
therefore, ESE decreases
filtration
increasing in filtration results in an overall ESE reduction and reduction of patient dose
field size
decrease in primary beam size
decrease in patient dose
gonad shielding
accurate use of shielding will decrease patient dose
three major types:
flat contact
shadow
shaped contact
properly placed gonadal shields significantly reduce patient dose
grids
higher ratio grid
requires increase in mAs
increases patient dose
use the lowest ratio grid necessary to minimize patient dose, without jeopardizing image quality
film/screen image receptor systems
intensifying screens
faster screen speeds reduce dose dramatically
film
increased film speed decreases dose
film processing
when properly maintained, no effect on dose
digital image receptor systems
respond to 0.01 mR to 100 mR
digital systems have a wide dynamic range of exposure response — linear
extreme exposures not acceptable for image quality
produces digital data drop
excessive scatter/secondary
radiographers must be careful not to overexposure image receptor
despite ability to correct for this in post processing
discussing radiation risks versus benefit with patients
minimize patient dose by emphasizing risk
maximum diagnostic information by emphasizing benefit
help patients understand dose relative to lifetime risk of daily activities
minimizing patient dose by emphasizing risk
experienced radiographers can gain stature to permit consultation
patient advocate for reduction in dose and for additional exams, if needed
patient’s right to refuse
maximizing diagnostic information by emphasizing benefit
informed decisions
comparison of relative radiation risks
factors contributing to compton scatter
kVp
affects the penetrability of beam
volume of irradiated material
field size
patient thickness
increased kVp
affect on interaction:
increased transmission
decreased photoelectric absorption
increased compton scatter
affect on patient dose:
decreased dose
decreased photoelectric absorption
increase in kVp typically accompanied by reduction in mAs (same exit dose)
affect on image quality:
lower amount of subject contrast (penetration)
not as pronounced in digital systems, due to image post-processing
image contrast (displayed contrast is controlled by look-up table - applied in imaging processing)
decreased kVp
affect on interaction:
decreased transmission
increased photoelectric absorption
decreased compton scatter
affect on patient dose:
increased photoelectric absorption
decrease in kVp usually accompanied by increase in mAs (kept same exit dose)
which increases dose even more
affect on image quality
higher subject contrast
volume of irradiated material
field size (FS)
patient thickness
average tissue density
field size
increased FS increases volume of tissue irradiated
results in increased scatter
decreased FS decreases beam quantity
decreases scatter
decreases amount of remnant radiation hitting receptor
can increase image noise without mAs compensation
trade off
by decreasing FS, fewer photons reach image receptor
image receptor exposure decreased
increase in mAs accompany significant reduction in Fs to maintain image receptor exposure
patient thickness
thicker body parts produce more scatter
denser body parts produce more scatter
higher electron density present in thicker/denser tissue
increased likelihood of interactions occurring, particularly photoelectric
both of these factors increase number of interactions x-ray beam undergoes as it passes through the body
decreasing patient thickness
compression devices used to improve spatial resolution and contrast
decreases patient thickness
thickness becomes more uniform
results in lower patient dose
brings tissue closer to receptor
decreased OID improves spatial resolution
routinely used in mammography
control of scatter using beam-restricting devices
ideally, beam resistors decrease FS to anatomy of interest
unnecessary tissue exposure decreases
scatter decreases
scale of contrast shortens (higher contrast)
visibility of details increase
all good things!!
beam resistors
aperture diaphragms, cones, and cylinders
principal disadvantage of fixed FS
rarely used today
collimators
ancillary devices
collimator
modern equipment feature - regulate the field size
light localizing field light
provides indication of midpoint of central ray (CR)
two sets of shutters that permit infinite number of field sizes
length and width of field independently controlled
lead shutters
permits rectilinear collimation; perpendicular to each other
light localizing
collimator and penumbra
bottom shutters reduce penumbra
geometric unsharpness around periphery of image
also known as edge unsharpness
improves sharpness of recorded image edge
collimator and off-focus radiation
upper shutters reduce off-focus radiation reaching IR
off-focus radiation occurs from areas of x-ray tube other than focal spot areas
off-focus radiation produces images beyond exposed field or radiation
image shadows
light field
uses light reflected off mirror to project coverage of x-ray beam
proper adjustment of mirror necessary to accurately display location of exposure field
light field/x-ray beam coincidence testing should be part of quality control (QC) program
needs to be accurate within 2% of SID
features of collimator housing
central ray must be marked
some units project location of AEC sensors in light field
alignment light helps center beam with image receptor
newer systems will automatically adjust field size with changes in SID
positive beam limitation (PBL) devices
automatically collimates beam to size of image receptor
possible to override PBL
can reduce beam to smaller field than receptor size
no longer a federal requirement for x-ray equipment
still very popular among technologists
other collimator devices
aperture diaphragm, cones, cylinders
most effective of scatter control: cones
ancillary devices
lead blockers
shields
lead masks
attach to collimator
check vendor information for digital systems, before using lead blockers or masks