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Xray Emission
Bushong (9th; Ch 9)
Question | Answer |
---|---|
A measure of the number of ion pairs produced in air by a quantity of x-rays | roentgen (R) or milliGray [subscript a] (mGya) |
the number of x-rays in the useful beam | x-ray quantity |
X-ray intensity of most general purpose radiographic tubes, when operated at approx. 70 kVp | 5 mR/mAs (50 μGya) at 100cm SID |
Units of x-ray intensity | roentgens (R), mGya, mR/s, mR/min, or mR/mAs |
X-ray quantity or intensity; measured in roentgens (R) | radiation exposure |
radiation ________ = x-ray _________ = _____ quantity | exposure; intensity; x-ray |
x-ray ________ is ________ proportional to the mAs | quantity; directly |
a measure of the total number of electrons that travel from cathode to anode to produce x-rays | milliampere seconds (mAs) |
a measure of the electrostatic charges; 6.25 x 10¹⁸ electrons | Coulomb (C) |
Formula for x-ray quantity & mAs | I₁/I₂ = mAs₁/mAs₂ |
Formula for x-ray quality & kVp | I₁/I₂ = (kVp₁/kVp₂)² |
X-ray ________ is ____________ to the kVp² | quantity; proportional |
mC = ___ | mAs |
For optical density to remain constant, if kVp is increased by ___ then mAs should be _______ by ½ | 15%; reduced |
X-ray quantity is _________ proportional to the square of the ________ from the ______ | inversely; distance; source |
X-ray intensity varies _________ with the ______ of the ________ from the x-ray tube ______ | inversely; square; distance; target |
Formula for x-ray quantity & distance | I₁/I₂ = (d₂/d₁)² |
Square Law | mAs₁/mAs₂ = (SID₁)²/(SID₂)² |
When SID is increased, ___ must be increased by ____ to maintain constant exposure to the IR | mAs; SID² |
Purpose of filters | reduce number of low-energy x-rays |
Commonly used metal filter | 1-5mm Al |
Adding __________ to the useful x-ray beam reduces _______ ____. | filtration; patient dose |
Disadvantage of ↑ kVp & ↓ mAs for OD to remain constant | ↓ image contrast |
Disadvantage of added filtration | ↓ image contrast |
increases the number of high energy x-rays in the beam by removing the lower-energy nonpenetrating x-rays | beam hardening |
one description of the ability of x-rays to penetrate deeper in tissue | penetrability |
the penetrability of an x-ray beam | x-ray quality |
X-rays of any given energy are more penetrating in material of ____ atomic number than in material of ____ atomic number | low; high |
the reduction in x-ray intensity that results from absorption & scattering | attenuation |
the thickness of absorbing material necessary to ↓ reduce the x-ray intensity to ½ of its original value | Half-value layer (HVL) of an x-ray beam |
HVL of diagnostic x-ray beam | 3-5mm Al, or 3-6cm soft tissue |
the best method for specifying x-ray quality | HVL |
X-ray beam quality can be identified by _______ or __________, but ___ is most appropriate | voltage; filtration; HVL |
Atomic number of aluminum (AL) | 13 |
Atomic number of gadolinium | 64 |
Atomic number of holmium | 67 |
Atomic number of copper (Cu) | 29 |
Atomic number of tin | 50 |
Increasing the ___ peak _________ the quality of an x-ray beam | kVp; increases |
Amount of total filtration | 2.5mm Al |
Increasing filtration increases the _______ of an x-ray beam | quality |
Atomic number of Beryllium | 4 |
↑ filtration = ↑ beam _______ = ↓ beam ________ | quality; quantity |
part of the glass or metal enclosure of an x-ray tube through which x-rays are emitted | window |
reason why window is thin | provides for low inherent filtration |
type of filtration provided by the glass or metal enclosure of an x-ray tube; filters emitted x-ray beam | inherent filtration |
inherent filtration of a general purpose x-ray tube | 0.5mm Al equivalent |
type of special purpose tube with very thin window | mammography |
inherent filtration of mammography unit | 0.1mm Al; sometimes made of Beryllium rather than glass |
Added filtration results in ↑ ___ | HVL |
Added filtration resulting from the silver surface of the mirror in the collimator | 1mm Al equivalent |
material inserted between an x-ray source & a patient to shape the intensity of the x-ray beam; an x-ray beam filter designed to make the remnant beam more uniform in intensity | compensating filter |
special filters used with CT imaging systems to compensate for the shape of the head or body | "bow-tie"-shaped filters |
type of filter sometimes used in chest radiography; thin region over mediastinum & thick portions lateral over lung fields | bilateral wedge filter; trough filter |
type of filter applicable to digital fluoroscopy, where the IR, the image intensifier tube, is round; can be concave or convex | conic filters |
type of filter that compensates for OD variation of body parts that vary considerably in thickness | wedge filter |
type of filter used in special procedures involving long sections of anatomy on 2 or 3 separate IRs | step-wedge filter |