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physics7&8
physics
| Question | Answer |
|---|---|
| the 3 principle parts of an x-ray imaging system are | x-ray tube, control console and high voltage generator |
| the primary purpose of the glass envelope of an x-ray tube is | provide a vacuum |
| the protective housing of an x-ray tube is designed to | reduce the hazard of leakage radiation |
| a diagnostic x-ray tube is an example of what | diode |
| the large filament is used during radiography when the heat load is | high and visiblity of detail is less important |
| in most x-ray tubes, there are 2 filaments to | provide 2 focal spots |
| the focusing cup | is the grid in a grid-controlled x-ray tube |
| once filament temperature becomes adequate, a further small rise in filament temperatur will cause tube current to | increase very much |
| the cathode beam of an x-ray tube is the | focused electron beam within the tube |
| the x-ray tube current | is controlled by the filament current |
| most x-ray tubes used for radiography | are dual focused tubes |
| the cathoded is | one of the 2 parts of a diode |
| when a filament burns out | the filament current goes to zero |
| the space charge effect | occurs in the vicinity of the cathode |
| the x-ray tube filament | conducts approximately 5 A |
| if saturation is achieved and the filament current is fixed, tube current | remains fixed |
| x-ray tube current | is 0 when filament current is below thermionic emission |
| a staionary anode x-ray tube | incorporates the line-focus principle |
| the heel effect occurs because of | x-ray absorption in the anode |
| the main reason for using the line-focus principle is to | reduce focal spot size |
| rotating anode x-ray tubes | incorporate the line-focus principle |
| x-ray intensity is higher on the cathode side than on the anode side because of which of the following | x-ray absorption in the anode |
| what is the target angle for most rotating anode x-ray tubes | 10 degrees |
| small target angles result in | small focal spot size |
| molybdenum is used for the stem material because of which of the following | is has a high atomic number |
| tungsten is the choice material for x-ray anodes because of its | high atomic number |
| the effective focal spot is | smaller than the actual focal spot |
| the heel effect | requires that the cathode be positioned to the thicker anatomy |
| what is a prominent engineering difficulty in the manufacture of high speed rotating anodes | balance of the rotor |
| which is a component of an electromagnetic induction motor | stator |
| necessary properties of the x-ray target material include | high melting point |
| which is an advantage of the rotating anode tube over the stationary anode tube | higher heat capacity |
| the anode angle of an x-ray tube is increased to give which of the following | higher heat capacity |
| which of the following components of a diagnostic x-ray tube is on the positive side of the tube | stator |
| as the anode target angle increases | effective focal spot size increases |
| a stationary anode will most likely be used in which of the following | dentistry |
| which is not a function of the anode | thermionic emission |
| what is the principle hurdle in the design of an x-ray anode for high-capacity radiologic techniques | heat dissipation |
| the high speed rotor (10,000 rpm) permits longer exposure times that the low speed rotor at single phase operation (3400 rpm) | true |
| if the intersection of time and KVp falls on an mA curve, that mA is safe | true |
| most of the troublesome heat generated in an x-ray tube occurs at the filament | false |
| generally, a small focal spot allows longer exposure times than a large focal spot | false |
| the radiographic rating chart reports the time that should elapse between exposures | false |
| it is not possible to exceeed the heat capacity of the housing without first exceeding that of the anode | true |
| a tube can become "gassy" because of anode overheating and the release of gas | true |
| the radiographic rating chart is designed primarily to protect the filament | false |
| rotor speed does not influence heat capacity | false |
| to determine whether any set of tube rating charts is applicable for a given x-ray tube, one should | identify the type of tube, the anode rotation, the focal spot size, and the type of generator to make certain that all of these match the specifications on the chart |
| if a single exposure were made with factors slightly exceeding those permitted by the appropriate radiographic rating chart, what would be the most probable result | the useful life of the tube would be reduced |
| if a single exposure were made with factors greatly exceeding those permitted by the appropriate radiographic rating chart, what would be the most probable result | the anode would pit and crack |
| which of the following conditions will not damage the x-ray tube | exceeding the prescribed SID |
| in the design of a rotating anode x-ray tube | most anodes rotate at 3400 or 10,000 rpm |
| the formula for heat units (HU) is a single phase high-voltage generator in | kVp x mA x s |
| if mass is expressed in kg and velocity in m/s, kinetic energy will be expressed in | joules |
| the kinetic energy of the principle electron in an x-ray tube | is about 1% efficient in the production of x-rays |
| the shift of the characteristic x-ray spectrum to higher energy occurs because of which of the following | an increase in target atomic number |
| useful characteristic x-rays are produced in tungsten | by removal of a K-shell electron |
| an L-shell elctron (binding energy 26 keV) is removed from an atom that has M-shell binding energy of 4 keV and N-shell binding energy of 1 keV. If a free electron fills the vacancy in the L-shell, the characteristic x-ray producted will have energy of | 26 keV |
| what is produced when the projectile electron excites an outer-shell electron | heat |
| the energy of characteristic x-rays increases with increasing | atomic number of targer material |
| x-rays are produced when | projectile electrons interact with target atoms |
| characteristic x-rays | are characteristic of target Z |
| when tungsten-targeted x-ray tube is operated at 68 kVp | some principle electrons have 68 keV |
| when characteristic x-rays are produced, the energy is characteristic of | the atomic number of the target |
| the kinetic energy of a projectile electron can be measured in | joules |
| the efficiency of x-ray production is | independent of tube current |
| in a tungsten-targeted x-ray tube operated at 90 kVp, the most abundant x-ray would be a | 30 keV bremsstrahlung x-ray |
| which of the following electron transitions results in the most useful bremsstrahlung x-rays | none of them |
| bremsstrahlung radiation is produced by | conversion of projectiole electron kinetic energy to electromagnetic energy |
| when a bremsstrahlung x-ray is produced | a projectile electron loses energy |
| in bremsstrahlung x-ray production | the projectile electron is from the cathode |
| if an average radiographic technique is used | most x-rays are bremsstrahlung |
| bremsstrahlung x-rays are produced only at | energies up to projectile electron energy |
| if radiographic technique is 74 kVp/ 80 mAs | bremsstrahlung x-ray energy increases if the voltage is increased to 84 kVp |
| if radiographic technique in a tungsten target at 60 kVp/ 80 mAs is changed to 80 kVp/ 80 mAs | the number of x-rays produced increases |
| bremsstrahlung x-rays produced in a tungsten-targeted x-ray tube | outnumber characteristic x-rays |
| when a bremsstrahlung x-ray is emitted | this results from the conversion of kinetic energy |
| the wavelength of an x-ray | becomes longer as projectile electron kinetuc energy is reduced |
| when projectile electron energy is increased | more bremsstrahlung x-rays are produced |
| the efficiency of bremsstrahlung x-ray production increases with increasing | target atomic number |
| the output intensity of an x-ray tube | is primarilly due to bremsstrahlung x-rays |
| which of the following projectile electron target interactions results in x-ray emission | removal of inner shell electrons |
| when a projectile electron enters a target atom and interacts with the nuclear force field | it decreased in velocity |
| the area under the curve of the x-ray emission spectrum represents | the total number of x-rays |
| normally, the x-ray emission spectrum contains | both characteristic and bremsstrahlung x-rays |
| the characteristic x-ray emission spectrum principally depends on | target material |
| the continuous x-ray emission spectrum principally depends on | projectile electron energy |
| which of the following factors explains the low number of x-rays produced at low energy | added filtration |
| the x-ray emission spectrum represents | x-rays emitted from the x-ray tube |
| both the shape and the position of the characteristic x-ray emission spectrum | correspond to target electron binding energies |
| a diagnostic x-ray beam contains | mostly bremsstrahlung x-rays with some characteristic x-rays |
| the x-ray emission spectrum is a plot of | the number of x-rays vs energy |
| the amplitude of the bremsstrahlung x-ray emission spectrum | has maximum value at energy approximately 1/3 of the kVp |
| if an x-ray emission spectrum represents operation at 85 kVp with a tunsten target | the K-characteristic x-ray emission would occur at 69 keV |
| if an x-ray emission spectum represented operation at 26 kVp with a molybdenum target | the characteristic radiation would have an energy of approx 19 keV |
| which of the following factors principally accounts for the reduced x-ray intensity at low energy | added filtration |
| characteristic x-radiation is related to the | energy required to eject K-shell electrons |
| molybdenum has a lower atomic number that tungsten, therefore, the molybdenum x-ray emission spectrum | has lower amplitude |
| to construct an x-ray emission spectrum, one must know | number of x-rays at each energy interval |