Radiology Physics X-ray Production
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Transcript of Radiology Physics X-ray Production
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RADIOLOGY PHYSICS
X-RAY PRODUCTION
Reported by
MARIA THERESA M. NAVARRO, M.D.
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Part I
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X-RAY MACHINE
• X-ray tube
• Operating console
• High-voltage generator
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Operating Console
• Apparatus that allows the radiographer to control the x-ray tube current and voltage so that the useful beam is of proper quantity and quality
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High Voltage Generator
• Responsible for converting the low voltage from the electric power company into a kilovoltage of the proper waveform
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X-RAY TUBE
• 1. SUPPORT STRUCTURE
• 2. PROTECTIVE HOUSING
• 3. GLASS OR METAL ENVELOPE
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SUPPORT STRUCTURE
a. Ceiling support - allows the greatest case of movement and range of position
b. Floor-to-ceiling support
c. Floor-mount system
d. Fluoroscopy tube
e. C-arm – mobile fluoroscopy unit
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PROTECTIVE HOUSING
a. Reduces leakage radiation to 100mR per hour at 1 meter
b. Provides mechanical support protecting the tube from damage
c. To conduct heat away from the x-ray target
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GLASS OR METAL ENVELOPE
• Surrounds the cathode (-) and anode (+), which are the electrodes at the ends of the vacuum tube (Coolidge tube).
• made of Pyrex glass to withstand the tremendous heat generated.
• maintains a vacuum or empty space
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CATHODE
• negative side of the x-ray tube
• TWO PRIMARY PARTS– a. Filament– b. Focusing cup
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CATHODE
• A. FILAMENT
• THERMIONIC EMISSION
At 4 amperes and above, the outer-shell electrons are literally boiled off and ejected from the filament
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CATHODE
• B. FOCUSING CUP
-where the filament is embedded
- negatively charged
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FILAMENT CURRENT
• SPACE CHARGE
• SPACE CHARGE EFFECT
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ANODE
• positive side of the x-ray tube• Function:
– electrical conductor– mechanical support– thermal conductor
• Two Types:– Stationary anode– Rotating anode
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TARGET
• area of the anode struck by the electrons from the cathode
• TUNGSTEN a. High atomic number (74) – high efficiency in
x-ray production and in high energy x-rays
b. Thermal conductivity – nearly equal to that of copper ; efficient for dissipating heat
c. High melting point – 3400 C ; can stand up under high tube current without pitting or bubbling.
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Part II
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Two Types of X-rays
• CHARACTERIC X-RAYS- produced by transitions of orbital electrons
from outer to inner shells
• BREMSSTRAHLUNG X-RAYS - braking of projectile electrons by the nucleus - most x-rays in the diagnostic range
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1. mA
- a change in mA results in a directly proportional change in the amplitude of the x-ray emission spectrum at all energies.
2. KVP
- when kVP is increased, the relative distribution of emitted x-rays shifts to the right to higher energies
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3. Added Filtration - increase in the effective energy of the x-ray beam
(higher quality) with an accompanying reduction in x-ray quantity
4. Target Material - as the atomic number of the target material increases,
the efficiency of the Bremsstrahlung radiation increases and the high energy x-rays increase in number more than the low-energy
x-rays
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Part III
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X-RAY QUANTITY
• Number of x-rays in the useful beam, which is the beam forming the radiographic image
• INTENSITY of radiation, measured in mR.
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X-RAY QUANTITY
1. mAs
2. kVp
3. SID
4. filtration
FACTORS AFFECTING X-RAY QUANTITY
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X-RAY QUALITY
• PENETRABILITY or PENETRATING POWER of an x-ray beam
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X-RAY QUALITY
• FACTORS AFFECTING X-RAY QUALITY
1. Kilovoltage
2. Filtration
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Types of Filtration
1. Inherent Filtration - built into the glass or metal envelope
2. Added Filtration - in the form of aluminum sheets
3. Compensating Filters - provided variation in beam quality, depending on thickness
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Part IV
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Types of X-ray Interaction with Matter
1. Classical Scattering
2. Comptom Effect
3. Photoelectric Effect
4. Pair Production
5. Photodisintegration
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CLASSICAL SCATTERING
• COHERENT or THOMPSON SCATTERING
• interaction between low energy x-rays and atoms
• x-ray loses NO energy but changes direction slightly
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COMPTON EFFECT
• in moderate energy x-rays and outer-shell electrons
• source of most of the OCCUPATIONAL radiation
• ionization of the target atom change in the photon direction -> reduction in photon energy
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PHOTOELECTRIC EFFECT
• photon absorption interaction causes electron removal from the atom (photoelectron)
• Characteristic x-rays are produced
• also a secondary radiation and behave as scatter radiation
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PAIR PRODUCTION
• Occurs with x-rays that have energies greater than 1.02 meV.
• The photon interacts with nuclear force field, and 2 electrons that have opposite electrostatic charges are created.
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PHOTODISINTEGRATION
• interaction between high energy photons and nucleus.
• photon is absorbed by the nucleus ->nuclear fragment is emitted.
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•At lowlow energies, the majority of x-ray interactions are
photoelectric, photoelectric, whereas at high high energies
Compton scattering Compton scattering predominates