Produced ISOTROPICALLY and has EQUAL INTENSITY to all directions
Size is VARIABLE by using x-ray beam collimators
Intercepted by MATTER & TISSUE
ray production
1. Using a HIGH VOLTAGE and an ELECTRIC CURRENT
2. Fast moving electrons coming from the cathode interacts with the target in the anode
Primary Beam
X-rays emitted through the window of the x-ray tube are called the USEFUL BEAM or PRIMARY BEAM
Transmitted from the x-ray tube to the image receptor
The quality and quantity of the primary beam can be determined by the kVp and mAs
It should never be directed at the radiologic technologist, other personnel, or the control booth
The actual x-ray beam that is intercepted by the patient
Central Ray
Imaginary line in the useful beam
Centermost part of the x-ray beam
Should be aligned to the center of the structure being imaged and grid if being used
Particularly important in radiographic positioning and reducing image distortion
If the intensity of the central ray is 100%, then the x-ray intensity on the cathode side may be as high as 120% and the anode side as low as 75%
Exit/Remnant Beam
The part of the x-ray beam that exits the patient after interaction
Interact with the patient and are scattered away
Leakage Radiation
Any x-rays that escape the protective housing of the X-ray tube
Contributes nothing in the way of diagnostic information and results in unnecessary exposure of the patient and radiologic technologist
Must not exceed 100 mR/hr at 1 meter
Off-Focus/Stem Radiation
Also known as Extrafocal X-rays
X-rays tubes are designed so that the projectile electrons from the cathode interacts with the target only at the focal spot
Some electrons bounce off the focal spot and land on other areas of the target causing x-rays to be produced from outside of the focal spot
Undesirable because it extends the focal spot size increasing the skin dose unnecessarily
Can reduce the radiographic image contrast
Can be a reason that tissue that was meant to be excluded, appear on the radiograph
Can also be reduced by the use of metal enclosures which extract and conduct the reflected electrons
Reduced by using a fixed diaphragm inside the x-ray tube near its window
Radiography is the process of producing images using ionizing radiation.
Kinetic Energy
Energy in motion
Electrons with high kinetic energy focused toward a small spot on the anode are necessary for x-ray production
Kinetic Energy Equation
KE = (1/2)(mv^2)
M - mass in kg
V - velocity in meters per second
KE - kinetic energy in joules
Kilo electron volts
What energy of x-rays are expressed as
1 keV = 1.6 x 10^-16 J
ray imaging system
Primary function is to accelerate electrons from cathode to anode
1 cm - distance of the filament to the target
Heat
Most of the projectile electrons' kinetic energy is converted into this
Thermal Energy
99% of projectile electron interaction is converted into this
Projectile Electrons
Interact with outer shell electrons which causes excitation then return to the original state
Constant excitation and return to normal state - responsible for most heat generated in the Anode
Factors affecting the production of Anode Heat
Tube Current = increase mAs, increase anode heat
Tube Voltage = increase kVp, increase anode heat
1% - percentage of anode heat used in x-ray production
ray tube - considered to be an ineffective device
Projectile Electrons
Electrons traveling from the cathode to anode
When electrons hit the anode, they transfer their kinetic energy to the target atoms
These electrons interact with the orbital electrons or the nuclear field of the target atoms
These results in the formation of thermal energy and electromagnetic energy in the form of infrared and x-rays
Interact with an inner shell electron and ionizes it leaving a void to be filled by an outer shell electron
Characteristic Radiation
Produced when an outer shell electron fills an inner shell void
Emission of x-ray occurs as the outer shell electron fills the inner shell
Any other outer shell electron can fill in an inner void
K x-rays
Occurs when radiation is produced by any other outer shell electron filling a K shell vacancy
characteristic x-rays of tungsten - only ones useful in x-ray imaging as all other outer shell electron binding energy is lower than of a K-shell electron
shell x-rays - require an x-ray tube with a potential of 69 kVp and up since the K-shell electron of a tungsten target has an effective energy of 69 KeV
Bremsstrahlung
German word meaning "slowed down"
Bremsstrahlung Radiation
Results from the braking of projectile electrons by the nucleus of an atom
Where the projectile electrons completely avoids the orbital electrons as it passes through the target atom and may come close enough to the nucleus to interact with its electric field
Nuclear Force Field
Where projectile electron loses its kinetic energy as it interacts with this then changes direction
Electromagnetic energy
What lost kinetic energy is converted into
Electrostatic force of attraction
Causes the "braking" down of electrons
Occurs between nucleus of atom and projectile electrons
Nucleus of an atom is positively charged
Projectile Electrons are negatively charged
Low energy bremsstrahlung x-rays
Results when the projectile electrons barely interact with the nuclear force field
In diagnostic range, most x-rays are Bremsstrahlung x-rays
In bremsstrahlung radiation, energy produced can be 1 keV up to 70 keV
An electron with kinetic energy of 70 keV can lose ALL, NONE, or ANY intermediate level of that kinetic energy
Computed Tomography (CT) uses multiple views of the same area to create cross sectional images of the human body.