10. Interaction of Radiation with Matter Flashcards
is defined as the rate of emitted energy from unit surface area through unit solid angle
Radiation Intensity
The total reduction in the number of x-rays remaining in an x-ray beam after penetration through a given thickness of tissue
Attenuation
is the product of absorption and scattering
Attenuation
is an all-or-none condition for an x-ray
Absorption
is a quantity that characterizes how easily a material or medium can be penetrated
by a beam of light, sound, particles, or other energy or matter.
Attenuation Coefficient
The attenuation coefficient is also called
linear attenuation coefficient,
narrow beam attenuation coefficient, or
absorption coefficient
means that the beam is quickly “attenuated” (weakened) as it passes through the medium
large attenuation coefficient
means that the medium is relatively transparent to the beam
small attenuation coefficient
The difference in x-ray interaction
Differential Absorption
Increases as the kVp is reduced
Differential Absorption
Differential absorption and attenuation of the x-ray beam depend on the following factors:
o The atomic number (Z) of the atoms in tissue.
o The mass density of the atoms in tissue.
o The x-ray energy.
The Thickness of an absorber needed to reduce the intensity of the x-ray beam into half of its original value
Half-Value Layer (HVL)
The fraction of the beam that penetrates the block
Transmission Fraction
TF = 2^–n
Where n =
block thickness/half value thickness
X-ray Interaction Mechanism
- Coherent Scattering
- Compton Scattering
- Photoelectric Effect
- Pair Production
- Photodisintegration
Energies below approximately 10 keV
Coherent Scattering
Coherent Scattering sometimes called
Classical scattering or Thompson scattering, Rayleigh Scattering
No ionization
Coherent Scattering
is an interaction between low-energy x-rays and atoms.
Classical scattering
The x-ray loses no energy but changes direction slightly.
Classical scattering
The wavelength of the incident x-ray is equal to the wavelength of the scattered x-ray
Classical scattering
the incident x-ray interacts with an outer shell electron and ejects it from the atom,
thereby ionizing the atom
Compton Effect
The ejected electron is called a
Compton electron or a secondary electron
occurs between moderate-energy x-rays and outer-shell electrons.
Compton Effect