Interactions of x- and γ- rays with matter: classical Scattering, photo-absorption/photoelectric effect, Compton scattering, pair- production & Photodisintegration
Radioactive decay law & Activity
Attenuation of radiation – absorption coefficients; attenuation of homogeneous and heterogeneous beams
Radiographic image formation and characteristics
Mechanical Wave
A periodic disturbance in a medium that carries energy from one point to another
Types of mechanical waves
Longitudinal
Transverse
Wavelength (λ)
The horizontal distance along a wave between similar particles of the wave
Displacement
The distance of a particle of the wave from the equilibrium position at any particular time
Amplitude (a)
The maximum displacement of a particle of the wave from its equilibrium position
Period (T)
The time for one complete oscillation of the wave
Frequency (γ)
The number of waves produced per second
Velocity (v)
The velocity of a particle of a wave in the direction the wave is travelling
James Clerk Maxwell
Scottish mathematician and physicist
Defined the Non-mechanical waves in a vacuum of space
Unified existing laws of electricity and magnetism
Oscillating electric field produces a magnetic field (and vice versa) – propagates an EM wave
The Wave model can be described by 4 differential equations
Electromagnetic (EM) wave
Electric field (E) perpendicular to magnetic field (M)
Travels at velocity, c (3x10^8 ms^-1, in a vacuum)
At the atomic scale, electromagnetism governs the interactions between atoms and molecules
At the macroscopic scale, electromagnetism manifests itself in the familiar phenomena that give the force its name
Maxwell's Equations
Four equations relating electric (E) and magnetic fields (B) – vector fields
ε0 is electric permittivity of free space (or vacuum permittivity - a constant)
μ0 is magnetic permeability of free space (or magnetic constant – a constant)
EM Spectrum
The velocity (c) of propagation of EM radiation through space is constant but the wavelengths (λ) and frequencies (γ) varies
EM spectrum results from these waves propagating at different wavelengths and frequencies
Line spectra are the result of interaction between atoms (can also be atomic nuclei or molecule) and a single photon
When a photon has sufficient energy to change the energy state of the atom (where an electron changing orbitals), the photon is absorbed
The previously, absorbed energy will be re-emitted as light
The sum of the energies of the photons emitted will be equal to the energy of the one absorbed
Spectral lines are highly atom-specific, and can be used to identify the chemical composition of any medium capable of letting light pass through it (typically gas is used)
The line spectrum of an element results from the emission of photons with specific energies from the atoms of that element
Quanta
A discrete quantity of energy proportional in magnitude to a particular frequency (γ) of EM radiation and corresponding to a single photon or to a transition of an atom between two internal energy states
Photon energy
E = hγ, where h is Planck's constant and γ is the frequency of the wave
If only certain energies are allowed, the allowed energies correspond to the differences between energy levels
ray Production
X-rays are produced when rapidly moving electrons that have been accelerated through a potential different of the order 10^3 - 10^6 volts strike a metal target
Electron are "boiled off" from the heated cathode by the principle of thermionic emission and these electrons accelerated towards the anode (the target) by a large potential different Vac
The most energetic photon (with λ and γ) is produce when all the electron's kinetic energy goes to produce on photon (bremsstrahlung limits)
Characteristic X-ray
The second process gives peaks in the x-ray spectrum at characteristic frequencies and wavelengths that do depend on the target material
ray tube
Requires an electron source, electron acceleration potential, and target for X-ray production
The intensity of the electron beam determines the intensity of the X-ray radiation
The electron energy determines the shape of the bremsstrahlung's x-ray spectrum
Low energy X-rays are absorbed in the tube material to produce the characteristic x-ray spectrum
The X-ray energy determines also the emission of characteristic lines from the target material
Gamma radiation (γ-rays)
EM waves of an extremely high frequency and are therefore high energy photons
Produced by the decay of atomic nuclei as transition from a high energy state to a lower state known as gamma decay
Five forms of x-ray Interactions
Classical or Coherent Scattering
Compton Effect
Photoelectric Effect
Pair production
Photodisintegration
Coherent Scattering
Also known as classical, elastic, unmodified or Rayleigh scattering
The incident photon interacts with and excites the total atom
Occurs at low energy photons of less than 30keV
The wavelength of the incident and scattered photon/wave remain unchanged after the interaction
No net energy has been absorbed by the atom
Electrons are not ejected and thus ionization does not occur
In soft tissue, Rayleigh scattering accounts for less than 5% of x-ray interactions above 70 keV and at 12% of interactions at approximately 30 keV
Compton Scattering
Compton scattering (inelastic or non-classical) is the predominant interaction of x-ray photons in the diagnostic energy range with soft tissue
This interaction is most likely to occur between photons and outer ("valence") shell electrons, which are loosely bounded in the outer shell electron cloud
The ejected electron is called a Compton or recoil electron and scattered photon is called a Compton photon
The energy of the incident photon (Ei) is equal to the sum of the energy of the scattered photon (Esc) and the kinetic energy of the ejected electron (Ee-)
The freed electron possesses excess kinetic energy (Ek) and is capable of ionizing atoms
In radiography, photons scattered in the forward direction can reach the film and add to background fog and reduce image contrast
In diagnostic radiology, the probability of occurrence of Compton scattering relative to that of the photoelectric absorption is not influence increase as the energy of the x-ray photon increases