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atoms
composed of multiple subatomic particles:
protons: positively charged, mass of 1.007 AMU
neutrons: no charge, mass of 1.008 AMU
electrons: negatively charged, mass of 0.0005 AMU
orbit around nucleus in orbitals that have different energy levels
protons and neutrons make up the nucleus of an atom
atomic number
Z, equal to amound of protons
atomic mass
A, equal to number of protons and neutrons
ion
atom that has either a positive or negative charge
isotope
same atomic number (# of protons), but different atomic mass (protons + neutrons)
types of radiation
particulate radiation → alpha particles (2P + 2N), beta particles (1 e)
electromagnetic radiation → gamma rays, x-rays, microwave, visible light
sources of radiation
natural → radon (natural gas), terrestrial (rocks), cosmic (from space), internal (within body)
man-made → computed tomography, radiographs
radioactive decay
when unstable atoms spontaneously emit an alpha particle, beta particle, or gamma ray in attempt to be more stable
N is approximately P for small atoms
as atomic number increases, N/P ratio increases and results in an unstable atom
atoms above a certain atomic number will be unstable due to having too many neutrons
electromagnetic radiation
produced when velocity of charged particle is altered
x-rays produced when electrons interact with atoms, slowing them down
x-rays are ionizing radiation because it has enough energy to knock electrons off atoms and. turn them into ions
artificial x-ray generation
cathode is heated by power supply to release electrons
negatively charged to repel electrons away
anode. contains tungsten target where electrons hit
high voltage accelerates electrons towards positively charged anode
when electrons hit target, the energy is converted into heat (99%) and x-rays
components in x-ray machines
focusing cup: helps ensure electron beam is directed at tungsten target
power supply: provides a high voltage between cathode and anode, and low voltage to heat up cathode
current selector: measure in mA and indicates number of electrons sent from cathode to anode per second
voltage selector: measured in kVp and indicates maximum voltage of current
timer: controls duration of exposure, measured in seconds
rectifier: decreases variance in voltage by using capacitors to make it a steady stream of voltage to allow for better image quality
focal spot
area on tungsten target where electron beam from cathode hits and produces x-rays
anode should be angled for increased sharpness due to focal spot appearing smaller
larger surface area for ehat dissipation
will get a perfect image if all electrons in beam go to a single focal spot and image receptor
electron volt (eV)
change in energy of an electron moving across one volt
energy of x-ray photon measured in keV and usually range between 0 and 70 keV
more photons with lower photon energies and very rarely photons at high energies
Bremsstrahlung (breaking) radiation
energy emitted when directly hitting or passing near nucleus
electron slows down because positively charged protons slow electrons and change its trajectory
energy is released as electromagnetic wave, where resulting radiation is a whole spectrum of energies → conservation of energy
for direct hit → energy of incident electron = energy of resulting photon
for slowed electron → difference in kinetic energy = energy of resulting photon
characteristic radiation
incident electron interacts with and ejects inner shell electron
valence electron from outer shell fills vacancy in inner shell
outer shell electron is at a higher energy state, so difference in energy is released in form of a photon
resulting radiation is at very specific levels of energy → characteristic of target material