electromagnetic waves and x-ray creation Flashcards
gamma rays (10^-12m - 10^-16m)
- highest energy photons and have extremely short wavelength
- generated by changes in energy levels of the nucleus of atom
- used in nuclear medicine and PET scans
x-rays
- 10^-10m
- high energy photons
- generated by deceleration of fast moving e-s
- generated by changed in energy of innermost orbital e-s of atoms
- gamma n x are detected by photography, ionisation chamber and phosphorescence
properties of gamma and x
- penetrate matter
- ionise gas (remove e-s)
- cause fluorescence
- photoelectric emissions from metals
- reflected and diffracted by crystals
uv radiation
- 10^-8 m - 10^-9 m
- detected with light sensitive circuits (CCDs, photography and fluorescence
- absorbed by glass
- causes chem reactions e.g sun damage- skin damage
- the ionosphere, ayer high in atmosphere, was created by UV radiation from sun ionising atoms in this layer
- generated by orbital e-s of atoms
- also by sun and generated mercury vapour lamps
infrared radiation
- 10^-6m
- generated by outer e-s in atoms and molecules and changes in vibrational and rotational energies of molecules (all bonds between atoms vibrate and the freq of vibrations is characteristic of atomic bones involved
- makes colourful images depicting elevated skin temp
- night sights use IR radiation, thermal cameras
microwaves
- 10^-4 m - 10^-1m
- emerging biomedical imaging modality
- noninvasive assessments of functional and pathological conditions of soft tissue
- ultrawide band microwave imaging is promising method for detection of breast cancer
radio waves
- 10^3m
- astronomy
- MRI
- communication
- generated by oscillating e-s in special circuits to radioactive aerials (the transmitter)
- tuned oscillatory circuit (radio receiver)
electromagnetic waves
- single frequency EM wave exhibit a sinusoidal variation of electric and magnetic fields in space
- magnetic variation is perpendicular to electric field
- EM waves travel in straight lines
electromagnetic wave description
- sinusoidal wave
- amplitude- height of wave
- wavelength- length of one cycle
- frequency- cycles per second
electromagnetic wave equation
c=f x lambda
c= speed of wave (ms-1)
f= frequency (Hz)
lambda= wavelength
energy of electromagnetic radiation equation
E= h x f
h= plancks constant (6.626x10^-34)
f= frequency
photon
- think of light as a series of particles or photons
- elementary particle
- em radiation therefore consists of discrete quantises packets of energy which we call photons
- no mass, no electric charge and does not decay spontaneously
- consists of oscillating electric field component E and oscillating magnetic field component B
inverse square law
- expresses the way radiation energy propagates though space
- E= I / r^2
- E= energy
- I= radiation intensity
- r= distance from source
- rule states that the “power intensity per unit area from a power source, if the rays strike the surface at a right angle, varies inversely according to the square of the distance of the source”
x-ray creation
there are 2 types of interactions of electrons with the anode target produce radiation
1. interaction with the atomic nucleus produce bremsstrahung x-ray photons
2. interaction with e- shells which produces characteristic x-ray photons
bremsstrahlung spectrum
- energy distribution for a 90 kVp acceleration potential
bremsstrahlung radiation
- characterised by continuous distribution of radiation
- referred to as the continuous x-ray spectrum
- an e- with kin energy of 70 keV can lose all, none and any intermediate level of its kin energy in a bremsstrahung interaction
- for e-s with kin energy of 70 keV, the brem. emissions can have an energy in the range of 0-70 keV
- 70keV in joules corresponds to the cut off wavelength
bremsstrahlung equation
- E= h x c / lambda
- min lambda=. h x c / E max
- h= plancks
- c=. velocity of em radiation in a vacuum 3 x 10^8ms-1
characteristic radiation
- atomic electron from innermost shell is ejected by incoming high energy e-, creating a vacancy in the shell
- e- from next shell drops down to fill vacancy so charactertic x-ray unique to thus element is emitted
- produced a vacancy in that shell- transitions depend on differences in energy between shells
x-ray spectrum
2 production processes occur: bremsstrahlung rad. and characteristic x-rays