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Beam Therapy Equipment
1 Linear Accelerator Basics
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X-ray production Treatment beams produced by linear accelerators
Consists of an electron gun, RF source, waveguide, bending magnet and treatment head Electrons emitted from the gun, accelerated down the waveguide using microwaves, re-directed with a magnet and hit a tungsten target to produce x-rays
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Electron gun Made of thermionic material e.g. Thorium
Cathode – negative charge, electrons accelerated from it Electrons emitted when heated – ‘boil’ off Gun often gridded – has a positive grid in front to accelerate the electrons Grid is pulsed so get pulses of electrons Have pulses of electrons entering waveguide
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Microwave production Two devices invented in 1939 for WWII radar – Magnetron (GEC) and Klystron (Varian brothers) Operated at frequency of 3 GHz – wavelength of 10cm Required for high power radar systems
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Magnetron – self oscillator
Cathode in centre of evacuated, lobed chamber Magnetic field perpendicular Electrons spiral out inducing resonant radio-field Sampled and fed to waveguide
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Klystron - amplifier Electron gun produces stream of electron
Pulsed by low energy microwaves Pulsed electrons induce high energy microwaves in tuned cavity
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Waveguide Hollow, pressurised, rectangular tube – carries RF to linac waveguide Circular, linac waveguide under vacuum Made of copper – to conduct charge Electric fields from microwaves produce electric currents produce new magnetic and electric fields that travel along pipe Electrons enter waveguide accelerated by microwave radiation into bunches Varian – Standing wave Elekta – Travelling wave
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Standing wave Microwaves reflected from distal surface to produce a standing wave
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Travelling Wave Microwaves absorbed at distal surface – travelling wave
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Beam control Linacs have focusing magnets and steering magnets
Electric currents through wires produce magnetic fields These magnetic fields are used to move the electron beam (-ve charge) They focus the electrons into thin beam Also used to steer the beam vertically and horizontally in the waveguide for flatness
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When electron beam exits accelerator it is bent (90°/270°) and strikes target producing x-rays
These get flattened, measured and shaped and exit treatment head
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Bending magnet Only required if need to redirect electron beam
Doubly achromatic Needs to be cooled Change field strength and thus beam energy by adjusting current
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Problems with 90° bending magnets
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