Acceleration of Particles
Goethe, Faust
q*B = 2 Pi* m* f. At proton energies above 50 MeV, cyclotron begins to fail; as the speed of charged particle begins to approach the speed of light, the frequency of the particle decreases. The required radius of dees is increasing greatly (for 500-GeV proton in B=1.5T, r = 1.1 km). A synchrotron avoids these difficulties: Both B and f are programmed to change cyclically. The particle acquires high energy (~1TeV in Fermilab synchrotron, ~20TeV in CERN ), going in constant orbital radius. Learn about different types of particle accelerators (cyclotron, synchrocyclotron, linac, synchrotron) and ways to detect/observe particles.
Compare different types of particle accelerators, provide analysis of methods used for accelerating particles, particles accelerated, energies achieved.
What kind of the basic research can be done using various types of particles accelerators (gold-foil alpha scattering, early cyclotrons, synchrocyclotrons, linacs, Tevatron, CERN LHC? Provide ranges of typical particle energies for each type of accelerator and resolving ability of the particles (de Broglie wavelength lambda = h / (mv)).
Explain why high-energy particles are effective tools for resolving the finer details of the working of atoms.


