Acceleration of Particles
“I need to talk of what I don't know yet, So that I may perceive whatever holds The world together in its inmost folds, See all its seeds, its working power…”
Goethe, Faust
Goethe, Faust
One of the effective ways to analyze the structure of matter is to allow an energetic charged particle to collide into a solid target, or into another energetic charged particle. Studying the debris of the collisions is a very effective way to learn about the nature of the particles of matter. Charged particles can acquire the required for collision kinetic energy in acceleration process “falling” through potential difference or centripetal acceleration in magnetic field. Since it is difficult to establish necessary potential difference for higher energy particles, a charged particle can accelerate in magnetic field with periodic electrical boost (~100 keV per revolution). The device cyclotron is a particle accelerator that uses magnetic field to hold charged particle on circular orbit so that the modest accelerating potential can act on it rapidly, resulting in high energies. The frequency of circulation of the particle equals to the frequency of electrical oscillator.
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.
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.
