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Unformatted text preview: Ben Sauerwine Practice for Qualifying Exams Thanks to Ryan for his input in this problem. Problem Source: CMU February 2006 Qualifying Exam Consider an azimuthally symmetric magnetic field, such as might be produced by a dipole magnet with circular pole faces, of the form ( ) z r B B ˆ = v . An electron of charge e orbits in this field at a fixed radius R with momentum p v in the ( ) θ , r plane. (a) What is the frequency of the electron, ω , assuming the magnetic field is time independent? ( ) ( ) ( ) ( ) ( ) R B e m v R R B m eR v R eRB p R B m p e mR p r mR p r R v m F r R B m p e B v q F c B π π ω 2 2 ˆ ˆ ˆ 2 2 2 = = = = = − = − = − = × = v v v v (b) Suppose we inductively accelerate this electron by varying the magnetic field slowly in time in some way. We want the electron’s orbit to remain fixed at R. Derive a condition that relates ( ) r B and the average value of the field within the orbit, B , that allows this to happen. This is the so-called Betatron condition. Make a rough sketch of ( ) r B vs. r that allows this acceleration technique to work. The fact that we are working with the average value of the field inside the orbit seems to imply that Faraday’s Law would be a good place to start: ( ) ( ) B dt d R l d E dS n r B R B dS n r B dt d l d E C S S C 2 2 ˆ 1 ˆ π π − = ⋅ ⋅ = ⋅ − = ⋅ ∫ ∫ ∫ ∫ v v v v v v By symmetry, the electric field must be the same all the way around the loop. By symmetry, the electric field must be the same all the way around the loop....
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This note was uploaded on 04/07/2012 for the course PHYSICS 767 taught by Professor Dr.jaouni during the Spring '12 term at Abu Dhabi University.
- Spring '12