Effect of a magnetic field on a bean of particles.

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SUMMARY

The discussion centers on the effect of a magnetic field on a beam of charged particles, specifically demonstrating that the magnetic field focuses the beam to a point at a distance of z = 2πmv/|q|B. The relevant equations include the Lorentz force F = q(v × B) and the motion equation dv/dt = -q/m (B × v). The challenge lies in the beam's initial velocity being approximately parallel to the magnetic field, necessitating the use of a Taylor approximation to analyze the trajectory of particles at the beam's outer edge.

PREREQUISITES
  • Understanding of Lorentz force and its application in charged particle motion
  • Familiarity with vector cross products and their geometric implications
  • Basic knowledge of Taylor series approximations
  • Concept of angular dispersion in particle beams
NEXT STEPS
  • Study the derivation of the Lorentz force in electromagnetic theory
  • Learn about the application of Taylor series in physics problems
  • Explore the dynamics of charged particles in magnetic fields
  • Investigate angular dispersion effects in particle beam optics
USEFUL FOR

This discussion is beneficial for physics students, educators, and researchers focusing on electromagnetism, particle physics, and beam dynamics in accelerator physics.

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Homework Statement


a beam of particles of charge q with velocity v is emitted from a point source, roughly parallel with a magnetic field B, but with a small angle of angular dispersion. Show that the effect of the field is to focus the beam to a point at a distance z = 2[/pi]mv/|q|B.


Homework Equations


We know the force F= q vxB
dv/dt = -q/m Bxv


The Attempt at a Solution


I try to solve the problem with the force. However, since the beam is roughly parallel to B, the cross product tends to 0. I am now like clueless...
 
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The initial velocity is approximately parallel to B, not exactly parallel. Try calling the angle between v and B, \theta and calculating r(t) for a particle on the beams outer edge. Then use a Taylor approximation for your expression for small \theta to find the location where r(t) lies on the z-axis (assume that B points in the z-direction).
 

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