Deriving the E Cross B Drift Velocity: A Puzzling Explanation

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SUMMARY

The discussion centers on the derivation of the E cross B drift velocity in plasma physics, specifically addressing the justification for the drift velocity's perpendicularity to the magnetic field. The participant references a document from San Francisco State University and highlights the role of the Lorentz force law in establishing this relationship. It is concluded that the drift velocity must indeed be perpendicular to the magnetic field to satisfy the conditions set by the Lorentz force, confirming that this is not merely an ansatz but a fundamental aspect of plasma motion.

PREREQUISITES
  • Understanding of the Lorentz force law in electromagnetism
  • Familiarity with plasma physics concepts
  • Knowledge of vector calculus
  • Ability to interpret mathematical derivations in physics
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  • Study the implications of the Lorentz force law on charged particle motion
  • Explore the mathematical derivation of E cross B drift in plasma
  • Investigate applications of E cross B drift in magnetic confinement fusion
  • Learn about the role of magnetic fields in plasma stability
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This discussion is beneficial for plasma physicists, electrical engineers, and students studying electromagnetism who seek to understand the dynamics of charged particles in magnetic fields.

pierce15
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I am looking at this brief derivation of the E cross B drift for a plasma, starting at the top of page 3: http://www.physics.sfsu.edu/~lea/courses/grad/motion.PDF.

I am a bit confused as to the justification that the drift velocity is perpendicular to the magnetic field, as stated at the top of page 3. Is this an ansatz, which just happens to work out? One can immediately check that this velocity solves the equation preceding (5), and if I am not mistaken the solution is linear in components of drift velocity so it must be the unique solution.

Or am I missing something and is there a reason why the drift velocity is perpendicular to B?
 
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Yes, there is a reason why the drift velocity is perpendicular to B. This is because of the Lorentz force law, which states that the force on a particle in a magnetic field is proportional to the velocity and perpendicular to both the velocity and the magnetic field. Therefore, the drift velocity must be perpendicular to the magnetic field in order for the Lorentz force to be zero.
 

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