Particle movement in a non-static magnetic field

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SUMMARY

The discussion focuses on the movement of particles in a non-static magnetic field, specifically addressing the application of the Lorentz force equation. The user presents the equation for particle acceleration, incorporating electric field and magnetic field interactions, and explores the limitations of using magnetic flux conservation in coupled coils. A modified formula is proposed to account for the helical trajectory of ions in slowly varying magnetic fields, emphasizing the importance of the Cyclotron radius in these calculations.

PREREQUISITES
  • Understanding of the Lorentz force equation
  • Familiarity with electromagnetic theory and magnetic fields
  • Knowledge of plasma physics and particle dynamics
  • Basic principles of transformers and magnetic flux conservation
NEXT STEPS
  • Study the derivation and implications of the Lorentz force equation in varying magnetic fields
  • Research the concept of Cyclotron motion and its applications in plasma physics
  • Explore the behavior of particles in electromagnetic fields using simulation tools like COMSOL Multiphysics
  • Investigate advanced topics in electromagnetic induction and its effects on particle trajectories
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Physicists, electrical engineers, and researchers in plasma dynamics who are interested in the behavior of charged particles in varying magnetic fields.

Javier Lopez
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Particles follows accordingly the general equation:

$$
m*\overrightarrow{a}=q*\overrightarrow{E}+q*\overrightarrow{v}\wedge \overrightarrow{B}
$$

But in the case of two coupled coils the time varying current at primary coil (and its magnetic field variation) creates corresponding varying current in the secondary coil

To calculate it I use the magnetic flux conservation like in transforrmers where the plasma is the secondary coil but it does not work well to calculate the movement of each particle

Then, what formula is better to use to calculate the particle movement?

Accordingly Lorentz applied to a loop (where the ion describes a circled current):
$$
Fem=\oint \overrightarrow{E}\overrightarrow{dl}=-\frac{d\overrightarrow{\phi }}{dt}\\\\
2\pi r*\overrightarrow{E}=-\pi r^2*\frac{d\overrightarrow{B}}{dt}\\\\
\overrightarrow{E}=-0.5*r*\frac{d\overrightarrow{B}}{dt}
$$
So:
$$
m*\overrightarrow{a}=q*\overrightarrow{E}+q*\overrightarrow{v}\wedge \overrightarrow{B} - \frac{1}{2}*q*r* \frac{d\overrightarrow{B}}{dt}
$$

Where r is the Cyclotron radius. That is only true for slow varying magnetc fields because the ion does not describes a circle but an helix

Is it correct?
 
Last edited:
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Fun question, but unfortunately, for other reasons this user will not be returning to the PF. Thread is closed.
 

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