Dynamics of Lorentz force on a current carrying wire

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SUMMARY

The discussion centers on the dynamics of the Lorentz force acting on a current-carrying wire within a magnetic field. The primary equation referenced is F = ILB, where the force acts perpendicular to both the current and the magnetic field. Participants explore the implications of electric fields opposing current flow, particularly in relation to back electromotive force (back-EMF) and Lenz's law. The conversation also addresses the paradox of determining relative velocity in a uniform magnetic field and the necessity of transforming reference frames to understand the effects on the wire.

PREREQUISITES
  • Understanding of Lorentz force and its equation F = ILB
  • Knowledge of electric and magnetic field interactions
  • Familiarity with back electromotive force (back-EMF) and Lenz's law
  • Concept of reference frames in physics
NEXT STEPS
  • Research the implications of back-EMF in electric motors and generators
  • Study the transformation of electric and magnetic fields in different reference frames
  • Examine the effects of constant electric fields on charged particles
  • Explore the relationship between magnetic flux and velocity in electromagnetic systems
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Physicists, electrical engineers, and students studying electromagnetism who seek to deepen their understanding of the interactions between electric currents and magnetic fields.

bob012345
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Hello all,

I've been pondering a problem with a current carrying wire in a magnetic field. The Lorentz force is easy, ILB,
with a velocity 90 degrees to the B field. So let the force accelerate the wire. Assume only one segment of the wire that has current in one direction, say up, is in the field and the field is out of the page (screen!). The force is to the left. It now moves. For a fixed current, the force should be constant and thus the acceleration.

Now, let's look at it from a reference frame co-moving with the wire. At some instant we see an electric field pointing down, against the current flow according to how fields transform. The magnetic field is virtually the same for low velocity. It's clear that to maintain the acceleration we must maintain the current and to do that we must overcome the increasing electric field opposing the current flow.

First, is this correct? Second, does the electric field have to oppose the current? Does a current carrying wire immersed into an electric field have to be affected since conductors usually keep external fields out?

I'm bothered by the idea that if I found myself in a infinite uniform magentic field in space from an unknown source, why should I be able to compute my relative speed to it just by turning on a current in a wire? If the universe was filled with a uniform magnetic field, we could always know our velocity which seems wrong. I'm also bothered by the fact that I shouldn't have to transform into the moving frame to know what happens. I should be able to know all by staying in the original reference frame. Thanks.
 
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bob012345 said:
.
Isn't the opposing electric field the back-EMF experienced by all motors due to generator action?
The source of current must overcome this BEMF and must do work to provide KE for the moving wire.
Regarding the question about finding velocity in the Universe, I think you could find your velocity relative to the magnetic source.
 
tech99 said:
Isn't the opposing electric field the back-EMF experienced by all motors due to generator action?
The source of current must overcome this BEMF and must do work to provide KE for the moving wire.
Regarding the question about finding velocity in the Universe, I think you could find your velocity relative to the magnetic source.
Thanks. Back emf is usually attributed to Lenz's law which is dependent on changing magnetic flux. In my scenario, the flux is constant (or so I think it is). It should be possible to evaluate what will happen from the original frame. For instance, if the flux changed with the observed velocity that would be the case. Also, if an electric charge is accelerated by a constant electric field parallel to its motion, there appears that no such counter effects which will slow it down such as a relativistic transformation that provides a counter force. Interesting the magnetic case is not symmetric.
 
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