Moving along a current carrying conductor

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    Conductor Current
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SUMMARY

This discussion focuses on the effects of moving along a current-carrying conductor, particularly when the observer's speed approaches the drift velocity of electrons or the speed of light. It highlights that at drift velocity, electrons appear stationary while ions move in the opposite direction, maintaining the current. When moving near light speed, both electrons and ions appear to move backward, necessitating the use of Lorentz transformations to analyze the four-current, defined as ##J^\alpha = (c \rho, j)##. The discussion concludes that while the current density increases in the observer's frame, the total current remains constant due to length contraction.

PREREQUISITES
  • Understanding of Lorentz transformations in special relativity
  • Familiarity with four-current notation in electromagnetism
  • Knowledge of electric and magnetic field interactions
  • Basic concepts of charge density and current density
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  • Study Lorentz transformations in detail to understand their application in electromagnetism
  • Explore the concept of four-current and its implications in different reference frames
  • Investigate the relationship between electric fields and magnetic fields through Lorentz transformations
  • Examine the effects of relativistic speeds on charge and current densities in conductors
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Physicists, electrical engineers, and students studying electromagnetism and special relativity, particularly those interested in the behavior of current-carrying conductors at relativistic speeds.

quawa99
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What will happen if I move in the direction of drift of the electrons in a current carrying conductor?
What would happen if my speeds are equal to the drift velocity and in a second case close to the speed of light
 
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Lets say the electrons are moving at v in the conductor frame and the ions are not moving. If you move at v, then the electrons are not moving in your frame, but the ions are moving at -v, so the current is the same.

If you move near the speed of light, then both electrons and ions are moving backwards in your frame of reference at close to the speed of light. It is necessary to transform the 4-current, which is
##J^\alpha = (c \rho, j)##

What is the four-current in the frame moving at v/2?
Assume total charge in this frame is 0.
The current is -nv/2 - nv/2
so the four-current is
##J_1 = (0, -nv)##

Let u = your velocity relative to the frame moving at v/2.
Using Lorentz transformation,
##J_2 = (\gamma uvn/c, \gamma nv)##

The current density is much greater in your frame, by a factor of ##\gamma##, and there is a charge density as well. But the length of the conductor will also be contracted by a factor of ##\gamma##, so the total current is the same. In this frame, there will be an electric field as well as a magnetic field.

You can look at it two ways. The electric field arises from a Lorentz transformation of the magnetic field in the original frame. Or the electric field arises from the charge which results from a Lorentz transformation of the current in the original frame. Same thing.
 
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Put it simpler:

Since the drift velocity is typically much smaller than lightspeed in the frame of the wire, you wouldn't see big effects from the difference between the speeds (moving charges and wire) in your frame.

The usual way to treat these problems is to model the wire as two lines of charges... decide on a frame of reference and the charge densities in that frame.

Very important - if "you" are the observer, do not talk about "you" moving.
Everything else is moving. "You" are always stationary.

Reword the question with these things in mind and you should find it easier to cope with.
 
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