Sketching equipotentials for a moving charge

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SUMMARY

The discussion focuses on sketching equipotentials for a moving point charge, initially stationary at the origin and later displaced to position R at time t = R/c. At this time, equipotential lines are circular and centered around R/2, while outside R, they reflect the original position at the origin. At t = 4R/c, the charge is at 2R, and the equipotential circles extend to a maximum radius of 4R, with additional circles centered at the origin. The challenge lies in the transition region where magnetic fields complicate the potential concept.

PREREQUISITES
  • Understanding of electrostatics and electric potential
  • Familiarity with the concept of retarded time in electromagnetism
  • Knowledge of the behavior of point charges in motion
  • Basic grasp of magnetic fields and their relation to moving charges
NEXT STEPS
  • Study the concept of retarded time in electromagnetic theory
  • Learn about the mathematical formulation of equipotential surfaces
  • Explore the effects of moving charges on electric and magnetic fields
  • Investigate the implications of special relativity on electric potentials
USEFUL FOR

Students of electromagnetism, physics educators, and anyone interested in advanced concepts of electric potential and field theory related to moving charges.

CAF123
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Homework Statement


A point charge remains stationary at the origin for a long time but then, at time t = 0, is displaced, at uniform speed c/2, to a new position R, where it stops.

Sketch with care the equipotentials of ##\phi## at a time t = R/c, and then again at time t = 4R/c. Your sketches should including distances both large and small compared to R.

Homework Equations


[/B]
retarded time ##t_R = t - |r-r'|/c##

The Attempt at a Solution


[/B]
What is t? the position of the charge or the retarded position as measured by some observer? Assuming the former, when ##t=R/c,## the charge is at position R/2. So ct=R and so we have circles centered around the point R/2. Outside R, the equipotentials are those from when the charge was at origin. So should draw circles centered at R/2 and with radii between 0 and R?

Similar analysis for t=4R/c, the charge is at 2R and ct=4R so have circles centered at 2R until max radius 4R. Beyond that, have circles centered at origin. Is it right?
 
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Such a fast motion will introduce magnetic fields, and make the concept of a potential alone problematic, but I guess we have to ignore this problem here.

tR determines your fields, t is the current time. That will give different circles.
CAF123 said:
Outside R, the equipotentials are those from when the charge was at origin.
Right.
CAF123 said:
Similar analysis for t=4R/c, the charge is at 2R and ct=4R so have circles centered at 2R until max radius 4R. Beyond that, have circles centered at origin. Is it right?
The transition region is more complicated.
 

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