Induction in electrostatic equilibrium conductor

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SUMMARY

The discussion centers on the properties of electrostatic equilibrium in conductors, specifically addressing whether the surface of a charged conductor remains equipotential when influenced by external objects. It is established that both the interior and surface of an electrostatically balanced conductor are equipotential. Furthermore, the electric field lines are confirmed to be perpendicular to the surface, ensuring that charge movement ceases when equilibrium is achieved.

PREREQUISITES
  • Understanding of electrostatics principles
  • Knowledge of electric field lines and their behavior
  • Familiarity with conductors and insulators in electrostatic contexts
  • Basic grasp of equipotential surfaces
NEXT STEPS
  • Study the behavior of electric field lines around charged conductors
  • Explore the concept of equipotential surfaces in different materials
  • Investigate the effects of external electric fields on conductors
  • Learn about Gauss's Law and its applications in electrostatics
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This discussion is beneficial for physics students, electrical engineers, and anyone interested in understanding the principles of electrostatics and the behavior of conductors in electric fields.

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Homework Statement
Consider a conductor in electrostatic equilibrium, approach if charged objects so that one region of that conductor has an excess of positive charges and another region with an excess of negative charges.
Relevant Equations
Equipotential regions
We know that both the interior and the surface of an electrostatically balanced conductor are equipotential. My question is if when we approach the loaded objects, the surface of the conductor will continue to be an equipotential. If not, then there could be a field line that left the region with an excess of positive charges going to the region with an excess of negative charges?
 
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Correct. The electric field lines are perpendicular to the surface. If they were not, charge would move until they are perpendicular.

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