The potential at the center of the sphere

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SUMMARY

The electric field at the surface of a charged, solid copper sphere with a radius of 0.160m is measured at 3600 N/C, directed toward the center. The potential at the center of the sphere is equal to the potential at any point on the surface due to the uniform charge distribution. Using the formulas Q = R²E/k and V = kQ/R, the potential can be calculated, confirming that the electric field inside a conductor is zero while the potential remains constant throughout the conductor.

PREREQUISITES
  • Understanding of electric fields and potentials
  • Familiarity with the properties of conductors in electrostatics
  • Knowledge of the formulas for electric field (E) and potential (V)
  • Basic grasp of spherical symmetry in charge distribution
NEXT STEPS
  • Study the concept of electric fields in conductors and their implications
  • Learn about Gauss's Law and its application to spherical charge distributions
  • Explore the relationship between electric field and potential in electrostatics
  • Investigate the behavior of electric fields and potentials in different geometries
USEFUL FOR

Physics students, electrical engineers, and anyone interested in electrostatics and the behavior of electric fields in conductors.

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Homework Statement




the electric field at the surface of a charged, solid, copper sphere with radius 0.160m is 3600N/C , directed toward the center of the sphere.
what is the potential at the center of the sphere, if we take the potential to be zero infinitely far from the sphere?
answer in V
thanks



. The attempt at a solution
v=u/q
how to find the u and q thanks
 
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Think about what's the electric field inside the sphere (copper is a conductor!).
 
vanhees71 said:
Think about what's the electric field inside the sphere (copper is a conductor!).
Q=R^2E/k , v=kQ/R
use these two?
 
Pretty sure there was a theorem that said the electric field inside an isolated conductor is zero, but the potential has the same value at all points on the surface whether inside the surface or not. That is, the potential is the same at the center as it would be anywhere else on the conductor.

This is because the charge distributes itself uniformly on the surface of a spherical conductor.
 

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