Electrostatics of Conductors

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Electrostatics of Conductors

Electrostatics of Conductors

Conductors contain mobile charge carriers. In metallic conductors, these charge carriers are electrons. In a metal, the outer (valence) electrons part away from their atoms and are free to move. These electrons are free of the metal but not free to leave the metal.

In an external electric field, they drift against the direction of the field. The positive ions made up of the nuclei and the bound electrons remain held in their fixed positions. In electrolytic conductors, the charge carriers are both positive and negative ions.

Important results regarding electrostatics of conductors.

  • Inside a conductor, the electrostatic field is zero: In the static situation, the free charges have so distributed themselves that the electric field is zero everywhere inside. The electrostatic field is zero inside a conductor.
  • At the surface of a charged conductor, the electrostatic field must be normal to the surface at every point: In the static situation, therefore, E should have no tangential component. Thus electrostatic field at the surface of a charged conductor must be normal to the surface at every point.
  • The interior of a conductor can have no excess charge in the static situation: There is no net charge at any point inside the conductor, and any excess charge must reside on the surface.
  • The electrostatic potential is constant throughout the volume of the conductor and has the same value (as inside) on its surface: Since E = 0 inside the conductor and has no tangential component on the surface, no work is done in moving a small test charge within the conductor and on its surface. That is, there is no potential difference between any two points inside or on the surface of the conductor.
  • The electric field at the surface of a charged conductor:

where σ is the surface charge density and nˆ is a unit vector normal to the surface in the outward direction.

  • Electrostatic shielding: The proofs of the results noted in Fig are omitted here, but we note their important implication. Whatever be the charge and field configuration outside, any cavity in a conductor remains shielded from outside electric influence: the field inside the cavity is always zero. This is known as electrostatic shielding.

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