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Gauss's Law in Physics

Coulomb's law tells you the field of a single charge, and adding up thousands of those contributions is possible but rarely pleasant. Gauss's law replaces the adding with a piece of geometry. Wrap any closed surface around a charge and the field lines poking out through it always carry the same total, no matter what shape you chose, because field lines can only begin and end on charge. That makes the law a shortcut for anything with enough symmetry, a sphere, a long cylinder or a broad sheet, and it gives the whole story of conductors in a couple of lines, which is why it also explains why the field inside a conductor is always nothing.

Electric flux through a flat surface

Given

  • (N/C)
  • (m²)
  • (rad)
Electric flux through a closed surface

Given

  • (N/C)
  • (m²)
Gauss's law

Given

  • (C)
  • (C²/(N m²))

Constant used

Gauss's law when the enclosing surface holds no charge

Given

  • (C)
Field outside a uniformly charged insulating sphere

Given

  • (C)
  • (m)

Constant used

Field inside a uniformly charged insulating sphere

Given

  • (C)
  • (m)
  • (m)

Constant used

Field inside a conductor in electrostatic equilibrium

Given

  • (N/C)
Field just outside the surface of a charged conductor

Given

  • (C/m²)
  • (C²/(N m²))

Constant used

Field of an infinite line of charge

Given

  • (C/m)
  • (m)

Constant used

Field of an infinite sheet of charge

Given

  • (C/m²)
  • (C²/(N m²))

Constant used

Field between two oppositely charged parallel sheets

Given

  • (C/m²)
  • (C²/(N m²))

Constant used