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Sources and Laws of Magnetism in Physics

Magnetism has no monopoles, so a magnetic field can never begin or end anywhere. Every field line has to close on itself, which is why the list of sources on this page is nothing but moving charge. Take any current, break it into small pieces, and the Biot-Savart law tells you the field each piece contributes. For the shapes worth remembering, a straight wire, a loop, a solenoid or a toroid, Ampere's law gets the same answer in a single line by choosing a loop that follows the symmetry. The blocks end with what happens once a material is placed in the field, where the material's own tiny currents either help the field along or push back against it.

Biot-Savart law for a small element of current

Given

  • (A)
  • (m)
  • (m)
  • (rad)

Constant used

Magnetic field of a long straight current-carrying wire

Given

  • (A)
  • (m)

Constant used

Magnetic field at the centre of a circular loop

Given

  • (A)
  • (m)

Constant used

Force per unit length between two parallel current-carrying wires

Given

  • (A)
  • (m)

Constant used

Ampere's law around a closed loop

Given

  • (T)
  • (m)
  • (A)

Constant used

Magnetic field inside a long solenoid

Given

  • (1/m)
  • (A)

Constant used

Magnetic field inside a toroid

Given

  • (A)
  • (m)

Constant used

Gauss's law for magnetism

Given

  • (T)
  • (m²)
Magnetic field inside a material

Given

  • (A/m)

Constant used

Magnetization written into the field relation

Given

  • (A/m)
  • (A/m)

Constant used