The induced birefringence in the Voigt effect is directly proportional to the square of this quantity, while the second London equation allows one to solve a second-order differential equation in this quantity for the penetration depth.
The induced birefringence in the Voigt effect is directly proportional to the square of this quantity, while the second London equation allows one to solve a second-order differential equation in this quantity for the penetration depth. The same equation describes the complete exclusion of one of these from a superconductor, which is called the Meissner effect. A strong one can split atomic energy levels in the Paschen-Back effect, while a weaker one does the same in the Zeeman effect.  FTP, name this quantity, derived from the Lorentz transformation of the electric field, whose strength for a current-carrying wire can be computed via the Biot-Savart Law or Ampere's Law. .
The induced birefringence in the Voigt effect is directly proportional to the square of this quantity, while the second London equation allows one to solve a second-order differential equation in this quantity for the penetration depth.
{Magnetic Field}