Constant current in a wire

This is a problem of disequilibium in the boson, fermion distribution.  The charge gradient i equal across the wire, constant current. The disequilibrium has to be split perpindicular to the wire axis.  But at the wire surface, the Boson./spin distribution has to match the nomal environment.

The Markov system splits the count in various even spots on the Markov tree. It does this by shiftin the disequilibrium with the magnetic field. Hence the magnetice disequilbirium will extant out from the wire and be perpindicular to the line of axis.  This is essentially the same disequilibrium partition as is done in spin disequilibrium. The were breaks into a distinc set of energy bands and in the error tree the most probable result at the each partition tends to be magnetic / spin interaction, setting the dipole moments.

Electro megnetic effects are mostly about magnetic spin interactions in a medium where the density of fermions is fixed and the density of bosons at diseuqilibrium. If we change the current pediodically,m the magnetic field cannot keep up do to the fixed number of steps in light. Photons will be issued at the surface as the environment and wire cannot balance equal distributions. Since Plank is constant the number of partitions needed is a fixed quantity, each partition balancing N density to a Plank uncertainty. Hence energy levels.

Thermo dynamics about gas, a phase of matter in which fermion disequilibrium is always spread in all directions. In both cases it is about returning N density to normalcy, as close to possible via partition where each partition handles some portion of the disequilbrium.