In a uniform perpendicular magnetic field , force on charged particle cause change in direction of momentum. How do we explain it using conservation of momentum?
I don't know what is Hamilton or canonical or something like that.
In a uniform perpendicular magnetic field , force on charged particle cause change in direction of momentum. How do we explain it using conservation of momentum?
I don't know what is Hamilton or canonical or something like that.
Electromagnetic field itself can be ascribed momentum in such a way that momentum is locally conserved (i.e. momentum of a space region changes continuously and its rate of change can be expressed as a surface integral of certain field function).