The orbital magnetic dipole moment of a proton is a complex topic due to the proton's structure as a bound state of quarks and gluons. It differs from intrinsic magnetic moments and is influenced by the contributions of both the valence quarks and a "sea" of virtual particles. The parton model provides a framework for understanding these dynamics, but the current understanding involves abstract parton distribution functions. The total spin of the proton, which is 1/2, arises from the combined orbital and spin angular momentum of its constituents. The challenge lies in the theoretical separation of these contributions within relativistic quantum field theory.