Dirac magnetic monopoles and quark fractional electric charge quantization When applying the Dirac quantization rule for electric and magnetic charge, I assume one is considering unit electric charges such as electrons.  How does the Dirac quantization rule apply for the fractional electric charges of quarks?
 A: The Dirac quantization rule comes from integrating the angular momentum of the superposed electromagnetic field of a charge and a monopole. This angular momentum turns out to be finite and independent of the distance $h$ between the charge and the monopole. The argument then goes that if it's possible to isolate a single fundamental charge $e$ and a single fundamental monopole $g$ in some region of space, then the total angular momentum in that region has to be a multiple of $\hbar$. Here "isolation" means that the distance to any other particle is $\gg h$.
But note that the isolation of the particles is critical. If you put a monopole near a hydrogen atom, the total angular momentum of the electromagnetic field vanishes, because the angular momentum density is of the form $\textbf{E}\times\textbf{B}$, which is bilinear in the fields.
Since quarks are confined, the argument can never be applied to a quark.
A: The logic is the same:  If $q$ is an electric charge and $g$ is a magnetic charge, one must have $gq \in 2\pi\mathbb{Z}$ (in lazy theorist units).  So if there is a largest magnetic charge, then there is necessarily a smallest electric charge.  You don't have to assume that you are dealing with unit charges to make this argument.  
