The question is even actually slightly more interesting then that. There is what is called a duality transformation for Maxwells equations which can transform E and B into E' and B', and electric charge and current into a mixture of electric charge, current, and also magnetic charges and currents. That is, for example, an electron would be partially an electric monopole and partially a magnetic monopole in the new fields instead of pure electric monopole. It would also then be partially magnetic dipole and electric dipole instead of pure magnetic dipole. So what is important is if the *ratio* of magnetic charge/current to electric charge/current is the same everywhere. If so, then one can conveniently transform away one or the other. Historically, the fields are chosen such that magnetic charge/current = zero.
Duality transformation from Jackson p. 274
[tex]\vec{E} = \vec{E}'cos(\theta) + Z_0\vec{H}'sin(\theta)[/tex]
[tex]Z_0\vec{H} = -\vec{E}'sin(\theta) + Z_0\vec{H}'cos(\theta)[/tex]
[tex]Z_0\vec{D} = Z_0\vec{D}'cos(\theta) + \vec{B}'sin(\theta)[/tex]
[tex]\vec{B} = -Z_0\vec{D}'sin(\theta) + \vec{B}'cos(\theta)[/tex]
[tex]Z_0\rho_e = Z_0\rho_e'cos(\theta) + \rho_m'sin(\theta)[/tex]
[tex]\rho_m = -Z_0\rho_e'sin(\theta) + \rho_m'cos(\theta)[/tex]
[tex]Z_0\vec{J_e} = Z_0\vec{J_e}'cos(\theta) + \vec{J_m}'sin(\theta)[/tex]
[tex]\vec{J_m} = -Z_0\vec{J_e}'sin(\theta) + \vec{J_m}'cos(\theta)[/tex]
[tex]Z_0 = \sqrt{\mu_0/\epsilon_0}[/tex]
Subscripts e or m indicate electric and magnetic sources respectively.
It can be fun to play around with these to come up with different configurations.