  We discuss the calculation of the strange magnetic radius of the proton in
chiral perturbation theory. In particular we investigate the low energy
component of the loop integrals involving kaons. We separate the chiral
calculation into a low energy part and a high energy component through use of a
momentum space separation scale. This separation shows that most of the chiral
calculation comes from high energies where the effective field theory treatment
is not valid. The resulting low energy prediction is in better agreement with
dispersive treatments. Finally, we briefly discuss magnetic moments and show
how our techniques can help resolve an old puzzle in understanding the magnetic
moments of the proton and Sigma^+.
