We determine where a given concentration of ferromagnetic (FM) bonds d
oped into a square lattice antiferromagnet must go to minimize the sys
tem's total magnetic energy. We find i) an infinite degeneracy of grou
nd-state arrangements of FM bonds that correspond to completely unfrus
trated configurations for classical spins, and ii) this degeneracy is
lifted when quantum fluctuations are included, and phase-separated gro
und states, such as periodic arrays of stripes of FM bonds, are found.
A discussion of the application of these ideas to doped cuprate high-
T-c superconductors with annealed disorder is presented.