The spinel series Ge
x
Cu
1–x
Fe
2O
4 (
x=0.0 to 0.9) has been studied in detail by means of Mössbauer spectroscopy, X-ray diffraction and magnetization measurements at room temperature (298 K). Analysis of X-ray diffraction intensity data and Mössbauer intensity data suggest that this system remains in single phase up to
x=0.4 then it phase separates into two different phases for
x=0.5 to 0.9. Lattice constants of this system deviate from Vegard's law. Mössbauer spectra for x=0.0 to 0.4 suggest the existence of two hyperfine fields, one due to the Fe
3+ tetrahedral ions (A-sites) and the other due to the Fe
3+ octrahedral ions (B-sites), while for
x=0.5 to 0.9 it gives Mössbauer patterns corresponding to two separate phases. The systematic composition dependence of quadrupole interactions and nuclear hyperfine fields of
57Fe
3+ ions also support the concept of phase separation for
x=0.5 to 0.9. The observed variation of
57Fe
3+ hyperfine field on A- and B-sites with
x for
x=0.0 to 0.4 can be explained qualitatively on the basis of supertransferred hyperfine interactions.