A trace element may substitute into a mineral by more than one substitution mechanism, complicating the thermodynamic description of its partition coefficients. In order to understand this phenomenon better, the mineral/melt partition coefficients for all 14 rare earth elements (REE) plus Y and Sc were measured experimentally for coexisting forsterite and protoenstatite in the system CaO-MgO-SiO 2 ±Al 2 O 3 ±TiO 2 at 1406 °C and atmospheric pressure. For both phases, the results show these large trivalent cations (REE 3+) replace Mg 2+ on octahedral sites, but with charge-balanced achieved by two different mechanisms: 1) cation vacancies (2 REE 3+ + vacancy = 3 Mg 2+); and 2) substitution of Al for Here we report an experimental study of this problem, in which we investigate how the partitioning of REE between olivine and melt changes as a function of Al 2 O 3 in the melt, while holding temperature, pressure and a SiO 2 melt constant. The buffering of a SiO melt was achieved with coexisting protoenstatite, Mg 2 Si 2 O 6 ; serendipitously, this mineral shows the same two substitution mechanisms for REE as forsterite (i.e., the components REE 4/3 □ 2/3 Si 2 O 6 and REEMgSiAlO 6), allowing the same phenomenon to be compared side-by-side in different minerals. The partition coefficients of all 14 REEs plus Y and Sc were determined, to see whether the two mechanisms affect the REE differently, with implications for the use of lattice strain theory in modelling trace element partitioning. We also included a melt composition rich in TiO 2 in order to change melt composition independently of olivine composition and alumina activity. Our aim is to obtain quantitative information on an example of the phenomenon of multiple substitution mechanisms in trace-element partitioning, which will be of heuristic value in refining the way mineral/melt trace-element partition coefficients in general are parameterized. The