Alternatively, molecular-dynamics (MD) simulations have shown that relaxors can be interpreted as exhibiting a multidomain state without a nonpolar matrix (i.e., polar nanodomains or PNDs). [4] The exact nature of order in relaxors, however, remains an ongoing debate [5] and, in turn, new approaches to study these complex materials are required to further illuminate the structure and how it can be controlled and can impact material properties. [5-9] In any case, it is essential to understand the evolution of the polar structure in relaxors (be they PNRs or PNDs) under applied stimuli as these are key to understanding relaxor behavior and large electromechanical effects in relaxors. Over the years, X-ray and neutron diffuse-scattering measurements have emerged as an essential tool to study the structural signatures of relaxor behavior [10-19] and studies on single-crystal relaxors have investigated the evolution of polar regions/domains (e.g., size, morphology) and suggested that they alter their size [14-17] and orientation [18] under different external stimuli. For example, under applied electric fields, which were expected to enhance polar order, the local order was found to align perpendicular to the field [18] and induce an asymmetry in the lattice dynamics [19] that could ultimately be responsible for the large electromechanical effects. [20] Other studies used pressure to push the material in the opposite directionto destabilize polar order [17]-and even induce a crossover from Understanding and ultimately controlling the large electromechanical effects in relaxor ferroelectrics requires intimate knowledge of how the local-polar order evolves under applied stimuli. Here, the biaxial-strain-induced evolution of and correlations between polar structures and properties in epitaxial films of the prototypical relaxor ferroelectric 0.68PbMg 1/3 Nb 2/3 O 3-0.32PbTiO 3 are investigated. X-ray diffuse-scattering studies reveal an evolution from a butterfly-to disc-shaped pattern and an increase in the correlation-length from ≈8 to ≈25 nm with increasing compressive strain. Molecular-dynamics simulations reveal the origin of the changes in the diffuse-scattering patterns and that strain induces polarization rotation and the merging of the polar order. As the magnitude of the strain is increased, relaxor behavior is gradually suppressed but is not fully quenched. Analysis of the dynamic evolution of dipole alignment in the simulations reveals that, while, for most unit-cell chemistries and configurations, strain drives a tendency toward more ferroelectric-like order, there are certain unit cells that become more disordered under strain, resulting in stronger competition between ordered and disordered regions and enhanced overall susceptibilities. Ultimately, this implies that deterministic creation of specific local chemical configurations could be an effective way to enhance relaxor performance.