We present a magnetic-field-and pressure-dependent Raman scattering study of the complex orbital, magnetic, and conducting phases of Ca 3 Ru 2 O 7 , which result from a rich interplay between the orbital, spin, and electronic degrees of freedom. The Raman-active phonon and magnon excitations in Ca 3 Ru 2 O 7 convey sufficient information to map out the orbital, magnetic, and conducting ͑H , T͒ and ͑P , T͒ phase diagrams of this material. We find that quasihydrostatic pressure causes a linear suppression of the orbital-ordering temperature ͑T OO =48 K at P =0͒, up to a T = 0 critical point near P * ϳ 55 kbar, above which the material is in a metallic, orbital-degenerate phase. We associate this pressure-induced collapse of the antiferromagnetic orbital-ordered phase with a suppression of the RuO 6 octahedral distortions that are responsible for orbital-ordering. We also find that an applied magnetic field at low temperatures induces a change from an orbital-ordered to orbitaldegenerate phase for fields aligned along the in-plane b-axis ͑H ʈ hard axis͒, but induces a reentrant orbitalordered to orbital-disordered to orbital-ordered phase change for fields aligned along the in-plane a-axis ͑H ʈ easy axis͒. This complex magnetic field dependence betrays the importance of spin-orbit coupling in this system, which makes the field-induced phase behavior highly sensitive to both the applied magnetic-field magnitude and direction. It is further shown that rapid field-induced changes in the structure and orbital populations are responsible for the highly field-tunable conducting properties of Ca 3 Ru 2 O 7 , and that the most dramatic magnetoconductivities are associated with an "orbital disordered" phase regime in which there is a random mixture of a-and b-axis oriented Ru moments and d-orbital populations on the Ru ions.