At rest, the magnetopause lies along the locus of points where the sum of the thermal and magnetic pressures in the magnetosheath balance the sum of those same quantities in the magnetosphere. Magnetic pressures generally dominate the total pressure on the magnetospheric side. Pressure imbalances cause the magnetopause to move. When the solar wind dynamic pressure increases, the sum of the thermal and magnetic pressures in the magnetosheath increases proportionally and the dayside magnetopause moves Earthward to a location where an equivalent magnetospheric pressure can be found, that is, a place where dipole magnetic field strengths are greater (Martyn, 1951). When the solar wind dynamic pressure decreases, the dayside magnetopause moves outward to a place where dipolar magnetic field strengths are lower. When solar wind dynamic pressures remain constant but magnetospheric magnetic pressures increase, perhaps in response to enhanced ring current strengths during the main phase of a geomagnetic storm, the dayside magnetopause moves outward at much as 7% to a location some ∼0.7 R E outside its normal position where dipolar magnetic field strengths are weaker and pressure balance can be reestablished (Schield, 1969). When dayside magnetospheric magnetic pressures decrease in response to enhanced Region 1 Birkeland current strengths driven by reconnection and magnetic flux removal from the dayside magnetosphere (Hill & Rassbach, 1975;Maltsev & Lyatsky, 1975), the dayside magnetopause moves inward to a location where the dipole magnetic field strength suffices to restore pressure balance. Magnetotail magnetic field strengths increase during the growth phase of substorms, but decrease abruptly at substorm onset. The corresponding variation in the cross-tail current first weakens but later enhances dayside magnetospheric magnetic field strengths, consistent with inward dayside magnetopause motion during the growth phase but outward motion following substorm onset.There is a specific time scale for magnetopause motion associated with each of the drivers above. The pressure variations associated with solar wind discontinuities transmitted into the magnetosheath propagate antisunward at velocities comparable to those of the solar wind, and consequently require only several minutes to transit the entire dayside magnetosphere. Consistent with this expectation, the rise (or fall) times for the corresponding step function changes in dayside magnetopause location, magnetospheric magnetic field strength, and global current perturbations range from ∼2 to 4 min (Patel & Cahill, 1974). The durations of ring current enhancements are much longer, for the weakest geomagnetic storms on the order of 6 hr, for moderate storms on the order of 30 hr, and for the most intense storms from 12 to 93 hr (Vennerstrøm et al., 2016), These storms can be divided into growth, main, and recovery phases, each lasting from several to many hours, indicating only gradual inflations of the dayside magnetosphere followed by very gradual deflations. Steady...