We propose a mechanism for baryogenesis in which the baryon asymmetry is generated as an \emph{equilibrium response} of weak sphalerons in a region where electroweak sphaleron transitions remain unsuppressed, $h/T\lesssim 1$. A nonzero equilibrium baryon density arises in the presence of an approximately conserved global charge $X$, carried by states with nonzero hypercharge and, after electroweak symmetry breaking, electric charge. Plasma screening enforces gauge-charge neutrality, so an $X$ asymmetry induces compensating gauge-charge densities in the Standard Model plasma, which in turn bias weak sphaleron transitions toward a state with nonvanishing baryon number. The required $X$ asymmetry is generated during a phase transition that changes the strength of electroweak symmetry breaking, but need not coincide with the final electroweak phase transition. In particular, the mechanism can operate during an inverse electroweak phase transition, where baryon number is produced behind the advancing wall, in contrast to conventional electroweak baryogenesis. Because baryon production is decoupled from a direct first-order electroweak phase transition, the scenario can be realized at parametrically higher temperatures than standard electroweak baryogenesis, thereby weakening current experimental constraints. This framework provides a qualitatively distinct route to electroweak baryogenesis, with different parametric dependence, phase-transition dynamics, and phenomenological signatures.