The coupled nonequilibrium dynamics of electrons and phonons in monolayer MoS 2 is investigated by combining first-principles calculations of the electron-phonon and phononphonon interaction with the time-dependent Boltzmann equation. Strict phase-space constraints in the electron-phonon scattering are found to influence profoundly the decay path of excited electrons and holes, restricting the emission of phonons to crystal momenta close to few high-symmetry points in the Brillouin zone. As a result of momentum selectivity in the phonon emission, the nonequilibrium lattice dynamics is characterized by the emergence of a highlyanisotropic population of phonons in reciprocal space, which persists for up to 10 ps until thermal equilibrium is restored by phonon-phonon scattering. Achieving control of the nonequilibrium dynamics of the lattice may provide unexplored opportunities to selectively enhance the phonon population of two-dimensional crystals and, thereby, transiently tailor electron-phonon interactions over sub-picosecond time scales.Transition-metal dichalcogenides (TMDs) exhibit strong light-matter coupling, 1 a rich photo-physics, 2 and a unique interplay of spin, 3,4 valley, 5,6 lattice, 7 and electronic 8 degrees of freedom. These characteristics, alongside with numerous possibilities to tailor screening, 9 charge-carrier density, 7 and dimensionality, 10,11 make them promising candidates for the exploration of new pathways to achieve