Abstract.We study low-speed flows of a highly compressible, single-phase fluid in the presence of gravity, for example, in a regime appropriate for modeling recent spaceshuttle experiments on fluids near the liquid-vapor critical point. In the equations of motion, we include forces due to capillary stresses that arise from a contribution made by strong density gradients to the free energy. We derive formally simplified sets of equations in a low-speed limit analogous to the zero Mach number limit in combustion theory.When viscosity is neglected and gravity is weak, the simplified system includes: a hyperbolic equation for velocity, a parabolic equation for temperature, an elliptic equation related to volume expansion, an integro-differential equation for mean pressure, and an algebraic equation (the equation of state). Solutions are determined by initial values for the mean pressure, the temperature field, and the divergence-free part of the velocity field. To model multi-dimensional flows with strong gravity, we offer an alternative to the anelastic approximation, one which admits stratified fluids in thermodynamic equilibrium, as well as gravity waves but not acoustic waves.1. Introduction. Near the liquid-vapor critical point, many of the thermophysical properties of a fluid exhibit a singular behavior. For instance, the isothermal compressibility and the isobaric thermal expansion coefficients, as well as the isobaric specific heat, all diverge strongly at the critical point. Critical enhancement effects are also encountered in the behavior of the thermal conductivity and the viscosity in the vicinity of the critical point, while the thermal diffusivity approaches zero. These singularities play a major role in the thermal equilibration of near-critical fluids.Understanding the effect of singular fluid properties on dynamics is not always straightforward. For example, it has been shown that even though thermal diffusivity is small,