We study a layer of grains atop a plate which oscillates sinusoidally in the direction of gravity, using three-dimensional, time-dependent numerical solutions of continuum equations to Navier-Stokes order as well as hard-sphere molecular dynamics simulations. For high accelerational amplitudes of the plate, the layer exhibits a steady-state "density inversion" in which a high-density portion of the layer is supported by a lower-density portion. At low accelerational amplitudes, the layer exhibits oscillatory time dependence that is strongly correlated to the motion of the plate. We show that continuum simulations yield results consistent with molecular dynamics results in both regimes. 05.65.+b,47.57.Gc Although experimental [1,2] and computational [3][4][5][6][7] evidence demonstrate the potential for hydrodynamic models to describe important aspects of granular flow, a general set of governing equations for granular media is not yet recognized [8,9]. Several proposed rapid granular flow models use binary, inelastic hard-sphere collision operators in kinetic theory to derive equations of motion for the continuum fields: number density n, velocity u, and granular temperature T [10-12]. As Eshuis, et al [9] stated in 2010, "The holy grail question in research on granular dynamics is [13,14], To what extent can granular flow be described by a continuum approach?" Density inversion, in which a low-density region near the bottom of a granular layer supports a higher-density region above it, has proven to be significant for the study of granular hydrodynamics. This phenomenon has been identified in vertically shaken layers [7,9,[15][16][17] as well as in layers flowing parallel to a surface, such as in gravity-driven flow down an incline [18,19].In their seminal investigation [7], Lan and Rosato studied density inversion in vertically vibrated granular media. A layer of grains with depth H and uniform diameter σ atop a plate that oscillates sinusoidally with frequency f and amplitude A will leave the plate at some time in the oscillation cycle if the maximum acceleration of the plate a max = A (2πf ) 2 exceeds the acceleration of gravity g. The oscillating plate can be characterized by the dimensionless parameters Γ = a max /g and f * = f H/g. Lan and Rosato studied density inversion in such a system by conducting soft-sphere discrete element method (DEM) simulations and comparing these results to kinetic theory predictions of Richman and Martin [20].These continuum predictions did not account for the time dependence of the layer or the plate, but rather treated the oscillating plate as a source of thermal energy and assumed one-dimensional (1-D) steady-state density and temperature distributions as functions of height in the cell. To characterize the rate of kinetic energy input through shaking, they used the dimensionless RMS speed of the bottom plate V b = (2πf A) / √ 2σg as their control parameter. It has since become common to instead use the dimensionless shaking strength [15]In Fig. 5 of their manuscript, L...