Under the combined forces of pressure and gravity, the two modes remain distinct. Figure 2.1 shows the dispersion relation for waves propagating in the vertical direction (i.e., along the z axis). Acoustic waves propagate for ω > ωac, with group and phase velocity greater and less than the sound speed respectively, and approaching zero and infinity at ωac respectively. At high frequencies, the waves are purely acoustic. Gravity waves are propagating for ω < ωac, with phase and group velocity less than the sound speed. For large kx, the waves are purely gravitational. The acoustic cut-off is larger than the Brunt-Väisälä frequency by a factor,
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