Abstract

AbstractGravity wave propagation from the troposphere into the thermosphere has often been modeled by assuming a complex vertical wave number m, with the imaginary part accounting for viscous and thermal dissipation. An alternative is to assume a complex wave frequency ω, which leads to a simpler form of the dispersion relation and different wave solutions described by complex‐ω ray theory. Here the solutions of complex ω and complex m are analyzed in terms of the compatibility conditions ∇×k=0 and kt=−∇ω, where k is the wave number vector. Estimates derived here suggest that the complex‐ω ray solutions can violate compatibility conditions above altitudes of weak viscosity. A possible consequence of this violation is an overestimation of the viscous damping of thermospheric gravity waves. The present results are based on a numerical solution of the viscous gravity‐wave dispersion relation in the anelastic approximation with a Prandtl number of unity and using conventional specifications of the dynamic viscosity of the thermosphere. Theoretical solutions for complex m are also derived in the weak and strong viscosity limits.

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