It has been recognized for many years that gravity waves (GWs) play fundamental roles in a wide range of atmospheric processes from the surface to very high altitudes (Fritts & Alexander, 2003). Understanding these processes and their influences requires more complete quantification of the mechanisms by which GWs are generated, together with their characteristics, distributions, and responses in a wide range of environments. Of the recognized GW sources, secondary GWs (GWs) are important because they extend the vertical range of GW influences into the thermosphere and can do so quickly because of their often-large scales and vertical group velocities. Importantly, however, their generation mechanisms are the least rigorously studied and understood to date. This is because their sources are challenging to quantify observationally, and their associated dynamics are intrinsically nonlinear.Our focus in this paper is on GWs excited by Kelvin-Helmholtz instabilities (KHI), which have been less studied to date. Theory and modeling have suggested that GWs are excited by two types of instabilities. First, GW "self-acceleration" (SA) instability dynamics due to localized and transient GW/mean-flow interactions excite GWs having spatial scales dictated by the geometry and timescale of the local induced body forcing (Dong et al., 2020(Dong et al., , 2021(Dong et al., , 2022Fritts et al., 2020). Importantly, this mechanism can lead to GW generation prior to, and perhaps in the absence of, primary GW instabilities. Second, where KHI arise in an unstable shear due in part to inertia gravity waves (IGWs), they can radiate smaller-scale and higher-frequency GWs. As examples, previous studies have suggested that GWs can be emitted from small-scale KHI, localized KHI "packets," and turbulent wakes (e.g.,