Hydraulic jumps and other related phenomena have been studied for many decades (Long, 1953; Lyra, 1943; Rayleigh, 1883), and readers are referred to the survey of Chanson (2009) for details on the progress of experiments conducted in controlled channels mainly. Although results from theoretical studies and controlled experiments have provided us with the basis for understanding the jump mechanisms in the atmosphere, studies, and particularly, observations of atmospheric hydraulic jumps are not as common. Clarke (1972) was perhaps the first one who attempted to combine large-scale observations with simulations to explain an atmospheric phenomenon, the "morning glory," which is a frequent squall that occurs near dawn on the southern coast of the Gulf of Carpentaria, Australia, quite recognizable due to its narrow cloud bands. He concluded that the morning glory is a propagating undular hydraulic jump formed in a katabatic flow. He also suggested some of the conditions that favor the occurrence of such phenomena, among others, shallow inversions, steep slopes, and topographic funneling. However, observational studies of atmospheric jumps can be tracked further back (Manley, 1939; Holmboe & Klieforth, 1957). More recently, the studies of Mobbs et al. (2005) and Gohm et al. (2008) showed the close connection between mountain waves, downslope winds, and jump events. Other recent observational and numerical studies have further detailed the conditions at which atmospheric hydraulic jumps occur (Juliano et al., 2017; Rotunno & Bryan, 2018), To understand how an atmospheric hydraulic jump develops, we can start by assuming, very simplistically, that the flow can be represented by a two-layer model, the lowest layer being the atmospheric boundary layer (ABL) and the upper layer the free atmosphere (Samuelson, 1992). In complex terrain, for example, mountainous regions, the depth of the ABL, h, can be of the order of the terrain elevation and the nature of the flow depends upon the Froude number (Fr),