Anthes et al. (1971) and Anthes (1972) presented some of the earliest attempts at three-dimensional numerical modeling of a tropical cyclone (TC). Despite using horizontal grid spacings of 30 km and only three model levels, the simulations did produce some of the desired features, such as low-level flow spiraling toward the center that abruptly rose to the tropopause, and then diverged outward into asymmetric patterns. Long spiral bands of enhanced precipitation were also evident, about 90 km wide, and propagating outward at 24 knots (12 m s −1 ). Anthes (1972) explained that these were probably inertia-gravity waves and perhaps not correct representations of spiral rainbands in real TCs. Kurihara and Tuleya (1974) presented a three-dimensional simulation with 20 km grid spacing and 11 vertical levels. They also noted robust spiral bands of vertical motion, in their case propagating outward at 27 m s −1 , with temperature and vertical motion out of phase, thus consistent with gravity waves.After those early attempts, the vertical and horizontal grid spacings of TC models steadily decreased while the realisms of their simulated TCs steadily increased (Braun et al., 2006;Liu et al., 1997;Rogers et al., 2003). The TC eye and eyewall became well-resolved while the spiral bands of precipitation became narrower and moved more slowly to the point where it can be difficult to differentiate their motion with that of the tangential circulation (Moon & Nolan, 2015a, 2015b. At the same time, vertical motions associated with gravity waves have become steadily less prominent in numerical simulations and have received accordingly less interest. An exception is the study by Chow et al. (2002), who analyzed outward propagating spirals in a Mesoscale Model 5 (MM5)