“…For the first class, the directly forced zonal jets can be shear‐driven by differentially moving boundaries (e.g., Aguiar et al., 2010; Hide & Titman, 1967) or result from the conservation of angular momentum and an imposed radial flow between sources and sinks at different radii (e.g., Hide, 1968; Solomon et al., 1993; Sommeria et al., 1989; Tian et al., 2001; Weeks et al., 1997). Indirectly forced jets are the product of flow dynamics; for example, active forcing can generate and maintain an eddy field characterized by relatively small length scales, which becomes anisotropic due to the β ‐effect and cascades energy into larger‐scale zonal flows, and ultimately, an eddy‐driven zonal jet (e.g., Afanasyev & Wells, 2005; Cabanes et al., 2017; Lemasquerier et al., 2021; Matulka et al., 2016; Zhang & Afanasyev, 2016). Indirectly forced jets can also arise from the turbulence associated with small‐scale convection (e.g., Condie & Rhines, 1994; Matulka et al., 2016; Read et al., 2007; Zhang & Afanasyev, 2014), electromagnetic forcing with a conductive working fluid (e.g., Afanasyev & Wells, 2005; Afanasyev, 2019; Espa et al., 2008, 2019), or the radiation of Rossby waves by eddies via beta‐plume mechanisms (e.g., Afanasyev et al., 2011; Afanasyev & Ivanov, 2019; Zhang & Afanasyev, 2015).…”