“…An infinitesimally thin, spatially homogeneous, isothermal and non‐self‐gravitating fluid annulus in equilibrium is considered, whose evolution is described by the momentum and continuity equations. As we only consider the two‐dimensional coplanar orbits, the equations of motion are similar to the ones used in Goldreich & Tremaine (1982), Meyer‐Vernet & Sicardy (1987), Griv (2006, 2007) and Griv et al (2008). The linearized equations of motion read (written with respect to a rotating frame with angular velocity Ω Nep ) where v r , v ϕ and Σ 1 are, respectively, the perturbations of the radial velocity, azimuthal velocity and surface density of the proto‐KBO subsystem, Σ=Σ 0 +Σ 1 ( r , t ), Σ 0 is the equilibrium surface density, |Σ 1 /Σ 0 | ≪ 1, c s is the local speed of sound, ω * = m (Ω−Ω Nep ), Ω( r ) is the angular velocity at a distance r from the Sun and Ω Nep = ( M Sun G / r 3 ) 1/2 .…”