“…The simplest dynamical model of the omnivehicle is based on the no-slip constraints of wheels: the omniwheel is modeled as a rigid disk which does not slip in the direction of the contact roller axis (so the dynamics of the rollers is neglected). Different methods are used to derive equations that govern the dynamics of the vehicle (for example, analysis of the reaction force [11,17], Lagrange's multipliers method [6,12,14], Chaplygin's equations [18], Ferrers' equations [19], the Appel -Gibbs method [15,20,21], and Tatarinov's laconic equations [22,23]). All of them give three ordinary differential equations that determine the change of the center of mass velocity and angular velocity due to controls.…”