A self balancing system analysis is presented which utilizes freely moving balancing bodies (balls) rotating in unison with a rotor to be balanced. Using Lagrange´s Equation, we derive the non-linear equations of motion for an autonomous system with respect to the polar coordinate system. From the equations of motion for the autonomous system, the equilibrium positions and the linear variational equations are obtained by the perturbation method. Because of resistance to motion, eccentricity of race over which the balancing bodies are moving and the influence of external vibrations, it is impossible to attain a complete balance. Based on the variational equations, the dynamic stability of the system in the neighborhood of the equilibrium positions is investigated. The results of the stability analysis provide the design requirements for the self balancing system. Keywords: Self balancing system, variational, Rayleigh disipation function.
RESUMENSe presenta el análisis de un sistema de autobalance el cual utiliza bolas libres de movimiento rotando con el rotor que será balanceado. Se usa la ecuación de Lagrange para derivar un sistema de ecuaciones no lineales para un sistema autónomo con respecto a un sistema de coordenadas polares. De las ecuaciones de movimiento, se obtienen ecuaciones linealizadas variacionalmente y posiciones de equilibrio por el método de perturbación. A causa de la resistencia al movimiento, la excentricidad y el movimiento de los cuerpos libres que son provocados por la influencia de vibraciones externas, hace imposible obtener un balanceo completo. Basado en el método variacional, se investiga el comportamiento dinámico del sistema en la frontera de la posición de equilibrio. Los resultados del análisis de estabilidad proveen los requerimientos de diseño para el sistema de autobalance. In that case they adopted Stodola-Green rotor instead of the Jeffcott model. In this study, authors got a similar analysis for a flexible shaft and two self balancing systems on the ends. Describing the rotor centre with polar coordinates, the non-linear equations of motion for an autonomous system are derived from Lagrange´s equation. After a balanced equilibrium position and linearized equations in the neighborhood of the equilibrium position are obtained by the perturbation method and theoretically it shows that after critical speed rotor can be balanced. The system has a small lubrication on its balls and they are collocated themselves by inertial motion upper first natural frequency. The rotor with double self balancing system is shown in Fig. 1, where the shaft is supporting two self balancing systems on the ends. It is assumed that the shaft mass is negligible compared to the rotor mass. The XYZ coordinate system is a space-fixed inertia reference frame end the points C and G of both rotors are centroid and mass centre respectively.
EQUATIONS OF MOTIONPoint O may be regarded as projection of the centroid C onto the axis O´Z. The ball balancer consists of a circular rotor with a groove contain...