one of the most important concepts in mechanics. The motion of any mechanical system, such as a machine, gyroscopic device, aircraft, or missile, is dependent on the forces at work and on the initial conditions, that is, on the positions and velocities of the points in the system at the moment when the motion is initiated. Given these forces and initial conditions, it is possible to calculate theoretically how the system will move. The motion thus calculated is called unperturbed. However, since all measurements are made only to some degree of accuracy, the true values of the initial conditions in practice will usually differ somewhat from the calculated values. In addition, a mechanical system may be subjected in the course of the motion to small, random influences that were not considered in calculations. This is also equivalent to a change in the initial conditions. Departures of the initial conditions from the calculated values that occur for various reasons are called initial perturbations, and the motion that the system will undergo with such perturbations present is called the perturbed motion.
The effect of initial perturbations on the characteristics of a system’s motion, such as the trajectories and velocities of the system’s points, may be twofold. With fairly small initial perturbations, if any of the characteristics differs very little from the value they should have for unperturbed motion continuing ad infinitum, the motion of the system with respect to such characteristics is termed stable. However, with initial perturbations that are arbitrarily small but not zero, if a characteristic differs more and more from the value it should have for unperturbed motion, the motion of the system with respect to the characteristic is termed unstable. These definitions correspond to A. M. Liapunov’s definition of stable motion. The conditions for which the motion of a mechanical system is stable are called stability criteria.
As an example, we will discuss a gyroscope that has a vertical axis and that rotates about this axis with an angular velocity ω (Figure 1). Theoretically the axis of the gyroscope ought to remain vertical for any value of ω in practice, however, when ω is less than a certain value ωcr, with any small perturbation the axis will deviate more and more from the vertical. If ω is greater than ωcr, small perturbations cause practically no change in the direction of the axis. Consequently, when ω < ωcr, the gyroscope is unstable with respect to the direction of its axis; it is stable when ω > ωcr. The latter inequality is the stability criterion. Here 
where P is the weight of the gyroscope, a is the distance from the point of support O to the center of gravity C, and Ix and Iy are the moments of inertia of the gyroscope relative to the x and y axes, respectively.
The theory of stability of motion is of great practical importance in many fields of technology, inasmuch as various types of engines, motor vehicles, aircraft, rockets, gyroscopic devices, and automatic control systems should exhibit stability of motion. The problem of stability of motion arises in celestial mechanics in connection with studies of how long the structure of the solar system will be maintained and in research on binary stars.
REFERENCES
Liapunov, A. M. Obshchaia zadacha ob ustoichivosti dvizheniia, Moscow-Leningrad, 1950.Chetaev, N. G. Ustoichivost’ dvizheniia, 2nd ed. Moscow, 1955.
Duboshin, G. N. Osnovy teorii ustoichivosti dvizheniia. [Moscow] 1952.
Krasovskii, N. N. Nekotorye zadachi teorii ustoichivosti dvizheniia. Moscow, 1959.
Malkin, I. G. Teoriia ustoichivosti dvizheniia. Moscow-Leningrad, 1952.
Merkin, D. R. Vvedenie v teoriiu ustoichivosti dvizheniia. Moscow, 1971. (Contains bibliography.)
Want to thank TFD for its existence? Tell a friend about us, add a link to this page, add the site to iGoogle, or visit the webmaster's page for free fun content.
| ?Page tools | ||
|---|---|---|
|