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An asymptotic symmetry of the rapidly forced pendulum

Technical Report ·
DOI:https://doi.org/10.2172/6504138· OSTI ID:6504138
 [1];  [2]
  1. Colorado Univ., Boulder, CO (USA). Applied Mathematics Program State Univ. of New York, Buffalo, NY (USA). Dept. of Mathematics
  2. Colorado Univ., Boulder, CO (USA). Applied Mathematics Program

The inhomogeneous differential equation (x{double prime} + sin x = {delta} sin (t + t{sub 0}){var epsilon}) describes the motion of a sinusoidally forced pendulum. The orbits that connect the two saddle points of the unforced ({delta} = 0) pendulum, (x = {pi}) and (x = {minus}{pi}), are called separatrices. If {var epsilon} {Omicron}(1), then one can use Melnikov's method to show that these separatrices can split for weak forcing ({delta} {much lt} 1), and that the perturbed motion is chaotic. If {var epsilon} 1, Melnikov's method fails because the perturbation term is not analytic in {var epsilon} at {var epsilon} = 0. In this paper we show that for {delta} {much lt} 1 and {var epsilon} {much lt} 1, the solution of the perturbed problem exhibits a symmetry to all orders in an asymptotic expansion. From the asymptotic expansion it follows that the separatrices split by an amount that is at most transcendentally small. This proof differs from that of Holmes, Marsden and Scheurle. 16 refs.

Research Organization:
Colorado Univ., Boulder, CO (USA). Applied Mathematics Program; State Univ. of New York, Buffalo, NY (USA). Dept. of Mathematics
Sponsoring Organization:
DOE/ER
DOE Contract Number:
FG02-86ER25021
OSTI ID:
6504138
Report Number(s):
DOE/ER/25021-T1; ON: DE91001868
Country of Publication:
United States
Language:
English