释义 |
Floquet AnalysisGiven a system of periodic Ordinary Differential Equations of the form
 | (1) |
the solution can be written as a linear combination of functions of the form
 | (2) |
where is a function periodic with the same period as the equations themselves. Given an OrdinaryDifferential Equation of the form
 | (3) |
where is periodic with period , the ODE has a pair of independent solutions given by the Real and Imaginary Parts of
Plugging these into (3) gives
 | (7) |
so the Real and Imaginary Parts are
 | (8) |
 | (9) |
From (9),
Integrating gives
 | (11) |
where is a constant which must equal 1, so is given by
 | (12) |
The Real solution is then
 | (13) |
so
and
which is an integral of motion. Therefore, although is not explicitly known, an integral always exists.Plugging (10) into (8) gives
 | (16) |
which, however, is not any easier to solve than (3). References
Abramowitz, M. and Stegun, C. A. (Eds.). Handbook of Mathematical Functions with Formulas, Graphs, and Mathematical Tables, 9th printing. New York: Dover, p. 727, 1972.Binney, J. and Tremaine, S. Galactic Dynamics. Princeton, NJ: Princeton University Press, p. 175, 1987. Lichtenberg, A. and Lieberman, M. Regular and Stochastic Motion. New York: Springer-Verlag, p. 32, 1983. Margenau, H. and Murphy, G. M. The Mathematics of Physics and Chemistry, 2 vols. Princeton, NJ: Van Nostrand, 1956-64. Morse, P. M. and Feshbach, H. Methods of Theoretical Physics, Part I. New York: McGraw-Hill, pp. 556-557, 1953.
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