A quantitative stability analysis of the Carson-Cambi equation [(l+ E cos t)(d'y/dt') + py = 0] is carried through, using a new, effective approach. The results are compared with a recent perturbation unalysis, and show that this should not be used for 1~1 BO.4. In the present analysis we go up to I
✦ LIBER ✦
Perturbation solutions of the Carson–Cambi equation
✍ Scribed by Barbara Epstein; Richard Barakat
- Publisher
- Elsevier Science
- Year
- 1977
- Tongue
- English
- Weight
- 586 KB
- Volume
- 303
- Category
- Article
- ISSN
- 0016-0032
No coin nor oath required. For personal study only.
✦ Synopsis
The periodic differential equation (1 + E cos t)y"+ py = 0, hereby termed the
Carson-Cambi equation, is the simplest second-order differential equation having a periodic coefficient associated with the second derivative. Provided (e( < 1, which is the case we examine, then the differential equation is a Hill's equation and thus possesses regions of stability and instability in the p-e plane. Ordinary perturbation theory is employed to obtain the stable (periodic) solutions to e3. Two-timing theory is employed to obtain solutions for values of k near the critical points
k = *f, *$, *$. Three-timing is employed to extend the solution near k = *f. The solutions of the Carson-Cambi equation are compared with the solutions of the corresponding Mathieu equation.
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