Abstract
Starting with a given equation of the form
, where λ > 0 and ɛ ≪ l is a small parameter [heref(t) may be periodic, and so Hill's equation is included], we construct an equation of the form y + [λ + ɛf (t) + ɛ2 g (t)]y = 0, integrable by quadratures, close in a certain sense to the original equation. For x0 = y0 and x ′0 = y ′0 , an upper bound is obtained for ¦y—x¦ on an interval of length Δt.
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Literature cited
E. Kamke,Ordinary Differential Equations [Russian translation], Moscow (1961), pp. 152–153.
I. G. Malkin, The Theory of the Stability of Motion [in Russian], Moscow (1966), pp. 245–253.
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Translated from Matematicheskie Zametki, Vol. 8, No. 6, pp. 784–786, December, 1970.
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Popov, G.E. A method of constructing integrable linear equations and its application to Hill's equation. Mathematical Notes of the Academy of Sciences of the USSR 8, 914–916 (1970). https://doi.org/10.1007/BF01673694
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DOI: https://doi.org/10.1007/BF01673694