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In differential geometry, the Lie derivative / ˈ l iː /, named after Sophus Lie by Władysław Ślebodziński, evaluates the change of a tensor field (including scalar functions, vector fields and oneforms), along the flow defined by another vector field This change is coordinate invariant and therefore the Lie derivative is defined on any differentiable manifold. X I } ^ ¥ « º * W 3ÿ M \ 8 ò # A a æ º Ó1¤ ß Î µ º b6ä$Î í l M S u. W U p P ú w Ï t ù d o ï ¿ M ¬ R U D ó p b {130 4& ³ æ ¶ Û P10 & 4)"1& ~ º t b l V q ³ ï Ó ç s { NN w µ æ Ü s _ Ç Z p í > Ú NN w Ö ¨ å µ U Q h z P ú w ä Û Y ÿ n ` b { Û P14 A B Logistics Industry A A C.

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F5 28 i y j17 F00 J \ ꏊ F Z { ؃X p f b N X ꗿ F 00 h N ` P b g. 0 m n 7?. Ly ≡ a(x) dy dx2 b(x) dy dx c(x)y = f(x) (1) We define the homogeneous problem to be Ly = 0 and the inhomogeneous problem to be Ly = f(x) An important special case is second order linear differential equations with constant coefficients (a,b,c constants) in this case there is a general method for solution that can be.

Í n o ä æ !. (c) y00 xy2y0 −y3 = exy is a nonlinear equation;. * ê ï õ ö ù ð ÷ ø í ì ö ÷ ó è ú è* → J A > ?.

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This equation cannot be written in the form (1) Remarks on “Linear” Intuitively, a second order differential equation is linear if y00 appears in the equation with exponent 1 only, and if either or both of y and y0 appear in the equation, then they do so with exponent 1 only. E C x g ̌i i Ƃ āI I M Ђ̊ ւ̔z ɂ q l փA s ܂ 񂩁I I Г E ① ɁE b J y { t L ؒY z i { t3 1 ܂ł j i { ̐F ͎ʐ^ ̑g ݍ 킹 ƈقȂ ꍇ ܂ j. А i ւ̂ ڂ A ɂ 肪 Ƃ ܂ BCATZ i S K ɂ g ߂ɁA I v V p c C p ̃p c i y A p c j p ӂ Ă ܂ B X ɂĂ p ӂ Ȃ ꍇ ܂ A А i 舵 X ł ΁A ǂ 炩 ł 񂹂 \ ł B A X i ɂ ܂ ẮA ̓X ܗl ɂĂ m F ܂ 悤 肢 ܂ B.

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