On steady solutions of the Kuramoto-Sivashinsky equation (Q2771080)

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scientific article; zbMATH DE number 1705190
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On steady solutions of the Kuramoto-Sivashinsky equation
scientific article; zbMATH DE number 1705190

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    11 June 2002
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    Kuramoto-Sivashinsky equation
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    monotonic global solutions
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    On steady solutions of the Kuramoto-Sivashinsky equation (English)
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    The author studies the Kuramoto-Sivashinsky equation NEWLINE\[NEWLINEu_t+ u_{xxxx}+ u_{xx}+ \textstyle{{1\over 2}}u^2_x= 0,\quad u= u(x,t).\tag{1}NEWLINE\]NEWLINE This equation can be reduced, by using an appropriate transformation, into one of the following third-order ordinary differential equationsNEWLINENEWLINENEWLINE(2) \(\lambda y'''(x)+ y'(x)= 1- y(x)^2\), \(\lambda:= c^2/2\), \(c\approx\sqrt{1.2}\),NEWLINENEWLINENEWLINE(3) \(\lambda y'''(x)+ y'(x)= -y(x)^2\),NEWLINENEWLINENEWLINEand, respectively,NEWLINENEWLINENEWLINE(4) \(\varepsilon y'''(x)+ y'(x)= \cos y(x)\), \(\varepsilon> 0\).NEWLINENEWLINENEWLINEThe attention is focused on two problems:NEWLINENEWLINENEWLINE(i) a proof of the nonexistence of monotonic global solutions;NEWLINENEWLINENEWLINE(ii) the existence of solutions which blow up on bounded intervals.NEWLINENEWLINENEWLINEThe first main result states that if \(\lambda> 8/27\) in (2) (resp. \(\varepsilon\geq 32/27\) in (4)), then there is no solution \(y\) satisfying \(y'> 0\) and \(y(x)\to \pm 1\) (resp. \(y(x)\to \pm\pi/2\)) as \(x\to\pm\infty\), respectively.NEWLINENEWLINENEWLINETo give the second result, the author supplements (2) or (3) with the initial conditionNEWLINENEWLINENEWLINE(5) \(y(0)= 0\), \(y'(0)= -\beta< 0\), \(y''(0)= 0\).NEWLINENEWLINENEWLINEFor all large values of \(\beta> 0\), there exists finite \(x_\beta> 0\) such that there are solutions \(y\) to (2), (5) verifying \(y'(x)< 0\) on \(-x_\beta< x< x_\beta\) and \(y(x)\to \mp\infty\) as \(x\to \pm x_\beta\), respectively. Moreover, there hold NEWLINE\[NEWLINE\limsup_{x\uparrow x_\beta} (x_\beta- x)^3(- y(x))\leq 30\sqrt{10} \lambda,\;\liminf_{x\uparrow x_\beta} (x_\beta- x)^3(-y(x))\geq 24\lambda.NEWLINE\]NEWLINE Connected to (3), (5), there also exist similar blow-up solutions with possibly different \(x_\beta\).NEWLINENEWLINENEWLINEThe proof of these results is based on the reduction of the third-order equation into a second-order one, which is assured by the monotonicity of the solution.NEWLINENEWLINEFor the entire collection see [Zbl 0972.00046].
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