Heteroclinic orbits, mobility parameters and stability for thin film type equations

We study the phase space of the evolution equation $$ h_t = -(h^n h_{xxx})_x - mathcal{B} (h^m h_x)_x , $$ where $h(x,t) geq 0$. The parameters $n>0$, $m in mathbb{R}$, and the Bond number $mathcal{B}>0$ are given. We find numerically, for some ranges of $n$ and $m$, that perturbing the positi...

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Main Authors: Richard. S. Laugesen, Mary C. Pugh
Format: Article
Language:English
Published: Texas State University 2002-11-01
Series:Electronic Journal of Differential Equations
Subjects:
Online Access:http://ejde.math.txstate.edu/Volumes/2002/95/abstr.html
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spelling doaj-6d444048092d4bc6ac87b39ccc4299b82020-11-24T23:26:42ZengTexas State UniversityElectronic Journal of Differential Equations1072-66912002-11-01200295129Heteroclinic orbits, mobility parameters and stability for thin film type equationsRichard. S. LaugesenMary C. PughWe study the phase space of the evolution equation $$ h_t = -(h^n h_{xxx})_x - mathcal{B} (h^m h_x)_x , $$ where $h(x,t) geq 0$. The parameters $n>0$, $m in mathbb{R}$, and the Bond number $mathcal{B}>0$ are given. We find numerically, for some ranges of $n$ and $m$, that perturbing the positive periodic steady state in a certain direction yields a solution that relaxes to the constant steady state. Meanwhile perturbing in the opposite direction yields a solution that appears to touch down or `rupture' in finite time, apparently approaching a compactly supported `droplet' steady state. We then investigate the structural stability of the evolution by changing the mobility coefficients, $h^n$ and $h^m$. We find evidence that the above heteroclinic orbits between steady states are perturbed but not broken, when the mobilities are suitably changed. We also investigate touch-down singularities, in which the solution changes from being everywhere positive to being zero at isolated points in space. We find that changes in the mobility exponent $n$ can affect the number of touch-down points per period, and affect whether these singularities occur in finite or infinite time. http://ejde.math.txstate.edu/Volumes/2002/95/abstr.htmlNonlinear PDE of parabolic typeheteroclinic orbitsstability problemslubrication theory.
collection DOAJ
language English
format Article
sources DOAJ
author Richard. S. Laugesen
Mary C. Pugh
spellingShingle Richard. S. Laugesen
Mary C. Pugh
Heteroclinic orbits, mobility parameters and stability for thin film type equations
Electronic Journal of Differential Equations
Nonlinear PDE of parabolic type
heteroclinic orbits
stability problems
lubrication theory.
author_facet Richard. S. Laugesen
Mary C. Pugh
author_sort Richard. S. Laugesen
title Heteroclinic orbits, mobility parameters and stability for thin film type equations
title_short Heteroclinic orbits, mobility parameters and stability for thin film type equations
title_full Heteroclinic orbits, mobility parameters and stability for thin film type equations
title_fullStr Heteroclinic orbits, mobility parameters and stability for thin film type equations
title_full_unstemmed Heteroclinic orbits, mobility parameters and stability for thin film type equations
title_sort heteroclinic orbits, mobility parameters and stability for thin film type equations
publisher Texas State University
series Electronic Journal of Differential Equations
issn 1072-6691
publishDate 2002-11-01
description We study the phase space of the evolution equation $$ h_t = -(h^n h_{xxx})_x - mathcal{B} (h^m h_x)_x , $$ where $h(x,t) geq 0$. The parameters $n>0$, $m in mathbb{R}$, and the Bond number $mathcal{B}>0$ are given. We find numerically, for some ranges of $n$ and $m$, that perturbing the positive periodic steady state in a certain direction yields a solution that relaxes to the constant steady state. Meanwhile perturbing in the opposite direction yields a solution that appears to touch down or `rupture' in finite time, apparently approaching a compactly supported `droplet' steady state. We then investigate the structural stability of the evolution by changing the mobility coefficients, $h^n$ and $h^m$. We find evidence that the above heteroclinic orbits between steady states are perturbed but not broken, when the mobilities are suitably changed. We also investigate touch-down singularities, in which the solution changes from being everywhere positive to being zero at isolated points in space. We find that changes in the mobility exponent $n$ can affect the number of touch-down points per period, and affect whether these singularities occur in finite or infinite time.
topic Nonlinear PDE of parabolic type
heteroclinic orbits
stability problems
lubrication theory.
url http://ejde.math.txstate.edu/Volumes/2002/95/abstr.html
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