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Автор Andreas Münch
Дата выпуска 2000-05-01
dc.description Thin films of silicon oil driven up an inclined silicon wafer by a thermally induced Marangoni force develop unusual shock profiles involving a non-classical undercompressive shock, if the counteracting parallel component of gravity is sufficiently large (Bertozzi et al 1998 Phys. Rev. Lett. 81 5169-72). They arise as a result of the interaction of a non-convex flux with the fourth-order diffusion generated by surface tension. In this work, we investigate how the dynamical behaviour of the solution is affected by including second-order diffusion resulting from the normal component of gravity; this component was neglected in the previous study. Then the governing equation for the film profile h (x , t ) becomes h<sub>t</sub> + ( h <sup>2</sup> - h <sup>3</sup> )<sub>x </sub> = - ( h <sup>3</sup> h<sub>xxx</sub> )<sub>x </sub> + D ( h <sup>3</sup> h<sub>x</sub> )<sub>x </sub>               D 0. The numerical simulations in this paper confirm that neglecting second-order diffusion is justified for small D , but find that for larger D , the structure of the solution changes dramatically. We give a detailed account of the transitions that occur while increasing D and make predictions for future experiments carried out at small inclination angles, corresponding to moderately large D .
Формат application.pdf
Издатель Institute of Physics Publishing
Название Shock transitions in Marangoni gravity-driven thin-film flow
Тип paper
DOI 10.1088/0951-7715/13/3/312
Electronic ISSN 1361-6544
Print ISSN 0951-7715
Журнал Nonlinearity
Том 13
Первая страница 731
Последняя страница 746
Аффилиация Andreas Münch; Zentrum Mathematik, Technische Universität München (H4), D-80290 Munich, Germany
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