Traveling-wave solutions to thin-film equations.
Traveling-wave solutions to thin-film equations.
复制标题
薄膜方程的行波解。
DOI：
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发表时间：
1993
期刊：
影响因子：
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通讯作者：
P. Olla
中科院分区：
文献类型：
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作者：
S. Boatto;L. Kadanoff;P. Olla
Thin films can be effectively described by the lubrication approximation, in which the equation of motion is ${mathit{h}}_{mathit{t}}$+(${mathit{h}}^{mathit{n}}$${mathit{h}}_{mathit{x}mathit{x}mathit{x}}$${)}_{mathit{x}}$=0. Here h is a necessarily positive quantity which represents the height or thickness of the film. Different values of n, especially 1, 2, and 3 correspond to different physical situations. This equation permits solutions in the form of traveling disturbances with a fixed form. If u is the propagation velocity, the resulting equation for the disturbance is ${mathit{uh}}_{mathit{x}}$=(${mathit{h}}^{mathit{n}}$${mathit{h}}_{mathit{x}mathit{x}mathit{x}}$${)}_{mathit{x}}$. Here, quantitative and qualitative solutions to the equation are presented. The study has been limited to the intervals in x where the solutions are positive. It is found that transitions between different qualitative behaviors occur at n=3, 2, 3/2, and 1/2. For example, if u is not zero, solitonlike solutions defined on a finite interval are only possible for n3. More specific results can be obtained. In the case in which the velocity is zero, solitons occur for n2. For n=1, the region 3/2n is characterized by the presence of advancing-front solutions, with support on (-ensuremath{infty},t). For ng1/2, single-minimum solutions diverging at ifmmodepmelse extpmfi{}ensuremath{infty} are possible. The generic solution, present for all positive values of n, is a receding front, which diverges at finite x for n0.
Thin films can be effectively described by the lubrication approximation, in which the equation of motion is ${mathit{h}}_{mathit{t}}$+(${mathit{h}}^{mathit{n}}$${mathit{h}}_{mathit{x}mathit{x}mathit{x}}$${)}_{mathit{x}}$=0. Here h is a necessarily positive quantity which represents the height or thickness of the film. Different values of n, especially 1, 2, and 3 correspond to different physical situations. This equation permits solutions in the form of traveling disturbances with a fixed form. If u is the propagation velocity, the resulting equation for the disturbance is ${mathit{uh}}_{mathit{x}}$=(${mathit{h}}^{mathit{n}}$${mathit{h}}_{mathit{x}mathit{x}mathit{x}}$${)}_{mathit{x}}$. Here, quantitative and qualitative solutions to the equation are presented. The study has been limited to the intervals in x where the solutions are positive. It is found that transitions between different qualitative behaviors occur at n=3, 2, 3/2, and 1/2. For example, if u is not zero, solitonlike solutions defined on a finite interval are only possible for n3. More specific results can be obtained. In the case in which the velocity is zero, solitons occur for n2. For n=1, the region 3/2n is characterized by the presence of advancing-front solutions, with support on (-ensuremath{infty},t). For ng1/2, single-minimum solutions diverging at ifmmodepmelse extpmfi{}ensuremath{infty} are possible. The generic solution, present for all positive values of n, is a receding front, which diverges at finite x for n0.