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1.
Symmetries and solutions to the thin film equations 总被引:1,自引:0,他引:1
Changzheng Qu 《Journal of Mathematical Analysis and Applications》2006,317(2):381-397
We study symmetries and solutions of the generalized fourth-order nonlinear partial differential equations which arise from studies of thin liquid films. It is shown that the equations admit extended scaling and rotation symmetries and a class of generalized conditional symmetries for certain coefficient functions. Exact solutions associated to the symmetries are obtained. 相似文献
2.
Maria Santos Bruzón Nail H. Ibragimov 《Journal of Mathematical Analysis and Applications》2009,357(1):307-313
In this work we consider a class of fourth-order nonlinear partial differential equation containing several un-specified coefficient functions of the dependent variable which encapsulates various mathematical models used, e.g. for describing the dynamics of thin liquid films. We determine the subclasses of these equations which are self-adjoint. By using a general theorem on conservation laws proved by one of the authors (NHI) we find conservation laws for some of these partial differential equations without classical Lagrangians. 相似文献
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R. M. Taranets 《Siberian Mathematical Journal》2006,47(4):751-766
We study the evolution of the support of an arbitrary strong generalized solution to the Cauchy problem for the thin film equation with nonlinear diffusion and convection. We find an upper bound exact (in a sense) for the propagation speed of the support of this solution. 相似文献
5.
Well-posedness and stability for a mixed order system arising in thin film equations with surfactant
Gabriele Bruell 《Mathematische Nachrichten》2020,293(5):879-892
The objective of the present work is to provide a well-posedness result for a capillary driven thin film equation with insoluble surfactant. The resulting parabolic system of evolution equations is not only strongly coupled and degenerated, but also of mixed orders. To the best of our knowledge the only well-posedness result for a capillary driven thin film with surfactant is provided in [4] by the same author, where a severe smallness condition on the surfactant concentration is assumed to prove the result. Thus, in spite of an intensive analytical study of thin film equations with surfactant during the last decade, a proper well-posedness result is still missing in the literature. It is the aim of the present paper to fill this gap. Furthermore, we apply a recently established result on asymptotic stability in interpolation spaces [15] to prove that the flat equilibrium of our system is asymptotically stable. 相似文献
6.
Peng Feng 《Journal of Mathematical Analysis and Applications》2010,370(2):573-583
We consider the structure of positive radial solutions of
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We study positive solutions of the equation
8.
Using the theory of fiber bundles we construct a new model of a thin polycrystal film. The quantum equations of motion thereby obtained are used to determine the regularity of the influence of substructural ordering on the physical characteristics of the film.Translated fromMatematicheskie Metody i Fiziko-Mekhanicheskie Polya, Issue 28, 1988, pp. 36–40. 相似文献
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Our first basic model is the fully nonlinear dual porous medium equation with source
for which we consider the Cauchy problem with given nonnegative bounded initial data u0. For the semilinear case m=1, the critical exponent
was obtained by H. Fujita in 1966. For p ∈(1, p0] any nontrivial solution blows up in finite time, while for p > p0 there exist sufficiently small global solutions. During last thirty years such critical exponents were detected for many
semilinear and quasilinear parabolic, hyperbolic and elliptic PDEs and inequalities. Most of efforts were devoted to equations
with differential operators in divergent form, where classical techniques associated with weak solutions and integration by
parts with a variety of test functions can be applied. Using this fully nonlinear equation, we propose and develop new approaches
to calculating critical Fujita exponents in different functional settings.
The second models with a “semi-divergent” diffusion operator is the thin film equation with source
for which the critical exponent is shown to be
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P. E. Tovstik T. P. Tovstik N. V. Naumova 《Vestnik St. Petersburg University: Mathematics》2017,50(2):198-207
The asymptotic integrating method is used to investigate long-wave oscillations and waves in an infinite heterogeneous (with respect to width) anisotropic beam-belt. A dispersion equation of the second-order accuracy with respect to the relative width of the beam-belt is constructed and additional qualitative effects related to the anisotropy are found. 相似文献
14.
We consider the Cauchy problem for the first and the second order differential equations in Banach and Hilbert spaces with an operator coefficient depending on the parameter . We develop discretization methods with high parallelism level and without accuracy saturation; i.e., the accuracy adapts automatically to the smoothness of the solution. For analytical solutions the rate of convergence is exponential. These results can be viewed as a development of parallel approximations of the operator exponential and of the operator cosine family with a constant operator possessing exponential accuracy and based on the Sinc-quadrature approximations of the corresponding Dunford-Cauchy integral representations of solutions or the solution operators.
15.
A. Krsova 《Mechanics of Composite Materials》1974,10(4):615-619
The individual stages of deformation of spherulitic specimens of polycaprolactam have been studied by a microscopic method. An empirical relation between the total deformation of the specimen and the deformation of the individual spherulite is obtained. 相似文献
16.
Laurent Chupin 《Comptes Rendus Mathematique》2009,347(17-18):1041-1046
This Note has as objective to determine, in a rigorous way, a simplified expression of the constitutive law for a visco-elastic fluid of FENE type in thin domains. The proof uses the FENE model behavior for long times and the existence of a stationary solution for this behavioral law. Some possible applications of this study are then briefly described in the domains of lubrication, blood flow, microfluidic, boundary layers, …. To cite this article: L. Chupin, C. R. Acad. Sci. Paris, Ser. I 347 (2009). 相似文献
17.
Jean-François Babadjian 《Calculus of Variations and Partial Differential Equations》2006,26(1):69-118
This paper deals with the quasistatic crack growth of a homogeneous elastic brittle thin film. It is shown that the quasistatic
evolution of a three-dimensional cylinder converges, as its thickness tends to zero, to a two-dimensional quasistatic evolution
associated with the relaxed model. Firstly, a Γ-convergence analysis is performed with a surface energy density which does
not provide weak compactness in the space of Special Functions of Bounded Variation. Then, the asymptotic analysis of the
quasistatic crack evolution is presented in the case of bounded solutions that is with the simplifying assumption that every
minimizing sequence is uniformly bounded in L∞.
Mathematics Subject Classification (2000) 74K30, 49J45, 74K30, 35R35, 49Q20 相似文献
18.
In this work we give a complete group classification of the thin film equation ut = –(f (u)xxx )x – kg (u)x . By using Lie classical method the corresponding reductions are performed and some solutions are characterized. Some nonclassical symmetries for an associated potential system are derived. (© 2008 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
19.
We prove a regularity result in the two-dimensional theory of soft ferromagnetic films. The associated Euler–Lagrange equation is given by a nonlocal degenerate variational inequality involving fractional derivatives. A difference quotient type argument based on a dual formulation in terms of magnetostatic potentials yields a Hölder estimate for the uniquely determined gradient projection of the magnetization field. 相似文献
20.
B. S. Dandapat A. Kitamura B. Santra 《Zeitschrift für Angewandte Mathematik und Physik (ZAMP)》2006,45(11):623-635
In this paper we have studied a non-planar thin liquid film flow on a planar stretching surface. The stretching surface is
assumed to stretch impulsively from rest and the effect of inertia of the liquid is considered. Equations describing the laminar
flow on the stretching surface are solved analytically. It is observed that faster stretching causes quicker thinning of the
film on the stretching surface. Velocity distribution in the liquid film and the transient film profile as functions of time
are obtained. 相似文献