共查询到20条相似文献,搜索用时 15 毫秒
1.
Julien Lequeurre 《Journal of Mathematical Fluid Mechanics》2013,15(2):249-271
We consider a fluid–structure interaction problem coupling the Navier–Stokes equations with a damped wave equation which describes the displacement of a part of the boundary of the fluid domain. The system is considered first in the two-dimensional setting and in a second part it is adapted to the three-dimensional setting. 相似文献
2.
We consider initial layers and uniqueness of weak entropy solutions to hyperbolic conservation laws through the scalar case.
The entropy solutions we address assume their initial data only in the sense of weak-star in L
∞ as t→0+ and satisfy the entropy inequality in the sense of distributions for t>0. We prove that, if the flux function has weakly genuine nonlinearity, then the entropy solutions are always unique and
the initial layers do not appear. We also discuss applications to the zero relaxation limit for hyperbolic systems of conservation
laws with relaxation.
Accepted: October 26, 1999 相似文献
3.
Robert Jensen Changyou Wang Yifeng Yu 《Archive for Rational Mechanics and Analysis》2008,190(2):347-370
For a bounded domain and , assume that is convex and coercive, and that has no interior points. Then we establish the uniqueness of viscosity solutions to the Dirichlet problem of Aronsson’s equation:
For H = H(p, x) depending on x, we illustrate the connection between the uniqueness and nonuniqueness of viscosity solutions to Aronsson’s equation and
that of the Hamilton–Jacobi equation .
Supported by NSF DMS 0601162.
Supported by NSF DMS 0601403. 相似文献
4.
Caballero R. Marín-Rubio P. Valero José 《Journal of Dynamics and Differential Equations》2022,34(1):443-480
In this paper we study a nonlocal reaction–diffusion equation in which the diffusion depends on the gradient of the solution. Firstly, we prove the existence and uniqueness of regular and strong solutions. Secondly, we obtain the existence of global attractors in both situations under rather weak assumptions by defining a multivalued semiflow (which is a semigroup in the particular situation when uniqueness of the Cauchy problem is satisfied). Thirdly, we characterize the attractor either as the unstable manifold of the set of stationary points or as the stable one when we consider solutions only in the set of bounded complete trajectories.
相似文献5.
Stanislav Antontsev João-Paulo Dias Mário Figueira 《Journal of Mathematical Fluid Mechanics》2014,16(2):211-223
In this paper we study the time-dependent complex Ginzburg–Landau equation with a nonlinear absorbing term in ${\Omega \times(0,T),\, \Omega }$ open bounded set in ${\mathbb{R}^{n}}$ . We prove global existence and uniqueness of solutions for the initial and boundary-value problem and study the properties of localization and extinction of solutions in some special cases. 相似文献
6.
Emmanuel Chasseigne Juan Luis Vazquez 《Archive for Rational Mechanics and Analysis》2002,164(2):133-187
This paper is devoted to constructing a general theory of nonnegative solutions for the equation called “the fast-diffusion equation” in the literature. We consider the Cauchy problem taking initial data in the set ?+ of all nonnegative Borel measures, which forces us to work with singular solutions which are not locally bounded, not even locally integrable. A satisfactory theory can be formulated in this generality in the range 1 > m > m c = max {(N? 2)/N,0}, in which the limits of classical solutions are also continuous in ? N as extended functions with values in ?+∪{∞}. We introduce a precise class of extended continuous solutions ? c and prove (i) that the initial-value problem is well posed in this class, (ii) that every solution u(x,t) in ? c has an initial trace in ?+, and (iii) that the solutions in ? c are limits of classical solutions. Our results settle the well-posedness of two other related problems. On the one hand, they solve the initial-and-boundary-value problem in ?× (0,∞) in the class of large solutions which take the value u=∞ on the lateral boundary x∈??, t>0. Well-posedness is established for this problem for m c < m > 1 when ? is any open subset of ? N and the restriction of the initial data to ? is any locally finite nonnegative measure in ?. On the other hand, by using the special solutions which have the separate-variables form, our results apply to the elliptic problem Δf=f q posed in any open set ?. For 1 > q > N/(N? 2)+ this problem is well posed in the class of large solutions which tend to infinity on the boundary in a strong sense. As is well known, initial data with such a generality are not allowed for m≧ 1. On the other hand, the present theory fails in several aspects in the subcritical range 0> m≦m c , where the limits of smooth solutions need not be extended-continuously. 相似文献
7.
This paper is devoted to time-global solutions of the Fisher-KPP equation in ℝ
N
:
where f is a C
2 concave function on [0,1] such that f(0)=f(1)=0 and f>0 on (0,1). It is well known that this equation admits a finite-dimensional manifold of planar travelling-fronts solutions.
By considering the mixing of any density of travelling fronts, we prove the existence of an infinite-dimensional manifold
of solutions. In particular, there are infinite-dimensional manifolds of (nonplanar) travelling fronts and radial solutions.
Furthermore, up to an additional assumption, a given solution u can be represented in terms of such a mixing of travelling fronts.
Accepted October 30, 2000?Published online March 21, 2001 相似文献
8.
9.
The initial boundary value problem for the compressible Navier–Stokes equation is considered in an infinite layer of . It is proved that if the Reynolds and Mach numbers are sufficiently small, then strong solutions to the compressible Navier–Stokes equation around parallel flows exist globally in time for sufficiently small initial perturbations. The large time behavior of the solution is described by a solution of a one-dimensional viscous Burgers equation. The proof is given by a combination of spectral analysis of the linearized operator and a variant of the Matsumura–Nishida energy method. 相似文献
10.
Christiaan le Roux 《Archive for Rational Mechanics and Analysis》1999,148(4):309-356
. This paper treats the solvability of the equations of motion for an incompressible fluid of grade two subject to nonlinear
partial slip boundary conditions in a bounded simply‐connected domain. The existence of a unique classical solution, global
in time, is proved under suitable regularity and growth restrictions on the initial data, the slip law and the body and surface
forces. The method is based on a fixed-point formulation of the problem.
(Accepted October 5, 1998) 相似文献
11.
Antonin Novotný Adélia Sequeira Juha H. Videman 《Archive for Rational Mechanics and Analysis》1999,149(1):49-67
. We study systems of nonlinear partial differential equations governing the steady motion of certain viscoelastic non‐Newtonian fluids around a rigid body ${\cal B}\subset\real^{3}$ . Considering the equations in a suitably decomposed form, we obtain, for small and sufficiently regular data, existence of a unique solution using a fixed‐point argument in an appropriate functional setting. This setting contains also the asymptotic decay of the solution. Our model equations include the second‐grade and the Maxwell fluid. 相似文献
12.
The development and validation of a numerical simulation model of the flow through embankment dams is described. The paper focuses on basic verification studies, that is, comparisons with analytical solutions and data from laboratory experiments. Two experimental studies, one dealing with the flow in a Hele–Shaw cell and the other with the flow through a bed of packed glass beads, are also described. Comparisons are carried out with respect to the phreatic surfaces, pressure profiles, seepage levels and discharges. It is concluded that the agreement between experimental, analytical and numerical results is generally satisfactory. 相似文献
13.
K. Pileckas 《Journal of Mathematical Fluid Mechanics》2006,8(4):542-563
The existence and uniqueness of a solution to the nonstationary Navier–Stokes system having a prescribed flux in an infinite
cylinder is proved. We assume that the initial data and the external forces do not depend on x3 and find the solution (u, p) having the following form
where x′ = (x1, x2). Such solution generalize the nonstationary Poiseuille solutions. 相似文献
14.
We study monotonicity and 1-dimensional symmetry for positive solutions with algebraic growth of the following elliptic system: $$\left\{\begin{array}{ll} -\Delta u = -u \upsilon^2 &\quad {\rm in}\, \mathbb{R}^N\\ -\Delta \upsilon= -u^2 \upsilon &\quad {{\rm in}\, \mathbb{R}^N},\end{array}\right.$$ for every dimension ${N \geqq 2}$ . In particular, we prove a Gibbons-type conjecture proposed by Berestycki et al. 相似文献
15.
For a nonsmooth positively one-homogeneous convex function φ:ℝ
n
→ [0,+∞[, it is possible to introduce the class ?φ (ℝ
n
) of smooth boundaries with respect to φ, to define their φ-mean curvature κφ, and to prove that, for E∈?φ (ℝ
n
), κφ∈L
∞(δE) [9]. Based on these results, we continue the analysis on the structure of δE and on the regularity properties of κφ. We prove that a facet F of δE is Lipschitz (up to negligible sets) and that κφ has bounded variation on F. Further properties of the jump set of κφ are inspected: in particular, in three space dimensions, we relate
the sublevel sets of κφ on F to the geometry of the Wulff shape ?φ≔{φ≤ 1 }.
Accepted October 11, 2000?Published online 14 February, 2001 相似文献
16.
E. Juárez Hurtado O. H. Miyagaki R. S. Rodrigues 《Journal of Dynamics and Differential Equations》2018,30(2):405-432
In this paper we establish, using variational methods, the existence and multiplicity of weak solutions for a general class of quasilinear problems involving \(p(\cdot )\)-Laplace type operators, with Dirichlet boundary conditions involving variable exponents without Ambrosetti and Rabinowitz (A-R) type growth conditions, namely By different types of versions of the Mountain Pass Theorem with Cerami condition, as well as, the Fountain and Dual Theorem with Cerami condition, we obtain some existence of weak solutions for the above problem under some considerations. Moreover, we show that the problem treated has at least one nontrivial solution for any parameter \(\lambda >0\) small enough, and also that the solution blows up, in the Sobolev norm, as \(\lambda \rightarrow 0^{+}.\) Finally, by imposing additional hypotheses on the nonlinearity \(f(x,\cdot ),\) we get the existence of infinitely many weak solutions by using the Genus Theory introduced by Krasnoselskii.
相似文献
$$\begin{aligned} \left\{ \begin{array}{rcll} -{\text {div}}(a(|\nabla u|^{p(x)})|\nabla u|^{p(x)-2}\nabla u)&{}=&{}\lambda f(x,u) &{} \text{ in } \Omega ,\\ u&{}=&{}0 &{} \text{ on } \partial \Omega . \end{array} \right. \end{aligned}$$
17.
Jiří Neustupa 《Archive for Rational Mechanics and Analysis》2010,198(1):331-348
We prove the existence of a weak solution to the steady Navier–Stokes problem in a three dimensional domain Ω, whose boundary
∂Ω consists of M unbounded components Γ1, . . . , Γ
M
and N − M bounded components Γ
M+1, . . . , Γ
N
. We use the inhomogeneous Dirichlet boundary condition on ∂Ω. The prescribed velocity profile α on ∂Ω is assumed to have an L
3-extension to Ω with the gradient in L
2(Ω)3×3. We assume that the fluxes of α through the bounded components Γ
M+1, . . . , Γ
N
of ∂Ω are “sufficiently small”, but we impose no restriction on the size of fluxes through the unbounded components Γ1, . . . , Γ
M
. 相似文献
18.
A. E. Medvedev 《Journal of Applied Mechanics and Technical Physics》2001,42(2):211-218
Reflection of an oblique shock wave in a reacting gas with a finite length of the chemical–reaction zone is studied. Shock polars for an arbitrary heat release behind the oblique shock wave are constructed. Transition criteria from regular to Mach reflection and back are obtained. It is shown that transition criteria are significantly changed if the reaction–zone length is taken into account. 相似文献
19.
The interior transmission problem (ITP), which plays a fundamental role in inverse scattering theories involving penetrable
defects, is investigated within the framework of mechanical waves scattered by piecewise-homogeneous, elastic or viscoelastic
obstacles in a likewise heterogeneous background solid. For generality, the obstacle is allowed to be multiply connected,
having both penetrable components (inclusions) and impenetrable parts (cavities). A variational formulation is employed to
establish sufficient conditions for the existence and uniqueness of a solution to the ITP, provided that the excitation frequency does not belong
to (at most) countable spectrum of transmission eigenvalues. The featured sufficient conditions, expressed in terms of the
mass density and elasticity parameters of the problem, represent an advancement over earlier works on the subject in that
(i) they pose a precise, previously unavailable provision for the well-posedness of the ITP in situations when both the obstacle
and the background solid are heterogeneous, and (ii) they are dimensionally consistent, i.e., invariant under the choice of
physical units. For the case of a viscoelastic scatterer in an elastic solid it is further shown, consistent with earlier
studies in acoustics, electromagnetism, and elasticity that the uniqueness of a solution to the ITP is maintained irrespective
of the vibration frequency. When applied to the situation where both the scatterer and the background medium are viscoelastic, i.e., dissipative, on the other hand, the same type of analysis
shows that the analogous claim of uniqueness does not hold. Physically, such anomalous behavior of the “viscoelastic-viscoelastic”
case (that has eluded previous studies) has its origins in a lesser known fact that the homogeneous ITP is not mechanically
insulated from its surroundings—a feature that is particularly cloaked in situations when either the background medium or
the scatterer are dissipative. A set of numerical results, computed for ITP configurations that meet the sufficient conditions
for the existence of a solution, is included to illustrate the problem. Consistent with the preceding analysis, the results
indicate that the set of transmission values is indeed empty in the “elastic-viscoelastic” case, and countable for “elastic-elastic”
and “viscoelastic-viscoelastic” configurations. 相似文献
20.
Zhi-Qiang Shao 《Journal of Elasticity》2010,98(1):25-64
In this paper, we investigate the asymptotic behavior of global classical solutions to the mixed initial-boundary value problem
with small BV data for linearly degenerate quasilinear hyperbolic systems with general nonlinear boundary conditions in the
half space {(t,x)|t≥0,x≥0}. Based on the existence result on the global classical solution, we prove that when t tends to the infinity, the solution approaches a combination of C
1 traveling wave solutions, provided that the C
1 norm of the initial and boundary data is bounded and the BV norm of the initial and boundary data is sufficiently small.
Applications to quasilinear hyperbolic systems arising in physics and mechanics, particularly to the system describing the
motion of the relativistic string in the Minkowski space-time R
1+n
, are also given. 相似文献