166 research outputs found

    On convergence of solutions of fractal Burgers equation toward rarefaction waves

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    In the paper, the large time behavior of solutions of the Cauchy problem for the one dimensional fractal Burgers equation ut+(−∂x2)α/2u+uux=0u_t+(-\partial^2_x)^{\alpha/2} u+uu_x=0 with α∈(1,2)\alpha\in (1,2) is studied. It is shown that if the nondecreasing initial datum approaches the constant states u±u_\pm (u−<u+u_-<u_+) as x→±∞x\to \pm\infty, respectively, then the corresponding solution converges toward the rarefaction wave, {\it i.e.} the unique entropy solution of the Riemann problem for the nonviscous Burgers equation.Comment: 15 page

    Critical dynamics of self-gravitating Langevin particles and bacterial populations

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    We study the critical dynamics of the generalized Smoluchowski-Poisson system (for self-gravitating Langevin particles) or generalized Keller-Segel model (for the chemotaxis of bacterial populations). These models [Chavanis & Sire, PRE, 69, 016116 (2004)] are based on generalized stochastic processes leading to the Tsallis statistics. The equilibrium states correspond to polytropic configurations with index nn similar to polytropic stars in astrophysics. At the critical index n3=d/(d−2)n_{3}=d/(d-2) (where d≥2d\ge 2 is the dimension of space), there exists a critical temperature Θc\Theta_{c} (for a given mass) or a critical mass McM_{c} (for a given temperature). For Θ>Θc\Theta>\Theta_{c} or M<McM<M_{c} the system tends to an incomplete polytrope confined by the box (in a bounded domain) or evaporates (in an unbounded domain). For Θ<Θc\Theta<\Theta_{c} or M>McM>M_{c} the system collapses and forms, in a finite time, a Dirac peak containing a finite fraction McM_c of the total mass surrounded by a halo. This study extends the critical dynamics of the ordinary Smoluchowski-Poisson system and Keller-Segel model in d=2d=2 corresponding to isothermal configurations with n3→+∞n_{3}\to +\infty. We also stress the analogy between the limiting mass of white dwarf stars (Chandrasekhar's limit) and the critical mass of bacterial populations in the generalized Keller-Segel model of chemotaxis

    Finite-time blowup in a supercritical quasilinear parabolic-parabolic Keller-Segel system in dimension 2

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    In this paper we prove finite-time blowup of radially symmetric solutions to the quasilinear parabolic-parabolic two-dimensional Keller-Segel system for any positive mass. This is done in case of nonlinear diffusion and also in the case of nonlinear cross-diffusion provided the nonlinear chemosensitivity term is assumed not to decay. Moreover, it is shown that the above-mentioned lack of non-decay assumption is essential with respect to keeping the dichotomy finite-time blowup against boundedness of solutions. Namely, we prove that without the non-decay assumption possible asymptotic behaviour of solutions includes also infinite-time blowup.Comment: 14 page

    Spikes and diffusion waves in one-dimensional model of chemotaxis

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    We consider the one-dimensional initial value problem for the viscous transport equation with nonlocal velocity ut=uxx−(u(K′∗u))xu_t = u_{xx} - \left(u (K^\prime \ast u)\right)_{x} with a given kernel K′∈L1(R)K'\in L^1(\R). We show the existence of global-in-time nonnegative solutions and we study their large time asymptotics. Depending on K′K', we obtain either linear diffusion waves ({\it i.e.}~the fundamental solution of the heat equation) or nonlinear diffusion waves (the fundamental solution of the viscous Burgers equation) in asymptotic expansions of solutions as t→∞t\to\infty. Moreover, for certain aggregation kernels, we show a concentration of solution on an initial time interval, which resemble a phenomenon of the spike creation, typical in chemotaxis models

    Porous medium equation with nonlocal pressure

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    We provide a rather complete description of the results obtained so far on the nonlinear diffusion equation ut=∇⋅(um−1∇(−Δ)−su)u_t=\nabla\cdot (u^{m-1}\nabla (-\Delta)^{-s}u), which describes a flow through a porous medium driven by a nonlocal pressure. We consider constant parameters m>1m>1 and 0<s<10<s<1, we assume that the solutions are non-negative, and the problem is posed in the whole space. We present a theory of existence of solutions, results on uniqueness, and relation to other models. As new results of this paper, we prove the existence of self-similar solutions in the range when N=1N=1 and m>2m>2, and the asymptotic behavior of solutions when N=1N=1. The cases m=1m = 1 and m=2m = 2 were rather well known.Comment: 24 pages, 2 figure

    Multiple peak aggregations for the Keller-Segel system

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    In this paper we derive matched asymptotic expansions for a solution of the Keller-Segel system in two space dimensions for which the amount of mass aggregation is 8Ï€N8\pi N, where N=1,2,3,...N=1,2,3,... Previously available asymptotics had been computed only for the case in which N=1

    The one-dimensional Keller-Segel model with fractional diffusion of cells

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    We investigate the one-dimensional Keller-Segel model where the diffusion is replaced by a non-local operator, namely the fractional diffusion with exponent 0<α≤20<\alpha\leq 2. We prove some features related to the classical two-dimensional Keller-Segel system: blow-up may or may not occur depending on the initial data. More precisely a singularity appears in finite time when α<1\alpha<1 and the initial configuration of cells is sufficiently concentrated. On the opposite, global existence holds true for α≤1\alpha\leq1 if the initial density is small enough in the sense of the L1/αL^{1/\alpha} norm.Comment: 12 page

    A study of blow-ups in the Keller-Segel model of chemotaxis

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    We study the Keller-Segel model of chemotaxis and develop a composite particle-grid numerical method with adaptive time stepping which allows us to accurately resolve singular solutions. The numerical findings (in two dimensions) are then compared with analytical predictions regarding formation and interaction of singularities obtained via analysis of the stochastic differential equations associated with the Keller-Segel model
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