Processing math: 100%
World Scientific
Skip main navigation

Cookies Notification

We use cookies on this site to enhance your user experience. By continuing to browse the site, you consent to the use of our cookies. Learn More
×

System Upgrade on Tue, May 28th, 2024 at 2am (EDT)

Existing users will be able to log into the site and access content. However, E-commerce and registration of new users may not be available for up to 12 hours.
For online purchase, please visit us again. Contact us at customercare@wspc.com for any enquiries.

The two-dimensional Keller–Segel system with singular sensitivity and signal absorption: Global large-data solutions and their relaxation properties

    https://doi.org/10.1142/S0218202516500238Cited by:95 (Source: Crossref)

    We consider the chemotaxis system

    {ut=Δu(uvv),vt=Δvuv,
    as originally introduced in 1971 by Keller and Segel in the second of their seminal works. This system constitutes a prototypical model for taxis-driven pattern formation and front propagation in various biological contexts such as tumor angiogenesis, but in the higher-dimensional context any global existence theory for large-data solutions is yet lacking. In this work it is shown that in bounded planar domains Ω with smooth boundary, for all reasonably regular initial data u00 and v0>0, the corresponding Neumann initial-boundary value problem possesses a global generalized solution. Thus particularly addressing arbitrarily large initial data, this goes beyond previously gained results asserting global existence of solutions only in spatial one-dimensional problems, or under certain smallness conditions on the initial data. The derivation of this result is based on a priori estimates for the quantities ln(u+1) and v in spatio-temporal L2 spaces, where further boundedness and compactness properties are derived from the former by relying on the planar spatial setting in using an associated Moser–Trudinger inequality. Furthermore, some further boundedness and relaxation properties are derived, inter alia indicating that for any such solution we have v(,t)0 in Lp(Ω) as t for all finite p>1, and that in an appropriate generalized sense the quantities u and lnv eventually enter bounded sets in Lp(Ω) and L2(Ω), respectively, with diameters only determined by the total population size Ωu0. Finally, some numerical experiments illustrate the analytically obtained results.

    Communicated by N. Bellomo

    AMSC: Primary 35D30, Primary 35B40, Secondary 35K55, Secondary 35B65, Secondary 92C17, Secondary 35Q92