325,541 research outputs found
Global existence, uniqueness and stability for nonlinear dissipative bulk-interface interaction systems
We show global well-posedness and exponential stability of equilibria for a
general class of nonlinear dissipative bulk-interface systems. They correspond
to thermodynamically consistent gradient structure models of bulk-interface
interaction. The setting includes nonlinear slow and fast diffusion in the bulk
and nonlinear coupled diffusion on the interface. Additional driving mechanisms
can be included and non-smooth geometries and coefficients are admissible, to
some extent. An important application are volume-surface reaction-diffusion
systems with nonlinear coupled diffusion.Comment: 21 page
Nonlinear diffusion equations as asymptotic limits of Cahn-Hilliard systems
An asymptotic limit of a class of Cahn-Hilliard systems is investigated to
obtain a general nonlinear diffusion equation. The target diffusion equation
may reproduce a number of well-known model equations: Stefan problem, porous
media equation, Hele-Shaw profile, nonlinear diffusion of singular logarithmic
type, nonlinear diffusion of Penrose-Fife type, fast diffusion equation and so
on. Namely, by setting the suitable potential of the Cahn-Hilliard systems, all
of these problems can be obtained as limits of the Cahn-Hilliard related
problems. Convergence results and error estimates are proved
Markov vs. nonMarkovian processes A comment on the paper Stochastic feedback, nonlinear families of Markov processes, and nonlinear Fokker-Planck equations by T.D. Frank
The purpose of this comment is to correct mistaken assumptions and claims
made in the paper Stochastic feedback, nonlinear families of Markov processes,
and nonlinear Fokker-Planck equations by T. D. Frank. Our comment centers on
the claims of a nonlinear Markov process and a nonlinear Fokker-Planck
equation. First, memory in transition densities is misidentified as a Markov
process. Second, Frank assumes that one can derive a Fokker-Planck equation
from a Chapman-Kolmogorov equation, but no proof was given that a
Chapman-Kolmogorov equation exists for memory-dependent processes. A nonlinear
Markov process is claimed on the basis of a nonlinear diffusion pde for a
1-point probability density. We show that, regardless of which initial value
problem one may solve for the 1-point density, the resulting stochastic
process, defined necessarily by the transition probabilities, is either an
ordinary linearly generated Markovian one, or else is a linearly generated
nonMarkovian process with memory. We provide explicit examples of diffusion
coefficients that reflect both the Markovian and the memory-dependent cases. So
there is neither a nonlinear Markov process nor nonlinear Fokker-Planck
equation for a transition density. The confusion rampant in the literature
arises in part from labeling a nonlinear diffusion equation for a 1-point
probability density as nonlinear Fokker-Planck, whereas neither a 1-point
density nor an equation of motion for a 1-point density defines a stochastic
process, and Borland misidentified a translation invariant 1-point density
derived from a nonlinear diffusion equation as a conditional probability
density. In the Appendix we derive Fokker-Planck pdes and Chapman-Kolmogorov
eqns. for stochastic processes with finite memory
Quasichemical Models of Multicomponent Nonlinear Diffusion
Diffusion preserves the positivity of concentrations, therefore,
multicomponent diffusion should be nonlinear if there exist non-diagonal terms.
The vast variety of nonlinear multicomponent diffusion equations should be
ordered and special tools are needed to provide the systematic construction of
the nonlinear diffusion equations for multicomponent mixtures with significant
interaction between components. We develop an approach to nonlinear
multicomponent diffusion based on the idea of the reaction mechanism borrowed
from chemical kinetics.
Chemical kinetics gave rise to very seminal tools for the modeling of
processes. This is the stoichiometric algebra supplemented by the simple
kinetic law. The results of this invention are now applied in many areas of
science, from particle physics to sociology. In our work we extend the area of
applications onto nonlinear multicomponent diffusion.
We demonstrate, how the mechanism based approach to multicomponent diffusion
can be included into the general thermodynamic framework, and prove the
corresponding dissipation inequalities. To satisfy thermodynamic restrictions,
the kinetic law of an elementary process cannot have an arbitrary form. For the
general kinetic law (the generalized Mass Action Law), additional conditions
are proved. The cell--jump formalism gives an intuitively clear representation
of the elementary transport processes and, at the same time, produces kinetic
finite elements, a tool for numerical simulation.Comment: 81 pages, Bibliography 118 references, a review paper (v4: the final
published version
Nonlinear diffusion equations with degenerate fast-decay mobility by coordinate transformation
We prove an existence and uniqueness result for solutions to nonlinear
diffusion equations with degenerate mobility posed on a bounded interval for a
certain density . In case of \emph{fast-decay} mobilities, namely mobilities
functions under a Osgood integrability condition, a suitable coordinate
transformation is introduced and a new nonlinear diffusion equation with linear
mobility is obtained. We observe that the coordinate transformation induces a
mass-preserving scaling on the density and the nonlinearity, described by the
original nonlinear mobility, is included in the diffusive process. We show that
the rescaled density is the unique weak solution to the nonlinear
diffusion equation with linear mobility. Moreover, the results obtained for the
density allow us to motivate the aforementioned change of variable and
to state the results in terms of the original density without prescribing
any boundary conditions
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