2005
DOI: 10.1016/j.anihpc.2004.06.001
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On self-similarity and stationary problem for fragmentation and coagulation models

Abstract: We prove the existence of a stationary solution of any given mass to the coagulation-fragmentation equation without assuming a detailed balance condition, but assuming instead that aggregation dominates fragmentation for small particles while fragmentation predominates for large particles. We also show the existence of a self-similar solution of any given mass to the coagulation equation and to the fragmentation equation for kernels satisfying a scaling property. These results are obtained, following the theor… Show more

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Cited by 131 publications
(228 citation statements)
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References 35 publications
(40 reference statements)
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“…(6). When k = −1 or 0, the condition g 0 k,ν < ∞ is redundant, as it is already implied by g 0 e νy < ∞ and g ′ 0 ∈ L 1 .…”
Section: The Relative Entropy Fmentioning
confidence: 99%
See 1 more Smart Citation
“…(6). When k = −1 or 0, the condition g 0 k,ν < ∞ is redundant, as it is already implied by g 0 e νy < ∞ and g ′ 0 ∈ L 1 .…”
Section: The Relative Entropy Fmentioning
confidence: 99%
“…It is expected that for a general class of homogeneous coagulation kernels, there is a unique self-similar profile with given mass ρ > 0, and that for a very wide class of initial conditions solutions to Smoluchowski's equation approximate, for large times, the self-similar solution with the same mass, in a sense to be precised. For general homogeneous coagulation rates there are no rigorous proofs of this behavior, except for recent results that have shown the existence of self-similar profiles [7,6] and given some of their properties [8,4]. Nevertheless, for the specific coagulation rates given by a(x, y) = x + y and a(x, y) = 1 (our case), it is known that the self-similar profile is unique for each given finite mass, and the convergence to it has been proved in [9,14,15,12].…”
Section: The Self-similar Equationmentioning
confidence: 99%
“…In both cases the expected behaviour is of self-similar form (except for some particular kernels with homogeneity 1) but the time and mass scales are only well identified for non-gelling kernels and for the multiplicative kernel K 2 (x, y) = xy, see the survey articles [18,51] and the references therein. Existence of mass-conserving self-similar solutions for a large class of nongelling kernels have been constructed recently [29,31] and their properties studied in [11,26,32,60,65]. Still for non-gelling kernels, the existence of other self-similar solutions (with a different scaling and possibly infinite mass) is uncovered in [8] for the additive kernel K 1 (x, y) = x + y and in [62] for the constant kernel K 0 (x, y) = 2, both results relying on the use of the Laplace transform which maps (1.5) either to Burgers' equation or to an ordinary differential equation.…”
Section: Introductionmentioning
confidence: 99%
“…In fact, for other homogeneous coagulation kernels, the first difficulty encountered is the existence of the scaling profile g S which satisfies a nonlinear and nonlocal integro-differential equation. For a wide class of homogeneous coagulation kernels, such an existence result has been recently obtained in [9,11]. Still, the uniqueness of the profile (in a suitable class) and the convergence to self-similar solutions are open problems.…”
Section: Introductionmentioning
confidence: 97%