Matches in SemOpenAlex for { <https://semopenalex.org/work/W2162483424> ?p ?o ?g. }
- W2162483424 endingPage "2036" @default.
- W2162483424 startingPage "2012" @default.
- W2162483424 abstract "We propose a new spectral Lagrangian based deterministic solver for the non-linear Boltzmann transport equation (BTE) in d-dimensions for variable hard sphere (VHS) collision kernels with conservative or non-conservative binary interactions. The method is based on symmetries of the Fourier transform of the collision integral, where the complexity in its computation is reduced to a separate integral over the unit sphere Sd-1. The conservation of moments is enforced by Lagrangian constraints. The resulting scheme, implemented in free space, is very versatile and adjusts in a very simple manner to several cases that involve energy dissipation due to local micro-reversibility (inelastic interactions) or elastic models of slowing down process. Our simulations are benchmarked with available exact self-similar solutions, exact moment equations and analytical estimates for the homogeneous Boltzmann equation, both for elastic and inelastic VHS interactions. Benchmarking of the simulations involves the selection of a time self-similar rescaling of the numerical distribution function which is performed using the continuous spectrum of the equation for Maxwell molecules as studied first in Bobylev et al. [A.V. Bobylev, C. Cercignani, G. Toscani, Proof of an asymptotic property of self-similar solutions of the Boltzmann equation for granular materials, Journal of Statistical Physics 111 (2003) 403–417] and generalized to a wide range of related models in Bobylev et al. [A.V. Bobylev, C. Cercignani, I.M. Gamba, On the self-similar asymptotics for generalized non-linear kinetic Maxwell models, Communication in Mathematical Physics, in press. URL: <http://arxiv.org/abs/math-ph/0608035>]. The method also produces accurate results in the case of inelastic diffusive Boltzmann equations for hard spheres (inelastic collisions under thermal bath), where overpopulated non-Gaussian exponential tails have been conjectured in computations by stochastic methods [T.V. Noije, M. Ernst, Velocity distributions in homogeneously cooling and heated granular fluids, Granular Matter 1(57) (1998); M.H. Ernst, R. Brito, Scaling solutions of inelastic Boltzmann equations with over-populated high energy tails, Journal of Statistical Physics 109 (2002) 407–432; S.J. Moon, M.D. Shattuck, J. Swift, Velocity distributions and correlations in homogeneously heated granular media, Physical Review E 64 (2001) 031303; I.M. Gamba, S. Rjasanow, W. Wagner, Direct simulation of the uniformly heated granular Boltzmann equation, Mathematical and Computer Modelling 42 (2005) 683–700] and rigorously proven in Gamba et al. [I.M. Gamba, V. Panferov, C. Villani, On the Boltzmann equation for diffusively excited granular media, Communications in Mathematical Physics 246 (2004) 503–541(39)] and [A.V. Bobylev, I.M. Gamba, V. Panferov, Moment inequalities and high-energy tails for Boltzmann equations with inelastic interactions, Journal of Statistical Physics 116 (2004) 1651–1682]." @default.
- W2162483424 created "2016-06-24" @default.
- W2162483424 creator A5060670182 @default.
- W2162483424 creator A5087543049 @default.
- W2162483424 date "2009-04-01" @default.
- W2162483424 modified "2023-10-15" @default.
- W2162483424 title "Spectral-Lagrangian methods for collisional models of non-equilibrium statistical states" @default.
- W2162483424 cites W1484911079 @default.
- W2162483424 cites W1493709430 @default.
- W2162483424 cites W1532647343 @default.
- W2162483424 cites W1584425277 @default.
- W2162483424 cites W1588244485 @default.
- W2162483424 cites W1618995300 @default.
- W2162483424 cites W1646421803 @default.
- W2162483424 cites W1985860315 @default.
- W2162483424 cites W200524003 @default.
- W2162483424 cites W2008823806 @default.
- W2162483424 cites W2018049572 @default.
- W2162483424 cites W2031051349 @default.
- W2162483424 cites W2037850364 @default.
- W2162483424 cites W2040421729 @default.
- W2162483424 cites W2042306419 @default.
- W2162483424 cites W2042542512 @default.
- W2162483424 cites W2043953726 @default.
- W2162483424 cites W2044550158 @default.
- W2162483424 cites W2045278224 @default.
- W2162483424 cites W2051248608 @default.
- W2162483424 cites W2051358691 @default.
- W2162483424 cites W2064011954 @default.
- W2162483424 cites W2066790872 @default.
- W2162483424 cites W2067234929 @default.
- W2162483424 cites W2070716540 @default.
- W2162483424 cites W2080735958 @default.
- W2162483424 cites W2085927003 @default.
- W2162483424 cites W2086700458 @default.
- W2162483424 cites W2090621896 @default.
- W2162483424 cites W2094981671 @default.
- W2162483424 cites W2149570896 @default.
- W2162483424 cites W2167108735 @default.
- W2162483424 cites W3101662299 @default.
- W2162483424 cites W3102142367 @default.
- W2162483424 cites W3102616830 @default.
- W2162483424 cites W3122950674 @default.
- W2162483424 cites W4240562014 @default.
- W2162483424 doi "https://doi.org/10.1016/j.jcp.2008.09.033" @default.
- W2162483424 hasPublicationYear "2009" @default.
- W2162483424 type Work @default.
- W2162483424 sameAs 2162483424 @default.
- W2162483424 citedByCount "108" @default.
- W2162483424 countsByYear W21624834242012 @default.
- W2162483424 countsByYear W21624834242013 @default.
- W2162483424 countsByYear W21624834242014 @default.
- W2162483424 countsByYear W21624834242015 @default.
- W2162483424 countsByYear W21624834242016 @default.
- W2162483424 countsByYear W21624834242017 @default.
- W2162483424 countsByYear W21624834242018 @default.
- W2162483424 countsByYear W21624834242019 @default.
- W2162483424 countsByYear W21624834242020 @default.
- W2162483424 countsByYear W21624834242021 @default.
- W2162483424 countsByYear W21624834242022 @default.
- W2162483424 countsByYear W21624834242023 @default.
- W2162483424 crossrefType "journal-article" @default.
- W2162483424 hasAuthorship W2162483424A5060670182 @default.
- W2162483424 hasAuthorship W2162483424A5087543049 @default.
- W2162483424 hasBestOaLocation W21624834242 @default.
- W2162483424 hasConcept C121332964 @default.
- W2162483424 hasConcept C121864883 @default.
- W2162483424 hasConcept C126255220 @default.
- W2162483424 hasConcept C134306372 @default.
- W2162483424 hasConcept C165995430 @default.
- W2162483424 hasConcept C186603090 @default.
- W2162483424 hasConcept C27016315 @default.
- W2162483424 hasConcept C2778770139 @default.
- W2162483424 hasConcept C33923547 @default.
- W2162483424 hasConcept C62520636 @default.
- W2162483424 hasConcept C74650414 @default.
- W2162483424 hasConceptScore W2162483424C121332964 @default.
- W2162483424 hasConceptScore W2162483424C121864883 @default.
- W2162483424 hasConceptScore W2162483424C126255220 @default.
- W2162483424 hasConceptScore W2162483424C134306372 @default.
- W2162483424 hasConceptScore W2162483424C165995430 @default.
- W2162483424 hasConceptScore W2162483424C186603090 @default.
- W2162483424 hasConceptScore W2162483424C27016315 @default.
- W2162483424 hasConceptScore W2162483424C2778770139 @default.
- W2162483424 hasConceptScore W2162483424C33923547 @default.
- W2162483424 hasConceptScore W2162483424C62520636 @default.
- W2162483424 hasConceptScore W2162483424C74650414 @default.
- W2162483424 hasIssue "6" @default.
- W2162483424 hasLocation W21624834241 @default.
- W2162483424 hasLocation W21624834242 @default.
- W2162483424 hasLocation W21624834243 @default.
- W2162483424 hasOpenAccess W2162483424 @default.
- W2162483424 hasPrimaryLocation W21624834241 @default.
- W2162483424 hasRelatedWork W1982305278 @default.
- W2162483424 hasRelatedWork W1989208673 @default.
- W2162483424 hasRelatedWork W1996666735 @default.
- W2162483424 hasRelatedWork W2027536053 @default.
- W2162483424 hasRelatedWork W2031724134 @default.