Boltzmann kinetic equation for filtered fluid turbulence
We develop a kinetic Boltzmann equation for describing filtered fluid turbulence applicable for continuum and noncontinuum effects. The effect of unresolved turbulent motion on the resolved distribution function is elucidated and closure modeling issues of kinetic Boltzmann and Navier-Stokes descrip...
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Published in: | Physical review letters Vol. 99; no. 3; p. 034501 |
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Format: | Journal Article |
Language: | English |
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20-07-2007
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Abstract | We develop a kinetic Boltzmann equation for describing filtered fluid turbulence applicable for continuum and noncontinuum effects. The effect of unresolved turbulent motion on the resolved distribution function is elucidated and closure modeling issues of kinetic Boltzmann and Navier-Stokes descriptions are reconciled. This could pave the way for unifying turbulence modeling at kinetic and continuum levels and the development of numerical methods that are valid over a wide range of flow physics. |
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AbstractList | We develop a kinetic Boltzmann equation for describing filtered fluid turbulence applicable for continuum and noncontinuum effects. The effect of unresolved turbulent motion on the resolved distribution function is elucidated and closure modeling issues of kinetic Boltzmann and Navier-Stokes descriptions are reconciled. This could pave the way for unifying turbulence modeling at kinetic and continuum levels and the development of numerical methods that are valid over a wide range of flow physics. |
ArticleNumber | 034501 |
Author | Girimaji, Sharath S |
Author_xml | – sequence: 1 givenname: Sharath S surname: Girimaji fullname: Girimaji, Sharath S organization: Aerospace Engineering Department, Texas A&M University, College Station, Texas 77843, USA |
BackLink | https://www.ncbi.nlm.nih.gov/pubmed/17678288$$D View this record in MEDLINE/PubMed |
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CitedBy_id | crossref_primary_10_1063_5_0098032 crossref_primary_10_1088_0031_8949_2013_T155_014040 crossref_primary_10_1017_jfm_2021_955 crossref_primary_10_1115_1_4023323 crossref_primary_10_1016_j_ces_2019_115428 crossref_primary_10_1016_j_compfluid_2014_05_015 crossref_primary_10_1103_PhysRevE_84_046318 crossref_primary_10_1038_srep27172 crossref_primary_10_1016_j_jcp_2021_110571 crossref_primary_10_1103_PhysRevE_80_036702 crossref_primary_10_1016_j_camwa_2009_08_051 crossref_primary_10_1016_j_compfluid_2017_07_005 crossref_primary_10_1002_fld_5085 crossref_primary_10_1016_j_ces_2016_09_012 crossref_primary_10_1080_14685248_2018_1540879 crossref_primary_10_1063_1_2842379 crossref_primary_10_1063_5_0079461 crossref_primary_10_1063_1_5128379 crossref_primary_10_1016_j_jcp_2020_109713 crossref_primary_10_1016_j_compfluid_2017_10_023 crossref_primary_10_3390_atmos14071109 crossref_primary_10_4208_cicp_181210_090911a crossref_primary_10_1016_j_physleta_2009_01_058 crossref_primary_10_1103_PhysRevFluids_3_071402 crossref_primary_10_1007_s42102_022_00085_2 crossref_primary_10_1017_jfm_2012_155 crossref_primary_10_1063_5_0203934 |
Cites_doi | 10.1103/PhysRevE.59.R2527 10.1103/PhysRevLett.61.2332 10.1103/PhysRevA.45.R5339 10.1103/PhysRevE.71.016708 10.1016/S0376-0421(03)00003-4 10.1007/s00021-002-8545-8 10.1126/science.1085048 10.1016/j.physa.2004.02.013 10.1017/S0022112092001733 10.1023/A:1014570923357 10.1063/1.2140021 10.1016/0370-1573(92)90090-M 10.1098/rsta.1895.0004 10.1146/annurev.fluid.30.1.329 |
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References | S. Harris (PhysRevLett.99.034501Cc3R1) 2004 PhysRevLett.99.034501Cc15R1 PhysRevLett.99.034501Cc14R1 PhysRevLett.99.034501Cc13R1 PhysRevLett.99.034501Cc12R1 PhysRevLett.99.034501Cc11R1 PhysRevLett.99.034501Cc10R1 PhysRevLett.99.034501Cc9R1 PhysRevLett.99.034501Cc8R1 PhysRevLett.99.034501Cc7R1 PhysRevLett.99.034501Cc6R1 PhysRevLett.99.034501Cc5R1 PhysRevLett.99.034501Cc4R1 PhysRevLett.99.034501Cc2R1 PhysRevLett.99.034501Cc1R1 |
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