{"id":"W2043561882","doi":"10.1016/j.ijthermalsci.2010.05.022","title":"Double dispersion, natural convection in an open end cavity simulation via Lattice Boltzmann Method","year":2010,"lang":"en","type":"article","venue":"International Journal of Thermal Sciences","topic":"Lattice Boltzmann Simulation Studies","field":"Engineering","cited_by":55,"is_retracted":false,"has_abstract":false,"ca_institutions":"University of Calgary","funders":"","keywords":"Buoyancy; Prandtl number; Lewis number; Natural convection; Lattice Boltzmann methods; Mechanics; Rayleigh number; Materials science; Thermal; Thermodynamics; Physics; Convection; Mass transfer","routes":{"ca_aff":true,"ca_fund":false,"ca_venue":false,"about_ca":false,"invisible_to_affiliation_only":false},"retraction":null,"screen":null,"direct_labels":[],"prediction":{"model_version":"metacan-v3-hybrid-931329e0061c","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.000427574,0.0003168209,0.0008212505,0.0003475841,0.0009470671,0.001094596,0.001092669,0.001607424,0.002187907],"category_scores_gemma":[0.001654663,0.0003938768,0.0004273441,0.0003439513,0.001264364,0.0008165801,0.001131147,0.000972372,0.0001832652],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0006594691,"about_ca_system_score_gemma":0.00123299,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.01188757,"about_ca_topic_score_gemma":0.005660212,"domain_scores_codex":[0.9997975,0.00005351994,0.000007899545,0.00003195234,0.00006278436,0.00004634172],"domain_scores_gemma":[0.9993899,0.0003087381,0.00004891864,0.00005734438,0.0001060406,0.00008907849],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"simulation_or_modeling","study_design_gemma":"simulation_or_modeling","study_design_scores_codex":[0.00008599253,0.0000802823,0.0008241356,0.00002220968,0.00001259209,0.0000824198,0.00007003375,0.9888124,0.002546163,0.005821738,0.0001470659,0.00149498],"study_design_scores_gemma":[0.00001075494,0.000009883244,0.00007510625,0.000001514796,0.000001584982,0.000003586541,0.000008935445,0.9992583,0.0002353565,0.0003008315,0.00009055344,0.000003443394],"study_design_candidate":"simulation_or_modeling","study_design_consensus":"simulation_or_modeling","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.827019,0.0002399528,0.1452709,0.0004685524,0.0001750263,0.0001347932,0.0001823714,0.0003009298,0.02620844],"genre_scores_gemma":[0.9792413,0.0000434978,0.01609837,0.00006176739,0.00001661195,0.00009801782,0.00005573708,0.00004693264,0.004337866],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.01188757,"threshold_uncertainty_score":0.02363676,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.03538978054679235,"score_gpt":0.3744796657934015,"score_spread":0.3390898852466091,"validation_status":"score_only:v0-immature-baseline","note":"Baseline scores from an immature model (maturity gate not passed). Scores rank; they never assert a category."}}