{"id":"W1977420432","doi":"10.1016/j.ijheatmasstransfer.2015.03.062","title":"Effects of radiation on the uncertainty of flame speed determination using spherically propagating flames with CO/CO2/H2O dilutions at elevated pressures","year":2015,"lang":"en","type":"article","venue":"International Journal of Heat and Mass Transfer","topic":"Combustion and flame dynamics","field":"Engineering","cited_by":26,"is_retracted":false,"has_abstract":false,"ca_institutions":"","funders":"Basic Energy Sciences; Korea Institute of Energy Technology Evaluation and Planning; Ministry of Education, Science and Technology; Ministry of Trade, Industry and Energy; U.S. Department of Energy; National Research Foundation of Korea; Canadian Hemophilia Society","keywords":"Adiabatic process; Radiative transfer; Materials science; Flame speed; Radiation; Laminar flame speed; Speed of sound; Combustion; Thermal radiation; Mechanics; Adiabatic flame temperature; Laminar flow; Dilution; Flame structure; Physics; Diffusion flame; Optics; Thermodynamics; Chemistry; Combustor","routes":{"ca_aff":false,"ca_fund":true,"ca_venue":false,"about_ca":false,"invisible_to_affiliation_only":true},"retraction":null,"screen":null,"direct_labels":[],"prediction":{"model_version":"metacan-v3-hybrid-931329e0061c","candidate_categories":[],"consensus_categories":[],"category_scores_codex":[0.003810466,0.0005815729,0.0004542425,0.0004503388,0.0006793251,0.0009480444,0.0006912848,0.001052174,0.0004707614],"category_scores_gemma":[0.01232285,0.0003263798,0.0005174145,0.0006124927,0.001140121,0.0006472095,0.0005748703,0.0007750434,0.00009662859],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0008559537,"about_ca_system_score_gemma":0.0004996122,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.0030567,"about_ca_topic_score_gemma":0.001972436,"domain_scores_codex":[0.9971837,0.0008680077,0.0001870047,0.0005604671,0.001034406,0.0001663813],"domain_scores_gemma":[0.9833002,0.01314055,0.0008948691,0.001067439,0.001469482,0.0001274669],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"bench_or_experimental","study_design_gemma":"bench_or_experimental","study_design_scores_codex":[0.006012023,0.0001765421,0.02104332,0.0002787654,0.0001570444,0.0005493563,0.0007560314,0.04709376,0.9025565,0.001040924,0.0001290743,0.02020659],"study_design_scores_gemma":[0.00002857292,0.0004294057,0.009819849,0.0000137413,0.0000778038,0.0001368114,0.00008669739,0.03317484,0.9558231,0.0001254681,0.0002375109,0.00004626317],"study_design_candidate":"bench_or_experimental","study_design_consensus":"bench_or_experimental","genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9829353,0.0004137431,0.01551789,0.00007512364,0.00004216462,0.00002328689,0.00008773543,0.000130177,0.0007744781],"genre_scores_gemma":[0.9951689,0.0001027642,0.004445054,0.00001620447,0.000008659778,0.000009117731,0.00005153078,0.00003725489,0.0001605405],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.003810466,"threshold_uncertainty_score":0.02015191,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.01088684989317035,"score_gpt":0.2335753360554621,"score_spread":0.2226884861622918,"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."}}