{"id":"W1989450453","doi":"10.1002/1521-4001(200006)80:6<399::aid-zamm399>3.0.co;2-e","title":"The Spread of a Non-Newtonian Power Law Fluid under a Shallow Ambient Layer","year":2000,"lang":"en","type":"article","venue":"ZAMM ‐ Journal of Applied Mathematics and Mechanics / Zeitschrift für Angewandte Mathematik und Mechanik","topic":"Rheology and Fluid Dynamics Studies","field":"Chemical Engineering","cited_by":9,"is_retracted":false,"has_abstract":true,"ca_institutions":"University of Alberta","funders":"","keywords":"Newtonian fluid; Non-Newtonian fluid; Power-law fluid; Lubrication; Mechanics; Similarity solution; Constant (computer programming); Power law; Plane (geometry); Limiting; Layer (electronics); Generalized Newtonian fluid; Similarity (geometry); Lubrication theory; Inclined plane; Rheology; Physics; Classical mechanics; Materials science; Mathematics; Geometry; Thermodynamics; Boundary layer; Engineering; Computer science; Mechanical engineering; Composite material","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":[0.0002636078,0.0003779914,0.0005633426,0.0003857649,0.0003456556,0.0007051814,0.0004250936,0.0007732618,0.0008531664],"category_scores_gemma":[0.001410773,0.0002040681,0.0003570336,0.0001476193,0.0009263945,0.001252015,0.001174649,0.0005058108,0.0001319626],"about_ca_system_candidate":false,"about_ca_system_consensus":false,"about_ca_system_score_codex":0.0003783737,"about_ca_system_score_gemma":0.0003653979,"about_ca_topic_candidate":false,"about_ca_topic_consensus":false,"about_ca_topic_score_codex":0.00137071,"about_ca_topic_score_gemma":0.0005221905,"domain_scores_codex":[0.999864,0.00001821401,0.000005565226,0.00003002439,0.00003994719,0.00004227662],"domain_scores_gemma":[0.9996017,0.0001426278,0.00008796643,0.00003776227,0.00005154603,0.00007843073],"domain_codex":null,"domain_gemma":null,"domain_candidate":null,"domain_consensus":null,"study_design_codex":"bench_or_experimental","study_design_gemma":"simulation_or_modeling","study_design_scores_codex":[0.0005914912,0.0002235736,0.006052025,0.0002228972,0.00006823624,0.002979022,0.0009616922,0.2181661,0.7285427,0.02209744,0.0002244184,0.01987037],"study_design_scores_gemma":[0.0001720605,0.001475487,0.009903622,0.00002712311,0.00006929453,0.000913035,0.0007731795,0.8822875,0.09586976,0.007340008,0.001083873,0.00008500174],"study_design_candidate":"simulation_or_modeling","study_design_consensus":null,"genre_codex":"empirical","genre_gemma":"empirical","genre_scores_codex":[0.9730006,0.000225103,0.02540812,0.00006622112,0.00001568526,0.00002361317,0.000009469454,0.00004598549,0.001205169],"genre_scores_gemma":[0.9967276,0.0001169476,0.002022725,0.0000157544,0.000009981232,0.000006393888,0.000009634185,0.000007502867,0.001083351],"genre_candidate":"empirical","genre_consensus":"empirical","teacher_disagreement_score":0.00137071,"threshold_uncertainty_score":0.002854168,"prediction_status":"machine_predicted_unvalidated"},"machine_scores":{"provisional":true,"baseline":true,"maturity_gate_passed":false,"score_opus":0.00895052340684122,"score_gpt":0.24096542928216,"score_spread":0.2320149058753188,"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."}}