{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:5TWE2WNQMIHRYXZQN6S6SPYZXG","short_pith_number":"pith:5TWE2WNQ","schema_version":"1.0","canonical_sha256":"ecec4d59b0620f1c5f306fa5e93f19b997007748e2899606cf41fbd1065adab0","source":{"kind":"arxiv","id":"1604.06926","version":1},"attestation_state":"computed","paper":{"title":"A numerical study of the transition to oscillatory flow in 3D lid-driven cubic cavity flows","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.flu-dyn","authors_text":"Aixia Guo, Jiwen He, Roland Glowinski, Shang-Huan Chiu, Tsorng-Whay Pan","submitted_at":"2016-04-23T16:47:08Z","abstract_excerpt":"In this article, three dimensional (3D) lid-driven cubic cavity flows have been studied numerically for various values of Reynolds number ($Re$). The numerical solution of the Navier-Stokes equations modeling incompressible viscous fluid flow in a cubic cavity is obtained via a methodology combining a first order accurate operator-splitting, $L^2$-projection Stokes solver, a wave-like equation treatment of the advection and finite element methods. The numerical results obtained for Re$=$400, 1000, and 3200 show a good agreement with available numerical and experimental results in literature. S"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1604.06926","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2016-04-23T16:47:08Z","cross_cats_sorted":[],"title_canon_sha256":"6d667fdefecb0904b5acc3f9c71a4452748647ce8e39826e5400aaa5122ab4e8","abstract_canon_sha256":"d5acdb455987be564cd5bf60b863cad8141c69f43c9e4322b88a01aa6f1986ed"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:16:23.578911Z","signature_b64":"LylHLB1SzBcb9Sme8AoTri+Yh8ucEMvb3OILiBwpb0RLRGJeaJfhWTdxRHHxhcUD0/rkFY/YpkX7jOCOdODfDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ecec4d59b0620f1c5f306fa5e93f19b997007748e2899606cf41fbd1065adab0","last_reissued_at":"2026-05-18T01:16:23.578326Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:16:23.578326Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A numerical study of the transition to oscillatory flow in 3D lid-driven cubic cavity flows","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.flu-dyn","authors_text":"Aixia Guo, Jiwen He, Roland Glowinski, Shang-Huan Chiu, Tsorng-Whay Pan","submitted_at":"2016-04-23T16:47:08Z","abstract_excerpt":"In this article, three dimensional (3D) lid-driven cubic cavity flows have been studied numerically for various values of Reynolds number ($Re$). The numerical solution of the Navier-Stokes equations modeling incompressible viscous fluid flow in a cubic cavity is obtained via a methodology combining a first order accurate operator-splitting, $L^2$-projection Stokes solver, a wave-like equation treatment of the advection and finite element methods. The numerical results obtained for Re$=$400, 1000, and 3200 show a good agreement with available numerical and experimental results in literature. S"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.06926","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"1604.06926","created_at":"2026-05-18T01:16:23.578407+00:00"},{"alias_kind":"arxiv_version","alias_value":"1604.06926v1","created_at":"2026-05-18T01:16:23.578407+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.06926","created_at":"2026-05-18T01:16:23.578407+00:00"},{"alias_kind":"pith_short_12","alias_value":"5TWE2WNQMIHR","created_at":"2026-05-18T12:30:01.593930+00:00"},{"alias_kind":"pith_short_16","alias_value":"5TWE2WNQMIHRYXZQ","created_at":"2026-05-18T12:30:01.593930+00:00"},{"alias_kind":"pith_short_8","alias_value":"5TWE2WNQ","created_at":"2026-05-18T12:30:01.593930+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5TWE2WNQMIHRYXZQN6S6SPYZXG","json":"https://pith.science/pith/5TWE2WNQMIHRYXZQN6S6SPYZXG.json","graph_json":"https://pith.science/api/pith-number/5TWE2WNQMIHRYXZQN6S6SPYZXG/graph.json","events_json":"https://pith.science/api/pith-number/5TWE2WNQMIHRYXZQN6S6SPYZXG/events.json","paper":"https://pith.science/paper/5TWE2WNQ"},"agent_actions":{"view_html":"https://pith.science/pith/5TWE2WNQMIHRYXZQN6S6SPYZXG","download_json":"https://pith.science/pith/5TWE2WNQMIHRYXZQN6S6SPYZXG.json","view_paper":"https://pith.science/paper/5TWE2WNQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1604.06926&json=true","fetch_graph":"https://pith.science/api/pith-number/5TWE2WNQMIHRYXZQN6S6SPYZXG/graph.json","fetch_events":"https://pith.science/api/pith-number/5TWE2WNQMIHRYXZQN6S6SPYZXG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5TWE2WNQMIHRYXZQN6S6SPYZXG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5TWE2WNQMIHRYXZQN6S6SPYZXG/action/storage_attestation","attest_author":"https://pith.science/pith/5TWE2WNQMIHRYXZQN6S6SPYZXG/action/author_attestation","sign_citation":"https://pith.science/pith/5TWE2WNQMIHRYXZQN6S6SPYZXG/action/citation_signature","submit_replication":"https://pith.science/pith/5TWE2WNQMIHRYXZQN6S6SPYZXG/action/replication_record"}},"created_at":"2026-05-18T01:16:23.578407+00:00","updated_at":"2026-05-18T01:16:23.578407+00:00"}