{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:3X3W5ENDW5ICUQKR6FEXWGX3P4","short_pith_number":"pith:3X3W5END","schema_version":"1.0","canonical_sha256":"ddf76e91a3b7502a4151f1497b1afb7f142977f130dad695b081159dfb8d2b62","source":{"kind":"arxiv","id":"0910.2580","version":1},"attestation_state":"computed","paper":{"title":"A Numerical Simulation of a Plunging Breaking Wave","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.ao-ph","physics.comp-ph"],"primary_cat":"physics.flu-dyn","authors_text":"Douglas Dommermuth, Kevin George, Kyle A. Brucker, Mike Stephens, Paul Adams, Thomas O'Shea","submitted_at":"2009-10-14T19:21:12Z","abstract_excerpt":"This article describes the fluid dynamics video, \"A Numerical Simulation of a Plunging Breaking Wave\", which was submitted to the gallery of fluid motion at the 2009 APS/DFD conference. The simulation was of a deep-water plunging breaking wave. It was a two-phase calculation which used a Volume of Fluid (VOF) method to simulate the interface between the two immiscible fluids. Surface tension and viscous effects were not considered. The initial wave was generated by applying a spatio-temporal pressure forcing on the free surface. The video shows the 50% isocontour of the volume fraction from se"},"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":"0910.2580","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2009-10-14T19:21:12Z","cross_cats_sorted":["physics.ao-ph","physics.comp-ph"],"title_canon_sha256":"5fea5fc75bee241b434d9d8a64fa0fcd5ed92880027897a6385ecfc5dfc1d629","abstract_canon_sha256":"336381aabc8dc85df425515488c37c645c562560598dd90fa5a6adfc54e160b2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:11:23.770481Z","signature_b64":"qRIYNrcNLAVBuDL1uG/kh+bJpbvxB1/GdgGfqbInExXN0aiIYRqb+IwVUDLkuApw3ZiTi1k6XwYHJYOVcDVYBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ddf76e91a3b7502a4151f1497b1afb7f142977f130dad695b081159dfb8d2b62","last_reissued_at":"2026-05-18T02:11:23.769677Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:11:23.769677Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A Numerical Simulation of a Plunging Breaking Wave","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.ao-ph","physics.comp-ph"],"primary_cat":"physics.flu-dyn","authors_text":"Douglas Dommermuth, Kevin George, Kyle A. Brucker, Mike Stephens, Paul Adams, Thomas O'Shea","submitted_at":"2009-10-14T19:21:12Z","abstract_excerpt":"This article describes the fluid dynamics video, \"A Numerical Simulation of a Plunging Breaking Wave\", which was submitted to the gallery of fluid motion at the 2009 APS/DFD conference. The simulation was of a deep-water plunging breaking wave. It was a two-phase calculation which used a Volume of Fluid (VOF) method to simulate the interface between the two immiscible fluids. Surface tension and viscous effects were not considered. The initial wave was generated by applying a spatio-temporal pressure forcing on the free surface. The video shows the 50% isocontour of the volume fraction from se"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0910.2580","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":"0910.2580","created_at":"2026-05-18T02:11:23.769810+00:00"},{"alias_kind":"arxiv_version","alias_value":"0910.2580v1","created_at":"2026-05-18T02:11:23.769810+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0910.2580","created_at":"2026-05-18T02:11:23.769810+00:00"},{"alias_kind":"pith_short_12","alias_value":"3X3W5ENDW5IC","created_at":"2026-05-18T12:25:58.018023+00:00"},{"alias_kind":"pith_short_16","alias_value":"3X3W5ENDW5ICUQKR","created_at":"2026-05-18T12:25:58.018023+00:00"},{"alias_kind":"pith_short_8","alias_value":"3X3W5END","created_at":"2026-05-18T12:25:58.018023+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/3X3W5ENDW5ICUQKR6FEXWGX3P4","json":"https://pith.science/pith/3X3W5ENDW5ICUQKR6FEXWGX3P4.json","graph_json":"https://pith.science/api/pith-number/3X3W5ENDW5ICUQKR6FEXWGX3P4/graph.json","events_json":"https://pith.science/api/pith-number/3X3W5ENDW5ICUQKR6FEXWGX3P4/events.json","paper":"https://pith.science/paper/3X3W5END"},"agent_actions":{"view_html":"https://pith.science/pith/3X3W5ENDW5ICUQKR6FEXWGX3P4","download_json":"https://pith.science/pith/3X3W5ENDW5ICUQKR6FEXWGX3P4.json","view_paper":"https://pith.science/paper/3X3W5END","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0910.2580&json=true","fetch_graph":"https://pith.science/api/pith-number/3X3W5ENDW5ICUQKR6FEXWGX3P4/graph.json","fetch_events":"https://pith.science/api/pith-number/3X3W5ENDW5ICUQKR6FEXWGX3P4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3X3W5ENDW5ICUQKR6FEXWGX3P4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3X3W5ENDW5ICUQKR6FEXWGX3P4/action/storage_attestation","attest_author":"https://pith.science/pith/3X3W5ENDW5ICUQKR6FEXWGX3P4/action/author_attestation","sign_citation":"https://pith.science/pith/3X3W5ENDW5ICUQKR6FEXWGX3P4/action/citation_signature","submit_replication":"https://pith.science/pith/3X3W5ENDW5ICUQKR6FEXWGX3P4/action/replication_record"}},"created_at":"2026-05-18T02:11:23.769810+00:00","updated_at":"2026-05-18T02:11:23.769810+00:00"}