{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:2QVPTYQJHFXHGSYDYQHOJN7LMO","short_pith_number":"pith:2QVPTYQJ","schema_version":"1.0","canonical_sha256":"d42af9e209396e734b03c40ee4b7eb63a8f098bb28dc30d33c0bc5671d32b46f","source":{"kind":"arxiv","id":"2508.05711","version":1},"attestation_state":"computed","paper":{"title":"Thermodynamically consistent modelling and simulation of the moving contact line problem in non-isothermal compressible two-phase flows","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"physics.flu-dyn","authors_text":"Junkai Wang, Qiaolin He","submitted_at":"2025-08-07T07:51:06Z","abstract_excerpt":"According to the dynamic van der Waals theory, we propose a thermodynamically consistent model for non-isothermal compressible two-phase flows with contact line motion. In this model, fluid temperature is treated as a primary variable, characterized by the proposed temperature equation instead of being obtained from intermediate variables such as total energy density, internal energy density and entropy density. The hydrodynamic boundary conditions, which represent a generalization of the generalized Navier slip boundary condition in non-isothermal flows, are imposed on the proposed model. We "},"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":"2508.05711","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2025-08-07T07:51:06Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"6e982511cd47a92f2f58d5a7708279a49b468d842a7c521a2c2cbc406b453f6d","abstract_canon_sha256":"e80d6f17d5a7419881aa05fce309e0f752f1068d52a70898f14488375e7314fa"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:50:41.950341Z","signature_b64":"cBcATm+DupcL++9/11k69ui3/+CdmX139jkXv3z2S35TrYGvfAfIlWWdgAn5w9OXkYI+gZzgW9eJNzIMswc4AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d42af9e209396e734b03c40ee4b7eb63a8f098bb28dc30d33c0bc5671d32b46f","last_reissued_at":"2026-07-05T11:50:41.949836Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:50:41.949836Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Thermodynamically consistent modelling and simulation of the moving contact line problem in non-isothermal compressible two-phase flows","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"physics.flu-dyn","authors_text":"Junkai Wang, Qiaolin He","submitted_at":"2025-08-07T07:51:06Z","abstract_excerpt":"According to the dynamic van der Waals theory, we propose a thermodynamically consistent model for non-isothermal compressible two-phase flows with contact line motion. In this model, fluid temperature is treated as a primary variable, characterized by the proposed temperature equation instead of being obtained from intermediate variables such as total energy density, internal energy density and entropy density. The hydrodynamic boundary conditions, which represent a generalization of the generalized Navier slip boundary condition in non-isothermal flows, are imposed on the proposed model. We "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2508.05711","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2508.05711/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2508.05711","created_at":"2026-07-05T11:50:41.949900+00:00"},{"alias_kind":"arxiv_version","alias_value":"2508.05711v1","created_at":"2026-07-05T11:50:41.949900+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2508.05711","created_at":"2026-07-05T11:50:41.949900+00:00"},{"alias_kind":"pith_short_12","alias_value":"2QVPTYQJHFXH","created_at":"2026-07-05T11:50:41.949900+00:00"},{"alias_kind":"pith_short_16","alias_value":"2QVPTYQJHFXHGSYD","created_at":"2026-07-05T11:50:41.949900+00:00"},{"alias_kind":"pith_short_8","alias_value":"2QVPTYQJ","created_at":"2026-07-05T11:50:41.949900+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2508.05687","citing_title":"Risk Analysis Techniques for Governed LLM-based Multi-Agent Systems","ref_index":1,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/2QVPTYQJHFXHGSYDYQHOJN7LMO","json":"https://pith.science/pith/2QVPTYQJHFXHGSYDYQHOJN7LMO.json","graph_json":"https://pith.science/api/pith-number/2QVPTYQJHFXHGSYDYQHOJN7LMO/graph.json","events_json":"https://pith.science/api/pith-number/2QVPTYQJHFXHGSYDYQHOJN7LMO/events.json","paper":"https://pith.science/paper/2QVPTYQJ"},"agent_actions":{"view_html":"https://pith.science/pith/2QVPTYQJHFXHGSYDYQHOJN7LMO","download_json":"https://pith.science/pith/2QVPTYQJHFXHGSYDYQHOJN7LMO.json","view_paper":"https://pith.science/paper/2QVPTYQJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2508.05711&json=true","fetch_graph":"https://pith.science/api/pith-number/2QVPTYQJHFXHGSYDYQHOJN7LMO/graph.json","fetch_events":"https://pith.science/api/pith-number/2QVPTYQJHFXHGSYDYQHOJN7LMO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2QVPTYQJHFXHGSYDYQHOJN7LMO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2QVPTYQJHFXHGSYDYQHOJN7LMO/action/storage_attestation","attest_author":"https://pith.science/pith/2QVPTYQJHFXHGSYDYQHOJN7LMO/action/author_attestation","sign_citation":"https://pith.science/pith/2QVPTYQJHFXHGSYDYQHOJN7LMO/action/citation_signature","submit_replication":"https://pith.science/pith/2QVPTYQJHFXHGSYDYQHOJN7LMO/action/replication_record"}},"created_at":"2026-07-05T11:50:41.949900+00:00","updated_at":"2026-07-05T11:50:41.949900+00:00"}