{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:EX5EG6ANCB6FZ54N6OC4GPCDFD","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"ee1f8cae1da236ced09d517b0711110692a05bd69107a5c84eb8862fd895929f","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2026-08-06T09:21:31Z","title_canon_sha256":"9f37cd0336491561c9bf6cca251cd775b27132ce1493b5bb0061c361a899f512"},"schema_version":"1.0","source":{"id":"2608.05787","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2608.05787","created_at":"2026-08-07T00:52:45Z"},{"alias_kind":"arxiv_version","alias_value":"2608.05787v1","created_at":"2026-08-07T00:52:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2608.05787","created_at":"2026-08-07T00:52:45Z"},{"alias_kind":"pith_short_12","alias_value":"EX5EG6ANCB6F","created_at":"2026-08-07T00:52:45Z"},{"alias_kind":"pith_short_16","alias_value":"EX5EG6ANCB6FZ54N","created_at":"2026-08-07T00:52:45Z"},{"alias_kind":"pith_short_8","alias_value":"EX5EG6AN","created_at":"2026-08-07T00:52:45Z"}],"graph_snapshots":[{"event_id":"sha256:ccf51759be52e2647e172d4628fab08746f9c8e06a1edec93837a8ced9ffec41","target":"graph","created_at":"2026-08-07T00:52:45Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2608.05787/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Multiphase electrohydrodynamic (EHD) flows play a crucial role in various engineering applications. However, existing numerical studies on three-phase electrohydrodynamic systems predominantly rely on phenomenological models, often neglecting thermodynamic consistency and critical surface charge convection mechanisms. To address these fundamental gaps, this paper proposes a thermodynamically consistent three-phase EHD model derived strictly from the Onsager variational principle. This theoretical framework intrinsically guarantees thermodynamic consistency and accurately captures complex multi","authors_text":"Fang Xiong, Lei Wang, Xinyue Liu, Xu Qian","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2026-08-06T09:21:31Z","title":"Onsager-variational-principle-based Lattice Boltzmann Model For Three-phase Dielectric Fluid Flows"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2608.05787","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:0cffb617eb9f09495e1edb591e80c4487bac17091b406aebfe4b947086e4d81d","target":"record","created_at":"2026-08-07T00:52:45Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"ee1f8cae1da236ced09d517b0711110692a05bd69107a5c84eb8862fd895929f","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2026-08-06T09:21:31Z","title_canon_sha256":"9f37cd0336491561c9bf6cca251cd775b27132ce1493b5bb0061c361a899f512"},"schema_version":"1.0","source":{"id":"2608.05787","kind":"arxiv","version":1}},"canonical_sha256":"25fa43780d107c5cf78df385c33c4328c424fa86e63b35f2fc5e8479a24e827e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"25fa43780d107c5cf78df385c33c4328c424fa86e63b35f2fc5e8479a24e827e","first_computed_at":"2026-08-07T00:52:45.061847Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-08-07T00:52:45.061847Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"nrK5aMJ84YD7EFa+CNqZxLXBmn3fF7XPQ/LaqzgVLPJ53eUrqflkpEhj4o4F1j/jo128DmaEZ+4tnFXtLByVAg==","signature_status":"signed_v1","signed_at":"2026-08-07T00:52:45.063301Z","signed_message":"canonical_sha256_bytes"},"source_id":"2608.05787","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0cffb617eb9f09495e1edb591e80c4487bac17091b406aebfe4b947086e4d81d","sha256:ccf51759be52e2647e172d4628fab08746f9c8e06a1edec93837a8ced9ffec41"],"state_sha256":"8c6a2f11a794e8e8afb6838f1dad518931ca2da68f32abdfa222a2097f2d7de7"}