{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2002:C3LLJ3G36KGD6LEPTAUOMHWL3A","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":"d0fdbb6d4e883bd6671e05b00aabf042e82a4ada7aa652f2024d33b0edb64209","cross_cats_sorted":["physics.comp-ph","physics.flu-dyn"],"license":"","primary_cat":"cond-mat.soft","submitted_at":"2002-10-24T03:11:18Z","title_canon_sha256":"44e8700344c14ce1eef142c7c968da619f26e58f92fc9aeb3569d825bd19aa19"},"schema_version":"1.0","source":{"id":"cond-mat/0210534","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0210534","created_at":"2026-07-04T16:33:15Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0210534v2","created_at":"2026-07-04T16:33:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0210534","created_at":"2026-07-04T16:33:15Z"},{"alias_kind":"pith_short_12","alias_value":"C3LLJ3G36KGD","created_at":"2026-07-04T16:33:15Z"},{"alias_kind":"pith_short_16","alias_value":"C3LLJ3G36KGD6LEP","created_at":"2026-07-04T16:33:15Z"},{"alias_kind":"pith_short_8","alias_value":"C3LLJ3G3","created_at":"2026-07-04T16:33:15Z"}],"graph_snapshots":[{"event_id":"sha256:38f719b35f5927cd7b7c9dfd1c53f910340e09e10db834491f627b48e342220d","target":"graph","created_at":"2026-07-04T16:33:15Z","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/cond-mat/0210534/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"From extensive molecular dynamics simulations on immiscible two-phase flows, we find the relative slipping between the fluids and the solid wall everywhere to follow the generalized Navier boundary condition, in which the amount of slipping is proportional to the sum of tangential viscous stress and the uncompensated Young stress. The latter arises from the deviation of the fluid-fluid interface from its static configuration. We give a continuum formulation of the immiscible flow hydrodynamics, comprising the generalized Navier boundary condition, the Navier-Stokes equation, and the Cahn-Hilli","authors_text":"Ping Sheng, Tiezheng Qian, Xiao-Ping Wang","cross_cats":["physics.comp-ph","physics.flu-dyn"],"headline":"","license":"","primary_cat":"cond-mat.soft","submitted_at":"2002-10-24T03:11:18Z","title":"Molecular scale contact line hydrodynamics of immiscible flows"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0210534","kind":"arxiv","version":2},"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:d0fdc14eae180453eca743afa5bbc6b9960d26595d45e914adf01d2be1703f2d","target":"record","created_at":"2026-07-04T16:33:15Z","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":"d0fdbb6d4e883bd6671e05b00aabf042e82a4ada7aa652f2024d33b0edb64209","cross_cats_sorted":["physics.comp-ph","physics.flu-dyn"],"license":"","primary_cat":"cond-mat.soft","submitted_at":"2002-10-24T03:11:18Z","title_canon_sha256":"44e8700344c14ce1eef142c7c968da619f26e58f92fc9aeb3569d825bd19aa19"},"schema_version":"1.0","source":{"id":"cond-mat/0210534","kind":"arxiv","version":2}},"canonical_sha256":"16d6b4ecdbf28c3f2c8f9828e61ecbd804a0f82df449fdb7a5c13309144c2027","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"16d6b4ecdbf28c3f2c8f9828e61ecbd804a0f82df449fdb7a5c13309144c2027","first_computed_at":"2026-07-04T16:33:15.601676Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:33:15.601676Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"UTAh7Mld+lejhyldRRYFG2b63psbJrHA0xjxfjIpLXiIybXdhUsWHW+ihXZdL98tz4AWjv6iD44CoAE0FN+zCw==","signature_status":"signed_v1","signed_at":"2026-07-04T16:33:15.602041Z","signed_message":"canonical_sha256_bytes"},"source_id":"cond-mat/0210534","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d0fdc14eae180453eca743afa5bbc6b9960d26595d45e914adf01d2be1703f2d","sha256:38f719b35f5927cd7b7c9dfd1c53f910340e09e10db834491f627b48e342220d"],"state_sha256":"7a1e7eb4e316d5bd0b758686ae03a3b46336549cbc7ac68be1d5045a880dd27a"}