{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:VONVCQN4EMCUAI474M7QLPNBHB","short_pith_number":"pith:VONVCQN4","schema_version":"1.0","canonical_sha256":"ab9b5141bc230540239fe33f05bda1386c5e34be079082f6b6bc3f343dcd37fe","source":{"kind":"arxiv","id":"1601.06644","version":1},"attestation_state":"computed","paper":{"title":"Equation of motion of the triple contact line along an inhomogeneous surface","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.flu-dyn","authors_text":"D. Beysens (PMMH, SBT - UMR 9004), Vadim Nikolayev (SPEC - UMR3680","submitted_at":"2016-01-25T15:53:13Z","abstract_excerpt":"Wetting flows are controlled by the contact line motion. We derive an equation that describes the slow time evolution of the triple solid-liquid-fluid contact line for an arbitrary distribution of defects on a solid surface. The capillary rise along a partially wetted infinite vertical wall is considered. The contact line is assumed to be only slightly deformed by the defects. The derived equation is solved exactly for a simple example of a single defect. Introduction."},"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":"1601.06644","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2016-01-25T15:53:13Z","cross_cats_sorted":[],"title_canon_sha256":"567376637004f824149a8dbb41f50db203e2893d7d84ccc7fe29e4e9af9dfb85","abstract_canon_sha256":"d852fa66bd3439902eece59f25c3104b51388690193966e8f621b26e1928571b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:22:04.026480Z","signature_b64":"ntEpjaBUkS/t3Gen23a9UlgjOG2DU02vAEicyT0nQTZQ/GyyNCN2fLEJ8lC6cXIfa1not1vs4byGP2nzoMWpAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ab9b5141bc230540239fe33f05bda1386c5e34be079082f6b6bc3f343dcd37fe","last_reissued_at":"2026-05-18T01:22:04.025832Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:22:04.025832Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Equation of motion of the triple contact line along an inhomogeneous surface","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.flu-dyn","authors_text":"D. Beysens (PMMH, SBT - UMR 9004), Vadim Nikolayev (SPEC - UMR3680","submitted_at":"2016-01-25T15:53:13Z","abstract_excerpt":"Wetting flows are controlled by the contact line motion. We derive an equation that describes the slow time evolution of the triple solid-liquid-fluid contact line for an arbitrary distribution of defects on a solid surface. The capillary rise along a partially wetted infinite vertical wall is considered. The contact line is assumed to be only slightly deformed by the defects. The derived equation is solved exactly for a simple example of a single defect. Introduction."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1601.06644","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":"1601.06644","created_at":"2026-05-18T01:22:04.025919+00:00"},{"alias_kind":"arxiv_version","alias_value":"1601.06644v1","created_at":"2026-05-18T01:22:04.025919+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1601.06644","created_at":"2026-05-18T01:22:04.025919+00:00"},{"alias_kind":"pith_short_12","alias_value":"VONVCQN4EMCU","created_at":"2026-05-18T12:30:48.956258+00:00"},{"alias_kind":"pith_short_16","alias_value":"VONVCQN4EMCUAI47","created_at":"2026-05-18T12:30:48.956258+00:00"},{"alias_kind":"pith_short_8","alias_value":"VONVCQN4","created_at":"2026-05-18T12:30:48.956258+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/VONVCQN4EMCUAI474M7QLPNBHB","json":"https://pith.science/pith/VONVCQN4EMCUAI474M7QLPNBHB.json","graph_json":"https://pith.science/api/pith-number/VONVCQN4EMCUAI474M7QLPNBHB/graph.json","events_json":"https://pith.science/api/pith-number/VONVCQN4EMCUAI474M7QLPNBHB/events.json","paper":"https://pith.science/paper/VONVCQN4"},"agent_actions":{"view_html":"https://pith.science/pith/VONVCQN4EMCUAI474M7QLPNBHB","download_json":"https://pith.science/pith/VONVCQN4EMCUAI474M7QLPNBHB.json","view_paper":"https://pith.science/paper/VONVCQN4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1601.06644&json=true","fetch_graph":"https://pith.science/api/pith-number/VONVCQN4EMCUAI474M7QLPNBHB/graph.json","fetch_events":"https://pith.science/api/pith-number/VONVCQN4EMCUAI474M7QLPNBHB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VONVCQN4EMCUAI474M7QLPNBHB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VONVCQN4EMCUAI474M7QLPNBHB/action/storage_attestation","attest_author":"https://pith.science/pith/VONVCQN4EMCUAI474M7QLPNBHB/action/author_attestation","sign_citation":"https://pith.science/pith/VONVCQN4EMCUAI474M7QLPNBHB/action/citation_signature","submit_replication":"https://pith.science/pith/VONVCQN4EMCUAI474M7QLPNBHB/action/replication_record"}},"created_at":"2026-05-18T01:22:04.025919+00:00","updated_at":"2026-05-18T01:22:04.025919+00:00"}