{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:CECYB3SQ2RR5YKY7GFKHPDN443","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":"589afed7c09ecf8676be3e93d85b3d9800e186e1c29017bfa223e06689940c06","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2024-10-22T14:48:49Z","title_canon_sha256":"249b929af42eaf685d5570a838a2834f04dba845b73e92366d00c57c36bbba23"},"schema_version":"1.0","source":{"id":"2410.17071","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2410.17071","created_at":"2026-07-05T11:26:24Z"},{"alias_kind":"arxiv_version","alias_value":"2410.17071v2","created_at":"2026-07-05T11:26:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2410.17071","created_at":"2026-07-05T11:26:24Z"},{"alias_kind":"pith_short_12","alias_value":"CECYB3SQ2RR5","created_at":"2026-07-05T11:26:24Z"},{"alias_kind":"pith_short_16","alias_value":"CECYB3SQ2RR5YKY7","created_at":"2026-07-05T11:26:24Z"},{"alias_kind":"pith_short_8","alias_value":"CECYB3SQ","created_at":"2026-07-05T11:26:24Z"}],"graph_snapshots":[{"event_id":"sha256:ac9f132869414716237589f07e71501c8848d52b6e9d4fabe02df1c7bdb1fdf3","target":"graph","created_at":"2026-07-05T11:26:24Z","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/2410.17071/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"When an evaporating water droplet is deposited on a thermally conductive substrate, the minimum temperature will be at the apex due to evaporative cooling. Consequently, density and surface tension gradients emerge within the droplet and at the droplet-gas interface, giving rise to competing flows from, respectively, the apex towards the contact line (thermal-buoyancy-driven flow) and the other way around (thermal Marangoni flow). In small droplets with a diameter below the capillary length, the thermal Marangoni effects are expected to dominate over thermal buoyancy (\"thermal Rayleigh\") effec","authors_text":"Alvaro Marin, Christian Diddens, Detlef Lohse, Duarte Rocha, Philip L. Lederer, Pim J. Dekker","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2024-10-22T14:48:49Z","title":"Evaporating sessile droplets: solutal Marangoni effects overwhelm thermal Marangoni flow"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2410.17071","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:f1134619f15782056f0664bfdad93a1098d1da3afae88fc908a7e234a0b1e87f","target":"record","created_at":"2026-07-05T11:26:24Z","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":"589afed7c09ecf8676be3e93d85b3d9800e186e1c29017bfa223e06689940c06","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2024-10-22T14:48:49Z","title_canon_sha256":"249b929af42eaf685d5570a838a2834f04dba845b73e92366d00c57c36bbba23"},"schema_version":"1.0","source":{"id":"2410.17071","kind":"arxiv","version":2}},"canonical_sha256":"110580ee50d463dc2b1f3154778dbce6e16137ef910bb94bc7da8369f04ceae3","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"110580ee50d463dc2b1f3154778dbce6e16137ef910bb94bc7da8369f04ceae3","first_computed_at":"2026-07-05T11:26:24.241713Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:26:24.241713Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"LtKTbsr65kLO8h6wCtRqOGWkwNf/C5TiebPVik7HtF5ywq7je4zFoM3Ti7BuUzXscdRka/wkzuR+4VrC6LIbAg==","signature_status":"signed_v1","signed_at":"2026-07-05T11:26:24.242473Z","signed_message":"canonical_sha256_bytes"},"source_id":"2410.17071","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f1134619f15782056f0664bfdad93a1098d1da3afae88fc908a7e234a0b1e87f","sha256:ac9f132869414716237589f07e71501c8848d52b6e9d4fabe02df1c7bdb1fdf3"],"state_sha256":"879b51fb1ba355c1ea424978aa3ba1746b8c0de8e2fe8c0967c0f72715aae15a"}