{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:EUNAU7ZZ6FBHEK42OKDRVNCKWC","short_pith_number":"pith:EUNAU7ZZ","schema_version":"1.0","canonical_sha256":"251a0a7f39f142722b9a72871ab44ab0a344e057a36768713b492386a5107f8f","source":{"kind":"arxiv","id":"1708.06281","version":1},"attestation_state":"computed","paper":{"title":"Edge contact angle and modified Kelvin equation for condensation in open pores","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.soft","physics.chem-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Alexandr Malijevsk\\'y, Andrew O. Parry, Martin Posp\\'i\\v{s}il","submitted_at":"2017-08-21T15:19:58Z","abstract_excerpt":"We consider capillary condensation transitions occurring in open slits of width $L$ and finite height $H$ immersed in a reservoir of vapour. In this case the pressure at which condensation occurs is closer to saturation compared to that occurring in an infinite slit ($H=\\infty$) due to the presence of two menisci which are pinned near the open ends. Using macroscopic arguments we derive a modified Kelvin equation for the pressure, $p_{cc}(L;H)$, at which condensation occurs and show that the two menisci are characterised by an edge contact angle $\\theta_e$ which is always larger than the equil"},"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":"1708.06281","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-08-21T15:19:58Z","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.soft","physics.chem-ph"],"title_canon_sha256":"bd256ab92d59948ed5aad03a80773452ccf3cf061fb87dd66362659f62ccd43e","abstract_canon_sha256":"5d9902430fc9c6b59c3ccadba9dcfe421dba992030d4124447d7ff148a11a4f8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:37:42.751497Z","signature_b64":"u674l42wk+1QZQ32zVkccJwPGl+HXBxft+n10YhZlsCB2UMiRn4szmK+/Aj6WYQcY9tuewdF7rrnW3jL9BcKBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"251a0a7f39f142722b9a72871ab44ab0a344e057a36768713b492386a5107f8f","last_reissued_at":"2026-05-18T00:37:42.750708Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:37:42.750708Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Edge contact angle and modified Kelvin equation for condensation in open pores","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.soft","physics.chem-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Alexandr Malijevsk\\'y, Andrew O. Parry, Martin Posp\\'i\\v{s}il","submitted_at":"2017-08-21T15:19:58Z","abstract_excerpt":"We consider capillary condensation transitions occurring in open slits of width $L$ and finite height $H$ immersed in a reservoir of vapour. In this case the pressure at which condensation occurs is closer to saturation compared to that occurring in an infinite slit ($H=\\infty$) due to the presence of two menisci which are pinned near the open ends. Using macroscopic arguments we derive a modified Kelvin equation for the pressure, $p_{cc}(L;H)$, at which condensation occurs and show that the two menisci are characterised by an edge contact angle $\\theta_e$ which is always larger than the equil"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.06281","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":"1708.06281","created_at":"2026-05-18T00:37:42.750813+00:00"},{"alias_kind":"arxiv_version","alias_value":"1708.06281v1","created_at":"2026-05-18T00:37:42.750813+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.06281","created_at":"2026-05-18T00:37:42.750813+00:00"},{"alias_kind":"pith_short_12","alias_value":"EUNAU7ZZ6FBH","created_at":"2026-05-18T12:31:12.930513+00:00"},{"alias_kind":"pith_short_16","alias_value":"EUNAU7ZZ6FBHEK42","created_at":"2026-05-18T12:31:12.930513+00:00"},{"alias_kind":"pith_short_8","alias_value":"EUNAU7ZZ","created_at":"2026-05-18T12:31:12.930513+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/EUNAU7ZZ6FBHEK42OKDRVNCKWC","json":"https://pith.science/pith/EUNAU7ZZ6FBHEK42OKDRVNCKWC.json","graph_json":"https://pith.science/api/pith-number/EUNAU7ZZ6FBHEK42OKDRVNCKWC/graph.json","events_json":"https://pith.science/api/pith-number/EUNAU7ZZ6FBHEK42OKDRVNCKWC/events.json","paper":"https://pith.science/paper/EUNAU7ZZ"},"agent_actions":{"view_html":"https://pith.science/pith/EUNAU7ZZ6FBHEK42OKDRVNCKWC","download_json":"https://pith.science/pith/EUNAU7ZZ6FBHEK42OKDRVNCKWC.json","view_paper":"https://pith.science/paper/EUNAU7ZZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1708.06281&json=true","fetch_graph":"https://pith.science/api/pith-number/EUNAU7ZZ6FBHEK42OKDRVNCKWC/graph.json","fetch_events":"https://pith.science/api/pith-number/EUNAU7ZZ6FBHEK42OKDRVNCKWC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EUNAU7ZZ6FBHEK42OKDRVNCKWC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EUNAU7ZZ6FBHEK42OKDRVNCKWC/action/storage_attestation","attest_author":"https://pith.science/pith/EUNAU7ZZ6FBHEK42OKDRVNCKWC/action/author_attestation","sign_citation":"https://pith.science/pith/EUNAU7ZZ6FBHEK42OKDRVNCKWC/action/citation_signature","submit_replication":"https://pith.science/pith/EUNAU7ZZ6FBHEK42OKDRVNCKWC/action/replication_record"}},"created_at":"2026-05-18T00:37:42.750813+00:00","updated_at":"2026-05-18T00:37:42.750813+00:00"}