{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2025:6BMVLVIMBELELVDR2LQ26IAIRP","short_pith_number":"pith:6BMVLVIM","canonical_record":{"source":{"id":"2506.02270","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2025-06-02T21:29:44Z","cross_cats_sorted":["physics.comp-ph"],"title_canon_sha256":"e9c6bbfdf75b95ab881f340253a9e6d3097f8cef627e0ad3e09d2d0cd56dac85","abstract_canon_sha256":"4a517ca31fd66d2ae35aa849550f6489f0e381d35b76bfae3126860f6a2efc08"},"schema_version":"1.0"},"canonical_sha256":"f05955d50c091645d471d2e1af20088bf397ad387a4e635481df8ce98cd11418","source":{"kind":"arxiv","id":"2506.02270","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2506.02270","created_at":"2026-07-05T11:14:35Z"},{"alias_kind":"arxiv_version","alias_value":"2506.02270v1","created_at":"2026-07-05T11:14:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2506.02270","created_at":"2026-07-05T11:14:35Z"},{"alias_kind":"pith_short_12","alias_value":"6BMVLVIMBELE","created_at":"2026-07-05T11:14:35Z"},{"alias_kind":"pith_short_16","alias_value":"6BMVLVIMBELELVDR","created_at":"2026-07-05T11:14:35Z"},{"alias_kind":"pith_short_8","alias_value":"6BMVLVIM","created_at":"2026-07-05T11:14:35Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2025:6BMVLVIMBELELVDR2LQ26IAIRP","target":"record","payload":{"canonical_record":{"source":{"id":"2506.02270","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2025-06-02T21:29:44Z","cross_cats_sorted":["physics.comp-ph"],"title_canon_sha256":"e9c6bbfdf75b95ab881f340253a9e6d3097f8cef627e0ad3e09d2d0cd56dac85","abstract_canon_sha256":"4a517ca31fd66d2ae35aa849550f6489f0e381d35b76bfae3126860f6a2efc08"},"schema_version":"1.0"},"canonical_sha256":"f05955d50c091645d471d2e1af20088bf397ad387a4e635481df8ce98cd11418","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:14:35.623652Z","signature_b64":"nmEv445XbqzRVE24VdYV1VMSbDkEYCPTmhkYajZKr3oiTQyriKpkkJcAIKY4JqyQTRPyUbFgoo1mtwsylZUTCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f05955d50c091645d471d2e1af20088bf397ad387a4e635481df8ce98cd11418","last_reissued_at":"2026-07-05T11:14:35.623153Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:14:35.623153Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2506.02270","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T11:14:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DWW26/Az+RVxoqi5VlInWS00o4Xc2df54daThG/c0f/bPt7q4xPLZFkMOjEnAVaWnQBnM9agmzjI/Euvwqs0Bg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-08T12:49:08.441298Z"},"content_sha256":"2044d063f415de600850066dcfabdeb5f8c967bd4fdb9cf9ee9c47f0769b3775","schema_version":"1.0","event_id":"sha256:2044d063f415de600850066dcfabdeb5f8c967bd4fdb9cf9ee9c47f0769b3775"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2025:6BMVLVIMBELELVDR2LQ26IAIRP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Analytical solution for dynamic evaporation of liquid in isothermal condition","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["physics.comp-ph"],"primary_cat":"physics.flu-dyn","authors_text":"Alexander J. Wagner, Luiz Eduardo Czelusniak, Mathias J. Krause, Stephan Simonis, Tim Niklas Bingert","submitted_at":"2025-06-02T21:29:44Z","abstract_excerpt":"An analytical solution based on a diffuse interface model is presented for an isothermal evaporation problem under sub-saturation pressure. The macroscopic equations are derived from the free-energy method, widely recognized in the lattice Boltzmann literature, distinguishing our approach from conventional evaporation models that rely on jump conditions or pure kinetic theory. The interface behavior is fully described by differential equations, eliminating the need for assumptions such as local equilibrium at the interface. We derive an exact analytical solution for the inviscid case and propo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2506.02270","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2506.02270/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T11:14:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6OkSexghLvajiNkau/kpOFsCqINkrMz2tFNQGvMOFzQ8oP6bPPYrOEsZDY5ZuAv+J7qIiUaXLPINic3cR6F/DA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-08T12:49:08.441793Z"},"content_sha256":"eb237278ba166136ab4516a4093e7c120d94fe22cc518b2524aa836c876db585","schema_version":"1.0","event_id":"sha256:eb237278ba166136ab4516a4093e7c120d94fe22cc518b2524aa836c876db585"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6BMVLVIMBELELVDR2LQ26IAIRP/bundle.json","state_url":"https://pith.science/pith/6BMVLVIMBELELVDR2LQ26IAIRP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6BMVLVIMBELELVDR2LQ26IAIRP/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-08-08T12:49:08Z","links":{"resolver":"https://pith.science/pith/6BMVLVIMBELELVDR2LQ26IAIRP","bundle":"https://pith.science/pith/6BMVLVIMBELELVDR2LQ26IAIRP/bundle.json","state":"https://pith.science/pith/6BMVLVIMBELELVDR2LQ26IAIRP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6BMVLVIMBELELVDR2LQ26IAIRP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:6BMVLVIMBELELVDR2LQ26IAIRP","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":"4a517ca31fd66d2ae35aa849550f6489f0e381d35b76bfae3126860f6a2efc08","cross_cats_sorted":["physics.comp-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2025-06-02T21:29:44Z","title_canon_sha256":"e9c6bbfdf75b95ab881f340253a9e6d3097f8cef627e0ad3e09d2d0cd56dac85"},"schema_version":"1.0","source":{"id":"2506.02270","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2506.02270","created_at":"2026-07-05T11:14:35Z"},{"alias_kind":"arxiv_version","alias_value":"2506.02270v1","created_at":"2026-07-05T11:14:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2506.02270","created_at":"2026-07-05T11:14:35Z"},{"alias_kind":"pith_short_12","alias_value":"6BMVLVIMBELE","created_at":"2026-07-05T11:14:35Z"},{"alias_kind":"pith_short_16","alias_value":"6BMVLVIMBELELVDR","created_at":"2026-07-05T11:14:35Z"},{"alias_kind":"pith_short_8","alias_value":"6BMVLVIM","created_at":"2026-07-05T11:14:35Z"}],"graph_snapshots":[{"event_id":"sha256:eb237278ba166136ab4516a4093e7c120d94fe22cc518b2524aa836c876db585","target":"graph","created_at":"2026-07-05T11:14:35Z","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/2506.02270/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"An analytical solution based on a diffuse interface model is presented for an isothermal evaporation problem under sub-saturation pressure. The macroscopic equations are derived from the free-energy method, widely recognized in the lattice Boltzmann literature, distinguishing our approach from conventional evaporation models that rely on jump conditions or pure kinetic theory. The interface behavior is fully described by differential equations, eliminating the need for assumptions such as local equilibrium at the interface. We derive an exact analytical solution for the inviscid case and propo","authors_text":"Alexander J. Wagner, Luiz Eduardo Czelusniak, Mathias J. Krause, Stephan Simonis, Tim Niklas Bingert","cross_cats":["physics.comp-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2025-06-02T21:29:44Z","title":"Analytical solution for dynamic evaporation of liquid in isothermal condition"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2506.02270","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":"sha256:2044d063f415de600850066dcfabdeb5f8c967bd4fdb9cf9ee9c47f0769b3775","target":"record","created_at":"2026-07-05T11:14:35Z","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":"4a517ca31fd66d2ae35aa849550f6489f0e381d35b76bfae3126860f6a2efc08","cross_cats_sorted":["physics.comp-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.flu-dyn","submitted_at":"2025-06-02T21:29:44Z","title_canon_sha256":"e9c6bbfdf75b95ab881f340253a9e6d3097f8cef627e0ad3e09d2d0cd56dac85"},"schema_version":"1.0","source":{"id":"2506.02270","kind":"arxiv","version":1}},"canonical_sha256":"f05955d50c091645d471d2e1af20088bf397ad387a4e635481df8ce98cd11418","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f05955d50c091645d471d2e1af20088bf397ad387a4e635481df8ce98cd11418","first_computed_at":"2026-07-05T11:14:35.623153Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:14:35.623153Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"nmEv445XbqzRVE24VdYV1VMSbDkEYCPTmhkYajZKr3oiTQyriKpkkJcAIKY4JqyQTRPyUbFgoo1mtwsylZUTCQ==","signature_status":"signed_v1","signed_at":"2026-07-05T11:14:35.623652Z","signed_message":"canonical_sha256_bytes"},"source_id":"2506.02270","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2044d063f415de600850066dcfabdeb5f8c967bd4fdb9cf9ee9c47f0769b3775","sha256:eb237278ba166136ab4516a4093e7c120d94fe22cc518b2524aa836c876db585"],"state_sha256":"d298665e6b3be69bb389c2633aff87a3b57aa73989006ae51d823e99bf233d1d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AQ/Y1JQVvhi8jNcoLH3qwKwZmfqGdixP3QSeY/KVSl8isivmvNAHbWlfD2wxkwLfnQsqrdNHBOKZ6zP3mGKhCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-08T12:49:08.446366Z","bundle_sha256":"c5135fa9cd53251f93490d7f26525df238102d9a4584dda62ff9b2200c4b901c"}}