{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:NNBRACP7YWBIRSJKJ27RBHKJJG","short_pith_number":"pith:NNBRACP7","canonical_record":{"source":{"id":"1403.3240","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2014-03-13T11:38:08Z","cross_cats_sorted":[],"title_canon_sha256":"06700bfea9e7217f6ad9e049e5036b1aab12f889d5bacbf9bfbb7df3592235e4","abstract_canon_sha256":"395437fd45f1c5d228a5f5366f2848de3b8fd2522da06a4a9d62f889b67790a6"},"schema_version":"1.0"},"canonical_sha256":"6b431009ffc58288c92a4ebf109d4949926d30b4e8b709ec2edc73322bac07e4","source":{"kind":"arxiv","id":"1403.3240","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1403.3240","created_at":"2026-05-18T02:56:22Z"},{"alias_kind":"arxiv_version","alias_value":"1403.3240v1","created_at":"2026-05-18T02:56:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1403.3240","created_at":"2026-05-18T02:56:22Z"},{"alias_kind":"pith_short_12","alias_value":"NNBRACP7YWBI","created_at":"2026-05-18T12:28:41Z"},{"alias_kind":"pith_short_16","alias_value":"NNBRACP7YWBIRSJK","created_at":"2026-05-18T12:28:41Z"},{"alias_kind":"pith_short_8","alias_value":"NNBRACP7","created_at":"2026-05-18T12:28:41Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:NNBRACP7YWBIRSJKJ27RBHKJJG","target":"record","payload":{"canonical_record":{"source":{"id":"1403.3240","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2014-03-13T11:38:08Z","cross_cats_sorted":[],"title_canon_sha256":"06700bfea9e7217f6ad9e049e5036b1aab12f889d5bacbf9bfbb7df3592235e4","abstract_canon_sha256":"395437fd45f1c5d228a5f5366f2848de3b8fd2522da06a4a9d62f889b67790a6"},"schema_version":"1.0"},"canonical_sha256":"6b431009ffc58288c92a4ebf109d4949926d30b4e8b709ec2edc73322bac07e4","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:56:22.049505Z","signature_b64":"N7NGnyHBdW/K7uLBBydPHHn9nmK9NLVnO0yxuGXmLIKuFIeO/eNA/Ddz4nmdCOsERIee0HXAzUb+07OVlOenBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6b431009ffc58288c92a4ebf109d4949926d30b4e8b709ec2edc73322bac07e4","last_reissued_at":"2026-05-18T02:56:22.048963Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:56:22.048963Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1403.3240","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":"2026-05-18T02:56:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1W89RBFnR5fyMEIOGcuYbr6iMYgmHmcL8tvHlHNpwhMT6s/e+4P8l03sQT483DRlGgy+9E7uf4jBZdJkF4CbCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-26T03:51:03.255551Z"},"content_sha256":"4337449222017942573e12b887e1635eb889e8a1acb97d06c18c0ef9974ef60b","schema_version":"1.0","event_id":"sha256:4337449222017942573e12b887e1635eb889e8a1acb97d06c18c0ef9974ef60b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:NNBRACP7YWBIRSJKJ27RBHKJJG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Mixed-convection laminar film condensation on a semi-infinite vertical plate","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.flu-dyn","authors_text":"Graham Wilks, Jian-Jun Shu","submitted_at":"2014-03-13T11:38:08Z","abstract_excerpt":"A comprehensive study of the problem of laminar film condensation with both a gravitational type body force and a moving vapour concurrent and parallel to the surface has been presented here. It demonstrates where both the body force and vapour velocity are significant through a comprehensive numerical solution obtained by a modified Keller box method. Important parameters governing condensation and heat transfer of pure vapour are determined. A perturbation analysis is applied in the leading edge and downstream regimes. The thin film approximations for the both regimes are obtained and compar"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1403.3240","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:56:22Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+863sCa0OO0qxtr74A6zNdoMyguSg8BzXBDOw6Td/RaEYdfzvAsCy7uGumRgrZE9HTlVA2fkS2dmvdVOcqQNBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-26T03:51:03.256072Z"},"content_sha256":"5c44677f5649cbd856d7c235e427e5748875d0a0f05ab4941da5441c1bcb1e0b","schema_version":"1.0","event_id":"sha256:5c44677f5649cbd856d7c235e427e5748875d0a0f05ab4941da5441c1bcb1e0b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/NNBRACP7YWBIRSJKJ27RBHKJJG/bundle.json","state_url":"https://pith.science/pith/NNBRACP7YWBIRSJKJ27RBHKJJG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/NNBRACP7YWBIRSJKJ27RBHKJJG/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":"2026-06-26T03:51:03Z","links":{"resolver":"https://pith.science/pith/NNBRACP7YWBIRSJKJ27RBHKJJG","bundle":"https://pith.science/pith/NNBRACP7YWBIRSJKJ27RBHKJJG/bundle.json","state":"https://pith.science/pith/NNBRACP7YWBIRSJKJ27RBHKJJG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/NNBRACP7YWBIRSJKJ27RBHKJJG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:NNBRACP7YWBIRSJKJ27RBHKJJG","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":"395437fd45f1c5d228a5f5366f2848de3b8fd2522da06a4a9d62f889b67790a6","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2014-03-13T11:38:08Z","title_canon_sha256":"06700bfea9e7217f6ad9e049e5036b1aab12f889d5bacbf9bfbb7df3592235e4"},"schema_version":"1.0","source":{"id":"1403.3240","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1403.3240","created_at":"2026-05-18T02:56:22Z"},{"alias_kind":"arxiv_version","alias_value":"1403.3240v1","created_at":"2026-05-18T02:56:22Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1403.3240","created_at":"2026-05-18T02:56:22Z"},{"alias_kind":"pith_short_12","alias_value":"NNBRACP7YWBI","created_at":"2026-05-18T12:28:41Z"},{"alias_kind":"pith_short_16","alias_value":"NNBRACP7YWBIRSJK","created_at":"2026-05-18T12:28:41Z"},{"alias_kind":"pith_short_8","alias_value":"NNBRACP7","created_at":"2026-05-18T12:28:41Z"}],"graph_snapshots":[{"event_id":"sha256:5c44677f5649cbd856d7c235e427e5748875d0a0f05ab4941da5441c1bcb1e0b","target":"graph","created_at":"2026-05-18T02:56:22Z","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"},"paper":{"abstract_excerpt":"A comprehensive study of the problem of laminar film condensation with both a gravitational type body force and a moving vapour concurrent and parallel to the surface has been presented here. It demonstrates where both the body force and vapour velocity are significant through a comprehensive numerical solution obtained by a modified Keller box method. Important parameters governing condensation and heat transfer of pure vapour are determined. A perturbation analysis is applied in the leading edge and downstream regimes. The thin film approximations for the both regimes are obtained and compar","authors_text":"Graham Wilks, Jian-Jun Shu","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2014-03-13T11:38:08Z","title":"Mixed-convection laminar film condensation on a semi-infinite vertical plate"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1403.3240","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":"sha256:4337449222017942573e12b887e1635eb889e8a1acb97d06c18c0ef9974ef60b","target":"record","created_at":"2026-05-18T02:56:22Z","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":"395437fd45f1c5d228a5f5366f2848de3b8fd2522da06a4a9d62f889b67790a6","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2014-03-13T11:38:08Z","title_canon_sha256":"06700bfea9e7217f6ad9e049e5036b1aab12f889d5bacbf9bfbb7df3592235e4"},"schema_version":"1.0","source":{"id":"1403.3240","kind":"arxiv","version":1}},"canonical_sha256":"6b431009ffc58288c92a4ebf109d4949926d30b4e8b709ec2edc73322bac07e4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6b431009ffc58288c92a4ebf109d4949926d30b4e8b709ec2edc73322bac07e4","first_computed_at":"2026-05-18T02:56:22.048963Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:56:22.048963Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"N7NGnyHBdW/K7uLBBydPHHn9nmK9NLVnO0yxuGXmLIKuFIeO/eNA/Ddz4nmdCOsERIee0HXAzUb+07OVlOenBg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:56:22.049505Z","signed_message":"canonical_sha256_bytes"},"source_id":"1403.3240","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4337449222017942573e12b887e1635eb889e8a1acb97d06c18c0ef9974ef60b","sha256:5c44677f5649cbd856d7c235e427e5748875d0a0f05ab4941da5441c1bcb1e0b"],"state_sha256":"225a5eee53e3489704cde3c9239fc4b9ca693f02eb525571c9c701d21184181b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XgzjgOQHCnrM7IFTWnjsmTks5RpyYrgrKTlVmEECvz3+IyP7TTgrLK/tpWY4CiQamEs/shNOQVZlztlxPtmiAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-26T03:51:03.258825Z","bundle_sha256":"30030c15fbedd89bb6e1b760b8342c7b028e465b494e4e5bc8922fa6055fb414"}}