{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:RKGCDAO7PEYINJ4U5TYYVOA2JX","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":"2e49130372730a416b271bef01dec04b0335c77fbbb2e8b5b82d20695b9fb97f","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2017-08-28T15:13:09Z","title_canon_sha256":"c65959c6e4c0b55484faf1394b8295be9ad6a8f1083ca1785eba78c10a1156dc"},"schema_version":"1.0","source":{"id":"1708.08366","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1708.08366","created_at":"2026-05-18T00:29:54Z"},{"alias_kind":"arxiv_version","alias_value":"1708.08366v3","created_at":"2026-05-18T00:29:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.08366","created_at":"2026-05-18T00:29:54Z"},{"alias_kind":"pith_short_12","alias_value":"RKGCDAO7PEYI","created_at":"2026-05-18T12:31:39Z"},{"alias_kind":"pith_short_16","alias_value":"RKGCDAO7PEYINJ4U","created_at":"2026-05-18T12:31:39Z"},{"alias_kind":"pith_short_8","alias_value":"RKGCDAO7","created_at":"2026-05-18T12:31:39Z"}],"graph_snapshots":[{"event_id":"sha256:a22cdf545032e96a691fc5f6c8b729d90c11571cbdb3606c48c82ca16fc17799","target":"graph","created_at":"2026-05-18T00:29:54Z","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":"To predict the mean temperature profiles in turbulent thermal convection, the thermal boundary layer (BL) equation including the effects of fluctuations has to be solved. In Shishkina et al., Phys. Rev. Lett. 114 (2015), the thermal BL equation with the fluctuations taken into account as an eddy thermal diffusivity has been solved for large Prandtl-number fluids for which the eddy thermal diffusivity and the velocity field can be approximated respectively as a cubic and a linear function of the distance from the plate. In the present work we make use of the idea of Prandtl's mixing length mode","authors_text":"Emily S. C. Ching, Mohammad S. Emran, Olga Shishkina, Susanne Horn","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2017-08-28T15:13:09Z","title":"Mean Temperature Profiles in Turbulent Thermal Convection"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.08366","kind":"arxiv","version":3},"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":"sha256:8f7641cc56f9b984ea7e38cb93a85263acfe6e7f888a8cbfda4eae239e80d30a","target":"record","created_at":"2026-05-18T00:29:54Z","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":"2e49130372730a416b271bef01dec04b0335c77fbbb2e8b5b82d20695b9fb97f","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2017-08-28T15:13:09Z","title_canon_sha256":"c65959c6e4c0b55484faf1394b8295be9ad6a8f1083ca1785eba78c10a1156dc"},"schema_version":"1.0","source":{"id":"1708.08366","kind":"arxiv","version":3}},"canonical_sha256":"8a8c2181df793086a794ecf18ab81a4dc085fa91348cf8ae4a186c391356d6d0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8a8c2181df793086a794ecf18ab81a4dc085fa91348cf8ae4a186c391356d6d0","first_computed_at":"2026-05-18T00:29:54.627574Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:29:54.627574Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"X2HGneghunqxCryKfdnfa9r8IxkCXea4FooDPxcoQ+oFEe7y3cwnJjmU1VNUpKjdfMkIfY14gR6ossVeVtg3DA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:29:54.628117Z","signed_message":"canonical_sha256_bytes"},"source_id":"1708.08366","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8f7641cc56f9b984ea7e38cb93a85263acfe6e7f888a8cbfda4eae239e80d30a","sha256:a22cdf545032e96a691fc5f6c8b729d90c11571cbdb3606c48c82ca16fc17799"],"state_sha256":"40992e237dfe120ff40eb119f8753e4cc0eee2b138e053496f9843abf4878eaf"}