{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:KJJXLPQJHDS4EFZ6AUPF47LSPH","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":"52ba0cbad344bfb081b1b20eebefb7c2147b13ea39bed29905f1f7164d18bff4","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2015-11-30T15:46:27Z","title_canon_sha256":"53ac7a15f1282897e5c152c1631f197836b8536e9993909a1011117414c768cb"},"schema_version":"1.0","source":{"id":"1511.09356","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1511.09356","created_at":"2026-05-18T01:25:40Z"},{"alias_kind":"arxiv_version","alias_value":"1511.09356v1","created_at":"2026-05-18T01:25:40Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1511.09356","created_at":"2026-05-18T01:25:40Z"},{"alias_kind":"pith_short_12","alias_value":"KJJXLPQJHDS4","created_at":"2026-05-18T12:29:29Z"},{"alias_kind":"pith_short_16","alias_value":"KJJXLPQJHDS4EFZ6","created_at":"2026-05-18T12:29:29Z"},{"alias_kind":"pith_short_8","alias_value":"KJJXLPQJ","created_at":"2026-05-18T12:29:29Z"}],"graph_snapshots":[{"event_id":"sha256:ec242f781ce41faaac5b3ef1ba7536ee93d25e839d591f34a5c120de368635de","target":"graph","created_at":"2026-05-18T01:25:40Z","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":"Wall-models are essential for enabling large-eddy simulations (LESs) of realistic problems at high Reynolds numbers. The present study is focused on approaches that directly model the wall shear stress, specifically on filling the gap between models based on wall-normal ordinary differential equations (ODEs) that assume equilibrium and models based on full partial differential equations (PDEs) that do not. We develop ideas for how to incorporate non-equilibrium effects (most importantly, strong pressure-gradient effects) in the wall-model while still solving only wall-normal ODEs. We test thes","authors_text":"Emile Touber, Johan Larsson, Julien Bodart, Stefan Hickel","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2015-11-30T15:46:27Z","title":"A parametrized non-equilibrium wall-model for large-eddy simulations"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1511.09356","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":"sha256:766de1562e004dd10645bc760b88158907438889eb8076db2e184ac1fcb610e5","target":"record","created_at":"2026-05-18T01:25:40Z","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":"52ba0cbad344bfb081b1b20eebefb7c2147b13ea39bed29905f1f7164d18bff4","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2015-11-30T15:46:27Z","title_canon_sha256":"53ac7a15f1282897e5c152c1631f197836b8536e9993909a1011117414c768cb"},"schema_version":"1.0","source":{"id":"1511.09356","kind":"arxiv","version":1}},"canonical_sha256":"525375be0938e5c2173e051e5e7d7279c2c4c052e478befd433d13255caa7ae9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"525375be0938e5c2173e051e5e7d7279c2c4c052e478befd433d13255caa7ae9","first_computed_at":"2026-05-18T01:25:40.458530Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:25:40.458530Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"6Nxkv5bSP0WJ8eaye//uz3iQYBn8WjKkj+q/gxoXGr0z0owkQxudy6z5d2QKW/HMfj7Ng+rWf6HiGo7ViY+MAA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:25:40.459130Z","signed_message":"canonical_sha256_bytes"},"source_id":"1511.09356","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:766de1562e004dd10645bc760b88158907438889eb8076db2e184ac1fcb610e5","sha256:ec242f781ce41faaac5b3ef1ba7536ee93d25e839d591f34a5c120de368635de"],"state_sha256":"9654e9182306aa5816ffb161b0e1b40c1ee0c2f14b78c5eae69c87ba4182750e"}