{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:H6QZDKE6YBZVOXPNZGJFDJGYMS","short_pith_number":"pith:H6QZDKE6","schema_version":"1.0","canonical_sha256":"3fa191a89ec073575dedc99251a4d86495e90b8103990c7f61deba016eb7eeff","source":{"kind":"arxiv","id":"1612.02585","version":3},"attestation_state":"computed","paper":{"title":"Turbulent diffusion of chemically reacting flows: theory and numerical simulations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.ao-ph"],"primary_cat":"physics.flu-dyn","authors_text":"A. Lipatnikov, I. Rogachevskii, M. Liberman, N. Kleeorin, R. Yu, T. Elperin","submitted_at":"2016-12-08T10:23:37Z","abstract_excerpt":"The theory of turbulent diffusion of chemically reacting gaseous admixtures developed previously (Phys. Rev. E {\\bf 90}, 053001, 2014) is generalized for large yet finite Reynolds numbers, and the dependence of turbulent diffusion coefficient versus two parameters, the Reynolds number and Damk\\\"ohler number (which characterizes a ratio of turbulent and reaction time scales) is obtained. Three-dimensional direct numerical simulations (DNS) of a finite thickness reaction wave for the first-order chemical reactions propagating in forced, homogeneous, isotropic, and incompressible turbulence are p"},"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":"1612.02585","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2016-12-08T10:23:37Z","cross_cats_sorted":["physics.ao-ph"],"title_canon_sha256":"32a61fcf528d7d00154670d28fee1c673f2d6b5e025f2505d2dd5406cf0e9459","abstract_canon_sha256":"591903a22055f214309d6181175faea352f313442aa88aea79d9dd1022293e52"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:15:10.606590Z","signature_b64":"ALtDVRAAnOlB9sj6wJiaQ+I3Pi+g1u3xPPrc0QQgjG2DWNHYaKg/kSZqNralSzErmHSWExK1ZgwV9iyCQcr0Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3fa191a89ec073575dedc99251a4d86495e90b8103990c7f61deba016eb7eeff","last_reissued_at":"2026-05-18T00:15:10.605787Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:15:10.605787Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Turbulent diffusion of chemically reacting flows: theory and numerical simulations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.ao-ph"],"primary_cat":"physics.flu-dyn","authors_text":"A. Lipatnikov, I. Rogachevskii, M. Liberman, N. Kleeorin, R. Yu, T. Elperin","submitted_at":"2016-12-08T10:23:37Z","abstract_excerpt":"The theory of turbulent diffusion of chemically reacting gaseous admixtures developed previously (Phys. Rev. E {\\bf 90}, 053001, 2014) is generalized for large yet finite Reynolds numbers, and the dependence of turbulent diffusion coefficient versus two parameters, the Reynolds number and Damk\\\"ohler number (which characterizes a ratio of turbulent and reaction time scales) is obtained. Three-dimensional direct numerical simulations (DNS) of a finite thickness reaction wave for the first-order chemical reactions propagating in forced, homogeneous, isotropic, and incompressible turbulence are p"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1612.02585","kind":"arxiv","version":3},"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":"1612.02585","created_at":"2026-05-18T00:15:10.605926+00:00"},{"alias_kind":"arxiv_version","alias_value":"1612.02585v3","created_at":"2026-05-18T00:15:10.605926+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1612.02585","created_at":"2026-05-18T00:15:10.605926+00:00"},{"alias_kind":"pith_short_12","alias_value":"H6QZDKE6YBZV","created_at":"2026-05-18T12:30:19.053100+00:00"},{"alias_kind":"pith_short_16","alias_value":"H6QZDKE6YBZVOXPN","created_at":"2026-05-18T12:30:19.053100+00:00"},{"alias_kind":"pith_short_8","alias_value":"H6QZDKE6","created_at":"2026-05-18T12:30:19.053100+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/H6QZDKE6YBZVOXPNZGJFDJGYMS","json":"https://pith.science/pith/H6QZDKE6YBZVOXPNZGJFDJGYMS.json","graph_json":"https://pith.science/api/pith-number/H6QZDKE6YBZVOXPNZGJFDJGYMS/graph.json","events_json":"https://pith.science/api/pith-number/H6QZDKE6YBZVOXPNZGJFDJGYMS/events.json","paper":"https://pith.science/paper/H6QZDKE6"},"agent_actions":{"view_html":"https://pith.science/pith/H6QZDKE6YBZVOXPNZGJFDJGYMS","download_json":"https://pith.science/pith/H6QZDKE6YBZVOXPNZGJFDJGYMS.json","view_paper":"https://pith.science/paper/H6QZDKE6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1612.02585&json=true","fetch_graph":"https://pith.science/api/pith-number/H6QZDKE6YBZVOXPNZGJFDJGYMS/graph.json","fetch_events":"https://pith.science/api/pith-number/H6QZDKE6YBZVOXPNZGJFDJGYMS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/H6QZDKE6YBZVOXPNZGJFDJGYMS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/H6QZDKE6YBZVOXPNZGJFDJGYMS/action/storage_attestation","attest_author":"https://pith.science/pith/H6QZDKE6YBZVOXPNZGJFDJGYMS/action/author_attestation","sign_citation":"https://pith.science/pith/H6QZDKE6YBZVOXPNZGJFDJGYMS/action/citation_signature","submit_replication":"https://pith.science/pith/H6QZDKE6YBZVOXPNZGJFDJGYMS/action/replication_record"}},"created_at":"2026-05-18T00:15:10.605926+00:00","updated_at":"2026-05-18T00:15:10.605926+00:00"}