{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2021:3LJDHPMVA3RYX6KIADNKXN3UWT","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":"9303fb37bfdccd796d061c6daa63d14d8b6768e97caf24e003a027c11384ce5c","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2021-06-08T18:02:37Z","title_canon_sha256":"7035942cb20157a259537bc2e61d057d94afd1c0c563beded9e0bf6ef2c23b5e"},"schema_version":"1.0","source":{"id":"2106.04611","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2106.04611","created_at":"2026-07-05T02:47:47Z"},{"alias_kind":"arxiv_version","alias_value":"2106.04611v1","created_at":"2026-07-05T02:47:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2106.04611","created_at":"2026-07-05T02:47:47Z"},{"alias_kind":"pith_short_12","alias_value":"3LJDHPMVA3RY","created_at":"2026-07-05T02:47:47Z"},{"alias_kind":"pith_short_16","alias_value":"3LJDHPMVA3RYX6KI","created_at":"2026-07-05T02:47:47Z"},{"alias_kind":"pith_short_8","alias_value":"3LJDHPMV","created_at":"2026-07-05T02:47:47Z"}],"graph_snapshots":[{"event_id":"sha256:5fb82cae98937e376e4377d6e306c04b42bee7d55963559600e4a5b44ca41a7e","target":"graph","created_at":"2026-07-05T02:47:47Z","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/2106.04611/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"An experimental investigation of secondary atomization of spray in plain-jet airblast atomizers with a circular array of six liquid jets is studied. Crossflow of air with controlled velocity and pressure is applied to transverse jets. The liquid jets (Re=12000) are injected into airflow (Weg of 1250-3000) analyzed experimentally for different injection diameters of 0.8-1.6 mm. Particle size distribution measurement is carried out by Malvern Mastersizer X in the fully atomized region of the atomizer. The droplet size distribution in the secondary or final atomization stage is also modeled by th","authors_text":"Abbas Elkaie, Armin Abdehkakha, Maziar Shafaee, Mohammad Hosein Sabour","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2021-06-08T18:02:37Z","title":"Size distribution modelling of secondary atomization in spray of plain-jet airblast atomizer with finite stochastic breakup model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2106.04611","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":"sha256:93cd64cff4b3597f4d0034b497f506cd561debaec0001cc00184cb2cc2474811","target":"record","created_at":"2026-07-05T02:47:47Z","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":"9303fb37bfdccd796d061c6daa63d14d8b6768e97caf24e003a027c11384ce5c","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2021-06-08T18:02:37Z","title_canon_sha256":"7035942cb20157a259537bc2e61d057d94afd1c0c563beded9e0bf6ef2c23b5e"},"schema_version":"1.0","source":{"id":"2106.04611","kind":"arxiv","version":1}},"canonical_sha256":"dad233bd9506e38bf94800daabb774b4d03916a04378b26b09a5686b6d467337","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"dad233bd9506e38bf94800daabb774b4d03916a04378b26b09a5686b6d467337","first_computed_at":"2026-07-05T02:47:47.165985Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T02:47:47.165985Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Tn3R5wCT/5qYbAcPFQ83/bXEN5meEfS0XTVSf0o9YwI7+BfPrTSfbH3U+d3DS0lOrfALIp7MFm4Sf4BRN8wABA==","signature_status":"signed_v1","signed_at":"2026-07-05T02:47:47.166537Z","signed_message":"canonical_sha256_bytes"},"source_id":"2106.04611","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:93cd64cff4b3597f4d0034b497f506cd561debaec0001cc00184cb2cc2474811","sha256:5fb82cae98937e376e4377d6e306c04b42bee7d55963559600e4a5b44ca41a7e"],"state_sha256":"b057b81af8b5d74f643e2ff61d4e61bd9ca177bcab9f034b0af4e7dc021079b9"}