{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:EJROFZ32VLTE6X4YDSO4ZHU6IL","short_pith_number":"pith:EJROFZ32","schema_version":"1.0","canonical_sha256":"2262e2e77aaae64f5f981c9dcc9e9e42d9e70bbe0343bbd29ee821c4c9d6d537","source":{"kind":"arxiv","id":"1407.1180","version":1},"attestation_state":"computed","paper":{"title":"Early-time interface instabilities in high intensity aero-breakup of liquid drop","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.flu-dyn","authors_text":"N. A. Adams, X. Y. Hu","submitted_at":"2014-07-04T10:32:09Z","abstract_excerpt":"The early-time interface instabilities in high intensity (high Weber number and high Reynolds number) aero-breakup of a liquid drop are investigated by numerical simulations. A combined analysis based on simulation results and linear-instability theory show that both RT (Rayleigh-Taylor) and KH (Kelvin-Helmholtz) instabilities contributes the dominant disturbances originate from about the half way from the stagnation point to the equator. This is verified further with a specially modified simulation, which decreases the effect of KH instability while keeps other flow properties unchanged."},"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":"1407.1180","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2014-07-04T10:32:09Z","cross_cats_sorted":[],"title_canon_sha256":"57ebc2d1aaaa1e65efa21b6afd1243267c84260afb10fd1bea426c55249d025c","abstract_canon_sha256":"ca92535b8ca934b44b46fb6140a2e7982d93ea0e170e19d5d63a41df6e01a7a4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:48:18.506493Z","signature_b64":"l2LPmxxhrxWLPZZbnBRDCYWKGdISoljz5uRqNT5P7qK0/P7SuE3KlAs5RwoYACcmtTdyS42uszUHF1CXBfx/BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2262e2e77aaae64f5f981c9dcc9e9e42d9e70bbe0343bbd29ee821c4c9d6d537","last_reissued_at":"2026-05-18T02:48:18.505971Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:48:18.505971Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Early-time interface instabilities in high intensity aero-breakup of liquid drop","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.flu-dyn","authors_text":"N. A. Adams, X. Y. Hu","submitted_at":"2014-07-04T10:32:09Z","abstract_excerpt":"The early-time interface instabilities in high intensity (high Weber number and high Reynolds number) aero-breakup of a liquid drop are investigated by numerical simulations. A combined analysis based on simulation results and linear-instability theory show that both RT (Rayleigh-Taylor) and KH (Kelvin-Helmholtz) instabilities contributes the dominant disturbances originate from about the half way from the stagnation point to the equator. This is verified further with a specially modified simulation, which decreases the effect of KH instability while keeps other flow properties unchanged."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1407.1180","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1407.1180","created_at":"2026-05-18T02:48:18.506055+00:00"},{"alias_kind":"arxiv_version","alias_value":"1407.1180v1","created_at":"2026-05-18T02:48:18.506055+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1407.1180","created_at":"2026-05-18T02:48:18.506055+00:00"},{"alias_kind":"pith_short_12","alias_value":"EJROFZ32VLTE","created_at":"2026-05-18T12:28:25.294606+00:00"},{"alias_kind":"pith_short_16","alias_value":"EJROFZ32VLTE6X4Y","created_at":"2026-05-18T12:28:25.294606+00:00"},{"alias_kind":"pith_short_8","alias_value":"EJROFZ32","created_at":"2026-05-18T12:28:25.294606+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/EJROFZ32VLTE6X4YDSO4ZHU6IL","json":"https://pith.science/pith/EJROFZ32VLTE6X4YDSO4ZHU6IL.json","graph_json":"https://pith.science/api/pith-number/EJROFZ32VLTE6X4YDSO4ZHU6IL/graph.json","events_json":"https://pith.science/api/pith-number/EJROFZ32VLTE6X4YDSO4ZHU6IL/events.json","paper":"https://pith.science/paper/EJROFZ32"},"agent_actions":{"view_html":"https://pith.science/pith/EJROFZ32VLTE6X4YDSO4ZHU6IL","download_json":"https://pith.science/pith/EJROFZ32VLTE6X4YDSO4ZHU6IL.json","view_paper":"https://pith.science/paper/EJROFZ32","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1407.1180&json=true","fetch_graph":"https://pith.science/api/pith-number/EJROFZ32VLTE6X4YDSO4ZHU6IL/graph.json","fetch_events":"https://pith.science/api/pith-number/EJROFZ32VLTE6X4YDSO4ZHU6IL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EJROFZ32VLTE6X4YDSO4ZHU6IL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EJROFZ32VLTE6X4YDSO4ZHU6IL/action/storage_attestation","attest_author":"https://pith.science/pith/EJROFZ32VLTE6X4YDSO4ZHU6IL/action/author_attestation","sign_citation":"https://pith.science/pith/EJROFZ32VLTE6X4YDSO4ZHU6IL/action/citation_signature","submit_replication":"https://pith.science/pith/EJROFZ32VLTE6X4YDSO4ZHU6IL/action/replication_record"}},"created_at":"2026-05-18T02:48:18.506055+00:00","updated_at":"2026-05-18T02:48:18.506055+00:00"}