{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:HDGFVIKZHSTRSZWDZORNSHR2L5","short_pith_number":"pith:HDGFVIKZ","schema_version":"1.0","canonical_sha256":"38cc5aa1593ca71966c3cba2d91e3a5f60d53d7e89daca0175f1b5defbfe2c94","source":{"kind":"arxiv","id":"2504.07218","version":2},"attestation_state":"computed","paper":{"title":"Numerical analysis of three-dimensional magnetohydrodynamic effects in an inductively coupled plasma wind tunnel","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":["physics.flu-dyn"],"primary_cat":"physics.plasm-ph","authors_text":"Alessandro Munafo, Daniel J Bodony, Marco Panesi, Sanjeev Kumar","submitted_at":"2025-04-09T18:47:39Z","abstract_excerpt":"This paper introduces a three-dimensional model for the 350 kW Plasmatron X inductively coupled plasma facility at the University of Illinois Urbana-Champaign, designed for testing high-temperature materials. Simulations of the facility have been performed using a three-dimensional, multiphysics computational framework, which reveals pronounced three-dimensional characteristics within the facility. The analysis of the plasma and electromagnetic field in the torch region reveals the influence of the helical coils, which cause a non-axisymmetric distribution of the plasma discharge. Additionally"},"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":"2504.07218","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"physics.plasm-ph","submitted_at":"2025-04-09T18:47:39Z","cross_cats_sorted":["physics.flu-dyn"],"title_canon_sha256":"b6104e4a3cf7fd56280c6bec7057eae33e2c90a9abe9c032e62b68994e465358","abstract_canon_sha256":"631845ab17456f92414fe8fe9f6a84c0736d1f84e9a38c4016a72be37c37be5a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-08-04T02:08:05.983407Z","signature_b64":"AeIGv6eGce1W+tZEBsQ/vYAwSD08lG9qeNQTFJY4R8l/+/UMRs3+3dX7zO9QqLBO3I7xE4JmIpMYCw7Y/CvlBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"38cc5aa1593ca71966c3cba2d91e3a5f60d53d7e89daca0175f1b5defbfe2c94","last_reissued_at":"2026-08-04T02:08:05.981600Z","signature_status":"signed_v1","first_computed_at":"2026-08-04T02:08:05.981600Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Numerical analysis of three-dimensional magnetohydrodynamic effects in an inductively coupled plasma wind tunnel","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":["physics.flu-dyn"],"primary_cat":"physics.plasm-ph","authors_text":"Alessandro Munafo, Daniel J Bodony, Marco Panesi, Sanjeev Kumar","submitted_at":"2025-04-09T18:47:39Z","abstract_excerpt":"This paper introduces a three-dimensional model for the 350 kW Plasmatron X inductively coupled plasma facility at the University of Illinois Urbana-Champaign, designed for testing high-temperature materials. Simulations of the facility have been performed using a three-dimensional, multiphysics computational framework, which reveals pronounced three-dimensional characteristics within the facility. The analysis of the plasma and electromagnetic field in the torch region reveals the influence of the helical coils, which cause a non-axisymmetric distribution of the plasma discharge. Additionally"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2504.07218","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2504.07218/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2504.07218","created_at":"2026-08-04T02:08:05.983136+00:00"},{"alias_kind":"arxiv_version","alias_value":"2504.07218v2","created_at":"2026-08-04T02:08:05.983136+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2504.07218","created_at":"2026-08-04T02:08:05.983136+00:00"},{"alias_kind":"pith_short_12","alias_value":"HDGFVIKZHSTR","created_at":"2026-08-04T02:08:05.983136+00:00"},{"alias_kind":"pith_short_16","alias_value":"HDGFVIKZHSTRSZWD","created_at":"2026-08-04T02:08:05.983136+00:00"},{"alias_kind":"pith_short_8","alias_value":"HDGFVIKZ","created_at":"2026-08-04T02:08:05.983136+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2506.02469","citing_title":"Characterization of the VKI Plasmatron subsonic ICP jet combining optical emission spectroscopy, intrusive measurements, and CFD simulations","ref_index":71,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/HDGFVIKZHSTRSZWDZORNSHR2L5","json":"https://pith.science/pith/HDGFVIKZHSTRSZWDZORNSHR2L5.json","graph_json":"https://pith.science/api/pith-number/HDGFVIKZHSTRSZWDZORNSHR2L5/graph.json","events_json":"https://pith.science/api/pith-number/HDGFVIKZHSTRSZWDZORNSHR2L5/events.json","paper":"https://pith.science/paper/HDGFVIKZ"},"agent_actions":{"view_html":"https://pith.science/pith/HDGFVIKZHSTRSZWDZORNSHR2L5","download_json":"https://pith.science/pith/HDGFVIKZHSTRSZWDZORNSHR2L5.json","view_paper":"https://pith.science/paper/HDGFVIKZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2504.07218&json=true","fetch_graph":"https://pith.science/api/pith-number/HDGFVIKZHSTRSZWDZORNSHR2L5/graph.json","fetch_events":"https://pith.science/api/pith-number/HDGFVIKZHSTRSZWDZORNSHR2L5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HDGFVIKZHSTRSZWDZORNSHR2L5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HDGFVIKZHSTRSZWDZORNSHR2L5/action/storage_attestation","attest_author":"https://pith.science/pith/HDGFVIKZHSTRSZWDZORNSHR2L5/action/author_attestation","sign_citation":"https://pith.science/pith/HDGFVIKZHSTRSZWDZORNSHR2L5/action/citation_signature","submit_replication":"https://pith.science/pith/HDGFVIKZHSTRSZWDZORNSHR2L5/action/replication_record"}},"created_at":"2026-08-04T02:08:05.983136+00:00","updated_at":"2026-08-04T02:08:05.983136+00:00"}