{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:VSH67YU672KMZWJN7QOZGEJVTH","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":"f95f15ee1af4a54231ad80aeb3c3b350750269243ad4b6b74524cb95c5fb148a","cross_cats_sorted":["physics.ao-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2010-12-31T01:59:46Z","title_canon_sha256":"a5f6f1fcabaf5328a56b2774e5057e44a3948b6f24e3fc3a7cf0d700b2da96ff"},"schema_version":"1.0","source":{"id":"1101.0188","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1101.0188","created_at":"2026-05-18T04:32:10Z"},{"alias_kind":"arxiv_version","alias_value":"1101.0188v1","created_at":"2026-05-18T04:32:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1101.0188","created_at":"2026-05-18T04:32:10Z"},{"alias_kind":"pith_short_12","alias_value":"VSH67YU672KM","created_at":"2026-05-18T12:26:15Z"},{"alias_kind":"pith_short_16","alias_value":"VSH67YU672KMZWJN","created_at":"2026-05-18T12:26:15Z"},{"alias_kind":"pith_short_8","alias_value":"VSH67YU6","created_at":"2026-05-18T12:26:15Z"}],"graph_snapshots":[{"event_id":"sha256:6dc32eac1317274ed53fddf3c42312fb390458c92d1e06dd109b06783b80fa70","target":"graph","created_at":"2026-05-18T04:32:10Z","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":"A modification of Mott-Smith method for predicting the one-dimensional shock wave solution is presented. Mott-Smith distribution function is used to construct the system of moment equations to study the steady-state structure of shock wave in a gas of Maxwell molecules and in argon. The predicted shock solutions using the newly proposed formalism are compared with the experimental data, direct-simulation Monte Carlo (DSMC) solution and the solutions predicted by other existing theories for Mach numbers M<11. The density, temperature, heat flux profiles and shock thickness calculated at differe","authors_text":"Maxim A. Solovchuk, Tony W. H. Sheu","cross_cats":["physics.ao-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2010-12-31T01:59:46Z","title":"Prediction of shock structure using the bimodal distribution function"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1101.0188","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:c9a4059c2356ba73ec3e9d5408bbbbf3189a5e9d853ee480d59bcfb60cf86fa5","target":"record","created_at":"2026-05-18T04:32:10Z","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":"f95f15ee1af4a54231ad80aeb3c3b350750269243ad4b6b74524cb95c5fb148a","cross_cats_sorted":["physics.ao-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.flu-dyn","submitted_at":"2010-12-31T01:59:46Z","title_canon_sha256":"a5f6f1fcabaf5328a56b2774e5057e44a3948b6f24e3fc3a7cf0d700b2da96ff"},"schema_version":"1.0","source":{"id":"1101.0188","kind":"arxiv","version":1}},"canonical_sha256":"ac8fefe29efe94ccd92dfc1d93113599fa4e645d12af5b8aaeb31476083dc08a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ac8fefe29efe94ccd92dfc1d93113599fa4e645d12af5b8aaeb31476083dc08a","first_computed_at":"2026-05-18T04:32:10.855531Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:32:10.855531Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"PNcz0i29LycBjAeU0LuHIl8+UtMJsbfKulqdxj/Qw9nWkfqQW+f2pr84JcWeLV8982Zj+tvtZ8bz8hcjHdyGDg==","signature_status":"signed_v1","signed_at":"2026-05-18T04:32:10.855998Z","signed_message":"canonical_sha256_bytes"},"source_id":"1101.0188","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c9a4059c2356ba73ec3e9d5408bbbbf3189a5e9d853ee480d59bcfb60cf86fa5","sha256:6dc32eac1317274ed53fddf3c42312fb390458c92d1e06dd109b06783b80fa70"],"state_sha256":"d46888d46bfd0a82cf26b9dfe1f105e5de57ad31b05161acd7b12d4495c1208e"}