{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:EIIIFJM4DPODNKEAGDHGJNNF3Y","short_pith_number":"pith:EIIIFJM4","schema_version":"1.0","canonical_sha256":"221082a59c1bdc36a88030ce64b5a5de323d1af6ed8eb63dcfb51038a384a38c","source":{"kind":"arxiv","id":"1204.2732","version":3},"attestation_state":"computed","paper":{"title":"Transition from viscous to inertial regime in dense suspensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.soft","authors_text":"Bruno Andreotti, Martin Trulsson, Philippe Claudin","submitted_at":"2012-04-12T14:08:23Z","abstract_excerpt":"Non-Brownian suspensions present a transition from Newtonian behavior in the zero-shear limit to a shear thickening behaviour at a large shear rate, none of which is clearly understood so far. Here, we carry out numerical simulations of such an athermal dense suspension under shear, at an imposed confining pressure. This set-up is conceptually identical to the recent experiments of Boyer and co-workers [Phys. Rev. Lett. 107,188301 (2011)]. Varying the interstitial fluid viscosities, we recover the Newtonian and Bagnoldian regimes and show that they correspond to a dissipation dominated by visc"},"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":"1204.2732","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2012-04-12T14:08:23Z","cross_cats_sorted":[],"title_canon_sha256":"be2267a986dd90abd71276686b9e88a8a6d4a43273a143e4d243efe8c7435a51","abstract_canon_sha256":"17569699468b93437ec0fb85d3846b03847c2d27ba7efe21d7bed507d7780c38"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:26:47.592794Z","signature_b64":"yTXxsRqo6PVTlVHtc9x+96yMHl8eHX8vlHz89ZPbiPzgiVzn1yH9A1NbJIZkHLfmkxzm+LPIH+XQR5kcikB7AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"221082a59c1bdc36a88030ce64b5a5de323d1af6ed8eb63dcfb51038a384a38c","last_reissued_at":"2026-05-18T00:26:47.592164Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:26:47.592164Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Transition from viscous to inertial regime in dense suspensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.soft","authors_text":"Bruno Andreotti, Martin Trulsson, Philippe Claudin","submitted_at":"2012-04-12T14:08:23Z","abstract_excerpt":"Non-Brownian suspensions present a transition from Newtonian behavior in the zero-shear limit to a shear thickening behaviour at a large shear rate, none of which is clearly understood so far. Here, we carry out numerical simulations of such an athermal dense suspension under shear, at an imposed confining pressure. This set-up is conceptually identical to the recent experiments of Boyer and co-workers [Phys. Rev. Lett. 107,188301 (2011)]. Varying the interstitial fluid viscosities, we recover the Newtonian and Bagnoldian regimes and show that they correspond to a dissipation dominated by visc"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1204.2732","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":"1204.2732","created_at":"2026-05-18T00:26:47.592279+00:00"},{"alias_kind":"arxiv_version","alias_value":"1204.2732v3","created_at":"2026-05-18T00:26:47.592279+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1204.2732","created_at":"2026-05-18T00:26:47.592279+00:00"},{"alias_kind":"pith_short_12","alias_value":"EIIIFJM4DPOD","created_at":"2026-05-18T12:27:04.183437+00:00"},{"alias_kind":"pith_short_16","alias_value":"EIIIFJM4DPODNKEA","created_at":"2026-05-18T12:27:04.183437+00:00"},{"alias_kind":"pith_short_8","alias_value":"EIIIFJM4","created_at":"2026-05-18T12:27:04.183437+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/EIIIFJM4DPODNKEAGDHGJNNF3Y","json":"https://pith.science/pith/EIIIFJM4DPODNKEAGDHGJNNF3Y.json","graph_json":"https://pith.science/api/pith-number/EIIIFJM4DPODNKEAGDHGJNNF3Y/graph.json","events_json":"https://pith.science/api/pith-number/EIIIFJM4DPODNKEAGDHGJNNF3Y/events.json","paper":"https://pith.science/paper/EIIIFJM4"},"agent_actions":{"view_html":"https://pith.science/pith/EIIIFJM4DPODNKEAGDHGJNNF3Y","download_json":"https://pith.science/pith/EIIIFJM4DPODNKEAGDHGJNNF3Y.json","view_paper":"https://pith.science/paper/EIIIFJM4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1204.2732&json=true","fetch_graph":"https://pith.science/api/pith-number/EIIIFJM4DPODNKEAGDHGJNNF3Y/graph.json","fetch_events":"https://pith.science/api/pith-number/EIIIFJM4DPODNKEAGDHGJNNF3Y/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EIIIFJM4DPODNKEAGDHGJNNF3Y/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EIIIFJM4DPODNKEAGDHGJNNF3Y/action/storage_attestation","attest_author":"https://pith.science/pith/EIIIFJM4DPODNKEAGDHGJNNF3Y/action/author_attestation","sign_citation":"https://pith.science/pith/EIIIFJM4DPODNKEAGDHGJNNF3Y/action/citation_signature","submit_replication":"https://pith.science/pith/EIIIFJM4DPODNKEAGDHGJNNF3Y/action/replication_record"}},"created_at":"2026-05-18T00:26:47.592279+00:00","updated_at":"2026-05-18T00:26:47.592279+00:00"}