{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:B7YBAYHBNA4G7S3ZTOLWYM66VX","short_pith_number":"pith:B7YBAYHB","schema_version":"1.0","canonical_sha256":"0ff01060e168386fcb799b976c33deade741892c1e19ed2e7a3f1af8d84e0502","source":{"kind":"arxiv","id":"1901.06941","version":1},"attestation_state":"computed","paper":{"title":"Induced charge electroosmotic flow with finite ion size and solvation effects","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.comp-ph"],"primary_cat":"physics.chem-ph","authors_text":"Alexander Linke, Christian Merdon, Clemens Guhlke, J\\\"urgen Fuhrmann, R\\\"udiger M\\\"uller","submitted_at":"2019-01-21T14:22:57Z","abstract_excerpt":"The most common mathematical models for electrolyte flows are based on the dilute solution assumption, leading to a coupled system of the Nernst--Planck--Poisson drift-diffusion equations for ion transport and the Stokes resp. Navier--Stokes equations for fluid flow of the solvent. In charged boundary layers the dilute solution assumption is in general not valid and volume exclusion and solvation effects have to be taken into account in a thermodynamically consistent way. Whenever boundary layer effects have a dominant impact on the global behavior of a certain electrochemical system, an accur"},"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":"1901.06941","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2019-01-21T14:22:57Z","cross_cats_sorted":["physics.comp-ph"],"title_canon_sha256":"bdd5febfcf6a32b20aad0164e3fb9a82ae28d8732967042ddaa325bd7b019530","abstract_canon_sha256":"24aad936fa718c2c3dd339856b6809f87dfd6964942d8f07fd86c315a0d51db5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:55:48.619434Z","signature_b64":"6Ytp03bQil+iC/wwp2CrYYfG1TAbSxTX2ORLGVu6DV9DWo2zp8CfF6BoO4dwLLqjgM9ye7ivpO+6LVzLCqcWCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0ff01060e168386fcb799b976c33deade741892c1e19ed2e7a3f1af8d84e0502","last_reissued_at":"2026-05-17T23:55:48.618658Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:55:48.618658Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Induced charge electroosmotic flow with finite ion size and solvation effects","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.comp-ph"],"primary_cat":"physics.chem-ph","authors_text":"Alexander Linke, Christian Merdon, Clemens Guhlke, J\\\"urgen Fuhrmann, R\\\"udiger M\\\"uller","submitted_at":"2019-01-21T14:22:57Z","abstract_excerpt":"The most common mathematical models for electrolyte flows are based on the dilute solution assumption, leading to a coupled system of the Nernst--Planck--Poisson drift-diffusion equations for ion transport and the Stokes resp. Navier--Stokes equations for fluid flow of the solvent. In charged boundary layers the dilute solution assumption is in general not valid and volume exclusion and solvation effects have to be taken into account in a thermodynamically consistent way. Whenever boundary layer effects have a dominant impact on the global behavior of a certain electrochemical system, an accur"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1901.06941","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":"1901.06941","created_at":"2026-05-17T23:55:48.618795+00:00"},{"alias_kind":"arxiv_version","alias_value":"1901.06941v1","created_at":"2026-05-17T23:55:48.618795+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1901.06941","created_at":"2026-05-17T23:55:48.618795+00:00"},{"alias_kind":"pith_short_12","alias_value":"B7YBAYHBNA4G","created_at":"2026-05-18T12:33:12.712433+00:00"},{"alias_kind":"pith_short_16","alias_value":"B7YBAYHBNA4G7S3Z","created_at":"2026-05-18T12:33:12.712433+00:00"},{"alias_kind":"pith_short_8","alias_value":"B7YBAYHB","created_at":"2026-05-18T12:33:12.712433+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/B7YBAYHBNA4G7S3ZTOLWYM66VX","json":"https://pith.science/pith/B7YBAYHBNA4G7S3ZTOLWYM66VX.json","graph_json":"https://pith.science/api/pith-number/B7YBAYHBNA4G7S3ZTOLWYM66VX/graph.json","events_json":"https://pith.science/api/pith-number/B7YBAYHBNA4G7S3ZTOLWYM66VX/events.json","paper":"https://pith.science/paper/B7YBAYHB"},"agent_actions":{"view_html":"https://pith.science/pith/B7YBAYHBNA4G7S3ZTOLWYM66VX","download_json":"https://pith.science/pith/B7YBAYHBNA4G7S3ZTOLWYM66VX.json","view_paper":"https://pith.science/paper/B7YBAYHB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1901.06941&json=true","fetch_graph":"https://pith.science/api/pith-number/B7YBAYHBNA4G7S3ZTOLWYM66VX/graph.json","fetch_events":"https://pith.science/api/pith-number/B7YBAYHBNA4G7S3ZTOLWYM66VX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/B7YBAYHBNA4G7S3ZTOLWYM66VX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/B7YBAYHBNA4G7S3ZTOLWYM66VX/action/storage_attestation","attest_author":"https://pith.science/pith/B7YBAYHBNA4G7S3ZTOLWYM66VX/action/author_attestation","sign_citation":"https://pith.science/pith/B7YBAYHBNA4G7S3ZTOLWYM66VX/action/citation_signature","submit_replication":"https://pith.science/pith/B7YBAYHBNA4G7S3ZTOLWYM66VX/action/replication_record"}},"created_at":"2026-05-17T23:55:48.618795+00:00","updated_at":"2026-05-17T23:55:48.618795+00:00"}