{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2008:B3B2DLMTIOKU26WNHF62ZOXFD5","short_pith_number":"pith:B3B2DLMT","schema_version":"1.0","canonical_sha256":"0ec3a1ad9343954d7acd397dacbae51f53e8be92bb31e35e4354f12689b1af40","source":{"kind":"arxiv","id":"0801.1037","version":1},"attestation_state":"computed","paper":{"title":"Lumped and Distributed Parameter SPICE Models of TE Devices Considering Temperature Dependent Material Properties","license":"","headline":"","cross_cats":[],"primary_cat":"physics.gen-ph","authors_text":"A. Turo, D. Mitrani, J. A. Ch\\'avez, J. Salazar, M. J. Garc\\'ia","submitted_at":"2008-01-07T16:10:08Z","abstract_excerpt":"Based on simplified one-dimensional steady-state analysis of thermoelectric phenomena and on analogies between thermal and electrical domains, we propose both lumped and distributed parameter electrical models for thermoelectric devices. For lumped parameter models, constant values for material properties are extracted from polynomial fit curves evaluated at different module temperatures (hot side, cold side, average, and mean module temperature). For the case of distributed parameter models, material properties are calculated according to the mean temperature at each segment of a sectioned de"},"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":"0801.1037","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"physics.gen-ph","submitted_at":"2008-01-07T16:10:08Z","cross_cats_sorted":[],"title_canon_sha256":"e98d04ca7a18e11e7b8aefbdd576c474339133b22ced4742f1d4ec57b520f138","abstract_canon_sha256":"65209a9770a7bdf4160e48b715cca2c8d3edac8fa437d320fd6dfd024cdc1298"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:06:40.855778Z","signature_b64":"mM6ux2eV1o6PwC/qLgepejTlK7Rj1JaUNQXM/nL1kU7vKABruq7slcu4PHAdQShOHdULuQtYr2zI3nRbgEcvBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0ec3a1ad9343954d7acd397dacbae51f53e8be92bb31e35e4354f12689b1af40","last_reissued_at":"2026-07-04T15:06:40.855435Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:06:40.855435Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Lumped and Distributed Parameter SPICE Models of TE Devices Considering Temperature Dependent Material Properties","license":"","headline":"","cross_cats":[],"primary_cat":"physics.gen-ph","authors_text":"A. Turo, D. Mitrani, J. A. Ch\\'avez, J. Salazar, M. J. Garc\\'ia","submitted_at":"2008-01-07T16:10:08Z","abstract_excerpt":"Based on simplified one-dimensional steady-state analysis of thermoelectric phenomena and on analogies between thermal and electrical domains, we propose both lumped and distributed parameter electrical models for thermoelectric devices. For lumped parameter models, constant values for material properties are extracted from polynomial fit curves evaluated at different module temperatures (hot side, cold side, average, and mean module temperature). For the case of distributed parameter models, material properties are calculated according to the mean temperature at each segment of a sectioned de"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0801.1037","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/0801.1037/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":"0801.1037","created_at":"2026-07-04T15:06:40.855495+00:00"},{"alias_kind":"arxiv_version","alias_value":"0801.1037v1","created_at":"2026-07-04T15:06:40.855495+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0801.1037","created_at":"2026-07-04T15:06:40.855495+00:00"},{"alias_kind":"pith_short_12","alias_value":"B3B2DLMTIOKU","created_at":"2026-07-04T15:06:40.855495+00:00"},{"alias_kind":"pith_short_16","alias_value":"B3B2DLMTIOKU26WN","created_at":"2026-07-04T15:06:40.855495+00:00"},{"alias_kind":"pith_short_8","alias_value":"B3B2DLMT","created_at":"2026-07-04T15:06:40.855495+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/B3B2DLMTIOKU26WNHF62ZOXFD5","json":"https://pith.science/pith/B3B2DLMTIOKU26WNHF62ZOXFD5.json","graph_json":"https://pith.science/api/pith-number/B3B2DLMTIOKU26WNHF62ZOXFD5/graph.json","events_json":"https://pith.science/api/pith-number/B3B2DLMTIOKU26WNHF62ZOXFD5/events.json","paper":"https://pith.science/paper/B3B2DLMT"},"agent_actions":{"view_html":"https://pith.science/pith/B3B2DLMTIOKU26WNHF62ZOXFD5","download_json":"https://pith.science/pith/B3B2DLMTIOKU26WNHF62ZOXFD5.json","view_paper":"https://pith.science/paper/B3B2DLMT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0801.1037&json=true","fetch_graph":"https://pith.science/api/pith-number/B3B2DLMTIOKU26WNHF62ZOXFD5/graph.json","fetch_events":"https://pith.science/api/pith-number/B3B2DLMTIOKU26WNHF62ZOXFD5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/B3B2DLMTIOKU26WNHF62ZOXFD5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/B3B2DLMTIOKU26WNHF62ZOXFD5/action/storage_attestation","attest_author":"https://pith.science/pith/B3B2DLMTIOKU26WNHF62ZOXFD5/action/author_attestation","sign_citation":"https://pith.science/pith/B3B2DLMTIOKU26WNHF62ZOXFD5/action/citation_signature","submit_replication":"https://pith.science/pith/B3B2DLMTIOKU26WNHF62ZOXFD5/action/replication_record"}},"created_at":"2026-07-04T15:06:40.855495+00:00","updated_at":"2026-07-04T15:06:40.855495+00:00"}