{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:B3D46KJQYI7QPVDA5CTXG43K3G","short_pith_number":"pith:B3D46KJQ","schema_version":"1.0","canonical_sha256":"0ec7cf2930c23f07d460e8a773736ad984563df0d772dd096dd8ed5dc89dd05a","source":{"kind":"arxiv","id":"1308.2981","version":1},"attestation_state":"computed","paper":{"title":"One dimensional Newton's equation with variable mass","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"M. Halilsoy, S. Habib Mazharimousavi","submitted_at":"2013-07-06T19:07:23Z","abstract_excerpt":"We revisit Newton's equation of motion in one dimension when the moving particle has a variable mass m(x,t) depending both on position (x) and time (t). Geometrically the mass function is identified with one of the metric function in a 1+1-dimensional spacetime. As a reflection of the equivalence principle geodesics equation gives the Newton's law of motion leaving the right hand side to be supplemented by the external forces. The resulting equation involves the speed of light so that our equation of motion addresses a wider scope than the customary classical mechanics. In the limit of infinit"},"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":"1308.2981","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2013-07-06T19:07:23Z","cross_cats_sorted":[],"title_canon_sha256":"ebc74a20f32658c39c206acb1456832815515259a688e76913a3908634a960fe","abstract_canon_sha256":"6155c4b50cc7d6ac7896ad937092254835ffed525e3cafcc69efdaec250cf4ef"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:15:57.030169Z","signature_b64":"4455aqpV1ZKULVVzpERu0H/W5vZQcveN6p4L3PJI2qqblnu9lRYKPB3iVFUFjTROGTvJtximztUoxqQ3s1nXAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0ec7cf2930c23f07d460e8a773736ad984563df0d772dd096dd8ed5dc89dd05a","last_reissued_at":"2026-05-18T03:15:57.029591Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:15:57.029591Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"One dimensional Newton's equation with variable mass","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"M. Halilsoy, S. Habib Mazharimousavi","submitted_at":"2013-07-06T19:07:23Z","abstract_excerpt":"We revisit Newton's equation of motion in one dimension when the moving particle has a variable mass m(x,t) depending both on position (x) and time (t). Geometrically the mass function is identified with one of the metric function in a 1+1-dimensional spacetime. As a reflection of the equivalence principle geodesics equation gives the Newton's law of motion leaving the right hand side to be supplemented by the external forces. The resulting equation involves the speed of light so that our equation of motion addresses a wider scope than the customary classical mechanics. In the limit of infinit"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1308.2981","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":"1308.2981","created_at":"2026-05-18T03:15:57.029679+00:00"},{"alias_kind":"arxiv_version","alias_value":"1308.2981v1","created_at":"2026-05-18T03:15:57.029679+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1308.2981","created_at":"2026-05-18T03:15:57.029679+00:00"},{"alias_kind":"pith_short_12","alias_value":"B3D46KJQYI7Q","created_at":"2026-05-18T12:27:38.830355+00:00"},{"alias_kind":"pith_short_16","alias_value":"B3D46KJQYI7QPVDA","created_at":"2026-05-18T12:27:38.830355+00:00"},{"alias_kind":"pith_short_8","alias_value":"B3D46KJQ","created_at":"2026-05-18T12:27:38.830355+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/B3D46KJQYI7QPVDA5CTXG43K3G","json":"https://pith.science/pith/B3D46KJQYI7QPVDA5CTXG43K3G.json","graph_json":"https://pith.science/api/pith-number/B3D46KJQYI7QPVDA5CTXG43K3G/graph.json","events_json":"https://pith.science/api/pith-number/B3D46KJQYI7QPVDA5CTXG43K3G/events.json","paper":"https://pith.science/paper/B3D46KJQ"},"agent_actions":{"view_html":"https://pith.science/pith/B3D46KJQYI7QPVDA5CTXG43K3G","download_json":"https://pith.science/pith/B3D46KJQYI7QPVDA5CTXG43K3G.json","view_paper":"https://pith.science/paper/B3D46KJQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1308.2981&json=true","fetch_graph":"https://pith.science/api/pith-number/B3D46KJQYI7QPVDA5CTXG43K3G/graph.json","fetch_events":"https://pith.science/api/pith-number/B3D46KJQYI7QPVDA5CTXG43K3G/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/B3D46KJQYI7QPVDA5CTXG43K3G/action/timestamp_anchor","attest_storage":"https://pith.science/pith/B3D46KJQYI7QPVDA5CTXG43K3G/action/storage_attestation","attest_author":"https://pith.science/pith/B3D46KJQYI7QPVDA5CTXG43K3G/action/author_attestation","sign_citation":"https://pith.science/pith/B3D46KJQYI7QPVDA5CTXG43K3G/action/citation_signature","submit_replication":"https://pith.science/pith/B3D46KJQYI7QPVDA5CTXG43K3G/action/replication_record"}},"created_at":"2026-05-18T03:15:57.029679+00:00","updated_at":"2026-05-18T03:15:57.029679+00:00"}