{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:TJ5QCORU6IPM4A7GCQIEGJHAC7","short_pith_number":"pith:TJ5QCORU","schema_version":"1.0","canonical_sha256":"9a7b013a34f21ece03e614104324e017ccb3c5f66467dc2129f2896f082c3aa4","source":{"kind":"arxiv","id":"1409.3292","version":2},"attestation_state":"computed","paper":{"title":"Gas bubble dynamics in soft materials","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.chem-ph"],"primary_cat":"cond-mat.soft","authors_text":"J. M. Solano-Altamirano, John D. Malcolm, Saul Goldman","submitted_at":"2014-09-11T01:35:42Z","abstract_excerpt":"Epstein and Plesset's seminal work on the rate of gas bubble dissolution and growth in a simple liquid is generalized to render it applicable to a gas bubble embedded in a soft elastic medium. Both the underlying diffusion equation and the expression for the gas bubble pressure were modified to allow for the non-zero shear modulus of the elastic medium. The extension of the diffusion equation results in a trivial shift (by an additive constant) in the value of the diffusion coefficient, and does not change the form of the rate equations. But the use of a Generalized Young-Laplace equation for "},"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":"1409.3292","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2014-09-11T01:35:42Z","cross_cats_sorted":["physics.chem-ph"],"title_canon_sha256":"b55229c423a9a6afd4e87c9ed146138ff7b9ba6901494c90ab828a10dc6798b0","abstract_canon_sha256":"24bf9691a28e4edeb6e86cfd8cbda47a09665782145be7c5a0d8c3200cf5170d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:19:16.264995Z","signature_b64":"GF+B3Ga4w9eIyrS8EXPapJ9Hw9QmTCdHcTCydQf2W4cA36PqQTaaWM8d7nSn3Qf8ZKz1iKjOWtklVKk4P3c4CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9a7b013a34f21ece03e614104324e017ccb3c5f66467dc2129f2896f082c3aa4","last_reissued_at":"2026-05-18T01:19:16.264599Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:19:16.264599Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Gas bubble dynamics in soft materials","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.chem-ph"],"primary_cat":"cond-mat.soft","authors_text":"J. M. Solano-Altamirano, John D. Malcolm, Saul Goldman","submitted_at":"2014-09-11T01:35:42Z","abstract_excerpt":"Epstein and Plesset's seminal work on the rate of gas bubble dissolution and growth in a simple liquid is generalized to render it applicable to a gas bubble embedded in a soft elastic medium. Both the underlying diffusion equation and the expression for the gas bubble pressure were modified to allow for the non-zero shear modulus of the elastic medium. The extension of the diffusion equation results in a trivial shift (by an additive constant) in the value of the diffusion coefficient, and does not change the form of the rate equations. But the use of a Generalized Young-Laplace equation for "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.3292","kind":"arxiv","version":2},"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":"1409.3292","created_at":"2026-05-18T01:19:16.264667+00:00"},{"alias_kind":"arxiv_version","alias_value":"1409.3292v2","created_at":"2026-05-18T01:19:16.264667+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.3292","created_at":"2026-05-18T01:19:16.264667+00:00"},{"alias_kind":"pith_short_12","alias_value":"TJ5QCORU6IPM","created_at":"2026-05-18T12:28:49.207871+00:00"},{"alias_kind":"pith_short_16","alias_value":"TJ5QCORU6IPM4A7G","created_at":"2026-05-18T12:28:49.207871+00:00"},{"alias_kind":"pith_short_8","alias_value":"TJ5QCORU","created_at":"2026-05-18T12:28:49.207871+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/TJ5QCORU6IPM4A7GCQIEGJHAC7","json":"https://pith.science/pith/TJ5QCORU6IPM4A7GCQIEGJHAC7.json","graph_json":"https://pith.science/api/pith-number/TJ5QCORU6IPM4A7GCQIEGJHAC7/graph.json","events_json":"https://pith.science/api/pith-number/TJ5QCORU6IPM4A7GCQIEGJHAC7/events.json","paper":"https://pith.science/paper/TJ5QCORU"},"agent_actions":{"view_html":"https://pith.science/pith/TJ5QCORU6IPM4A7GCQIEGJHAC7","download_json":"https://pith.science/pith/TJ5QCORU6IPM4A7GCQIEGJHAC7.json","view_paper":"https://pith.science/paper/TJ5QCORU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1409.3292&json=true","fetch_graph":"https://pith.science/api/pith-number/TJ5QCORU6IPM4A7GCQIEGJHAC7/graph.json","fetch_events":"https://pith.science/api/pith-number/TJ5QCORU6IPM4A7GCQIEGJHAC7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TJ5QCORU6IPM4A7GCQIEGJHAC7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TJ5QCORU6IPM4A7GCQIEGJHAC7/action/storage_attestation","attest_author":"https://pith.science/pith/TJ5QCORU6IPM4A7GCQIEGJHAC7/action/author_attestation","sign_citation":"https://pith.science/pith/TJ5QCORU6IPM4A7GCQIEGJHAC7/action/citation_signature","submit_replication":"https://pith.science/pith/TJ5QCORU6IPM4A7GCQIEGJHAC7/action/replication_record"}},"created_at":"2026-05-18T01:19:16.264667+00:00","updated_at":"2026-05-18T01:19:16.264667+00:00"}