{"paper":{"title":"Volume term of work of critical nucleus formation in terms of chemical potential difference relative to equilibrium one","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"physics.chem-ph","authors_text":"Atsushi Mori","submitted_at":"2013-05-02T03:16:09Z","abstract_excerpt":"The work of formation of a critical nucleus is sometimes written as W=n{\\Delta}{\\mu}+{\\gamma}A. The first term W_{vol}=n{\\Delta}{\\mu} is called the volume term and the second term {\\gamma}A the surface term with {\\gamma} being the interfacial tension and A the area of the nucleus. Nishioka and Kusaka [J. Chem. Phys. 96 (1992) 5370] derived W_{vol}=n{\\Delta}{\\mu} with n=V_{\\beta}/v_{\\beta} and {\\Delta}{\\mu}={\\mu}_{\\beta}(T,p_{\\alpha})-{\\mu}_{\\alpha}(T,p_{\\alpha}) by rewriting W_{vol}=-(p_{\\beta}-p_{\\alpha})V_{\\beta} by integrating the isothermal Gibbs-Duhem relation for an incompressible {\\beta"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1305.0332","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"}