{"paper":{"title":"Complementarity relation for irreversible processes near steady states","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"CBPF), CNEN, Eduardo D. Izquierdo (UBA), E. Sergio Santini (UNGS, M. Florencia Carusela (UNGS/CONICET)","submitted_at":"2012-01-03T19:29:07Z","abstract_excerpt":"A relation giving a minimum for the irreversible work in quasi-equilibrium processes was derived by Sekimoto et al. (K. Sekimoto and S. Sasa, J. Phys. Soc. Jpn. {\\bf 66} (1997), 3326) in the framework of stochastic energetics. This relation can also be written as a type of \"uncertainty principle\" in such a way that the precise determination of the Helmholtz free energy through the observation of the work $<W>$ requires an indefinitely large experimental time $\\Delta t$. In the present article, we extend this relation to the case of quasi-steady processes by using the concept of non-equilibrium"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.0923","kind":"arxiv","version":4},"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"}