{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2026,2,8]],"date-time":"2026-02-08T00:22:07Z","timestamp":1770510127067,"version":"3.49.0"},"reference-count":22,"publisher":"MDPI AG","issue":"3","license":[{"start":{"date-parts":[[2010,3,11]],"date-time":"2010-03-11T00:00:00Z","timestamp":1268265600000},"content-version":"vor","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/3.0\/"}],"content-domain":{"domain":[],"crossmark-restriction":false},"short-container-title":["Entropy"],"abstract":"<jats:p>Spontaneous transitions of an isolated system from one macroscopic state to another (relaxation processes) are accompanied by a change of entropy. Following Jaynes\u2019 MaxEnt formalism, it is shown that practically all the possible microscopic developments of a system, within a fixed time interval, are accompanied by the maximum possible entropy change. In other words relaxation processes are accompanied by maximum entropy production.<\/jats:p>","DOI":"10.3390\/e12030473","type":"journal-article","created":{"date-parts":[[2010,3,14]],"date-time":"2010-03-14T13:26:04Z","timestamp":1268573164000},"page":"473-479","update-policy":"https:\/\/doi.org\/10.3390\/mdpi_crossmark_policy","source":"Crossref","is-referenced-by-count":11,"title":["Relaxation Processes and the Maximum Entropy Production Principle"],"prefix":"10.3390","volume":"12","author":[{"given":"Pa\u0161ko","family":"\u017dupanovi\u0107","sequence":"first","affiliation":[{"name":"Faculty of Science, University of Split, Teslina 12, 21000 Split, Croatia"}]},{"given":"Sre\u0107ko","family":"Botri\u0107","sequence":"additional","affiliation":[{"name":"Faculty of Electrical Engineering, Mechanical Engineering and Naval Architecture, University of Split, R. 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