Onsager, Lars
Published: August 18, 2006, 6:32 pm
Updated: August 18, 2006, 6:32 pm
This article has been reviewed by the following Topic Editor:
Peter Saundry
Lars Onsager (1903-1976), a Norwegian-born US physical chemist whose pioneering work in non-equilibrium thermodynamics earned him the 1968 Nobel Prize for Chemistry. Onsager also formulated a general mathematical expression about the behavior of nonreversible chemical processes that has been described as the “fourth law of thermodynamics.” He formulated the Onsager reciprocal relations, which express the equality of certain relations between flows and forces in thermodynamic systems out of equilibrium, but where a notion of local equilibrium exists.
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Citation
Cutler J. Cleveland (Lead Author);Peter Saundry (Topic Editor) "Onsager, Lars". In: Encyclopedia of Earth. Eds. Cutler J. Cleveland (Washington, D.C.: Environmental Information Coalition, National Council for Science and the Environment). [First published in the Encyclopedia of Earth August 18, 2006; Last revised Date August 18, 2006; Retrieved May 23, 2013 <http://www.eoearth.org/article/Onsager,_Lars>
The Author
Cutler J. Cleveland is Professor of Earth and Environment at Boston University, where he also is on the faculty of the Center for Energy and Environmental Studies. Professor Cleveland is Editor-in-Chief of the Encyclopedia of Energy (Elsevier, 2004), winner of an American Library Association award, the Dictionary of Energy (Elsevier, 2005), Handbook of Energy (Elsevier, forthcoming), and is the Founding Editor-in-Chief of the Encyclopedia of Earth. He is the recipient of the Adelma ... (Full Bio)
Lars Onsager (1903-1976), a Norwegian-born US physical chemist whose pioneering work in non-equilibrium thermodynamics earned him the 1968 Nobel Prize for Chemistry. Onsager also formulated a general mathematical expression about the behavior of nonreversible chemical processes that has been described as the “fourth law of thermodynamics.” He formulated the Onsager reciprocal relations, which express the equality of certain relations between flows and forces in thermodynamic systems out of equilibrium, but where a notion of local equilibrium exists.
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