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Structure of amorphous sulfur

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dc.contributor.author Eichinger, BE
dc.contributor.author Wimmer, E
dc.contributor.author Pretorius, J
dc.date.accessioned 2007-08-15T07:48:15Z
dc.date.available 2007-08-15T07:48:15Z
dc.date.issued 2001-06
dc.identifier.citation Eichinger, BE, Wimmer, E and Pretorius, J. 2001. Structure of amorphous sulfur. Macromolecular Symposia, Vol. 171(1), pp 45-56 en
dc.identifier.issn 1022-1360
dc.identifier.uri http://hdl.handle.net/10204/1109
dc.description Copyright: 2001 WILEY-VCH Verlag GmbH en
dc.description.abstract The lambda-transition of elemental sulfur occurring at about 159°C has long been associated with the conversion of cyclic S8 rings (c-S8) to amorphous polymer (a-S) via a ring opening polymerization. It is demonstrated, with the use of both density functional and Hartree-Fock quantum mechanical calculations, the existence of an energetically accessible, locally stable, hypervalent state of S that can form branch sites in the polymer. The significance of this finding is that the lambda-transition is best described as a gelation transition. The geometry of the tetravalent S atom is trigonal bipyramidal, with a lone pair occupying one of the three equatorial sites; it lies in a local energy minimum about 31 kcal/mol above the normal divalent state, and so is accessible both thermally and photochemically. Because the branched structure is formed endothermically, Le Chatelier's principle confirms that a percolation network can form on heating the element. The reactions that form branched structures are reversible, implying that the gel is fluxional. It decomposes at higher temperatures as chain scission competes with branching. The hypervalent structure provides an essential insight into the chemistry of elemental sulfur. en
dc.language.iso en en
dc.publisher WILEY-VCH Verlag GmbH en
dc.subject Amorphous sulfur en
dc.subject Molecular simulations en
dc.subject Materials design en
dc.title Structure of amorphous sulfur en
dc.type Article en
dc.identifier.apacitation Eichinger, B., Wimmer, E., & Pretorius, J. (2001). Structure of amorphous sulfur. http://hdl.handle.net/10204/1109 en_ZA
dc.identifier.chicagocitation Eichinger, BE, E Wimmer, and J Pretorius "Structure of amorphous sulfur." (2001) http://hdl.handle.net/10204/1109 en_ZA
dc.identifier.vancouvercitation Eichinger B, Wimmer E, Pretorius J. Structure of amorphous sulfur. 2001; http://hdl.handle.net/10204/1109. en_ZA
dc.identifier.ris TY - Article AU - Eichinger, BE AU - Wimmer, E AU - Pretorius, J AB - The lambda-transition of elemental sulfur occurring at about 159°C has long been associated with the conversion of cyclic S8 rings (c-S8) to amorphous polymer (a-S) via a ring opening polymerization. It is demonstrated, with the use of both density functional and Hartree-Fock quantum mechanical calculations, the existence of an energetically accessible, locally stable, hypervalent state of S that can form branch sites in the polymer. The significance of this finding is that the lambda-transition is best described as a gelation transition. The geometry of the tetravalent S atom is trigonal bipyramidal, with a lone pair occupying one of the three equatorial sites; it lies in a local energy minimum about 31 kcal/mol above the normal divalent state, and so is accessible both thermally and photochemically. Because the branched structure is formed endothermically, Le Chatelier's principle confirms that a percolation network can form on heating the element. The reactions that form branched structures are reversible, implying that the gel is fluxional. It decomposes at higher temperatures as chain scission competes with branching. The hypervalent structure provides an essential insight into the chemistry of elemental sulfur. DA - 2001-06 DB - ResearchSpace DP - CSIR KW - Amorphous sulfur KW - Molecular simulations KW - Materials design LK - https://researchspace.csir.co.za PY - 2001 SM - 1022-1360 T1 - Structure of amorphous sulfur TI - Structure of amorphous sulfur UR - http://hdl.handle.net/10204/1109 ER - en_ZA


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