Line tension: Difference between revisions
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==References== | ==References== | ||
*[http://dx.doi.org/10.1063/1.2799990 L. Schimmele, M. Napiórkowski and S. Dietrich "Conceptual aspects of line tensions", Journal of Chemical Physics '''127''' 164715 (2007)] | |||
*[http://dx.doi.org/10.1063/1.3206735 Mantu Santra and Biman Bagchi "Line tension of a two dimensional gas-liquid interface", Journal of Chemical Physics '''131''' 084705 (2009)] | |||
[[Category: Confined systems]] | [[Category: Confined systems]] | ||
Revision as of 13:51, 26 August 2009
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The line tension () is attributed to the contact line along which three interfaces for the three thermodynamic phases, Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \alpha} , Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \beta} and Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \gamma} meet. It is defined as the line contribution to the grand potential per unit length of the contact line.
