Harmonic repulsion potential: Difference between revisions

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The '''Harmonic repulsion potential''' is given by (<ref>[http://dx.doi.org/10.1103/PhysRevLett.103.245701 Ning Xu, Thomas K. Haxton, Andrea J. Liu, and Sidney R. Nagel "Equivalence of Glass Transition and Colloidal Glass Transition in the Hard-Sphere Limit", Physical Review Letters '''103''' 245701 (2009)]</ref>  Eq. 2):
The '''Harmonic repulsion potential''', designed for studies of [[Polymers |polymer]] [[micelles]], [[dendrimers]], and [[Colloids |colloidal particles]],  is given by (<ref>[http://dx.doi.org/10.1103/PhysRevLett.103.245701 Ning Xu, Thomas K. Haxton, Andrea J. Liu, and Sidney R. Nagel "Equivalence of Glass Transition and Colloidal Glass Transition in the Hard-Sphere Limit", Physical Review Letters '''103''' 245701 (2009)]</ref>  Eq. 2):


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==References==
==References==
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;Related reading
*[http://dx.doi.org/10.1063/1.5002536 V. A. Levashov "Crystalline structures of particles interacting through the harmonic-repulsive pair potential", Journal of Chemical Physics '''147''' 114503 (2017)]
[[category: models]]
[[category: models]]

Latest revision as of 11:31, 25 September 2017

The Harmonic repulsion potential, designed for studies of polymer micelles, dendrimers, and colloidal particles, is given by ([1] Eq. 2):

where is the intermolecular pair potential, is the distance between site 1 and site 2. represents a length scale and an energy. For example, for the potential looks like

Phase diagram[edit]

The phase diagram in the pressure-temperature plane has been calculated by Zhu and Lu [2].

See also[edit]

References[edit]

Related reading