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): | ||
:<math> | :<math> | ||
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</math> | </math> | ||
where <math> \Phi_{12}\left( r \right) </math> is the [[intermolecular pair potential]], <math>r := |\mathbf{r}_1 - \mathbf{r}_2|</math> is the distance between site 1 and site 2. <math>\sigma</math> represents a length scale and <math>\epsilon</math> an energy. | where <math> \Phi_{12}\left( r \right) </math> is the [[intermolecular pair potential]], <math>r := |\mathbf{r}_1 - \mathbf{r}_2|</math> is the distance between site 1 and site 2. <math>\sigma</math> represents a length scale and <math>\epsilon</math> an energy. For example, for <math>\epsilon=20</math> the potential looks like | ||
:[[Image:harmonic_sphere.png|500px]] | |||
==Phase diagram== | ==Phase diagram== | ||
The [[Phase diagrams |phase diagram]] in the [[Phase diagrams: Pressure-temperature plane | pressure-temperature plane]] has been calculated by Zhu and Lu <ref>[http://dx.doi.org/10.1063/1.3548886 You-Liang Zhu and Zhong-Yuan Lu "Phase diagram of spherical particles interacted with harmonic repulsions", Journal of Chemical Physics '''134''' 044903 (2011)]</ref>. | The [[Phase diagrams |phase diagram]] in the [[Phase diagrams: Pressure-temperature plane | pressure-temperature plane]] has been calculated by Zhu and Lu <ref>[http://dx.doi.org/10.1063/1.3548886 You-Liang Zhu and Zhong-Yuan Lu "Phase diagram of spherical particles interacted with harmonic repulsions", Journal of Chemical Physics '''134''' 044903 (2011)]</ref>. | ||
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==References== | ==References== | ||
<references/> | <references/> | ||
;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]
- ↑ 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)
- ↑ You-Liang Zhu and Zhong-Yuan Lu "Phase diagram of spherical particles interacted with harmonic repulsions", Journal of Chemical Physics 134 044903 (2011)
- Related reading