Simulations and integral–equation theories for dipolar density interacting disks
- Autores
- Rufeil Fiori, Elena; Banchio, Adolfo Javier
- Año de publicación
- 2023
- Idioma
- inglés
- Tipo de recurso
- artículo
- Estado
- versión publicada
- Descripción
- Integral equation theories (IETs) based on the Ornstein–Zernike (OZ) relation can be used as an analytical tool to predict structural and thermodynamic properties and phase behavior of fluids with low numerical cost. However, there are no studies of the IETs for the dipolar density interaction potential in 2D systems, a relevant inter-domain interaction in lipid monolayers with phase coexistence. This repulsive interaction arises due to the excess dipole density of the domains, which are aligned perpendicular to the interface. This work studies the performance of three closures of the OZ equation for this novel system: Rogers–Young (RY), Modified Hypernetted Chain (MHNC), and Variational Modified Hypernetted Chain (VMHNC). For the last two closures the bridge function of a reference system is required, being the hard disk the most convenient reference system. Given that in 2D there is no analytical expressions for the hard disk correlation functions, two different approximations are proposed: one based on the Percus–Yevick approximation (PY), and the other based on an extension of the hard spheres Verlet–Weis–Henderson–Grundke parameterization (LB). The accuracy of the five approaches is evaluated by comparison of the pair correlation function and the structure factor with Monte Carlo simulation data. The results show that RY closure is only satisfactory for low–structured regimes. MHNCand VMHNC closures perform globally well and there are no significant differences between them. However, the reference system in some cases affects their performance; when the pair correlation function serves as the measure, the LB–based closures quantitatively outperform the PY ones. From the point of view of its applica-bility, LB–based closures do not have a solution for all studied interaction strength parameters, and, in general, PY–based closures are numerically preferable.
Fil: Rufeil Fiori, Elena. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - Córdoba. Instituto de Física Enrique Gaviola. Universidad Nacional de Córdoba. Instituto de Física Enrique Gaviola; Argentina
Fil: Banchio, Adolfo Javier. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - Córdoba. Instituto de Física Enrique Gaviola. Universidad Nacional de Córdoba. Instituto de Física Enrique Gaviola; Argentina - Materia
-
monolayers
integral equaiton theory
density dipolar interaction
structure - Nivel de accesibilidad
- acceso abierto
- Condiciones de uso
- https://creativecommons.org/licenses/by-nc-sa/2.5/ar/
- Repositorio
- Institución
- Consejo Nacional de Investigaciones Científicas y Técnicas
- OAI Identificador
- oai:ri.conicet.gov.ar:11336/229960
Ver los metadatos del registro completo
id |
CONICETDig_6a6a034bb97b6e562a99e30a98bfbc2b |
---|---|
oai_identifier_str |
oai:ri.conicet.gov.ar:11336/229960 |
network_acronym_str |
CONICETDig |
repository_id_str |
3498 |
network_name_str |
CONICET Digital (CONICET) |
spelling |
Simulations and integral–equation theories for dipolar density interacting disksRufeil Fiori, ElenaBanchio, Adolfo Javiermonolayersintegral equaiton theorydensity dipolar interactionstructurehttps://purl.org/becyt/ford/1.3https://purl.org/becyt/ford/1Integral equation theories (IETs) based on the Ornstein–Zernike (OZ) relation can be used as an analytical tool to predict structural and thermodynamic properties and phase behavior of fluids with low numerical cost. However, there are no studies of the IETs for the dipolar density interaction potential in 2D systems, a relevant inter-domain interaction in lipid monolayers with phase coexistence. This repulsive interaction arises due to the excess dipole density of the domains, which are aligned perpendicular to the interface. This work studies the performance of three closures of the OZ equation for this novel system: Rogers–Young (RY), Modified Hypernetted Chain (MHNC), and Variational Modified Hypernetted Chain (VMHNC). For the last two closures the bridge function of a reference system is required, being the hard disk the most convenient reference system. Given that in 2D there is no analytical expressions for the hard disk correlation functions, two different approximations are proposed: one based on the Percus–Yevick approximation (PY), and the other based on an extension of the hard spheres Verlet–Weis–Henderson–Grundke parameterization (LB). The accuracy of the five approaches is evaluated by comparison of the pair correlation function and the structure factor with Monte Carlo simulation data. The results show that RY closure is only satisfactory for low–structured regimes. MHNCand VMHNC closures perform globally well and there are no significant differences between them. However, the reference system in some cases affects their performance; when the pair correlation function serves as the measure, the LB–based closures quantitatively outperform the PY ones. From the point of view of its applica-bility, LB–based closures do not have a solution for all studied interaction strength parameters, and, in general, PY–based closures are numerically preferable.Fil: Rufeil Fiori, Elena. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - Córdoba. Instituto de Física Enrique Gaviola. Universidad Nacional de Córdoba. Instituto de Física Enrique Gaviola; ArgentinaFil: Banchio, Adolfo Javier. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - Córdoba. Instituto de Física Enrique Gaviola. Universidad Nacional de Córdoba. Instituto de Física Enrique Gaviola; ArgentinaAmerican Physical Society2023-12info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionhttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdfapplication/pdfhttp://hdl.handle.net/11336/229960Rufeil Fiori, Elena; Banchio, Adolfo Javier; Simulations and integral–equation theories for dipolar density interacting disks; American Physical Society; Physical Review E: Statistical, Nonlinear and Soft Matter Physics; 108; 6; 12-2023; 1-161539-37552470-0053CONICET DigitalCONICETenginfo:eu-repo/semantics/altIdentifier/url/https://link.aps.org/doi/10.1103/PhysRevE.108.064605info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevE.108.064605info:eu-repo/semantics/openAccesshttps://creativecommons.org/licenses/by-nc-sa/2.5/ar/reponame:CONICET Digital (CONICET)instname:Consejo Nacional de Investigaciones Científicas y Técnicas2025-09-17T11:16:15Zoai:ri.conicet.gov.ar:11336/229960instacron:CONICETInstitucionalhttp://ri.conicet.gov.ar/Organismo científico-tecnológicoNo correspondehttp://ri.conicet.gov.ar/oai/requestdasensio@conicet.gov.ar; lcarlino@conicet.gov.arArgentinaNo correspondeNo correspondeNo correspondeopendoar:34982025-09-17 11:16:15.679CONICET Digital (CONICET) - Consejo Nacional de Investigaciones Científicas y Técnicasfalse |
dc.title.none.fl_str_mv |
Simulations and integral–equation theories for dipolar density interacting disks |
title |
Simulations and integral–equation theories for dipolar density interacting disks |
spellingShingle |
Simulations and integral–equation theories for dipolar density interacting disks Rufeil Fiori, Elena monolayers integral equaiton theory density dipolar interaction structure |
title_short |
Simulations and integral–equation theories for dipolar density interacting disks |
title_full |
Simulations and integral–equation theories for dipolar density interacting disks |
title_fullStr |
Simulations and integral–equation theories for dipolar density interacting disks |
title_full_unstemmed |
Simulations and integral–equation theories for dipolar density interacting disks |
title_sort |
Simulations and integral–equation theories for dipolar density interacting disks |
dc.creator.none.fl_str_mv |
Rufeil Fiori, Elena Banchio, Adolfo Javier |
author |
Rufeil Fiori, Elena |
author_facet |
Rufeil Fiori, Elena Banchio, Adolfo Javier |
author_role |
author |
author2 |
Banchio, Adolfo Javier |
author2_role |
author |
dc.subject.none.fl_str_mv |
monolayers integral equaiton theory density dipolar interaction structure |
topic |
monolayers integral equaiton theory density dipolar interaction structure |
purl_subject.fl_str_mv |
https://purl.org/becyt/ford/1.3 https://purl.org/becyt/ford/1 |
dc.description.none.fl_txt_mv |
Integral equation theories (IETs) based on the Ornstein–Zernike (OZ) relation can be used as an analytical tool to predict structural and thermodynamic properties and phase behavior of fluids with low numerical cost. However, there are no studies of the IETs for the dipolar density interaction potential in 2D systems, a relevant inter-domain interaction in lipid monolayers with phase coexistence. This repulsive interaction arises due to the excess dipole density of the domains, which are aligned perpendicular to the interface. This work studies the performance of three closures of the OZ equation for this novel system: Rogers–Young (RY), Modified Hypernetted Chain (MHNC), and Variational Modified Hypernetted Chain (VMHNC). For the last two closures the bridge function of a reference system is required, being the hard disk the most convenient reference system. Given that in 2D there is no analytical expressions for the hard disk correlation functions, two different approximations are proposed: one based on the Percus–Yevick approximation (PY), and the other based on an extension of the hard spheres Verlet–Weis–Henderson–Grundke parameterization (LB). The accuracy of the five approaches is evaluated by comparison of the pair correlation function and the structure factor with Monte Carlo simulation data. The results show that RY closure is only satisfactory for low–structured regimes. MHNCand VMHNC closures perform globally well and there are no significant differences between them. However, the reference system in some cases affects their performance; when the pair correlation function serves as the measure, the LB–based closures quantitatively outperform the PY ones. From the point of view of its applica-bility, LB–based closures do not have a solution for all studied interaction strength parameters, and, in general, PY–based closures are numerically preferable. Fil: Rufeil Fiori, Elena. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - Córdoba. Instituto de Física Enrique Gaviola. Universidad Nacional de Córdoba. Instituto de Física Enrique Gaviola; Argentina Fil: Banchio, Adolfo Javier. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - Córdoba. Instituto de Física Enrique Gaviola. Universidad Nacional de Córdoba. Instituto de Física Enrique Gaviola; Argentina |
description |
Integral equation theories (IETs) based on the Ornstein–Zernike (OZ) relation can be used as an analytical tool to predict structural and thermodynamic properties and phase behavior of fluids with low numerical cost. However, there are no studies of the IETs for the dipolar density interaction potential in 2D systems, a relevant inter-domain interaction in lipid monolayers with phase coexistence. This repulsive interaction arises due to the excess dipole density of the domains, which are aligned perpendicular to the interface. This work studies the performance of three closures of the OZ equation for this novel system: Rogers–Young (RY), Modified Hypernetted Chain (MHNC), and Variational Modified Hypernetted Chain (VMHNC). For the last two closures the bridge function of a reference system is required, being the hard disk the most convenient reference system. Given that in 2D there is no analytical expressions for the hard disk correlation functions, two different approximations are proposed: one based on the Percus–Yevick approximation (PY), and the other based on an extension of the hard spheres Verlet–Weis–Henderson–Grundke parameterization (LB). The accuracy of the five approaches is evaluated by comparison of the pair correlation function and the structure factor with Monte Carlo simulation data. The results show that RY closure is only satisfactory for low–structured regimes. MHNCand VMHNC closures perform globally well and there are no significant differences between them. However, the reference system in some cases affects their performance; when the pair correlation function serves as the measure, the LB–based closures quantitatively outperform the PY ones. From the point of view of its applica-bility, LB–based closures do not have a solution for all studied interaction strength parameters, and, in general, PY–based closures are numerically preferable. |
publishDate |
2023 |
dc.date.none.fl_str_mv |
2023-12 |
dc.type.none.fl_str_mv |
info:eu-repo/semantics/article info:eu-repo/semantics/publishedVersion http://purl.org/coar/resource_type/c_6501 info:ar-repo/semantics/articulo |
format |
article |
status_str |
publishedVersion |
dc.identifier.none.fl_str_mv |
http://hdl.handle.net/11336/229960 Rufeil Fiori, Elena; Banchio, Adolfo Javier; Simulations and integral–equation theories for dipolar density interacting disks; American Physical Society; Physical Review E: Statistical, Nonlinear and Soft Matter Physics; 108; 6; 12-2023; 1-16 1539-3755 2470-0053 CONICET Digital CONICET |
url |
http://hdl.handle.net/11336/229960 |
identifier_str_mv |
Rufeil Fiori, Elena; Banchio, Adolfo Javier; Simulations and integral–equation theories for dipolar density interacting disks; American Physical Society; Physical Review E: Statistical, Nonlinear and Soft Matter Physics; 108; 6; 12-2023; 1-16 1539-3755 2470-0053 CONICET Digital CONICET |
dc.language.none.fl_str_mv |
eng |
language |
eng |
dc.relation.none.fl_str_mv |
info:eu-repo/semantics/altIdentifier/url/https://link.aps.org/doi/10.1103/PhysRevE.108.064605 info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevE.108.064605 |
dc.rights.none.fl_str_mv |
info:eu-repo/semantics/openAccess https://creativecommons.org/licenses/by-nc-sa/2.5/ar/ |
eu_rights_str_mv |
openAccess |
rights_invalid_str_mv |
https://creativecommons.org/licenses/by-nc-sa/2.5/ar/ |
dc.format.none.fl_str_mv |
application/pdf application/pdf |
dc.publisher.none.fl_str_mv |
American Physical Society |
publisher.none.fl_str_mv |
American Physical Society |
dc.source.none.fl_str_mv |
reponame:CONICET Digital (CONICET) instname:Consejo Nacional de Investigaciones Científicas y Técnicas |
reponame_str |
CONICET Digital (CONICET) |
collection |
CONICET Digital (CONICET) |
instname_str |
Consejo Nacional de Investigaciones Científicas y Técnicas |
repository.name.fl_str_mv |
CONICET Digital (CONICET) - Consejo Nacional de Investigaciones Científicas y Técnicas |
repository.mail.fl_str_mv |
dasensio@conicet.gov.ar; lcarlino@conicet.gov.ar |
_version_ |
1843606503193313280 |
score |
13.001348 |