Evaluation of the spreading thermal resistance for rough spheres
- Autores
- Luzi, Carlos Daniel; Keegan, Sergio Dario; Mariani, Nestor Javier; Barreto, Guillermo Fernando
- Año de publicación
- 2015
- Idioma
- inglés
- Tipo de recurso
- artículo
- Estado
- versión publicada
- Descripción
- The solid-solid contact of rough spherical particles in packed beds takes place by the deformation of individual asperities that transmit the stresses to the main body of the particles. This causes an elastically deformed area (a disk of radius a, most usually much smaller than the particle radius) enclosing the micro-contacts. Micro thermal resistances around the contact spots can be described in terms of a profile of thermal conductance h(r) that decreases toward the disk edge. An additional thermal resistance, the spreading resistance, is caused by the convergence of flux lines in the bulk of the spheres towards the reduced section of the disk. The described mechanism has been modeled by Bahrami et al. (2006) and a formulation was provided to predict the contribution of contact areas to the effective thermal conductivity. The spreading resistance Ωa is re-evaluated in this work on account of the h(r) profile, by means of numerical calculations. It is found that the shape of h(r) has a large impact on Ωa and a weaker, but still significant, effect on the overall contact resistance. The results of Ωa have been suitably correlated for a conductance profile of the form h(r) = h0 [1 - (r/a)2]p.
Fil: Luzi, Carlos Daniel. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - La Plata. Centro de Investigación y Desarrollo en Ciencias Aplicadas "Dr. Jorge J. Ronco". Universidad Nacional de la Plata. Facultad de Ciencias Exactas. Centro de Investigación y Desarrollo en Ciencias Aplicadas; Argentina
Fil: Keegan, Sergio Dario. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - La Plata. Centro de Investigación y Desarrollo en Ciencias Aplicadas "Dr. Jorge J. Ronco". Universidad Nacional de la Plata. Facultad de Ciencias Exactas. Centro de Investigación y Desarrollo en Ciencias Aplicadas; Argentina
Fil: Mariani, Nestor Javier. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - La Plata. Centro de Investigación y Desarrollo en Ciencias Aplicadas "Dr. Jorge J. Ronco". Universidad Nacional de la Plata. Facultad de Ciencias Exactas. Centro de Investigación y Desarrollo en Ciencias Aplicadas; Argentina
Fil: Barreto, Guillermo Fernando. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - La Plata. Centro de Investigación y Desarrollo en Ciencias Aplicadas "Dr. Jorge J. Ronco". Universidad Nacional de la Plata. Facultad de Ciencias Exactas. Centro de Investigación y Desarrollo en Ciencias Aplicadas; Argentina - Materia
-
Effective Thermal Conductivity
Overall Contact Resistance
Spreading Thermal Resistance - Nivel de accesibilidad
- acceso abierto
- Condiciones de uso
- https://creativecommons.org/licenses/by-nc-nd/2.5/ar/
- Repositorio
.jpg)
- Institución
- Consejo Nacional de Investigaciones Científicas y Técnicas
- OAI Identificador
- oai:ri.conicet.gov.ar:11336/71247
Ver los metadatos del registro completo
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Evaluation of the spreading thermal resistance for rough spheresLuzi, Carlos DanielKeegan, Sergio DarioMariani, Nestor JavierBarreto, Guillermo FernandoEffective Thermal ConductivityOverall Contact ResistanceSpreading Thermal Resistancehttps://purl.org/becyt/ford/2.4https://purl.org/becyt/ford/2https://purl.org/becyt/ford/2.4https://purl.org/becyt/ford/2The solid-solid contact of rough spherical particles in packed beds takes place by the deformation of individual asperities that transmit the stresses to the main body of the particles. This causes an elastically deformed area (a disk of radius a, most usually much smaller than the particle radius) enclosing the micro-contacts. Micro thermal resistances around the contact spots can be described in terms of a profile of thermal conductance h(r) that decreases toward the disk edge. An additional thermal resistance, the spreading resistance, is caused by the convergence of flux lines in the bulk of the spheres towards the reduced section of the disk. The described mechanism has been modeled by Bahrami et al. (2006) and a formulation was provided to predict the contribution of contact areas to the effective thermal conductivity. The spreading resistance Ωa is re-evaluated in this work on account of the h(r) profile, by means of numerical calculations. It is found that the shape of h(r) has a large impact on Ωa and a weaker, but still significant, effect on the overall contact resistance. The results of Ωa have been suitably correlated for a conductance profile of the form h(r) = h0 [1 - (r/a)2]p.Fil: Luzi, Carlos Daniel. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - La Plata. Centro de Investigación y Desarrollo en Ciencias Aplicadas "Dr. Jorge J. Ronco". Universidad Nacional de la Plata. Facultad de Ciencias Exactas. Centro de Investigación y Desarrollo en Ciencias Aplicadas; ArgentinaFil: Keegan, Sergio Dario. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - La Plata. Centro de Investigación y Desarrollo en Ciencias Aplicadas "Dr. Jorge J. Ronco". Universidad Nacional de la Plata. Facultad de Ciencias Exactas. Centro de Investigación y Desarrollo en Ciencias Aplicadas; ArgentinaFil: Mariani, Nestor Javier. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - La Plata. Centro de Investigación y Desarrollo en Ciencias Aplicadas "Dr. Jorge J. Ronco". Universidad Nacional de la Plata. Facultad de Ciencias Exactas. Centro de Investigación y Desarrollo en Ciencias Aplicadas; ArgentinaFil: Barreto, Guillermo Fernando. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - La Plata. Centro de Investigación y Desarrollo en Ciencias Aplicadas "Dr. Jorge J. Ronco". Universidad Nacional de la Plata. Facultad de Ciencias Exactas. Centro de Investigación y Desarrollo en Ciencias Aplicadas; ArgentinaPergamon-Elsevier Science Ltd2015-07info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionhttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdfapplication/pdfapplication/pdfhttp://hdl.handle.net/11336/71247Luzi, Carlos Daniel; Keegan, Sergio Dario; Mariani, Nestor Javier; Barreto, Guillermo Fernando; Evaluation of the spreading thermal resistance for rough spheres; Pergamon-Elsevier Science Ltd; International Journal Of Heat And Mass Transfer; 86; 7-2015; 826-8310017-9310CONICET DigitalCONICETenginfo:eu-repo/semantics/altIdentifier/doi/10.1016/j.ijheatmasstransfer.2015.03.048info:eu-repo/semantics/altIdentifier/url/https://www.sciencedirect.com/science/article/pii/S0017931015003063info:eu-repo/semantics/openAccesshttps://creativecommons.org/licenses/by-nc-nd/2.5/ar/reponame:CONICET Digital (CONICET)instname:Consejo Nacional de Investigaciones Científicas y Técnicas2025-11-05T09:40:06Zoai:ri.conicet.gov.ar:11336/71247instacron: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:34982025-11-05 09:40:07.0CONICET Digital (CONICET) - Consejo Nacional de Investigaciones Científicas y Técnicasfalse |
| dc.title.none.fl_str_mv |
Evaluation of the spreading thermal resistance for rough spheres |
| title |
Evaluation of the spreading thermal resistance for rough spheres |
| spellingShingle |
Evaluation of the spreading thermal resistance for rough spheres Luzi, Carlos Daniel Effective Thermal Conductivity Overall Contact Resistance Spreading Thermal Resistance |
| title_short |
Evaluation of the spreading thermal resistance for rough spheres |
| title_full |
Evaluation of the spreading thermal resistance for rough spheres |
| title_fullStr |
Evaluation of the spreading thermal resistance for rough spheres |
| title_full_unstemmed |
Evaluation of the spreading thermal resistance for rough spheres |
| title_sort |
Evaluation of the spreading thermal resistance for rough spheres |
| dc.creator.none.fl_str_mv |
Luzi, Carlos Daniel Keegan, Sergio Dario Mariani, Nestor Javier Barreto, Guillermo Fernando |
| author |
Luzi, Carlos Daniel |
| author_facet |
Luzi, Carlos Daniel Keegan, Sergio Dario Mariani, Nestor Javier Barreto, Guillermo Fernando |
| author_role |
author |
| author2 |
Keegan, Sergio Dario Mariani, Nestor Javier Barreto, Guillermo Fernando |
| author2_role |
author author author |
| dc.subject.none.fl_str_mv |
Effective Thermal Conductivity Overall Contact Resistance Spreading Thermal Resistance |
| topic |
Effective Thermal Conductivity Overall Contact Resistance Spreading Thermal Resistance |
| purl_subject.fl_str_mv |
https://purl.org/becyt/ford/2.4 https://purl.org/becyt/ford/2 https://purl.org/becyt/ford/2.4 https://purl.org/becyt/ford/2 |
| dc.description.none.fl_txt_mv |
The solid-solid contact of rough spherical particles in packed beds takes place by the deformation of individual asperities that transmit the stresses to the main body of the particles. This causes an elastically deformed area (a disk of radius a, most usually much smaller than the particle radius) enclosing the micro-contacts. Micro thermal resistances around the contact spots can be described in terms of a profile of thermal conductance h(r) that decreases toward the disk edge. An additional thermal resistance, the spreading resistance, is caused by the convergence of flux lines in the bulk of the spheres towards the reduced section of the disk. The described mechanism has been modeled by Bahrami et al. (2006) and a formulation was provided to predict the contribution of contact areas to the effective thermal conductivity. The spreading resistance Ωa is re-evaluated in this work on account of the h(r) profile, by means of numerical calculations. It is found that the shape of h(r) has a large impact on Ωa and a weaker, but still significant, effect on the overall contact resistance. The results of Ωa have been suitably correlated for a conductance profile of the form h(r) = h0 [1 - (r/a)2]p. Fil: Luzi, Carlos Daniel. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - La Plata. Centro de Investigación y Desarrollo en Ciencias Aplicadas "Dr. Jorge J. Ronco". Universidad Nacional de la Plata. Facultad de Ciencias Exactas. Centro de Investigación y Desarrollo en Ciencias Aplicadas; Argentina Fil: Keegan, Sergio Dario. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - La Plata. Centro de Investigación y Desarrollo en Ciencias Aplicadas "Dr. Jorge J. Ronco". Universidad Nacional de la Plata. Facultad de Ciencias Exactas. Centro de Investigación y Desarrollo en Ciencias Aplicadas; Argentina Fil: Mariani, Nestor Javier. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - La Plata. Centro de Investigación y Desarrollo en Ciencias Aplicadas "Dr. Jorge J. Ronco". Universidad Nacional de la Plata. Facultad de Ciencias Exactas. Centro de Investigación y Desarrollo en Ciencias Aplicadas; Argentina Fil: Barreto, Guillermo Fernando. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - La Plata. Centro de Investigación y Desarrollo en Ciencias Aplicadas "Dr. Jorge J. Ronco". Universidad Nacional de la Plata. Facultad de Ciencias Exactas. Centro de Investigación y Desarrollo en Ciencias Aplicadas; Argentina |
| description |
The solid-solid contact of rough spherical particles in packed beds takes place by the deformation of individual asperities that transmit the stresses to the main body of the particles. This causes an elastically deformed area (a disk of radius a, most usually much smaller than the particle radius) enclosing the micro-contacts. Micro thermal resistances around the contact spots can be described in terms of a profile of thermal conductance h(r) that decreases toward the disk edge. An additional thermal resistance, the spreading resistance, is caused by the convergence of flux lines in the bulk of the spheres towards the reduced section of the disk. The described mechanism has been modeled by Bahrami et al. (2006) and a formulation was provided to predict the contribution of contact areas to the effective thermal conductivity. The spreading resistance Ωa is re-evaluated in this work on account of the h(r) profile, by means of numerical calculations. It is found that the shape of h(r) has a large impact on Ωa and a weaker, but still significant, effect on the overall contact resistance. The results of Ωa have been suitably correlated for a conductance profile of the form h(r) = h0 [1 - (r/a)2]p. |
| publishDate |
2015 |
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2015-07 |
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info:eu-repo/semantics/article info:eu-repo/semantics/publishedVersion http://purl.org/coar/resource_type/c_6501 info:ar-repo/semantics/articulo |
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article |
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publishedVersion |
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http://hdl.handle.net/11336/71247 Luzi, Carlos Daniel; Keegan, Sergio Dario; Mariani, Nestor Javier; Barreto, Guillermo Fernando; Evaluation of the spreading thermal resistance for rough spheres; Pergamon-Elsevier Science Ltd; International Journal Of Heat And Mass Transfer; 86; 7-2015; 826-831 0017-9310 CONICET Digital CONICET |
| url |
http://hdl.handle.net/11336/71247 |
| identifier_str_mv |
Luzi, Carlos Daniel; Keegan, Sergio Dario; Mariani, Nestor Javier; Barreto, Guillermo Fernando; Evaluation of the spreading thermal resistance for rough spheres; Pergamon-Elsevier Science Ltd; International Journal Of Heat And Mass Transfer; 86; 7-2015; 826-831 0017-9310 CONICET Digital CONICET |
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eng |
| language |
eng |
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info:eu-repo/semantics/altIdentifier/doi/10.1016/j.ijheatmasstransfer.2015.03.048 info:eu-repo/semantics/altIdentifier/url/https://www.sciencedirect.com/science/article/pii/S0017931015003063 |
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Pergamon-Elsevier Science Ltd |
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Pergamon-Elsevier Science Ltd |
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