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Fluidity of the system produced in relativistic pp and heavy-ion collisions: Hadron resonance gas model approach
We have estimated the dimensionless parameters such as Reynolds number (Re), Knudsen number (Kn) and Mach number (Ma) for a multi-hadron system by using the excluded volume hadron resonance gas (EVHRG) model along with Hagedorn mass spectrum to include higher resonances in the system. The size depen...
Autores principales: | , , , , |
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Lenguaje: | eng |
Publicado: |
2022
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1140/epja/s10050-023-01052-1 http://cds.cern.ch/record/2800102 |
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author | Scaria, Ronald Sahu, Dushmanta Singh, Captain R. Sahoo, Raghunath Alam, Jan-e |
author_facet | Scaria, Ronald Sahu, Dushmanta Singh, Captain R. Sahoo, Raghunath Alam, Jan-e |
author_sort | Scaria, Ronald |
collection | CERN |
description | We have estimated the dimensionless parameters such as Reynolds number (Re), Knudsen number (Kn) and Mach number (Ma) for a multi-hadron system by using the excluded volume hadron resonance gas (EVHRG) model along with Hagedorn mass spectrum to include higher resonances in the system. The size dependence of these parameters indicate that the system formed in proton+proton collisions may achieve thermal equilibrium making it unsuitable as a benchmark to analyze the properties of the system produced in heavy ion collisions at similar energies. While the magnitude of Kn can be used to study the degree of thermalization and applicability of inviscid hydrodynamics, the variations of Re and Ma with temperature (T) and baryonic chemical potential ($\mu _B$) assist to understand the change in the nature of the flow in the system. Indeed the nature of flow changes from laminar to turbulent as Re increases and the system is characterized as incompressible for low $Ma (<<1)$ and compressible for larger Ma. Ma can also be used to understand whether the flow is subsonic or supersonic. |
id | cern-2800102 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2022 |
record_format | invenio |
spelling | cern-28001022023-06-29T03:46:51Zdoi:10.1140/epja/s10050-023-01052-1doi:10.1140/epja/s10050-023-01052-1http://cds.cern.ch/record/2800102engScaria, RonaldSahu, DushmantaSingh, Captain R.Sahoo, RaghunathAlam, Jan-eFluidity of the system produced in relativistic pp and heavy-ion collisions: Hadron resonance gas model approachnucl-thNuclear Physics - Theorynucl-exNuclear Physics - Experimenthep-exParticle Physics - Experimenthep-phParticle Physics - PhenomenologyWe have estimated the dimensionless parameters such as Reynolds number (Re), Knudsen number (Kn) and Mach number (Ma) for a multi-hadron system by using the excluded volume hadron resonance gas (EVHRG) model along with Hagedorn mass spectrum to include higher resonances in the system. The size dependence of these parameters indicate that the system formed in proton+proton collisions may achieve thermal equilibrium making it unsuitable as a benchmark to analyze the properties of the system produced in heavy ion collisions at similar energies. While the magnitude of Kn can be used to study the degree of thermalization and applicability of inviscid hydrodynamics, the variations of Re and Ma with temperature (T) and baryonic chemical potential ($\mu _B$) assist to understand the change in the nature of the flow in the system. Indeed the nature of flow changes from laminar to turbulent as Re increases and the system is characterized as incompressible for low $Ma (<<1)$ and compressible for larger Ma. Ma can also be used to understand whether the flow is subsonic or supersonic.We have estimated the dimensionless parameters such as Reynolds number ($Re$), Knudsen number ($Kn$) and Mach number ($Ma$) for a multi-hadron system by using the excluded volume hadron resonance gas (EVHRG) model along with Hagedorn mass spectrum to include higher resonances in the system. The size dependence of these parameters indicate that the system formed in proton+proton collisions may achieve thermal equilibrium making it unsuitable as a benchmark to analyze the properties of the system produced in heavy ion collisions at similar energies. While the magnitude of $Kn$ can be used to study the degree of thermalization and applicability of inviscid hydrodynamics, the variations of $Re$ and $Ma$ with temperature ($T$) and baryonic chemical potential ($\mu_B$) assist to understand the change in the nature of the flow in the system. Indeed the nature of flow changes from laminar to turbulent as $Re$ increases and the system is characterized as incompressible for low $Ma (<<1)$ and compressible for larger $Ma$. $Ma$ can also be used to understand whether the flow is subsonic or supersonic.arXiv:2201.08096oai:cds.cern.ch:28001022022-01-20 |
spellingShingle | nucl-th Nuclear Physics - Theory nucl-ex Nuclear Physics - Experiment hep-ex Particle Physics - Experiment hep-ph Particle Physics - Phenomenology Scaria, Ronald Sahu, Dushmanta Singh, Captain R. Sahoo, Raghunath Alam, Jan-e Fluidity of the system produced in relativistic pp and heavy-ion collisions: Hadron resonance gas model approach |
title | Fluidity of the system produced in relativistic pp and heavy-ion collisions: Hadron resonance gas model approach |
title_full | Fluidity of the system produced in relativistic pp and heavy-ion collisions: Hadron resonance gas model approach |
title_fullStr | Fluidity of the system produced in relativistic pp and heavy-ion collisions: Hadron resonance gas model approach |
title_full_unstemmed | Fluidity of the system produced in relativistic pp and heavy-ion collisions: Hadron resonance gas model approach |
title_short | Fluidity of the system produced in relativistic pp and heavy-ion collisions: Hadron resonance gas model approach |
title_sort | fluidity of the system produced in relativistic pp and heavy-ion collisions: hadron resonance gas model approach |
topic | nucl-th Nuclear Physics - Theory nucl-ex Nuclear Physics - Experiment hep-ex Particle Physics - Experiment hep-ph Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1140/epja/s10050-023-01052-1 https://dx.doi.org/10.1140/epja/s10050-023-01052-1 http://cds.cern.ch/record/2800102 |
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