Statistical Mechanics at Strong Coupling: A Bridge between Landsberg’s Energy Levels and Hill’s Nanothermodynamics
We review and show the connection between three different theories proposed for the thermodynamic treatment of systems not obeying the additivity ansatz of classical thermodynamics. In the 1950s, Landsberg proposed that when a system comes into contact with a heat bath, its energy levels are redistr...
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doaj-85181aaa2e4648348e11f1d5ef15a73d2020-12-11T00:00:54ZengMDPI AGNanomaterials2079-49912020-12-01102471247110.3390/nano10122471Statistical Mechanics at Strong Coupling: A Bridge between Landsberg’s Energy Levels and Hill’s NanothermodynamicsRodrigo de Miguel0J. Miguel Rubí1Department of Teacher Education, Norwegian University of Science and Technology, 7491 Trondheim, NorwayDepartment of Condensed Matter Physics, University of Barcelona, 08007 Barcelona, SpainWe review and show the connection between three different theories proposed for the thermodynamic treatment of systems not obeying the additivity ansatz of classical thermodynamics. In the 1950s, Landsberg proposed that when a system comes into contact with a heat bath, its energy levels are redistributed. Based on this idea, he produced an extended thermostatistical framework that accounts for unknown interactions with the environment. A decade later, Hill devised his celebrated <i>nanothermodynamics</i>, where he introduced the concept of <i>subdivision potential</i>, a new thermodynamic variable that accounts for the vanishing additivity of increasingly smaller systems. More recently, a thermostatistical framework <i>at strong coupling</i> has been formulated to account for the presence of the environment through a Hamiltonian of mean force. We show that this modified Hamiltonian yields a temperature-dependent energy landscape as earlier suggested by Landsberg, and it provides a thermostatistical foundation for the subdivision potential, which is the cornerstone of Hill’s nanothermodynamics.https://www.mdpi.com/2079-4991/10/12/2471thermodynamics at strong coupling<i>temperature-dependent</i> energy levelsthermodynamics of small systemsnanothermodynamics |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Rodrigo de Miguel J. Miguel Rubí |
spellingShingle |
Rodrigo de Miguel J. Miguel Rubí Statistical Mechanics at Strong Coupling: A Bridge between Landsberg’s Energy Levels and Hill’s Nanothermodynamics Nanomaterials thermodynamics at strong coupling <i>temperature-dependent</i> energy levels thermodynamics of small systems nanothermodynamics |
author_facet |
Rodrigo de Miguel J. Miguel Rubí |
author_sort |
Rodrigo de Miguel |
title |
Statistical Mechanics at Strong Coupling: A Bridge between Landsberg’s Energy Levels and Hill’s Nanothermodynamics |
title_short |
Statistical Mechanics at Strong Coupling: A Bridge between Landsberg’s Energy Levels and Hill’s Nanothermodynamics |
title_full |
Statistical Mechanics at Strong Coupling: A Bridge between Landsberg’s Energy Levels and Hill’s Nanothermodynamics |
title_fullStr |
Statistical Mechanics at Strong Coupling: A Bridge between Landsberg’s Energy Levels and Hill’s Nanothermodynamics |
title_full_unstemmed |
Statistical Mechanics at Strong Coupling: A Bridge between Landsberg’s Energy Levels and Hill’s Nanothermodynamics |
title_sort |
statistical mechanics at strong coupling: a bridge between landsberg’s energy levels and hill’s nanothermodynamics |
publisher |
MDPI AG |
series |
Nanomaterials |
issn |
2079-4991 |
publishDate |
2020-12-01 |
description |
We review and show the connection between three different theories proposed for the thermodynamic treatment of systems not obeying the additivity ansatz of classical thermodynamics. In the 1950s, Landsberg proposed that when a system comes into contact with a heat bath, its energy levels are redistributed. Based on this idea, he produced an extended thermostatistical framework that accounts for unknown interactions with the environment. A decade later, Hill devised his celebrated <i>nanothermodynamics</i>, where he introduced the concept of <i>subdivision potential</i>, a new thermodynamic variable that accounts for the vanishing additivity of increasingly smaller systems. More recently, a thermostatistical framework <i>at strong coupling</i> has been formulated to account for the presence of the environment through a Hamiltonian of mean force. We show that this modified Hamiltonian yields a temperature-dependent energy landscape as earlier suggested by Landsberg, and it provides a thermostatistical foundation for the subdivision potential, which is the cornerstone of Hill’s nanothermodynamics. |
topic |
thermodynamics at strong coupling <i>temperature-dependent</i> energy levels thermodynamics of small systems nanothermodynamics |
url |
https://www.mdpi.com/2079-4991/10/12/2471 |
work_keys_str_mv |
AT rodrigodemiguel statisticalmechanicsatstrongcouplingabridgebetweenlandsbergsenergylevelsandhillsnanothermodynamics AT jmiguelrubi statisticalmechanicsatstrongcouplingabridgebetweenlandsbergsenergylevelsandhillsnanothermodynamics |
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