Complementarity relation for irreversible processes near steady states

A relation giving a minimum for the irreversible work in quasi-equilibrium processes was derived by Sekimoto et al. [K. Sekimoto, S. Sasa, J. Phys. Soc. Japan 66 [1997] 3326] in the framework of stochastic energetics. This relation can also be written as a type of "uncertainty principle"...

Descripción completa

Guardado en:
Detalles Bibliográficos
Autor principal: Santini, E. S.
Otros Autores: Carusela, M. F., Izquierdo, E. D.
Formato: Artículo
Lenguaje:Inglés
Materias:
RNA
Acceso en línea:http://ri.agro.uba.ar/files/intranet/articulo/2013santini.pdf
LINK AL EDITOR
Aporte de:Registro referencial: Solicitar el recurso aquí
LEADER 06374cab a22011297a 4500
001 AR-BaUFA000466
003 AR-BaUFA
005 20210706174711.0
008 181208t2013 |||||o|||||00||||eng d
999 |c 46900  |d 46900 
022 |a 0378-4371 
024 |a 10.1016/j.physa.2013.06.045 
040 |a AR-BaUFA  |c AR-BaUFA 
100 1 |a Santini, E. S.  |9 72481 
245 0 0 |a Complementarity relation for irreversible processes near steady states 
520 |a A relation giving a minimum for the irreversible work in quasi-equilibrium processes was derived by Sekimoto et al. [K. Sekimoto, S. Sasa, J. Phys. Soc. Japan 66 [1997] 3326] in the framework of stochastic energetics. This relation can also be written as a type of "uncertainty principle" in such a way that the precise determination of the Helmholtz free energy through the observation of the work [W] requires an indefinitely large experimental time delta t. In the present article, we extend this relation to the case of quasi-steady processes by using the concept of non-equilibrium Helmholtz free energy. We give a formulation of the second law for these processes that extends that presented by Sekimoto [K. Sekimoto, Prog. Theoret. Phys. Suppl. No. 130 [1998] 17] by a term of the first order in the inverse of the experimental time. As an application of our results, two possible experimental situations are considered: stretching of a RNA molecule and the drag of a dipolar particle in the presence of a gradient of electric force. 
653 0 |a FLUCTUATION PHENOMENA 
653 0 |a LANGEVIN EQUATION 
653 0 |a STOCHASTIC ENERGETICS 
653 0 |a THERMODYNAMICS 
653 0 |a COMPLEMENTARITY RELATIONS 
653 0 |a IRREVERSIBLE PROCESS 
653 0 |a PRECISE DETERMINATIONS 
653 0 |a QUASI-EQUILIBRIUM PROCESS 
653 0 |a UNCERTAINTY PRINCIPLES 
653 0 |a DIFFERENTIAL EQUATIONS 
653 0 |a FREE ENERGY 
653 0 |a RNA 
653 0 |a STOCHASTIC SYSTEMS 
653 0 |a STATISTICAL MECHANICS 
700 1 |a Carusela, M. F.  |9 72482 
700 1 |a Izquierdo, E. D.  |9 72483 
773 |t Physica A: Statistical Mechanics and its Applications  |g vol.392, no.20 (2013), p.4856-4867 
856 |u http://ri.agro.uba.ar/files/intranet/articulo/2013santini.pdf  |i En reservorio  |q application/pdf  |f 2013santini  |x MIGRADOS2018 
856 |u http://www.elsevier.com/  |x MIGRADOS2018  |z LINK AL EDITOR 
900 |a as 
900 |a 20141009 
900 |a N13 
900 |a SCOPUS 
900 |a N13SCOPUS 
900 |a a 
900 |a s 
900 |a ARTICULO 
900 |a EN LINEA 
900 |a 03784371 
900 |a 10.1016/j.physa.2013.06.045 
900 |a ^tComplementarity relation for irreversible processes near steady states 
900 |a ^aSantini^bE.S. 
900 |a ^aCarusela^bM.F. 
900 |a ^aIzquierdo^bE.D. 
900 |a ^aSantini^bE. S. 
900 |a ^aCarusela^bM. F. 
900 |a ^aIzquierdo^bE. D. 
900 |a ^aSantini^bE.S.^tComissão Nacional de Energia Nuclear, Rua General Severiano 90, Botafogo [22290-901], Rio de Janeiro, RJ, Brazil 
900 |a ^aSantini, E.S.^tUniversidad Nacional de General Sarmiento, Instituto de Ciencias, J^tM^tGutiérrez 1150, Malvinas Argentinas (1613), Pcia de Buenos Aires, Argentina 
900 |a ^aSantini, E.S.^tCentro Brasileiro de Pesquisas Físicas - ICRA-BR, Rua Dr. Xavier Sigaud 150, Urca (22290-180), Rio de Janeiro, RJ, Brazil 
900 |a ^aCarusela^bM.F.^tUniversidad Nacional de General Sarmiento, Instituto de Ciencias, J. M. Gutiérrez 1150, Malvinas Argentinas [1613], Pcia de Buenos Aires, Argentina 
900 |a ^aCarusela, M.F.^tConsejo Nacional de Investigaciones Científicas y Técnicas, Av. Rivadavia 1917, (1033)-Buenos Aires, Argentina 
900 |a ^aIzquierdo, E.D.^tCiclo Básico Común, Universidad de Buenos Aires, Cdad. Universitaria, Pab. 3, (1428) Buenos Aires, Argentina 
900 |a ^aIzquierdo, E.D.^tFacultad de Agronomía, Universidad de Buenos Aires, Av. San Martín 4453, Cap^tFed., Buenos Aires (C1417DSE), Argentina 
900 |a ^tPhysica A: Statistical Mechanics and its Applications^cPhys A Stat Mech Appl 
900 |a en 
900 |a 4856 
900 |a ^i 
900 |a Vol. 392, no. 20 
900 |a 4867 
900 |a FLUCTUATION PHENOMENA 
900 |a LANGEVIN EQUATION 
900 |a STOCHASTIC ENERGETICS 
900 |a THERMODYNAMICS 
900 |a COMPLEMENTARITY RELATIONS 
900 |a IRREVERSIBLE PROCESS 
900 |a PRECISE DETERMINATIONS 
900 |a QUASI-EQUILIBRIUM PROCESS 
900 |a UNCERTAINTY PRINCIPLES 
900 |a DIFFERENTIAL EQUATIONS 
900 |a FREE ENERGY 
900 |a RNA 
900 |a STOCHASTIC SYSTEMS 
900 |a STATISTICAL MECHANICS 
900 |a A relation giving a minimum for the irreversible work in quasi-equilibrium processes was derived by Sekimoto et al. [K. Sekimoto, S. Sasa, J. Phys. Soc. Japan 66 [1997] 3326] in the framework of stochastic energetics. This relation can also be written as a type of "uncertainty principle" in such a way that the precise determination of the Helmholtz free energy through the observation of the work [W] requires an indefinitely large experimental time delta t. In the present article, we extend this relation to the case of quasi-steady processes by using the concept of non-equilibrium Helmholtz free energy. We give a formulation of the second law for these processes that extends that presented by Sekimoto [K. Sekimoto, Prog. Theoret. Phys. Suppl. No. 130 [1998] 17] by a term of the first order in the inverse of the experimental time. As an application of our results, two possible experimental situations are considered: stretching of a RNA molecule and the drag of a dipolar particle in the presence of a gradient of electric force. 
900 |a 392 
900 |a 20 
900 |a 2013 
900 |a ^cH 
900 |a AAG 
900 |a AGROVOC 
900 |a 2013santini 
900 |a AAG 
900 |a http://ri.agro.uba.ar/files/intranet/articulo/2013santini.pdf 
900 |a 2013santini.pdf 
900 |a http://www.elsevier.com/ 
900 |a http://www.scopus.com/inward/record.url?eid=2-s2.0-84883134463&partnerID=40&md5=95c1b4de811046ed8cc54c309be48899 
900 |a ^a^b^c^d^e^f^g^h^i 
900 |a OS 
942 0 0 |c ARTICULO  |2 udc 
942 0 0 |c ENLINEA  |2 udc