Abstract
The problem of how to define and compute temperature fluctuations for a small system in contact with a heat bath is an old one and originates from Einstein’s theory of Brownian motion. Only for a small enough system does their relative size allow a straightforward experimental verification. Here we focus on a mesoscopic system in contact with a heat bath at temperature T ∘ and provide a self-consistent argument showing as to why, and in what sense, the observable standard deviation of temperature from T ∘ equals \(\sqrt{k_{\rm B}/C}T_{\circ}\) where C is the mesoscopic system’s heat capacity. Our argument is based on ergodic decomposition, a simple fact that holds for a system in thermodynamic equilibrium and away from phase-transition points. In this way we close a line of argument opened by de Haas-Lorentz a century ago.
Similar content being viewed by others
Notes
Formally, Δ(1/T)=(ΔT)/T 2 so that with \(\Delta E = \sqrt{k_{\rm B} C} T\) we end up with (1).
References
Kittel, C.: Temperature fluctuation: an oxymoron. Phys. Today 41(5), 43 (1988)
Feshbach, H.: Small systems: when does thermodynamics apply? Phys. Today 40(11), 9–11 (1987)
Mandelbrot, B.B.: Temperature fluctuation: a well-defined and unavoidable notion. Phys. Today 42(1), 71–73 (1989). His statistical sampling argument has been reanalyzed recently by Falcioni et al. [4]
Falcioni, M., Villamaina, D., Vulpiani, A., Puglisi, A., Sarracino, A.: Estimate of temperature and its uncertainty in small systems. Am. J. Phys. 79, 777–785 (2011)
Einstein, A.: Über die Gültigkeitsgrenze des Satzes vom thermodynamischen Gleichgewicht und über die Möglichkeit einer neuen Bestimmung der Elementarquanta. Ann. Phys. (Leipz.) 22, 569–572 (1907)
de Haas-Lorentz, G.L.: Die Brownsche Bewegung und einige verwandte Erscheinungen, i.e., ‘Brownian motion and some related phenomena’. Vieweg, Braunschweig (1913). See in particular pp. 93–95. This is the German edition of the author’s Ph.D. thesis obtained the year before with H.A. Lorentz
Fermi, E.: Thermodynamics. Prentice Hall, New York (1937). Dover, New York (1956). Heat capacity is an accepted notion antedating the first edition of M. Planck’s classic on thermodynamics (1897)
Ornstein, L.S., Milatz, J.M.W.: Accidental deviations in the conduction of heat. Physica (Utrecht) 6, 1139–1145 (1939)
Milatz, J.M.W., van der Velden, H.A.: Natural limit of measuring radiation with a bolometer. Physica (Utrecht) 10, 369–380 (1943)
Chui, T.C.P., Swanson, D.R., Adriaans, M.J., Nissen, J.A., Lipa, J.A.: Temperature fluctuations in the canonical ensemble. Phys. Rev. Lett. 69, 3006–3008 (1992)
Lindhard, J.: “Complementarity” between energy and temperature. In: de Boer, J., Dal, E., Ulfbeck, O. (eds.) The Lesson of Quantum Theory, pp. 99–112. North-Holland, Amsterdam (1986). See in particular, §6
Uffink, J., van Lith, J.: Thermodynamic uncertainty relations. Found. Phys. 29, 655–692 (1999)
Phillies, G.D.J.: The polythermal ensemble: a rigorous interpretation of temperature fluctuations in statistical mechanics. Am. J. Phys. 52, 629–632 (1984)
Prosper, H.B.: Temperature fluctuations in a heat bath. Am. J. Phys. 61, 54–58 (1993)
Huang, K.: Statistical Mechanics, 2nd edn. Wiley, New York (1987). Sects. 7.2, 9.3 & 9.4
Balatsky, A.V., Zhu, J.-X.: Quantum Nyquist temperature fluctuations. Physica E 18, 341–342 (2003)
Hugenholtz, N.M.: States and representations in statistical mechanics. In: Streater, R.F. (ed.) Mathematics of Contemporary Physics, pp. 145–182. Academic, London (1972)
Jahnke, T., Lanéry, S., Mahler, G.: Operational approach to fluctuations of thermodynamic variables in finite quantum systems. Phys. Rev. E 83, 011109 (2011)
Touchette, H.: Temperature fluctuations and mixtures of equilibrium states in the canonical ensemble. In: Gell-Mann, M., Tsallis, C. (eds.) Nonextensive Entropy—Interdisciplinary Applications, pp. 159–176. Oxford University Press, Oxford (2004)
van Enter, A.C.D., van Hemmen, J.L.: Statistical-mechanical formalism for spin glasses. Phys. Rev. A 29, 355–365 (1984). Section II and Appendix. As exposed there in detail, similar arguments hold for quantum systems
Lanford, O.E. III, Lebowitz, J.L.: Time evolution and ergodic properties of harmonic systems. In: Springer Lecture Notes in Physics, vol. 38, pp. 144–177 (1975)
van Hemmen, J.L.: Dynamics and ergodicity of the infinite harmonic crystal. Phys. Rep. 65, 43–149 (1980)
Robinson, D.W.: Return to equilibrium. Commun. Math. Phys. 31, 171–189 (1973)
Heller, G., Kramers, H.A.: Ein klassisches Modell des Ferromagnetikums und seine nachträgliche Quantisierung im Gebiete tiefer Temperaturen. Proc. Roy. Acad. Sci. Amsterdam 37, 378–385 (1934)
Kramers, H.A.: Zur Theorie des Ferromagnetismus. In: 7e Congrès International du Froid, La Haye-Amsterdam, Juin (1936). Rapports et Communications. Also in: Commun. Kamerlingh Onnes Lab. Univ. Leiden 22(83), 1–22 (1936)
Dresden, M.: Kramers’s contributions to statistical mechanics. Phys. Today 41(9), 26–33 (1988). One may consult Dresden for, amongst others, a thoughtful evaluation of Kramers’ paper [25]
ter Haar, D.: Master of Modern Physics: the Scientific Contributions of H.A. Kramers. Princeton University Press, Princeton (1998)
de Finetti, B.: Theory of Probability, vols. I/II. Wiley, London (1974/5)
Vuillermot, P.A.: Intertwining relations between the dynamics of the infinite classical and quantum Heisenberg models: a new application of Trotter approximations and of the coherent-state formalism. Lett. Nuovo Cimento 24, 333–338 (1979)
Vuillermot, P.A.: Nonlinear dynamics of the infinite classical Heisenberg model: existence proof and classical limit of the corresponding quantum time evolution. Commun. Math. Phys. 76, 1–26 (1980)
Onsager, L.: Reciprocal relations in irreversible processes II. Phys. Rev. 38, 2265–2279 (1931)
Keizer, J.: Statistical Thermodynamics of Nonequilibrium Processes p. 68. Springer, New York (1987)
Emch, G.G., Radin, C.: Relaxation of local thermal deviations from equilibrium. J. Math. Phys. 12, 2043–2046 (1971)
van Hemmen, J.L.: Linear fermion systems, molecular field models, and the KMS condition. Fortschr. Phys. 26, 397–439 (1978). Sect. II
Landau, D.P., Binder, K.: A Guide to Monte Carlo Simulations in Statistical Physics, 3rd edn. Cambridge University Press, Cambridge (2009)
Sewell, G.L.: Quantum Theory of Collective Phenomena. Oxford University Press, Oxford (1986)
Simon, B.: The Statistical Mechanics of Lattice Gases, vol. I. Princeton University Press, Princeton (1993)
Hepp, K.: Quantum theory of measurement and macroscopic observables. Helv. Phys. Acta 45, 237–248 (1972)
Segel, L.A.: Mathematics Applied to Continuum Mechanics. Macmillan, London (1977). Appendix 9.1
Landau, L.D., Lifshitz, E.M.: Statistical Physics. Pergamon, Oxford (1980). Ch. 12
Acknowledgements
A.L. thanks the Humboldt Foundation for a Humboldt Award allowing his stay at the Technische Universität München. J.L.v.H. gratefully acknowledges the hospitality of the University of Ottawa, where this paper was finished. Both thank Aernout van Enter for constructive criticism.
Author information
Authors and Affiliations
Corresponding author
Rights and permissions
About this article
Cite this article
Leo van Hemmen, J., Longtin, A. Temperature Fluctuations for a System in Contact with a Heat Bath. J Stat Phys 153, 1132–1142 (2013). https://doi.org/10.1007/s10955-013-0867-9
Received:
Accepted:
Published:
Issue Date:
DOI: https://doi.org/10.1007/s10955-013-0867-9