Entropy and Ordering of Hard Rods in One Dimension

Abstract: We revisit the equilibrium properties of a classical one-dimensional system of hard-core particles in the framework provided by the multiparticle correlation expansion of the con-figurational entropy. The vanishing of the cumulative contribution of more-than-two-particlecorrelations to the excess entropy is put in relation with the onset of a solidlike behavior athigh densities.Keywords: Entropy; residual multiparticle entropy; hard rods; one dimension; Tonks gas.1. IntroductionThe entropy of a classical system can be expressed as an infinite sum of contributions associated withspatially integrated n -point density correlations: S =X 1n =0 S n ; (1)where S 0 is the entropy of the corresponding non-interacting gas. The above expansion was separatelyderived for closed [1] and open systems [2], but the two apparently different expressions were later shownto be in fact equivalent [3]. In the absence of external fields, the leading and quantitatively dominant termof the series is the so called “pair entropy”

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