We examine the long-term behaviour of non-integrable, energy-conserved, 1D systems of macroscopic grains interacting via a contact-only generalized Hertz potential and held between stationary walls. Existing dynamical studies showed the absence of energy equipartitioning in such systems, hence their long-term dynamics was described as quasi-equilibrium. Here we show that these systems do in fact reach thermal equilibrium at sufficiently long times, as indicated by the calculated heat capacity. As a byproduct, we show how fluctuations of system quantities, and thus the distribution functions, are influenced by the Hertz potential. In particular, the variance of the system's kinetic energy probability density function is reduced by a factor related to the contact potential.Recently, there has been broad interest in 1D systems of macroscopic grains held between stationary walls and interacting via a power-law contact potential [1][2][3][4][5][6]. A long-standing open problem is whether thermalization (equipartition) can occur in these chains of grains. Only very recently has it been shown that the related FPU chain of coupled oscillators does reach equilibrium after very long times [7]. In this paper, we show this is also true for so-called Hertz chains. In the process, we obtain wholly new approximate distribution functions for interacting particles in the microcanonical ensemble.Many power-law interacting systems are notable for supporting solitary wave (SW) propagation [3,6,8]. However, in response to singular perturbations, the breakup of SWs at the walls and from gaps between grains leads the system after a long time to an equilibrium-like, ergodic phase [2][3][4]. Unusually large [2-4] and occasionally persistent (rogue) [9] fluctuations in the system's kinetic energy are seen at late times for sufficiently strong and unique perturbations. This has been seen to impede an equal sharing of energy among all the grains in the system, hence the long-term dynamics of 1D systems of interacting grains has been described as quasi-equilibrium (QEQ) [2][3][4]. The question of whether QEQ is the final state for these systems is addressed in this letter.To the time scales previously studied, quasiequilibrium has been seen to be a general feature of the dynamics of systems with no sound propagation [3]. However, we find that at sufficiently late times, kinetic energy fluctuations relax, allowing for energy to be shared equally among all grains. Of course, energy equipartitioning happens only in an average sense in finite systems, and at any given instant each grain will not have exactly the same kinetic energy. Rather, each grain's kinetic energy fluctuates according to the same probability density function (pdf), the long tail of which determines the chance of large fluctuations.The fluctuations are quantified by treating the chain as a 1D gas of interacting spheres [10]. This requires new velocity and kinetic energy distribution functions different from hard spheres, which incorporate the interaction potential. These dis...