“…10 Recent evidence suggests that this -relaxation or, more precisely, the local cooperate dynamics of several  relaxations, give rise to one shear transformation event, or one ␣ relaxation, 11,12 and is thought to be the driving process for enhanced diffusion. 19 In this paper, evidence is provided that this aging process observed well below T g can be associated with the slow Johari-Goldstein type  relaxation, in the following denoted as  relaxation. This effect has been repeatedly observed as an increase in Young's modulus 14,15 or decrease of the free volume, 16 at temperatures at which irreversible aging of the macroscropic structure, the partial restoration of equilibrium structure below T g , where complete equilibration is significantly longer than the experimental time window, is negligible on experimental timescales.…”
Articles you may be interested inDetermination of the activation energy spectrum of structural relaxation in metallic glasses using calorimetric and shear modulus relaxation data Effect of physical aging on Johari-Goldstein relaxation in La-based bulk metallic glass Wetting of bulk metallic glass forming liquids on metals and ceramics
“…10 Recent evidence suggests that this -relaxation or, more precisely, the local cooperate dynamics of several  relaxations, give rise to one shear transformation event, or one ␣ relaxation, 11,12 and is thought to be the driving process for enhanced diffusion. 19 In this paper, evidence is provided that this aging process observed well below T g can be associated with the slow Johari-Goldstein type  relaxation, in the following denoted as  relaxation. This effect has been repeatedly observed as an increase in Young's modulus 14,15 or decrease of the free volume, 16 at temperatures at which irreversible aging of the macroscropic structure, the partial restoration of equilibrium structure below T g , where complete equilibration is significantly longer than the experimental time window, is negligible on experimental timescales.…”
Articles you may be interested inDetermination of the activation energy spectrum of structural relaxation in metallic glasses using calorimetric and shear modulus relaxation data Effect of physical aging on Johari-Goldstein relaxation in La-based bulk metallic glass Wetting of bulk metallic glass forming liquids on metals and ceramics
“…The physical aging of polymers and other "soft" materials was studied experimentally almost three decades ago by Struik and co-workers. 1,2 The interest of a wider community for this area was then greatly stimulated by the work of Lundgren et al 3 on the magnetic properties of spin glasses, and aging has since remained a source of important questions and insights in nonequilibrium statistical physics. 4 The basic features of aging were mainly established during the 1980s in studies of the magnetic linear susceptibility and autocorrelation functions of spin glasses [5][6][7][8] but are shared by many other systems, including, to cite only a few examples, type II superconductors, 9 glasses, [10][11][12][13][14] granular materials, 15 and soft condensed matter.…”
Section: Introductionmentioning
confidence: 99%
“…To detect the onset of ergodicity breaking and characterize the behavior in both the ergodic and nonergodic regions, we consider a number of relevant dynamic and thermodynamic measures: (1) The physical movement of the particles, as statistically characterized by the mean-square displacement (MSD), is diffusive in the ergodic region and subdiffusive elsewhere. (2) The related bond survival probability (BSP) 41 drops to a finite average close to zero on a characteristic time scale at sufficiently high temperatures but becomes scale-free and age-dependent in the nonergodic region.…”
We present extensive numerical investigations of the structural relaxation dynamics of a realistic model of the amorphous high-temperature ceramic a-Si3B3N7, probing the mean-square displacement of the atoms, the bond survival probability, the average energy, the specific heat, and the two-point energy average. Combining the information from these different sources, we identify a transition temperature Tc approximately 2000 K below which the system is no longer ergodic and physical quantities observed over a time t(obs) show a systematic parametric dependence on the waiting time t(w), or age, elapsed after the quench. The aging dynamics "stiffens" as the system becomes older, which is similar to the behavior of highly idealized models such as Ising spin glasses and Lennard-Jones glasses.
“…In plastics, it manifests as a physical aging process, common to all amorphous polymers, which consists of an ongoing vitrification process. Numerous electrical properties are affected by this, but it has been studied only to a very limited extent [100]. Several studies on creep of PVC have been published [101,102] but none directly address electric failures.…”
SUMMARYPVC is the most common insulation material used for wiring in low-voltage (LV) service. 'Low-voltage', in the context of this paper, is taken to be 120-240 VAC. The electrotechnical products considered include insulated wires, cables and cords, and also appurtenant termination devices, e.g. male plugs or female taps. Well-known factors leading to the ignition of PVC-insulated wiring and related products include: (a) manufacturing defects; (b) grossly excessive current; (c) over-insulation, sometimes augmented by overcurrent; (d) localized heating due to strand breakage; (e) localized heating due to mechanical strand severing by staples or nails; and (f) localized heating due to failed terminations. Other failure modes are known but have received only limited study. These include (i) excessive force and creep; (ii) chemical interaction effects; and (iii) breakdown under voltage surge conditions. Additional research is needed in these areas. The proximate cause of ignition involved with many of the above mechanisms is arc tracking (arcing across a carbonized path). In turn, it is shown that PVC is especially susceptible to becoming charred, it requiring only approximately 1608C for the material to become semiconducting during shortterm exposure (around 10 h), while longer-term exposure (around 1 month) may cause failures at temperatures as low as 1108C. Some limited data exist which suggest that standard UL and IEC temperature classifications are unduly optimistic, as applied to PVC. Fire can originate if wiring or equipment cannot withstand a powerline surge. Mains-connected electrical appliances need to be designed to resist 6000 V surge voltages, even though this is not mandated in most of the current UL and IEC standards. Data are presented showing that the IEC 60112 wet-tracking test gives especially misleading results for PVC and should be improved or abrogated.
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