“…We used samples of a PS glass previously obtained in our laboratory. The melting and casting procedure was described in reference, 48 and other studies on this particular batch of PS glass have been reported in references 50,51 . The glass‐transition temperature was measured by the onset of the glass–SCL transition of the differential scanning calorimetry (DSC, Netzsch 404 equipment) at a heating rate of 10 K min −1 , = 681 K. This particular composition was chosen because experimental values of isostructural viscosity 49 are available.…”
Knowledge of relaxation processes is fundamental in glass science and technology because relaxation is intrinsically related to vitrification, tempering as well as to annealing and several applications of glasses. However, there are conflicting reports—summarized here for different glasses—on whether the structural relaxation time of glass can be calculated using the Maxwell equation, which relates relaxation time with shear viscosity and shear modulus. Hence, this study aimed to verify whether these two relaxation times are comparable. The structural relaxation kinetics of a lead metasilicate glass were studied by measuring the refractive index variation over time at temperatures between 5 and 25 K below the fictive temperature, which was initially set 5 K below the glass‐transition temperature. Equilibrium shear viscosity was measured above and below the glass‐transition range, expanding the current knowledge by one order of magnitude. The Kohlrausch equation described very well the experimental structural relaxation kinetics throughout the investigated temperature range and the Kohlrausch exponent increased with temperature, in agreement with studies on other glasses. The experimental average structural relaxation times were much longer than the values computed from isostructural viscosity, as expected. Still, they were less than one order of magnitude higher than the average relaxation time computed through the Maxwell equation, which relies on equilibrium shear viscosity. Thus, these results demonstrate that the structural relaxation process is not controlled by isostructural viscosity and that equilibrium shear viscosity only provides a lower boundary for structural relaxation kinetics.
“…We used samples of a PS glass previously obtained in our laboratory. The melting and casting procedure was described in reference, 48 and other studies on this particular batch of PS glass have been reported in references 50,51 . The glass‐transition temperature was measured by the onset of the glass–SCL transition of the differential scanning calorimetry (DSC, Netzsch 404 equipment) at a heating rate of 10 K min −1 , = 681 K. This particular composition was chosen because experimental values of isostructural viscosity 49 are available.…”
Knowledge of relaxation processes is fundamental in glass science and technology because relaxation is intrinsically related to vitrification, tempering as well as to annealing and several applications of glasses. However, there are conflicting reports—summarized here for different glasses—on whether the structural relaxation time of glass can be calculated using the Maxwell equation, which relates relaxation time with shear viscosity and shear modulus. Hence, this study aimed to verify whether these two relaxation times are comparable. The structural relaxation kinetics of a lead metasilicate glass were studied by measuring the refractive index variation over time at temperatures between 5 and 25 K below the fictive temperature, which was initially set 5 K below the glass‐transition temperature. Equilibrium shear viscosity was measured above and below the glass‐transition range, expanding the current knowledge by one order of magnitude. The Kohlrausch equation described very well the experimental structural relaxation kinetics throughout the investigated temperature range and the Kohlrausch exponent increased with temperature, in agreement with studies on other glasses. The experimental average structural relaxation times were much longer than the values computed from isostructural viscosity, as expected. Still, they were less than one order of magnitude higher than the average relaxation time computed through the Maxwell equation, which relies on equilibrium shear viscosity. Thus, these results demonstrate that the structural relaxation process is not controlled by isostructural viscosity and that equilibrium shear viscosity only provides a lower boundary for structural relaxation kinetics.
“…The chosen interatomic potential was originally parameterized for PbSiO3 (i.e., x=50% in (PbO)x(SiO2)1-x) to generate the correct energy and length scales at the experimental density and zero pressure. [14] The potential reproduces most features of the neutron static-structure factor as well as vibrational density of states obtained using Raman spectroscopy for PbSiO3. [14] Here, we apply the interatomic potential to study three lead silicate compositions, with x=30%, 50% and 70%.…”
Section: Simulation Methodsmentioning
confidence: 72%
“…Classical molecular dynamics (MD) simulations employing a two-body interatomic potential [14] are used to study lead silicates in this work. The potential consists of four terms modelling the steric repulsion of the ions due to size effects, Coulomb interactions owing to charge transfer between the ions, charge-induced dipole attractions arising from the electronic polarizability of ions, and the van der Waals attraction.…”
“…In binary PbO-SiO 2 glasses, the structure-property relations have been explored through detailed short-range structures using diverse experimental techniques [e.g., X-ray/neutron diffraction, [26][27][28][29] X-ray absorption spectroscopy (XAS), 9,30 X-ray photoelectron spectroscopy (XPS), [31][32][33][34] and solid-state nuclear magnetic resonance (NMR) 10,11,[35][36][37] ] and theoretical studies (e.g., molecular dynamics simulations). 30,[38][39][40][41] In contrast, the structural details of more complex Pb-bearing silicate glasses have not been fully explored. The PbO-Na 2 O-SiO 2 glasses are of particular interest because of their importance as a fundamental model system for multicomponent Pb-bearing silicate glasses, as well as their industrial applications (e.g., radiation shielding glasses 42,43 ).…”
Section: Introductionmentioning
confidence: 99%
“…Such a remarkable glass‐forming ability of Pb‐bearing silicate glasses and the slower dissolution behavior of Pb can be explained from the short‐range configurations around Pb and oxygens (e.g., 9,11,12,26 ). In binary PbO‐SiO 2 glasses, the structure‐property relations have been explored through detailed short‐range structures using diverse experimental techniques [e.g., X‐ray/neutron diffraction, 26‐29 X‐ray absorption spectroscopy (XAS), 9,30 X‐ray photoelectron spectroscopy (XPS), 31‐34 and solid‐state nuclear magnetic resonance (NMR) 10,11,35‐37 ] and theoretical studies (e.g., molecular dynamics simulations) 30,38‐41 . In contrast, the structural details of more complex Pb‐bearing silicate glasses have not been fully explored.…”
Knowledge of the structure of lead (Pb)-bearing silicate glasses, such as degree of polymerization and arrangement among cations, provides improved prospects for understanding their macroscopic properties. Despite the importance, the detailed disorder in Pb-bearing silicate glasses with varying composition (i.e., Pb/alkali content) has not been systematically explored. Here, we reveal the first unambiguous structural information of PbO-Na 2 O-SiO 2 glasses with varying PbO content [i.e., X PbO = PbO/(Na 2 O + PbO)], which are the fundamental model system for multicomponent Pb-bearing glasses, using high-resolution 17 O solid-state NMR. 17 O NMR spectra clearly show the resolved multiple oxygen sites, such as Na-O-Si, Si-O-Si, and [Na,Pb]-O-Si. As X PbO increases, the fraction of [Na,Pb]-O-Si peak increases markedly at the expanse of substantial reduction in the fraction of Na-O-Si/ total NBO. This trend indicates the relative predominance of the dissimilar pairs around non-bridging oxygen (NBO) and, therefore, can be explained well with the pronounced chemical ordering among Na + and Pb 2+. These results confirm that Pb is primarily a network-modifier in the glasses studied here. Atomic environments around both NBO and BO are affected by the change in Na/Pb ratio, while topological disorder due to cation mixing around NBO is much more prominent in Pb endmember. The structural details of short-range configurations around oxygen in alkali Pb-silicate glasses provide atomistic insights for understanding the properties of Pb-bearing multicomponent silicate glasses.
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.