2019
DOI: 10.1111/jace.16850
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Structural origin of the anomalous density maximum in silica and alkali silicate glasses

Abstract: Silica, sharing the same tetrahedral order and many structural, thermodynamic and dynamic anomalies with water, has been speculated to have a density increase upon melting similar to water. In this work, an increase in density upon melting cristobalite silica and a shallow density maximum followed by a density minimum during cooling of silica liquid are observed in classical molecular dynamics simulations. The density maximum gradually diminishes with the increase in alkali size/content in alkali silicate glas… Show more

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Cited by 9 publications
(16 citation statements)
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References 49 publications
(61 reference statements)
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“…It can be also seen that the ring distributions of the 0‐8 GPa samples (the T 2 values of 0 and 4 GPa samples are around 3000 K and the T 2 of the 8 GPa is around 2700 K, see Table 1) from 3600 to 3000 K tend to become more centralized around 6~7 rings. In the study by Shih et al, 25 the density maximum, viz., the local minimum of L at T 2 , has been attributed to the tendency to form 6‐member rings. Based on these, we propose that the local density maximum (the reason for the existence of T 2 ) results from (a) the increase of CN Si‐O and CN Si‐Si , which tend to increase the glass density from T 1 to T 2 ; (b) the tendency to break rings whose sizes are close to 6 or 7 when the silica glass is further heated above T 2 ; and (c) the increase of bond length of Si–O or Si–Si at T > T 2 , which further helps increase the volume.…”
Section: Resultsmentioning
confidence: 99%
“…It can be also seen that the ring distributions of the 0‐8 GPa samples (the T 2 values of 0 and 4 GPa samples are around 3000 K and the T 2 of the 8 GPa is around 2700 K, see Table 1) from 3600 to 3000 K tend to become more centralized around 6~7 rings. In the study by Shih et al, 25 the density maximum, viz., the local minimum of L at T 2 , has been attributed to the tendency to form 6‐member rings. Based on these, we propose that the local density maximum (the reason for the existence of T 2 ) results from (a) the increase of CN Si‐O and CN Si‐Si , which tend to increase the glass density from T 1 to T 2 ; (b) the tendency to break rings whose sizes are close to 6 or 7 when the silica glass is further heated above T 2 ; and (c) the increase of bond length of Si–O or Si–Si at T > T 2 , which further helps increase the volume.…”
Section: Resultsmentioning
confidence: 99%
“…Therefore, only three definitions are eligible for ring size analyses in glass structures. Among RINGS' users, the primitive definition has been almost exclusively adopted (19)(20)(21), with the exception of ( 22) wherein the Guttman's definition was used. In most papers focusing on rings, no reasons are provided as to why a specific definition is adopted.…”
Section: Contribution Of Individual Ring Sizes To the Fsdpmentioning
confidence: 99%
“…G1 is formed as a result of the co‐assembly between TEOS and F127 as no hydrogel was obtained in the absence of TEOS under the same conditions (Table S1, entry 13). Although it is difficult to quantify the binding energy between the monomer and the template, the measured yield strain (Figure S6) of G1 reflects the energy required to extensively break the non‐covalent interactions between TEOS and F127 to facilitate the solid‐to‐liquid transition.…”
Section: Figurementioning
confidence: 99%