1970
DOI: 10.1016/s0008-6215(00)88001-5
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Thermodynamic properties of 1,6-anhydrohexopyranose crystals

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1971
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Cited by 22 publications
(3 citation statements)
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“…Thermodynamic studies of levoglucosan have been a popular endeavor during the past decade. It is known that solid levoglucosan exists as two crystal phases. The low-temperature phase (crII) is the orientationally ordered crystal phase (space group, P2 1 2 1 2 1 ), while the high-temperature phase (crI) is the orientationally disordered crystal (or plastic crystal) phase. The solid–solid phase transition occurs at T tr = 384.7 ± 0.2 K with a phase-transition enthalpy of Δ crII crI H m o = 24.3 ± 0.2 kJ·mol –1 . The plastic crystals (phase cr I) melt to a low-viscosity liquid at T fus = 455.3 ± 0.1 K with an enthalpy of fusion of Δ crI l H m o = 3.2 ± 0.1 kJ·mol –1 .…”
Section: Resultsmentioning
confidence: 99%
“…Thermodynamic studies of levoglucosan have been a popular endeavor during the past decade. It is known that solid levoglucosan exists as two crystal phases. The low-temperature phase (crII) is the orientationally ordered crystal phase (space group, P2 1 2 1 2 1 ), while the high-temperature phase (crI) is the orientationally disordered crystal (or plastic crystal) phase. The solid–solid phase transition occurs at T tr = 384.7 ± 0.2 K with a phase-transition enthalpy of Δ crII crI H m o = 24.3 ± 0.2 kJ·mol –1 . The plastic crystals (phase cr I) melt to a low-viscosity liquid at T fus = 455.3 ± 0.1 K with an enthalpy of fusion of Δ crI l H m o = 3.2 ± 0.1 kJ·mol –1 .…”
Section: Resultsmentioning
confidence: 99%
“…Interestingly, it was shown that besides ethanol, LG is so far the second-known compound capable of forming crystalline, plastic crystal (PC), liquid (LQ), orientational glass (OTG) and ordinary glass (OG) phases (Madejczyk et al, 2017;Srinivasan et al, 1996;Fayos et al, 1996). Besides many previous studies on the thermally induced transition of LG to PC at $383 K (Shafizadeh et al, 1970;Shafizadeh & Lai, 1972;Smith & Shafizadeh, 1971;Lienhard et al, 2012;Rocha et al, 2013;Tombari & Johari, 2015;Kamin ´ska et al, 2016), it is still of fundamental interest since, to the best of our knowledge, the LG structure in the orientationally disordered phase has not yet been solved. In this context, it is worth stressing that below 383 K LG exists as an ordered crystalline phase, first identified by Park et al (1971) through single-crystal X-ray diffraction as an orthorhombic system with space group P2 1 2 1 2 1 and four molecules per unit cell with unit-cell parameters a = 6.684 (2) A ˚, b = 13.266 (7) A ˚, c = 7.547 (2) A ˚.…”
Section: Introductionmentioning
confidence: 99%
“…It was concluded that LG molecules are linked into finite arrays formed by strong O-HÁ Á ÁO bonds supported by weaker C-HÁ Á ÁO interactions. Further heating of LG exhibits a second phase transition at around 460 K, corresponding to the melting point (Shafizadeh et al, 1970;Kamin ´ska et al, 2016). Our previous report showed that LG could also be obtained as OTG or OG phases from PC or LQ states, respectively, when undercooled below the glass transition temperature at $245 K with a very high cooling rate (Madejczyk et al, 2017).…”
Section: Introductionmentioning
confidence: 99%