Molecular dynamics and kinetics of isothermal cold crystallization with tunable dimensionality in a molecular glass former, 5′-(2,3-difluorophenyl)-2′-ethoxy-4-pentyloxy-2,3-difluorotolane
Abstract:This paper characterizes the molecular mobility that triggers the cold crystallization abilities in 5'-(2,3-difluorophenyl)-2'-ethoxy-4-pentyloxy-2,3-difluorotolane (short name DFP25DFT) material by broadband dielectric spectroscopy (BDS). We analyze the properties of identified molecular...
“…Under conditions of constant cooling, the crystal phase is not formed eventually and the glassy SmC A * is obtained. There are two discontinuous changes in luminance at 233 K and 213 K. The first one corresponds to T g obtained by DSC, the second one can be caused by small fractures in the vitrified sample, 27,28 even if they are not directly visible in textures. During heating, the glass softening is not detected by POM.…”
Section: Resultsmentioning
confidence: 99%
“…Their appearance is related to fractures in the material, which may be present below the glass transition temperature T g . 27,28…”
Section: Resultsmentioning
confidence: 99%
“…Their appearance is related to fractures in the material, which may be present below the glass transition temperature T g . 27,28 During heating of the sample, there is a visible step at 233 K, leading to the conclusion that the glass of the SmC A * phase softens. A large, wide exothermal anomaly from cold crystallization can be seen upon further heating.…”
The formation of glass of the anticlinic high-tilted smectic CA* phase even at low cooling rates (≥2 K min−1) is reported for (S)-4′-(1-ethylhexyloxycarbonyl)biphenyl-4-yl 4-[5-(2,2,3,3,4,4,4-heptafluorobutoxy)pentyl-1-oxy]benzoate.
“…Under conditions of constant cooling, the crystal phase is not formed eventually and the glassy SmC A * is obtained. There are two discontinuous changes in luminance at 233 K and 213 K. The first one corresponds to T g obtained by DSC, the second one can be caused by small fractures in the vitrified sample, 27,28 even if they are not directly visible in textures. During heating, the glass softening is not detected by POM.…”
Section: Resultsmentioning
confidence: 99%
“…Their appearance is related to fractures in the material, which may be present below the glass transition temperature T g . 27,28…”
Section: Resultsmentioning
confidence: 99%
“…Their appearance is related to fractures in the material, which may be present below the glass transition temperature T g . 27,28 During heating of the sample, there is a visible step at 233 K, leading to the conclusion that the glass of the SmC A * phase softens. A large, wide exothermal anomaly from cold crystallization can be seen upon further heating.…”
The formation of glass of the anticlinic high-tilted smectic CA* phase even at low cooling rates (≥2 K min−1) is reported for (S)-4′-(1-ethylhexyloxycarbonyl)biphenyl-4-yl 4-[5-(2,2,3,3,4,4,4-heptafluorobutoxy)pentyl-1-oxy]benzoate.
“…The activation energy of crystallization is contributed by the molecular structure and interactions, as well as the difference in the positional and conformational order of molecules between the initial phase and the forming crystal, and depends on thermodynamic and spatial conditions. In particular, molecular flexibility brings the additional activation barrier for crystal formation. , Therefore, high-weight flexible molecules exhibiting backbone conformations are prospective for a lower capability for melt crystallization than small ones . Additionally, in the wax material, a broad distribution of n -alkanes also favors an increase in the activation barrier for crystallization and thus the tendency to form an amorphous state.…”
The demand for the development of multifunctional materials
in
emerging technologies has stimulated intensive research on the control
of crystallization processes in numerous scientific and engineering
fields. In this article, we examine the kinetics of nonisothermal
melt crystallization in synthetic wax using differential scanning
calorimetry (DSC) supported by polarized optical microscopy (POM)
to describe crystallization modes in a multicomponent molecular system.
We detected the macroscopic growth of three crystal phases and the
formation of two crystal phases as a transformation from a disordered
crystal mesophase into an ordered crystal. To characterize individual
crystal phase formation, we examine the activation energy evaluated
by isoconversional analysis and utilize the Ozawa and Mo methods to
determine the kinetic details of the crystal growth from the isotropic
phase. Our investigation reveals the possibility of the design of
crystal growth dimensionality as three-dimensional spherulitic-like,
two-dimensional rodlike, and one-dimensional needle-shaped crystal
forms of shorter n-alkanes by controlling the solidification
pathway of long-chain n-alkanes and the interplay
of the thermodynamic and kinetic mechanisms of crystallization.
“…Recently, small molecules exhibiting cold crystallization via supercooled liquids, glass, [10][11][12][13][14][15][16][17][18][19] liquid crystals, [20][21][22][23][24] and ionic liquid crystals 25,26 have been reported. To develop better thermal-storage materials, the mechanism of the thermal behavior during cold crystallization must be analyzed in detail.…”
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