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. 10. Miyoshi , T , Pascui , O , Reichert , D 2004 Slow chain dynamics in isotactic-poly(4-methyl-1-pentene) crystallites near the glass transition temperature characterized by solid-state C-13 MAS exchange NMR
(about 9%) up to 160 °C. The adsorbed water content of CS and PS- g -starch copolymer determined by TG measurements is in the agreement with the literature data obtained in air-oven drying at 105 °C [ 13 ]. It refers to the highly hygroscopic nature of CS
transition from the variety of regular structure (C–In 2 (MoO 4 ) 3 , a = 13.34 ± 0.07 Å) [ 9 ] to the variety of orthorhombic structure (R–In 2 (MoO 4 ) 3 , a = 9.447 Å, b = 9.597 Å, c = 13.29 Å) [ 10 ]. The authors of the study [ 10 ] gave the
Study of thermal properties of intumescent additive
Pentaerythritol phosphate alcohol
C 13 H 14 1,4,5-Trimethylnaphthalene 20 15.88 184 C 14 H 16 1,2,3,4-Tetramethylnaphthalene
ceramic pastes ranging in the tempering: A pure clay, B 2/3 clay + 1/3 temper, C 1/3 clay + 2/3 temper. Mass loss: m 1 at dehydration and m 2 at dehydroxylation Fig. 3
. Knicker , H , Lüdemann , HD . N 15 and C- 13 CPMAS and solution NMR studies of N- 15 enriched plant material during 600 days of microbial degradation . Org Geochem 1995 23 : 329 – 341 10
of T h from −1.8 (a), −1.7 (b), −1.5 (c), −1.3 (d) to −1.1 °C (e), indicating that the amount of ice nuclei in the equilibrium sample decreased accordingly. Recrystallization of the melted part started immediately after the temperature dropped, and
the procedure was in both cases comparable, amounting to approximately 2 °C [ 13 ]. Burr et al. applied thermistor sensors in their research to measure temperature changes under the influence of sonotherapy in the interior structures of the
analyses From the analysis, the cell parameters of DGCC were found to be a = 8.2820 Å, b = 9.0720 Å, c = 13.734 Å, α = β = 90° and γ = 106.12°, the cell volume = 991.32 Å 3 . The structure was solved by the direct method using the SHELXL
the pre-treatments of samples and the optimization of experimental conditions [ 6a , 10c , 12 ]. Furthermore, several interferences, such as overlapping and shifts of peaks, baseline drifting, and noise, cause the difficulty of accurate analysis [ 6c
