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Journal of Thermal Analysis and Calorimetry
Authors: Giovanni Di Nicola, Caterina Brandoni, Cristiano Di Nicola, and Giuliano Giuliani

summarized. The global uncertainty of the temperature, considering also the contribution of the Rossini method correction, was estimated to be less than ±0.8 K, both for thermoresistor and thermocouple measurements. Since the measured vapor pressure

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the saturated vapor pressures of Ni and supersaturation values S . As seen from Table 4 , P sat varies by nearly 19 orders of magnitude in the temperature range considered. The average value of actual vapour pressure for Ni, P act , corresponding

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indium due to its relatively high vapor pressure at elevated temperatures [ 14 ]. Evolved gas analysis in nitrogen and in air atmospheres by online TG/DTA-EGA-MS and TG-EGA-FTIR systems Figure 5 shows the

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exceeds 802 °C (with regard to MoO 3 melting temperature), then this oxide melts and because of rather high vapor pressure, it is vaporized, leaving behind only silicon scale. Because of MoSi 2 decomposition, silicon remains in atomic form, and the issue

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oxygen isotope ratios in wood constituents of Pinus halepensis as indicators of precipitation, temperature and vapour pressure deficit . — Tellus B 57 ( 2 ): 164 – 173 . http://dx.doi.org/10.1111/j.1600-0889.2005.00137.x

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. , Leonardi , C. , Bertin , N. ( 2005 ) Analysis of growth and water relation of tomato fruits in relation to air vapor pressure deficit and plant fruit load . J. Plant Growth Regul. 24 , 1 – 13 . 17

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Journal of Thermal Analysis and Calorimetry
Authors: George G. G. de Oliveira, Humberto G. Ferraz, Patrícia Severino, and Eliana B. Souto

[ 17 ]. For the application of this technique, some requirements are needed. The melting point should be a triple point as gas phase, liquid and solid must be in balance and have the same vapour pressure at this temperature. Change in free energy (Δ G

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Journal of Thermal Analysis and Calorimetry
Authors: D. V. Pinakov, V. A. Logvinenko, G. N. Chekhova, and Yu. V. Shubin

compounds by the way of guest substitution [ 1 – 4 , 6 ] to be possible. The capability of (CH 3 ) 2 CO FGICs for thermoanalytical investigations at a room and adjacent temperatures was anticipated as well. (CH 3 ) 2 CO saturation vapour pressure is about

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heavy metal oxides have vapor pressures which are lower by several orders of magnitude and are not visible in Fig. 1 , except for CdO and PbO. Fig. 1 Gaseous fractions of six heavy metal chlorides. Vapor pressure

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thermal equilibrium was reached, the adsorption branch was drawn up step by step by introducing water vapor into the thermobalance. Desorption branch was performed from a saturated sample by decreasing the water vapor pressure. The equilibrium state was

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