Abstract:In this work we derive temperature-dependent functions for the most important material properties needed for phase change studies with octadecane. Over 80 references are reviewed in which at least one thermophysical property of octadecane is measured. The functions are valid ±40 K around the melting temperature and are surrounded by their confidence interval. It turns out that the values for the solid phase have much broader confidence intervals than the ones of the liquid phase. Hence, more accurate measureme… Show more
“…Both capillary force and surface tension will affect the flowability of PCM inside the carbon pores. The viscosity of coconut oil was reported to be 36 mPas and 7.6 mPas [50] and octadecane was reported to be 3.9 mPas and 1.6 mPas [51] at room temperature and 80 o C, respectively. Higher temperatures will increase the possibility of leakage; however, the capillary force caused by the micropore channels can prevent this leakage.…”
Section: Shape-stabilize and Leakage Performancementioning
“…Both capillary force and surface tension will affect the flowability of PCM inside the carbon pores. The viscosity of coconut oil was reported to be 36 mPas and 7.6 mPas [50] and octadecane was reported to be 3.9 mPas and 1.6 mPas [51] at room temperature and 80 o C, respectively. Higher temperatures will increase the possibility of leakage; however, the capillary force caused by the micropore channels can prevent this leakage.…”
Section: Shape-stabilize and Leakage Performancementioning
“…The thermal performance of a PCM layer of octadecane is determined by estimating the time evolution of the dynamical variables, the thermal energy released (absorbed) and the thermal energy released by the interior surface. The thermodynamic properties of octadecane are assumed to be constant in the temperature range considered in this work, and equal to their values close to the saturation temperature of the PCM [ 27 ]. For the liquid(solid) phase , and .…”
Section: Resultsmentioning
confidence: 99%
“…The volumetric effects produced by the density difference between liquid and solid phases is considered when the external surface is subjected to periodic boundary conditions and the temperature of the internal surface is constant and below . The temperature dependence of liquid and solid densities is negligible within the temperature range and PCM considered in this work [ 27 ]. Octadecane is used as the PCM, and within the experimental error, the density of the solid is practically constant in a wide temperature range .…”
Section: Description Of the Physical System And Mathematical Modelmentioning
The Stefan problem regarding the formation of several liquid–solid interfaces produced by the oscillations of the ambient temperature around the melting point of a phase change material has been addressed by several authors. Numerical and semi-analytical methods have been used to find the thermal response of a phase change material under these type of boundary conditions. However, volume changes produced by the moving fronts and their effects on the thermal performance of phase change materials have not been addressed. In this work, volume changes are incorporated through an additional equation of motion for the thickness of the system. The thickness of the phase change material becomes a dynamic variable of motion by imposing total mass conservation. The modified equation of motion for each interface is obtained by coupling mass conservation with a local energy–mass balance at each front. The dynamics of liquid–solid interface configurations is analyzed in the transient and steady periodic regimes. Finite element and heat balance integral methods are used to verify the consistency of the solutions to the proposed model. The heat balance integral method is modified and adapted to find approximate solutions when two fronts collide, and the temperature profiles are not smooth. Volumetric corrections to the sensible and latent heat released (absorbed) are introduced during front formation, annihilation, and in the presence of two fronts. Finally, the thermal energy released by the interior surface is estimated through the proposed model and compared with the solutions obtained through models proposed by other authors.
“…Compared to other passive TES methods such as sensible heat storage and thermochemical heat storage, PCMs often have advantages including low material cost, narrow range of operating temperatures, and relatively high heat storage capacity. 11 Broadly speaking, PCMs can be classified into two categories, namely organic PCMs (most commonly paraffin waxes, 12 or long chain alkanes, 13 but also fatty acids, 14 esters, 15 amines, 16 and sugar alcohols 17 ), and inorganic PCMs (such as salts, salt hydrates, metals, and alloys). 18 Each of these classes has their associated advantages and disadvantages.…”
A series of triazine-based compounds (M1–M7) have been prepared from 1,3,5-triazine, 2,4,6-triamino-1,3,5-triazine, 2,4-dichloro-6-methoxy-1,3,5-triazine and 2-chloro-4,6-dimethoxy-1,3,5-triazine, and their thermal phase change properties.
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