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Schematic diagram of the PCM thermal storage module.

Schematic diagram of the PCM thermal storage module.

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Thermal energy storage using the latent heat of phase change materials (PCMs) is a promising technique to solve the time mismatch between the availability and usage of flue gas heat in distributed generation systems (DGSs). A diesel-engine-powered DGS integrated with two-stage tube-type PCM modules for exhaust gas heat recovery was developed and st...

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... The LHTES systems using phase change materials (PCMs) have been applied in several engineering applications such as concentrating solar plants, thermal isolation, groundwater infiltration, solar energy, building sectors, nuclear reactors, and so on thanks to the phase transition process [1,2]. However, the only issue of these systems is the low thermal conductivity of PCM. ...
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... Li et al. [127] conducted energy and exergy analysis for exhaust gas heat recovery system of a diesel engine-powered generator integrated with cascaded two stages PCM modules (see Fig. 33). The experiments were conducted during charging and discharging stages. ...
... Demonstration system of diesel engine with cascaded PCM modules[127].A.A.M. Omara ...
... Li et al.[88] Theoretical study Diesel engine• NaOH.H 2 O Exhaust system 2 • C •The PCM increased the warming-up time by 40%. Li et al.[127] The two-stage storage system stored input energy and exergy of flue gas by 56.4% and 48.3%, respectively.• ...
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... As a trade-off to these advantages, most PCMs suffer from low thermal conductivity, which makes it hard to charge and discharge effectively [5,12]. To overcome this issue, several methods have been proposed in the literature, including using nano-additives [13,14], metal foams [15,16], solid fins [17], heat pipes [18], metallic meshes [19][20][21]. ...
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... This allows removing temperature peaks due to the intermittent high power demand and storing a large amount of solar energy without significantly increasing the system temperature. Furthermore, LHTESS using phase change materials (PCMs) are widely used in various engineering applications such as building temperature regulation, waste heat recovery, compact heat exchangers, solar energy storage, concentrating solar plants, etc. [2,3]. However, their low thermal conductivity is one of their weaknesses because it restricts thermal transport by giving rise to slow heat dissipation during charging/discharging periods. ...
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In this work, the two-dimensional laminar flow and the heat transfer in an open-ended rectangular porous channel (metal foam) including a phase change material (PCM; paraffin) under forced convection were numerically investigated. To gain further insight into the foam pore effect on charging/discharging processes, the Darcy–Brinkmann–Forchheimer (DBF) unsteady flow model and that with two temperature equations based on the local thermal non-equilibrium (LTNE) were solved at the representative elementary volume (REV) scale. The enthalpy-based thermal lattice Boltzmann method (TLBM) with triple distribution function (TDF) was employed at the REV scale to perform simulations for different porosities (0.7≤ε≤0.9) and pore per inch (PPI) density (10≤PPI≤60) at Reynolds numbers (Re) of 200 and 400. It turned out that increasing Re with high porosity and PPI (0.9 and 60) speeds up the melting process, while, at low PPI and porosity (10 and 0.7), the complete melting time increases. In addition, during the charging process, increasing the PPI with a small porosity (0.7) weakens the forced convection in the first two-thirds of the channel. However, the increase in PPI with large porosity and high Re number limits the forced convection while improving the heat transfer. To sum up, the study findings clearly evidence the foam pore effect on the phase change process under unsteady forced convection in a PCM-saturated porous channel under local thermal non-equilibrium (LTNE).
... This allows removing temperature peaks due to the intermittent high power demand and storing a large amount of solar energy without significantly increasing the system temperature. Furthermore, LHTESS using phase change materials (PCMs) are widely used in various engineering applications such as building temperature regulation, waste heat recovery, compact heat exchangers, solar energy storage, concentrating solar plants, etc. [2,3]. However, their low thermal conductivity is one of their weaknesses because it restricts thermal transport by giving rise to slow heat dissipation during charging/discharging periods. ...
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Full-text available
In this work, the two-dimensional laminar flow and the heat transfer in an open-ended rectangular porous channel (metal foam) including a phase change material (PCM; paraffin) under forced convection were numerically investigated. To gain further insight into the foam pore effect on charging/discharging processes, the Darcy–Brinkmann–Forchheimer (DBF) unsteady flow model and that with two temperature equations based on the local thermal non-equilibrium (LTNE) were solved at the representative elementary volume (REV) scale. The enthalpy-based thermal lattice Boltzmann method (TLBM) with triple distribution function (TDF) was employed at the REV scale to perform simulations for different porosities (0.7 ≤ " ≤ 0.9) and pore per inch (PPI) density (10 ≤ PPI ≤ 60) at Reynolds numbers (Re) of 200 and 400. It turned out that increasing Re with high porosity and PPI (0.9 and 60) speeds up the melting process, while, at low PPI and porosity (10 and 0.7), the complete melting time increases. In addition, during the charging process, increasing the PPI with a small porosity (0.7) weakens the forced convection in the first two-thirds of the channel. However, the increase in PPI with large porosity and high Re number limits the forced convection while improving the heat transfer. To sum up, the study findings clearly evidence the foam pore effect on the phase change process under unsteady forced convection in a PCM-saturated porous channel under local thermal non-equilibrium (LTNE).
... This makes the latent TES very promising for energy collection and reuse, which is beneficial to energy conservation and emission reduction. Consequently, it can be found in many industrial fields, like concentrating solar power plants, waste heat recovery, temperature regulation of buildings, compact heat exchangers, thermal management of electric devices, etc. [3][4][5]. However, the key disadvantage of PCM is its intrinsically low thermal conductivity, which limits the heat transfer rate during the charging and discharging cycles. ...
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The energy transport inside a phase change material (PCM) based thermal energy storage system using metal foam as an enhancement technique is investigated numerically. The paraffin is used as the PCM and water as the heat transfer fluid (HTF). The transient heat transfer during the charging and discharging processes is solved, based on the volume averaged conservation equations. The flow in PCM/foam and HTF/foam composites is modelled by the Forchheimer-extended Darcy equation, while the two-temperature model is employed to account for the local thermal non-equilibrium effect between the foam matrix and fluid phase. The results show that the overall performance is greatly improved by inserting metal foam in both HTF and PCM sides. A nearly 84.9% decrease in the time needed for the total process is found compared with the case of pure PCM, and 40% compared with the case of metal foam insert only in the PCM side. Foam porosity and HTF inlet temperature greatly affect the dynamic heat storage/release process.
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Developing phase change materials (PCMs) with excellent thermal properties and low cost is of great significance for accelerating the applications of the latent heat storage technology in waste heat recovery. In this work, a novel composite PCM based on sodium acetate trihydrate (SAT), expanded graphite (EG) and carbon nanotubes (CNTs) was prepared and optimized for efficient heat storage and release effect. To confirm the phase change effect of composite PCM was acted above 50 °C, urea was introduced to improve the melt uniformity of SAT and its proportion was optimized in the range of 0–10 wt% based on the DSC results. The nucleating promotion of disodium hydrogen phosphate dodecahydrate (DHPD) on the SAT-Urea mixture crystals was characterized by a metallographic microscope. EG was used as the porous carrier to eliminate the liquid mobility of melted PCM. CNTs were introduced to further enhance the thermal conductivity of the composite PCM. It is shown that 4 wt% urea can effectively inhibit the phase segregation of SAT and keep the phase change temperature of mixture above 55 °C. The melting enthalpy of SAT-Urea mixture is as high as 250.5 kJ/kg. It is observed from the microscope images that 4 wt% DHPD can promote the rapid formation of small crystals of SAT-Urea mixture, thereby providing more nuclei and accelerating the crystal growth rate. And the supercooling degree can be reduced to 0.6 °C. The porous network provided by EG and the addition of CNTs can significantly enhance the thermal conductivity of SAT-Urea mixture. As a result, the SAT-Urea/EG/CNTs composite PCM exhibits a high enthalpy of 180.1 kJ/kg, a high thermal conductivity of 6.904 W/(m·K), and excellent thermal reliability after 300 cycles of melt-solidification experiments.