Abstract

Thermal energy storage is a technique that has the potential to contribute to future energy grids to reduce fluctuations in supply from renewable energy sources. The principle of energy storage is to drive an endothermic phase change when excess energy is available and to allow the phase change to reverse and release heat when energy demand exceeds supply. Unwanted charge leakage and low heat transfer rates can limit the effectiveness of the units, but both of these problems can be mitigated by incorporating a metal foam into the design of the storage unit. This study demonstrates the benefits of adding copper foam into a thermal energy storage unit based on capric acid enhanced by copper nanoparticles. The volume fraction of nanoparticles and the location and porosity of the foam were optimized using the Taguchi approach to minimize the charge leakage expected from simulations. Placing the foam layer at the bottom of the unit with the maximum possible height and minimum porosity led to the lowest charge time. The optimum concentration of nanoparticles was found to be 4 vol.%, while the maximu possible concentration was 6 vol.%. The use of an optimized design of the enclosure and the optimum fraction of nanoparticles led to a predicted charging time for the unit that was approximately 58% shorter than that of the worst design. A sensitivity analysis shows that the height of the foam layer and its porosity are the dominant variables, and the location of the porous layer and volume fraction of nanoparticles are of secondary importance. Therefore, a well-designed location and size of a metal foam layer could be used to improve the charging speed of thermal energy storage units significantly. In such designs, the porosity and the placement-location of the foam should be considered more strongly than other factors.

Highlights

  • The storage of heat energy in a material by inducing a phase change, and the resulting heat transfer mechanisms, are the subject of much current research and development [1].This subject is of great interest in many engineering and industrial applications, such as buildings, solar collectors, power generation, and automotive applications [2,3,4]

  • A numerical study of conjugate heat transfer in a square enclosure filled with water that contained alumina nanoparticles, heated by a triangular region in one corner, found that the average Nusselt number in the system was directly proportional to the volumetric fraction of the nanoparticles and inversely proportional to the size of the triangular heat source [11]

  • Their findings indicated that at low Rayleigh numbers, where laminar flow dominates, increasing the volume fraction of the nanoparticles and the size of the heating region directly resulted in increasing the Nusselt number and so enhanced the convective heat transfer, while the same changes gave adverse effects on convection at high

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Summary

Introduction

The storage of heat energy in a material by inducing a phase change, and the resulting heat transfer mechanisms, are the subject of much current research and development [1].This subject is of great interest in many engineering and industrial applications, such as buildings, solar collectors, power generation, and automotive applications [2,3,4]. A numerical study of conjugate heat transfer in a square enclosure filled with water that contained alumina nanoparticles, heated by a triangular region in one corner, found that the average Nusselt number in the system was directly proportional to the volumetric fraction of the nanoparticles and inversely proportional to the size of the triangular heat source [11] This implies that convection becomes more important as the fraction of nanoparticles increases. The same authors have explored the convective heat transfer of a similar fluid that was nonhomogeneous in a similar square enclosure with a central square region acting as a heat source/sink [12] Their findings indicated that at low Rayleigh numbers, where laminar flow dominates, increasing the volume fraction of the nanoparticles and the size of the heating region directly resulted in increasing the Nusselt number and so enhanced the convective heat transfer, while the same changes gave adverse effects on convection at high

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