Abstract

A conical shell-tube design with non-uniform fins was addressed for phase change latent heat thermal energy storage (LHTES). The shell was filled with nano-enhanced phase change material (NePCM). The cone aspect ratio of the shell and the fins aspect ratio were adopted as the geometrical design parameters. The type and volume fraction of the nanoparticles were other design parameters. The investigated nanoparticles were alumina, graphite oxide, silver, and copper. The finite element method was employed to solve the natural convection flow and phase change thermal energy equations in the LHTES unit. The Taguchi optimization method was utilized to maximize the melting rate in the unit. Two cases of ascending and descending conical shells were investigated. The outcomes showed that the shell-aspect ratio and fin aspect ratio were the most important design parameters, followed by the type and concentration of nanoparticles. Both ascending and descending designs could lead to the same melting rate at their optimum design. The optimum design of LHTES could improve the melting rate by up to 18.5%. The optimum design for ascending (descending) design was a plain tube (a cone aspect ratio of 1.17) filled by 4.5% alumina-Bio-PCM (1.5% copper-Bio-PCM).

Highlights

  • Offering a high energy density and nearly isothermal operation, a latent heat thermal energy storage (LHTES) system is often a preferable choice over other thermal energy storage systems

  • The results showed that the decreased percentage in melting time relies on the heat transfer fluid (HTF) inlet temperature

  • The present study aims to maximize the melting rate at seven hours of charging time

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Summary

Introduction

Offering a high energy density and nearly isothermal operation, a latent heat thermal energy storage (LHTES) system is often a preferable choice over other thermal energy storage systems. LHTES systems use a phase change material (PCM) as the storage medium. Thermal energy is stored when the solid PCM undergoes a phase change to liquid, and when the phase change process is reversed, i.e., the molten PCM solidifies, the stored energy is released. The performance of an LHTES system might be degraded due to the low thermal conductivity of the PCMs; implementation of heat transfer enhancement techniques may become necessary. The heat transfer enhancement techniques can be divided into two categories: (1) improving the thermal physical properties of the 4.0/).

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