Abstract

Two mass-accommodation methods are proposed to describe the melting of paraffin wax used as a phase-change material in a centrally heated annular region. The two methods are presented as models where volume changes produced during the phase transition are incorporated through total mass conservation. The mass of the phase-change material is imposed as a constant, which brings an additional equation of motion. Volume changes in a cylindrical unit are pictured in two different ways. On the one hand, volume changes in the radial direction are proposed through an equation of motion where the outer radius of the cylindrical unit is promoted as a dynamical variable of motion. On the other hand, volume changes along the axial symmetry axis of the cylindrical unit are proposed through an equation of motion, where the excess volume of liquid constitutes the dynamical variable. The energy–mass balance at the liquid–solid interface is obtained according to each method of conceiving volume changes. The resulting energy–mass balance at the interface constitutes an equation of motion for the radius of the region delimited by the liquid–solid interface. Subtle differences are found between the equations of motion for the interface. The differences are consistent with mass conservation and local mass balance at the interface. Stationary states for volume changes and the radius of the region delimited by the liquid–solid interface are obtained for each mass-accommodation method. We show that the relationship between these steady states is proportional to the relationship between liquid and solid densities when the system is close to the high melting regime. Experimental tests are performed in a vertical annular region occupied by a paraffin wax. The boundary conditions used in the experimental tests produce a thin liquid layer during a melting process. The experimental results are used to characterize the phase-change material through the proposed models in this work. Finally, the thermodynamic properties of the paraffin wax are estimated by minimizing the quadratic error between the temperature readings within the phase-change material and the temperature field predicted by the proposed model.

Highlights

  • The second mass-accommodation method, described in Section 2, was applied to analyse the experimental results obtained from a melting process of paraffin wax used as the phase-change material (PCM)

  • The PCM is stored inside an annular region where water constitutes the heat-transfer fluid (HTF), and circulates through an inner copper tube with a radius of r0 = 6.35 mm concentric to an aluminium surface with an outer radius of R = 10.8 cm

  • Thermocouples for temperature measurements within the PCM domain were placed at a height equal to h = L/2, where L = 10 cm represents the total height of the heat storage unit

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Summary

Introduction

The relationship between melting and solidification times and the temperature of the HTF has been experimentally determined in a cylindrical unit, where paraffin was used as the PCM [8]. Melting and solidification experiments on three different paraffin types were carried out in tilted cylindrical units to determine the effects of the HTF temperature and flow rate, on the thermal performance of the PCM [11]. The authors did not consider heat transfer through natural convection and volume changes upon freezing of liquid water. The effects of natural convection have been considered for the prediction of the melting fraction, which was experimentally estimated from temperature field measurements in cylindrical units [10,15]. One of the proposed models introduces an additional equation of motion for the outer radius of the cylindrical unit and incorporates volume changes in the radial direction. The second method was applied to estimate the thermodynamic parameters of the paraffin through a least-square minimization procedure

Mass-Accommodation Methods
Mass Accommodation through Radial Changes
Mass Accommodation through Axial Growth
Steady-State Regime
Experimental Setup
Results and Discussion
Conclusions
Full Text
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