Review on thermal energy storage systems

 Souad BABAY, Hamza BOUGUETTAIA*, Djamel BECHKI,

 Slimane BOUGHALI, Bachir BOUCHEKIMA and Hocine MAHCENE

 Department of Physics, Laboratory of New and Renewable Energy in Arid Zones (LENREZA),

 Ouargla University, 30000, Algeria.

ABSTRACT

 In the past five thousand years human energy consumption per capita has risen from 9 to 230 kWh/capita.day.  At the current rate of usage, taking into consideration population increases, natural resources will be depleted within a few decades. One must therefore endeavour to take precautions today for a viable world for coming generations. There are many situations where available energy is wasted because it is in the wrong place and/or at the wrong time. Therefore, there is a desperate need for energy storage and a very wide range of techniques is used for this purpose. Most methods involve high capital investment; however, so a cheaper alternative has been widely exploited in which thermal energy is stored in a suitable medium. Sensible and latent heat thermal storage systems in general have been among main topics in research for the last two decades or so, but although the information is quantitatively enormous, it is also widely spread in the literature, and often quite difficult to find. This work provides a survey of studies dealing with thermal energy storage (TES) using sensible and solid–liquid phase change thermal energy storage units. Three aspects have been the focus of this review: storage media, heat transfer analysis and applications. The work described below falls within an area of international interest as it deals with energy saving, the efficient and rational use of available resources and the optimum use of renewable energies.

  KEYWORDS: Energy storage, Porous media, Phase change materials, Solar energy, Fixed beds.

  1. Introduction

    Energy production and consumption is the main driving force of all urban and industrial activities. More than 80% of world energy is provided by combustion of fossil fuels. In addition, 16% of the total energy consumption is provided by nuclear power and the remaining 4% includes other forms, such as hydro, wind and solar energy.

 There are many situations where available energy is wasted because it is in the wrong place and/or at the wrong time. There is therefore a need for energy storage and a very wide range of techniques is used for this purpose including electrical storage, air compression and the pumped storage of water. All such methods involve high capital investment; however, so a cheaper alternative has been widely exploited in which thermal energy is stored in suitable medium. Efforts of rational and effective energy management as well as environmental considerations increased the interest in utilizing renewable energy sources, especially solar energy. The work described below falls within an area of international interest as it deals with energy saving, the efficient and rational use of available resources and the optimum use of renewable energies [8]. Within this framework, thermal energy storage (TES) provides solutions in very specific areas:

 ·       The time delay between production or availability of energy and its con­sumption in receiving systems,

 ·       Security of energy supply (hospitals, computer centers, etc.)

 ·       Thermal inertia and thermal protection

 This work provides a survey of studies dealing with TES using sensible and phase change materials. The material in this review has been arranged within the main areas of work:

 ·      Energy storage media

 ·      Heat transfer analysis

 ·      Applications

      Useful classification of the substances used for TES is shown in Figure.1. The latter contains a complete review of the material types which have been used, their classification, characteristics, advantages and disadvantages and thevarious experimental techniques used to determine the behavior of these materials in melting and solidification [16].

Solar energy can be stored in insulated vessels of rocks or pebbles, and it is convenient for use in buildings. This type of storage is used very often for temperatures up to 100 °C in conjunction with solar air heaters. Typically, the characteristic size of the pieces of rock used is in the range 1-5 cm. An approximate rule followed for sizing is to use 300-500 kg of rock by m2 of solar collector area for space heating applications. For a temperature change of 50 °C, rocks and concrete can store up to 36 kJ/kg [14].

 2.3. Storage in metals

       Most of the materials proposed for high temperature (120-1400 °C) energy storage are either inorganic salts or metals. Among the metals, aluminum, magnesium and zinc have been mentioned as suitable examples. The use of metals media may be advantageous where high thermal conductivity is required and where cost is of secondary priority [20].

 2.          Latent heat storage

       In the latent heat storage, thermal energy is accumulated by means of a reversible change phase occurring in the medium. Solid-liquid transformation is most often used to avoid large pressure vessels required for vaporization or sublimation [2]. Latent heat storage is a particularly attractive technique, since it provides a high energy storage density and has the capacity to store as latent heat of fusion at a constant temperature corresponding to the phase transition temperature of the phase ­change materials (PCMs). This means that a much smaller weight and volume of material is needed to store a certain amount of energy [22].       

 PCMs may undergo solid-solid, liquid-gas or solid-liquid phase transformations. Relatively few solid-solid PCMs have been identified that have heats of fusion and transition temperatures suitable for thermal storage applications. Liquid-gas PCMs usually have high heats of transformations, however, due to their large volume change during transition, they are not usually considered for practical applications. Solid-liquid PCMs are useful because they store a relatively large quantity of energy over a narrow temperature range, without a corresponding large change in volume [24].

 Typically, the chosen PCM is placed in long thin tubes stacked in a container. During a heating cycle, the collected solar heat from the collector is circulated through narrow spaces between the tubes and melts the PCM by storing the sensible heat as well as the latent heat of fusion. During the heat recovery cycle, the circulation of cool air would pick up the stored energy from the PCM and transport it to the heat load. Therefore, the latent heat storage system uses the sensible heat in the solid and liquid phases and additionally the latent heat due to the phase change of the storage media. 

 The development of any latent heat thermal energy storage (LHTES) system, therefore, involves an understanding of two essentially diverse subjects: heat storage materials (or PCMs) and heat exchangers [17].

       Table.1 shows a comparison between the sensible heat storage using a rock bed and water tank and also shows the latent heat storage using organic and non-organic compounds. The advantage of the latent heat over the sensible heat is clear from the comparison of the volume and mass of the storage unit required for storing a certain amount of heat. It is also clear from Table.1 that inorganic compounds have a higher volumetric thermal storage density than the most of the organic compounds due to their higher latent heat and density [11].

 Through the comparison between the sensible and latent energy storage units, one can conclude that the latter solution is more appealing. In fact, the latent heat of most materials is much higher than their sensible heat, thus requiring a much smaller mass of storage medium for storing and then recovering a given amount of thermal energy. Moreover, the latent heat thermal storage process occurs at nearly constant temperature, which is typically desirable for efficient operation of most thermal systems.

5. Some geometrical configurationsand applications of heat storage units

    The application of energy storage with sensible and phase change materials is not limited only to solar energy heating andcooling but has also been considered in other applications. Some are discussed in the following sections.

 5.1. Aquifers thermal energy storage

       For large scale storage applications, underground natural aquifers have been considered. Aquifers are geological formations containing ground water, offering a potential way of storing heat for relatively long periods of time. For example, 105 m3 of aquifer material can store about 3 MJ of heat for each 10 °C temperature difference. This type of storage is well suited for seasonal storage. The attractiveness of aquifer storage is due to its low cost characteristics, its high input/output rates and its large capacity. Because of its bulk nature, aquifer storage is not feasible for small loads, such as individual houses.

 Aquifers hold great promise for underground energy storage, assuming that ones adequate for such storage can be found. In many systems, the heat source for aquifer thermal energy storage (ATES) is solar collectors. Several large-scale projects related to high-temperature un­derground storage (>50°C) of waste heat from co-generation plants and incineration plants are in planning in Europe and the US [13, 23, 25]. Estimation of the heat recovery rate is re­quired before the system is built.

 5.2. Solid media sensible heat storage for parabolic trough power plants

       For parabolic trough power plants using synthetic oil as the heat transfer medium, the application of solid media sen­sible heat storage is an attractive option regarding investment and maintenance costs. Solid media sensible heat storage materials have been widely researched in parabolic trough plants. For the development of solid media storage material, the thermo-physical properties of the materials like density, specific heat capacity, thermal conductivity, coefficient of thermal expan­sion (CTE) and cyclic stability as well as availabil­ity, cost and production methods are of great relevance.

 A high heat capacity reduces the storage volume and a high thermal conductivity increases the dynamics in the system. The CTE of the storage material should match the CTE of the embedded metallic heat exchanger material. A high cyclic stability is important for a long storage unit life­time [15].

 5.3. Indirect contact latent heat storage of solar energy

       Extensive efforts have been made to apply the latent heat storage method to solar energy systems, where heat is required to be stored during the day for use at night. The studies variedfrom those related to the fundamental aspects of heat transfer to those in which the PCM is tested in full size heat storage units.

 Most PCMs have low thermal conductivity that limits heat transfer rates during their appli­cations. Hence, the PCM must be encapsulated in such a way as to prevent the large drop in heattransfer rates during its melting and solidification. The PCM is usually contained in a number of thin flat containers, similar to plate type heat exchangers, as shown in Figure.3.

      Alternatively, it may be contained in small diameter tubes with the heat transferfluid flowing along or across the tubes. The idea of using finned tubes inwhich the PCM was placed between the fins has also been tested. Although a significant improvement in heat transfer rate was found, the high cost of the finned tubes may make their use uneconomical [26]. It is to be noted that such arrangements may improve heat transfer rates significantly only when a liquid isused as a heat transfer fluid. In air based systems, the heat transfer coefficients of both the air and the PCM sides are low [7, 8].

 A large improvement in the heat transfer rate was obtained by encapsulating the PCM in smallplastic spheres to form a packed bed storage unit. However, the expected high pressure drop through the bed and its initial cost may be major drawbacks of such units. Most of the PCMs undergo large changes in volume(~10%) during melting. This may causehigh stresses on the heat exchanger walls. Volume contraction during solidification may not onlyreduce heat transfer area but also separate the PCM from the heat transfer surface and increasing theheat transfer resistance dramatically. The problem is usually minimized by proper selection of thecontainers, which should be partially filled with the PCM. Spherical encapsulation can be a good solution to this problem.

 In an effort to improve the performance of phase change storage units, Farid et al [9] have suggested the use of more than one PCM with different melting temperatures in a thin flat container, as shown in Figure.4.

 

5.4. Spiral thermal energy storage unit

      The use of a vertical spiral heat exchanger in a latent heat energy storage system has been analyzed experimentally. A spiral heat exchanger, commonly used in chemical and food industries, seems to be a good candidate for this task. Compactness, enhanced heat transfer due to centrifugal forces, easy sealing, large heat transfer surface and a shorter undisturbed low length are the most appealing features of such a choice [1]. The thermal energy storage units are usually designed as a vertical cylindrical heat exchanger of Archimedes spiral geometry. It is shown in Figure.5 in its isometric view.  This is achieved by winding two sheets of a copper plate into the form of a spiral; two coaxial spiral cylinders are created

5.5. Combined sensible and latent heat storage system

       The sensible heat storage (SHS) system is simple and a well-developedtechnology. Latent heat storage (LHS) systems using phase change material (PCM) as storage medium offer advantages such as high heat storage capacity, small unit sizes and isothermal behavior during charging and discharging processes. But these types of systems are not in commercial use as much as SHSsystems because of the poor heat transfer rate during heat storage and recovery processes. The main reason is that during phase change, the solid–liquid interface moves away from theconvective heat transfer surface (during charging in cool storage process and discharging inhot storage process) due to which the thermal resistance of the growing layer of solidifiedPCM increases, thereby resulting in poor heat transfer rate.

       The combined sensible and latent systems eliminates the difficulties experienced in the SHS and LHS systems to some extent and posses the advantages of both systems.

 It is understood from the literature survey that most of the research work on TES is concerned only with either SHS systems or LHS systems and not much work has been reported on combined sensible and latentsystems. The thermal behavior of packed beds of combined sensible and latent heat TES system integrated with constant temperature water bath/solar flat plate collector has been studied. The packed bed contains encapsulated PCM in spherical capsules, which are surrounded by SHS material. The performance of these systems during discharging process is also compared with the conventional SHS system [18].

 5.6. Phase change thermal storage for shifting the peak heating load

        Electricity consumption varies during the day and night according to the demand by industrial,commercial and residential activities. The variation in electricity demand sometimes leads to a differential pricing system in peak and off peak periods, usually after midnight until early morning. The shift of electricity usage from peak periods to off peak periods will provide sig­nificant economic benefit. The development of an energy storage system may be one of the solutions to the problem when electricity supply and demand are out of phase. Energy storage systems will enable the surplus energy to be stored until such time as it is released when needed.

 Winter storage heating is a direct and a simple application of energy storage and has been used in many countries. The most common domestic storage heater uses ceramic bricks and structural cement, which is heated with electrical heating wires or heat transfer fluids (such as hot water)during the night. During the day, the heat is extracted from the heater by natural convection andradiation or by forced convection using an electric fan. Farid and Hasnain [9, 10] have introduced anew concept to the design of these storage heaters by replacing the ceramic bricks with a paraffinwax encapsulated in thin metal containers. During heat charge, the wax stores a larger amount ofheat than the latent heat of melting, which is continuously discharged during the other periods.

 5.7. Building applications

       The selection of PCMs to meet residential building specifications has received minor attention,although it is one of the most foreseeable applications of PCMs. The ability to store thermal energy is important for effective use of solar energy in buildings. Because of the low thermal massof lightweight building materials, they tend to have high temperature fluctuations, which result in high heating and cooling demands. It has been demonstrated that paraffins, as mixtures of several linear alkyl hydrocarbons, may be tailored by blending to obtain the desired melting point re­quired for a particular application. Pure paraffins with exceptionally good properties have notyet been tested further due to the unavailability of inexpensive bulk sources. In buildings, a more interesting approach to smooth the temperature variations within a space is by using wallboards containing a PCM. The wall large heat transfer area supports large heat transfer between the wall and the space. The wallboards are cheap and widely used in a variety of applications, making them very suitable for PCM encapsulation. However, the prin­ciples of latent heat storage can be applied to any appropriate building materials.

 Heat storage is applicable to both new and existing buildings and can be integrated with both air and water distribution systems. Building mass and structure cement can also be used with active or passive storage design. The most common configuration using building mass for thermal storage is floor warming. Heating and cooling of buildings were widely investigated using their floor. Solar radiation stored in the floor thermal mass was found to reduce heating energy consumption significantly (30% or more) [14, 21].Figure.6 shows a general layout of a standard solar air space-heating system. However, the development of reliable and practical thermal energy storage systems still faces some major hurdles, such as uncertainties concerning the long term thermal behavior and the small number of PCMs suitable for room temperature applications.

 

  6.       Conclusions

 The following may be established as conclusions:

 ·         Sensible heat storage and latent heat storage are among the major techniques of thermal energy storage considered nowadays for different applications, such as space heating and hot water production,

 ·         The operation of packed beds for energy storage depends mainly upon efficient heat transfer  coefficient between the fluid stream and the medium in the bed,

 ·         Most existing heat transfer correlations for the packed bed thermal energy storage are limited to relatively low temperature ranges and with spherical particles,

 ·         Latent heat storage is a developing technology that has been found quite promising in recent times. In the development of this field, research is underway in two axes, namely the investigation of phase change materials (PCM) and of heat exchangers,

 ·         Solid-liquid PCMs are useful because they store a relatively large quantity of energy over a narrow temperature range, without a corresponding large change in volume during transition,

 ·      The PCMs must undergo thermal cycling tests in order to determine whether these thermal exposures will result in migration of the PCM or may affect the thermal properties of the PCM,

 ·      Encapsulation results in the improvement of the physical and chemical stability of the heat sink material, increases heat transfer area, reduces PCMs reactivity towards the outside environment,

 ·         Spherical capsules are preferred due to favorable ratio of volume of energy stored to the area of heat transfer and also because of easiness of packing into the storage tank with good bed porosity,

 ·      Organic and inorganic compounds are the two most common groups of PCMs,

 ·      Most organic PCMs are non-corrosive, chemically and thermally stable; exhibit little or no sub-cooling and low vapor pressure. Their disadvantages are low thermal conductivity, high changes in volume on phase change and flammability,

 ·      Inorganic compounds have a higher volumetric thermal storage density than the most of the organic compounds due to their higher latent heat and density,

 ·      Inorganic compounds have a high thermal conductivity, non-flammable and low cost in comparison to organic compounds; however they are corrosive to most metals and suffer from decomposition,

 ·         There is a clear advantage of the latent heat over the sensible heat from the comparison of the volume and mass of the storage unit required for storing a certain amount of heat,

 ·         Despite that PCMs have been widely investigated by many researchers, many of their thermo-physical properties in the solid and liquid phases are lacking in the literature. It is suggested that further detailed calculations and experimental data for these properties should be made in order to assist the effective and appropriate design of the thermal storage units.

 References

 [1] J. Banazek, R. Domanski, M. Rebow and F. El-Sagier ; Experimental study of solid-liquid phase change in a spiral thermal energy storage unit ; Appl. Therm. Eng. 19, 1253-1277 (1999).

 [2] A. Benmansour and M.A Hamhan ; Simulation du stockage de l’énergie thermique dans un lit fixe de sphère contenant un matériau à changement de phase ; Revue d’Energie Renouvelable 4, 125-134 (2001).

 [3] H. Bouguettaia,D. Bechki and M.T Meftah ; Transfer de la chaleur dans un milieu poreux ; 5eme séminaire International sur la Physique Energétique, Béchar,  Algérie, Nov. 2000.

 [4] D. Bechki, H. Bouguettaia and M.T Meftah ; Propriétés thermiques d’un lit fixe ; La Marsa, Tunis, Tunisie, (2001).

 [5] D. Bechki, H. Bouguettaia, M.T Meftah and S. Boughali ; Détermination Expérimentale du Coefficient de Transfert de Chaleur Global dans un Lit Fixe ; 6eme séminaire International sur la Physique Energétique, Béchar,  Algérie, Oct. 2002.

 [6] B. Dhifauoi, S. BenJabllah, A. Belghith and J.P. Corriou ; Experimental study of the dynamic behavior of a porous medium submitted to a wall heat flux in view of thermal energy storage by sensible heat ; Int. J. Ther. Scien 46, 1056-1063 (2007).

 [7] H.M. Ettouney, I. Alatiqi, M. Al-Sahali and S.A. Al-Ali ; Heat transfer enhancement by metal screens and metal spheres in phase change energy storage systems ; Renewable Energy 29, 841-860 (2004).

 [8] M. Fang and G. Chen ; Effects of different multiple PCMs on the performance of a latent thermal energy storage system ; Appl. Therm. Eng. 27, 994-1000 (2007).

 [9] M.M. Farid, A.M. Khudhair, S.A.K. Razack and S. Al-Hallaj ; A review on phase change energy storage: Materials and applications ; Energy Convers. Manage. 45, 1597–1615 (2004).

 [10] S.M. Hasnain ; Review on sustainable thermal energy storage tech­nologies, Part I: Heat storage materials and techniques ; Energy Convers. Manage. 39, (11), 1127–1138 (1998).

 [11] K.A.R. Ismail and R. Stuginsky Jr ; A parametric study on possible fixed bed models for pcm and sensible heat storage ; Applied Thermal Engineering 19 757–788 (1999).

 [12] S. A. Kalogirou ; Solar thermal collectors and applications, progs in energy and combust sci. 30, 231-295 (2004).

 [13] M. Kangas and P. Lund ; Modeling and simulation of aquifer storage energy systems; Int. J. Solar Energy 53 (3), 237–247 (1994).

 [14] T. Kousksou and al. ; Second law analysis of latent thermal storage for solar system ; Solar Energy & Solar Cells 91, 1275-1281 (2007).

 [15] D. Laing, W. Steinmann, R. Tamme and C. Richter ; Solid media thermal storage for parabolic trough power plants ; Solar Energy 80, 1283-1289 (2006).

 [16] E.R. Lapwood ; Convection of a fluid in a porous medium ; Proc. Camb. Soc. 44, 508–521 (1948).

 [17] K. Nagano, S. Takeda, T. Mochida and K. Shimakure ; Thermal characteristics of a direct heat exchange system between granules with phase change material and air ; Applied Thermal Engineering 24, 2131-2144 (2004).

 [18] N. Nallusamy and al. ; Experimental investigation on a combined sensible and latent heat storage system integrated with constant/varying (solar) heat source ; Renewable Energy 32, 1206-1227 (2007).

 [19] T. Nishimura and al. ; Experiments of natural convection heat transfer in rectangular enclosure partially filled with particles ; Kagaku Kogaku Ronbunshu (Jpn. J. Chem. Eng.) 11 (4), 405–411 (1985).

 [20] E.C. Nsofor and G.A. Adebiyi ; Measurements of the gas-particle convective heat transfer coefficient in a packed bed for high-temperature energy storage ; Experi.Therm and Fluid Scien 24, 1-9 (2001).

 [21] V.V. Tyagi and D. Buddhi ; PCM thermal storage in buildings: A state of art ; Renew & Sustain Energ Reviews 11, 1146-1166 (2007).

 [22] P. Verna, Varun and S.K. Singal ; Review of mathematical modeling on latent heat thermal energy storage systems using phase-change material ; Renew & sustain Energ Reviews, accepted Nov 2006.

 [23] H. Watanabe and al. ; Effects of climate on closed seasonal thermal energy storage in a shallow aquifer, in: Proceedings of Seventh International conference of Energy Storage, Sapporo, Japan 18–21st June, 1997, pp. 721–726.

 [24] J.F. Wang, G.M. Chen and F. Zheng ; Study on phase change temper­ature distributions of composite PCMs in thermal energy storage systems ; Int. J. Energy Res. 23, 277–285 (1999).

 [25] T. Yokoyama and al. ; Temperature propagation in unconfined aquifer coupled with three dimensional two-phase analyses in multiple layers, in: Proceedings of Seventh International Conference of Energy Storage, Sapporo, Japan 18–21st June, 1997, pp. 691–696.

[26] Y.W. Zhang and A. Faghri ; Heat transfer enhancement in latent heat thermal energy storage system by using internally finned tube ; Int. J. heat Mass Transfer 39 (15), 3165-3173 (1996).