A REVIEW OF THERMAL ENERGY STORAGE SYSTEMS WITH SALT HYDRATE PHASE CHANGE MATERIALS FOR COMFORT COOLING Justin Ning-Wei Chiu*, Dr. Viktoria Martin, and Prof. Fredrik Setterwall *KTH – Department of Energy Technology, Brinellvägen 68, SE-100 44 Stockholm, SWEDEN Tel: +46 (0)87907476 [email protected] Abstract This paper presents a review of cold thermal energy storage technologies. Latent heat thermal energy storage (LHTES) with phase change materials (PCMs) deserves attention as they provide high energy density and small temperature change interval upon melting/solidifying. Salt hydrates are especially interesting since they demonstrate high latent heat of fusion, high thermal conductivity, low flammability, and facilitate the use in buildings as compared to organic PCMs. A review of system performance obtained from experimental work, theoretical analyses and real case studies has however shown some material shortcomings. To reach cost effectiveness, future work in the field of LHTES with salt hydrates lies in finding suitable methods for limiting incongruent melting and subcooling without compromising the storage density. Also, system integration of LHTES in cold applications can be further developed in terms of innovative design for high power and storage capacity, load optimized sizing, controls, and elimination of PCM encapsulation. 1 Introduction Many reviews have been conducted in the light of providing the state of the art of latent heat thermal storage in buildings (e.g., [1, 2, 3, 34, 77, 95]). Here, the focus is on reviewing cold thermal energy storage (CTES) systems using salt hydrates for comfort cooling. CTES systems can be effectively implemented in cooling systems where peak cooling demands are high and the capacity is limited. Advantages of running thermal energy storage (TES) systems have for example been high-lighted as cost effectiveness, and energy reduction [4]. However, when implemented in a district cooling network, peak cooling load may be reduced by offsetting the load to off peak period, therefore allowing district cooling plants to provide additional cooling power without the need of expanding existing infrastructure and hence reduction in capital cost. When installed in an electrical chiller based cooling system, peak grid electricity load may be alleviated by producing cold during offpeak hours and releasing cold during peak hours. Not only does peak shaving lower the marginal electricity cost by cutting down premium fuel use [5], but power plants operating at night also demonstrate higher electricity production efficiency. In addition, lower ambient temperature at night increases chiller performance if ambient air is used as heat sink, which further reduces the energy consumption. TES provides new means of thermal energy management and electric power distribution over the existing network. However, the payback period of a potential cold storage installation is not always as attractive as other energy saving technologies [4]. Research focus is now being put in improving the energy storage density, increasing the power extraction/storage rate and minimizing investment cost. This paper will first delve into water and ice based TES, followed with an introductory overview on material properties of salt hydrates in comparison with organic and eutectic mixtures, then a state of the art on salt hydrate based TES system performance will be illustrated with emphasis on cold storage applications. 2 Thermal Energy Storage Materials Water, as one of the most abundant natural resource, has been largely used in TES systems. Stratified chilled water storage (SCW) is technologically mature and is utilized in thermal storage applications. However, the small temperature interval in comfort cooling limits the stored capacity. Typically, a 10°C temperature difference of water storage corresponds to 12 kWh/m³ energy storage density. Therefore, the volume required for SCW for cooling storage may be enormous. The cost of SCW has been evaluated by Hasnain [6], who reported that such system is only economical in system where at least 7,000kWh of cooling is needed, and where space is available. Phase change material (PCM) utilizes the latent heat of the melting/solidification process to store energy. They are characterized by high volumetric storage density and a small temperature interval for thermal energy extraction and regeneration [ 7 ]. The feed in temperature for cooling may thus be maintained at constant level facilitating controls. Ice, as one of the first PCMs used, has been implemented in various cooling systems. Commercial ice storage systems have for example been installed in capacities ranging from 1,000kWh to 120,000kWh [8 9]. The advantages of using ice are the low cost and the high storage energy density, eight times the storage capacity of a SCW with a temperature difference of 10°C. However, ice storage systems require chillers capable of energy production below freezing point of water and shows large volume expansion upon solidification [10]. Thus, ice storage is not suitable for integration with district cooling, and limits the amount of natural cooling (free cooling) that can be used in a system. Using other PCM materials with higher melting temperatures overcomes the low energy storage density experienced with SCW, and facilitates direct integration to an existing cooling system [2]. For instance, higher coefficient of performance (COP) of cooling units is achieved with higher melting temperature PCMs as compared to ice production [11]. Thus, PCM LHTES may provide more economic and cost effective storage solutions than ice storage systems. PCMs are here divided into two main families: organic and inorganic [12]. Organic materials can be further classified into paraffin and non paraffins such as esters, fatty acids, alcohols and glycols. Inorganic materials are subdivided into salt hydrates and metallics. Mixtures of chemical compounds constitute practical PCM and this leads to a melting/solidification temperature range as compared to using pure chemicals. Eutectic mixtures of organic and/or inorganic materials are desirable in that they melt/solidify at a constant temperature like a pure chemical. A large variety of PCMs are currently available, however they must exhibit correct operating temperature range, desirable thermodynamic, kinetic and chemical properties as well as reasonable costs to be effectively integrated in TES systems [12, 13]. Table 1 Salt Hydrate and Wax Paraffin Comparison Organic Inorganic Eutectic Low Cost (120Euro/kWh) [14] Moderate cost (130 Euro/kWh) Sharp melting point Self nucleating [ 15 16] Low volumetric storage density Chemically inert and stable High volumetric storage density No phase segregation (180-300 MJ/m³) Recyclable Higher thermal conductivity Available in large temperature (0.6W/m°C) range Non flammable Low volume change Flammable Subcooling Limited available material property Low thermal conductivity Phase segregation data (0.2W/m°C) Corrosion of containment material Low volumetric storage density (90-200 MJ/m³) Some key characteristics of PCMs are summarized in Table 1. Organic compounds exhibit favorable characteristics such as congruent melting, low volume change, and non corrosiveness. However, they also show low thermal conductivity, high flammability, varying level of toxicity and non compatibility with certain plastic containers [17, 18, 19]. Salt hydrates have high storage density and higher thermal conductivity as compared to paraffins. For certain building codes, non toxicity and non flammability are also assets of salt hydrates. Nonetheless, corrosion, incongruent melting and subcooling are drawbacks that need to be mastered to provide technically and economically sound storage solutions. Several compilations of material properties exist [1, 11, 12, 20, 21, 22, 23]. From these sources, a summary of phase change enthalpy of commercialized salt hydrate mixtures has been derived (Figure 1, left). As shown, in the temperature range of comfort cooling, commercialized products have latent heat between 180kJ/L and 300kJ/L as compared to 90kJ/L and 200kJ/L of organics. Available salt hydrates are however limited in numbers. Potential analytical grade salt hydrate with phase change temperature located between 0°C and 40°C are shown in Figure 1 to the right. Many of the analytical salt hydrates fit in the temperature above 25°C, however from 0°C to 25°C, promising materials are limited. It is of great necessity to perform advanced material research to broaden the prospect of available salt hydrate materials covering wider range of comfort cooling temperatures at high storage density. Figure 1 Commercialized Salt Hydrate Products (left) Analytical Grade Salt Hydrates (right). 3 Salt Hydrate Based Thermal Energy Storage System Performance PCM-based CTES needs further development in order to cost-effectively serve as an alternative to SCW storage or direct cooling. To form the basis for this work, a state-of-theart assessment on PCM-based cold storage, with special interest in salt hydrates, is presented in terms of cold storage findings from the literatures. First, the optimal containment of PCM will be addressed, followed by power extraction of the TES. Then, findings on minimizing subcooling and incongruent melting are discussed along with control strategies. 3.1 Optimum Encapsulation Geometry Three types of PCM containment are identified: macro encapsulation, micro encapsulation and bulk storage. Encapsulation serves as heat transfer surface, prevents PCM from reacting with outside environment, and adds mechanical strength to the structure. Macro encapsulation has been produced in pouches, tubes, and ball type storage geometry [8, 24, 25, 26, 27]. They provide self supporting structure and are easily maneuverable [5]. It has been found by Wei [28] that the thermal transfer performance is the highest with spherical capsules, followed by cylindrical, plate type and tubular encapsulations. Microencapsulation overcomes the shortcoming of phase segregation [13, 29] and demonstrates notable heat transfer increase where Barba [30] showed the solidification time of the PCM being reduced as inversely proportional to the square of capsule radius. However, microencapsulation exhibits the highest production cost among the three containments [5] which limits the economical viability of such technology. The third type of storage, bulk storage of PCM, requires extensive heat exchanger design for sufficient thermal energy extraction power. One of the main concerns with bulk storage may be the air tightness of storage tank, without which salt hydrate would lose water content resulting in incomplete crystallization heat release. On the other hand, bulk storage can significantly reduce the PCM TES cost with elimination of the packaging process. Furthermore, the storage density can be made higher since bulk storage increases the ice packing factor (IPF). This reduces the cost by reducing the storage size and space needed for a certain amount of stored cooling. Thus it appears that enhancement of heat transfer through low conductive PCMs in bulk storage could be a highly desirable area for research and development. 3.2 Heat Transfer Enhancement The rate of heat transfer in gelled salt hydrate depends on three major heat transfer processes: convection from the heat transfer fluid (HTF) to the heat exchanger wall, conduction within the heat exchanger, and heat transfer from heat exchanger wall to the core PCM through conduction and/or convection. While salt hydrates exhibit thermal conductivity two to three folds that of organic materials, property acquired from databases shows that it rarely surpasses 0.6W/m.K [11, 20, 21, 22]. Moreover, in the solidification process, the solid layer formed on heat exchanger surface reduces the heat transfer rate. A large body of literatures commented on observing low TES power rate in freezing/crystallization [6, 31]. However, the issue of a slower solidification as compared to melting is, in CTES, presumably not a problem since charging of cold (freezing) may be extended over a longer period. The critical part in heat transfer is thus to have a high power at discharging (melting). Therefore, heat transfer enhancement should prioritize the discharging process. Experimental studies of heat transfer of CaCl2⋅6H2O in vertical cylindrical tubes led to a conclusion that the convective process was the major heat transfer process with non gelled PCM [32, 33]. Wei [28], Zalba [34] and Ismail [35, 36] have concluded from experimental and numerical parametric studies that the solidification rate of a LHTES can be improved with increasing HTF flow rate and decreasing HTF entry temperature. It was further mentioned that the duration of solidification time shortens with decreasing capsulation size and that increasing heat exchanger wall thickness lead to faster solidification rate. Non thickened organic PCMs have a higher heat transfer rate during melting process due to convective process [37], but such configuration may lead to phase separation if applied on salt hydrates. Numerical models for fixed bed of encapsulated PCM have been examined by Ismail [38]. In the same study, the HTF flow rate was shown to have less influence on storage performance as compared to the inlet temperature and void fraction of the bed. In addition, larger temperature difference between HTF and PCM was found to give higher charging/discharging rate. Investigation has been done to improve heat transfer coefficient by adding external fins [39, 40, 41, 42], internal fins [43] or with other types of heat transfer enhancing methods such as lessing rings or water steam [44]. Choi [45] studied the efficiency of thick finned tube showing heat transfer rates between 90W/m²K and 250W/m²K. Ismail [46] examined finned tube configurations and concluded that, for optimal performance, the fins should be placed in the same direction as the tubes with four to five fins of twice the tube diameter around the tube circumference. Also, the study showed that fin thickness has small influence on the solidification time of PCM. Other means of enhancing the heat transfer have been examined: dispersion of aluminum [47], and graphite [48 49] into the PCM; and absorption of PCM into expanded graphite [50]. Dispersing a highly conductive substance into high storage capacity PCM for thermal conductivity improvement has been tested since the 80’s by Knowles [51]. Recently, the scientific field has shown renewed interest in the concept; investigations are however more concentrated around organic compounds. Introduction of 50wt% of aluminum powder to paraffin wax increased the thermal conductivity by a factor of 20 [52]. Promising results on improving the conductivity of organic PCM have been reported: the introduction of 10% by weight of expanded graphite (EG) to a Capric–myristic acid/expanded perlite composite, the thermal conductivity is increased by 58% [53]; by introducing 2% of EG into Capric– myristic acid/vermiculite composite, 85% thermal conductivity improvement was observed [54] ;adding 10% into stearic acid increased its thermal conductivity by 266% [55]. Study of heat transfer enhancement by impregnating PCM into a graphite matrix has also been carried out [56, 57, 58]. Here, thermal conductivity improvements between 20 and up to a 1000 times were observed depending on the specific blends and methods. Among the salt hydrates, EG added to sodium acetate trihydrate has been studied within the IEA Solar Heating and Cooling program - Task 32 [59]. However, extensive studies on salt hydrate thermal property enhancement in the range of comfort cooling are lacking and thus still need to be carried out. 3.3 Phase Separation Minimization Incongruent melting, or phase separation, can cause a loss in enthalpy of solidification as reported by Cantor [60]. Such phase segregation can be reduced with the addition of extra water, use of microcapsules, rotary storage tank and thickening agents [63]. The addition of 3% super absorbent copolymer (SAP) has been found to completely prevent phase separation of Glauber’s Salt [61]. Thixotropic (attapulgite clay) and alginate have been tested as well [62]. Ryu [63] reported the effectiveness of SAP made from carboxymethyl cellulose (CMC), and polyvinyl alcohol (PVA) with addition of 3wt% to 5wt% for high hydrate inorganic salts and 2 wt% to 4 wt% for low hydrate inorganic salts. However, in another study it was shown the addition of bentonite, starch and cellulose to sodium acetate trihydrate still resulted in 20% to 35% of latent enthalpy drop [64]. Polymeric polycarboxylic acid, silica gel and diatomaceous earth are all potential gelling agents [63]. Although thickening agents have been added to prevent phase separation, thermal cycling may still lead to thermal capacity drop. For example a 48% drop in stored capacity for Glauber’s salt was noted after 200 cycles [65]. As explanation, it has been found that the cause of capacity drop is due to PCM crystal boundary behavior which leads to parting of thickeners and nucleating agents upon solidification. With the addition of 1% acrylamide/acrylic acid copolymer (AACP) and 0.1% of sodium hexametaphosphate (SHMP, (NaPO3)6) as crystal habit modifier, the storage capacity was maintained at 82% of ideal value after 1600 cycles [66]. Calcium chloride hexahydrate has shown good stability after 1000 cycle test, and may thus be a potential promising PCM for TES [67]. In order to minimize phase separation, rolling cylinder heat storage system that mixes the salt hydrate under constant rotation has been proposed by Herrick [68], after 200 cycles no performance degradation was found. However, a cost analysis for economical validation of the concept is required, as is the assessment of the parasitic electricity load due to the rolling. In order for salt hydrates to be fully competitive as PCM materials, technical design, phase separation and cyclic stability must be mastered, along with the subcooling minimization. 3.4 Subcooling Minimization The use of nucleating agents, cold finger and porous heat exchange surface has been utilized to prevent subcooling [69]. Carbon nanofibers, copper, titanium oxide as well as potassium sulfate and borax have also been demonstrated as good nucleating agents [63, 70, 71]. An extensive study of nucleating agents added to CaCl2·6H2O, MgCl2·6H2O, and Mg(NO3) ·6H2O was investigated by Lane [71]. The optimum addition in weight percentage of borax in Glauber’s salt was studied by various researchers [71 72], 0.95% to 1.9% of pulverized borax was found to be the most effective in subcooling minimization. The addition of Na2P2O7·10H20, K2SO4, TiO2, Na2SO4, SrSO4, K2SO4, SrCl2, BaI2, BaCl2, Ba(OH)2, BaCO3, CaC2O4, Sr(OH)2, SrCO3, CaO, MgSO4, and carbon power have also been tested by various investigators and are shown to be promising nucleating agents. Regarding subcooling, although research has given light to nucleating agents that limit subcooling from 20°C to 2°C, in comfort cooling where usable temperature difference is limited, 2°C subcooling may still lead to high efficiency loss from energetic approach. Incorporation of PCM LHTES in an application will have to address this challenging design issue. 3.5 Control System Analysis While control strategy optimization has mainly been focused on heat storage [73], it may be extended to CTES as well. Henze [74] investigated the potential of combination of active and passive cooling through effective control strategies. Commonly, storage control strategies are classified as full storage or partial storage. Full storage performs complete load shift from peak to off-peak power and is most cost effective with high peak hour energy fee. Partial storage is further divided to load leveling and demand limiting schemes, where refrigeration units run at either constant or variable power with storage that complements the load requirement. Peak electric demand for cooling on peak hour with use of proper control strategy may in the best case be reduced by 40% to 90% [6]. Integrated thermal storage system optimized by means of proactive control with use of local weather forecasts [75] may be extended for use in TES model enhancement. The correct control strategy and optimized load distribution management have a significant impact on the energy saving and deserve high consideration in system design. 3.6 Experimental and Numerical System Studies Many application studies on PCM storage are available, though, the major part concerns heating applications. Much information can however be deduced by examining heating applications using PCM technology. One case comparison of TES systems with chiller use scenario led to concluding that TES has lower operating cost and hence is preferred over chiller units [76]. Hasnain [77] performed an in depth study of CTES integration for peak electricity load leveling in Saudi Arabia, showing that the peak electrical load may be reduced by 15% to 23% and peak time cooling rate may be lowered by 35% to 40% upon adoption of CTES technology. Air conditioning application was studied numerically assuming CaCl2·6H2O and KF·4H2O as PCMs [78]. Among the numerous issues, one to be mentioned is the lack of accurate PCM thermal property data, especially for commercial grade products where divergence in heat capacity and phase change temperature may lead to discrepancies between design model and actual TES system [79]. He [80] conducted various phase equilibrium study of PCMs and concluded the results may further be altered with use of differential scanning calorimetry (DSC). Development of T-history method has been investigated and is shown as one important step towards standardization of property measurement [ 81 , 82 ]. Analytical and experimental investigation on heat removal of PCM [83] as well as numerical model for TES simulation [84] were developed to reproduce solidifying and melting phenomena. Blir [85] suggested a list of correlations expressing inward solidification time as a function of Stefan number, Biot number and superheat parameter for cylindrical container and spherical container. Numerical models of melting within capsules [86] and around cylindrical tube [87] were investigated; space thickness, HTF entry temperature, tube wall conductivity and solid phase PCM conductivity were shown to have significant influence on the overall solidification process. The focus of using phase change materials in comfort cooling applications has mainly been put in passive thermal control. Passive walls impregnated with PCM were shown to have better performance than masonry wall of five times the thickness [88] and may lead to effective energy saving in building [89]. Other passive designs that were widely studied are sandwich panels [90], floor heating systems [91], ceiling board thermal storage systems [92], wall boards [93] and window shutters [94]. Building materials impregnated with PCMs, such as gypsum wallboards, concrete ceilings and floors are cost efficient method of shifting thermal loads. Hydrated salts with phase change close to comfort temperature range are shown to be possible candidates as presented in Khudhair’s review [95]. Effect of heat leak through containment wall of cold LHTES was studied by Seeniraj [96] and limiting values of heat leak ratio were proposed. Finally, with the goal of achieving higher efficiency in charging and discharge of LHTES, Farid [97, 98] proposed the use of different melting temperature materials. Watanabe [99] further conducted the experiment using three PCMs with water as heat transfer medium and optimization of such system with exergetic approach was analyzed [100]. 4 Concluding Remarks Thermal energy storage comes in various forms and salt hydrate based latent heat thermal storage seems to be one of the most promising technologies in terms of energy conservation, grid load alleviation, and integration in a built environment. From this review it can be concluded that, significant findings are available in the literature for advancing the practical system design into functional storage units. However, system performance modeling, design optimization and experimental work in the area of cold storage are still required. More techno-economical feasible PCM systems with suitable material properties (e.g. lower cost, higher conductivity, and larger storage density) will be needed for comfort cooling applications. Here, adequate power and capacity sizing through advanced control scheme and novel design of compact TES by elimination of encapsulation are yet to be performed. Proposed work of PCM based cold storage should be focused in lowering the investment cost with elimination of expensive containment and provision of higher power extraction rate through enhancement of heat transfer design, while maintaining stable charge capacity with use of improved PCMs. Acknowledgement The authors would like to acknowledge Swedish Energy Agency for their financial support. We would also like to acknowledge Capital Cooling AB, Climator AB, Ecostorage Sweden AB, Fortum Värme, and Vesam AB for providing useful suggestions during the study. References [1] V. V. Tyagi, D. Buddhi. PCM thermal storage in buildings: A state of art. Renew. Sust. Energy Rev., Vol. 11, 2007, pp. 1146–1166. [2] I. Dincer. On thermal energy storage systems and applications in buildings. Energy and Buildings, Vol. 34, May 2002, pp. 377-388. [3] M. Ravikumar, Pss. Srinivasan. Phase change material as a thermal energy storage material for cooling of building. J. Theo. Appl. Info. Tech., Vol. 4, 2008, pp. 503-511. [4] I. Dincer, M. A. Rosen. Energetic, environmental and economic aspects of thermal energy storage systems for cooling capacity. Appl. Therm. Eng., Vol. 21, 2001, pp. 1105-1117. [5] A. F. Regin, S.C. Solanki, J.S. Saini. Heat transfer characteristics of thermal energy storage system using PCM capsules: A review. Renew. Sust. Energy Rev., Vol. 12, 2008, pp. 2438-2458. [6] S. M. Hasnain. Review on sustainable thermal energy storage technologies, Part II: cool thermal storage. Energy Convers. Manage., Vol. 39, 1998, pp. 1139-1153. [7] H. Mehling, L. F. Cabeza, Heat and Cold Storage with PCM. Springer, XVI, 2008, 308 p. [8] FAFCO. Last consulted on Jan 11, 2009. Available at http://www.fafco.ch/index.html. [9] Cristopia Energy Systems. Last consulsted on Dec 10, 2008. Available at www.cristopia.com. [10] H. W. Ryu, S. A. Hong, B. C. Shin, S. D. Kim. Heat transfer characteristics of cool-thermal storage systems. Energy, Vol. 16, 1991, pp. 727-737. [11] A. Hauer, H. Mehling, P. Schossig, M. Yamaha, L. Cabeza, V. Martin, F. Setterwall. Advanced Thermal Energy Storage through Application of Phase Change Materials and Chemical Reactions – Feasibility Studies and Demonstration Projects. ECES Annex 17, 2005. [12] A. Sharma, V.V. Tyagi, C.R. Chen, D. Buddhi. Review on thermal energy storage with phase change materials and Applications. Renew. Sust. Energy Rev., Vol. 13, 2009, pp. 318-345. [13] A. Pasupathy, R. Velraj, R.V. Seeniraj. Phase change material-based building architecture for thermal management in residential and commercial establishments. Renew. Sust. Energy Rev. 12, 2008, pp. 39–64. [14] H. Ribberink. Rubitherm Technologies GmbH. [email protected] Last contacted on Jan 7, 2009. [15] N. Julin. Climator AB. [email protected] Last contacted on Dec 3, 2008. [16] Z. Ure. Phase Change Material Products Limited. [email protected] Last contacted on Nov 27, 2008. [17] A. Sarı, A. Karaipekli. Thermal conductivity and latent heat thermal energy storage characteristics of paraffin/expanded graphite composite as phase change material. Appl. Therm. Eng., Vol. 27, 2007, pp. 1271-1277. [18] J. F. White. Flammability characterization of fat and oil derived phase change materials. MSc Thesis presented at university of Missouri-Columbia. July 2005. [19] D. Haillot, X. Py, V. Goetz, M. Benabdelkarim. Storage composites for the optimisation of solar water heating systems. Chem Eng Res Design, Vol. 86, 2008, pp. 612-617. [20] M. M. Farid, A. M. Khudhair, S. A. K. Razack, S. Al-Hallaj. A review on phase change energy storage: materials and Applications. Energy Convers. Manage., Vol. 45, Issues 9-10, June 2004, pp. 1597-1615. [21] R. Naumann and H. H. Emons. Results of thermal analysis for investigation of salt hydrates as latent heat storage materials. J. Thermal Analysis, Vol. 35, 1989, pp.1009-1031. [22] B. Zalba, J. M. Marín, L. F. Cabeza, H. Mehling. Review on thermal energy storage with phase change: materials, heat transfer analysis and Applications. Appl. Therm. Eng., Vol. 23, 2003, pp. 251-283. [23] W. Streicher, L. Cabeza, A. Heinz. Inventory of Phase Change Materials (PCM). IEA Solar Heating and Cooling programme - Task 32, Advanced storage concepts for solar and low energy buildings, 2005. [24] EPS. Available at: www.epsltd.co.uk/ Last consulted on Nov, 30, 2008. [25] Rubitherm. Available at: www.rubitherm.com/ Last consulted on Nov, 30. 2008. [26] Climator. Available at: www.climator.com/ Last consulted on Nov, 30. 2008. [27] Pluss. Available at: http://www.thermalenergystorage.in/ Last consulted on Nov, 30. 2008. [28] J. Wei, Y. Kawaguchi, S. Hirano, H. Takeuchi. Study on a PCM heat storage system for rapid heat supply. Appl. Therm. Eng., Vol. 25, 2005, pp. 2903-2920. [29] M. Hadjieva, R. Stoykov, T. Filipova. Composite salt-hydrate concrete system for building energy storage. Renew. Eng., Vol. 19, 2000, pp. 111-115. [30] A. Barba, M. Spiga. Discharge mode for encapsulated PCMs in storage tanks. Sol. Energy, Vol. 74, 2003, pp.141-148. [31] B. He. High-Capacity Cool Thermal Energy Storage for Peak Shaving. Doctoral Thesis. KTH Stockholm, Sweden, 2004. [32] M. Yanadori, T. Masuda. Heat transferential study on a heat storage container with phase change material. Sol. Energy, Vol. 36, 1986, pp. 169-177. [33] M. Yanadori, T. Masuda. Heat transfer study on a heat storage container with a phase change material. (Part 2. Heat transfer in the melting process in a cylindrical heat storage container). Sol. Energy, Vol. 42, Issue 1, 1989, pp. 27-34. [34] B. Zalba, J. M. Marín, L. F. Cabeza, H. Mehling. Free-cooling of buildings with phase change materials. Int. J. of Refrig., Vol. 27, 2004, pp. 839-849. [35] K. A. R. Ismail, A. B. de Jesus. Parametric study of solidification of PCM around a cylinder for ice-bank Applications. Int. J. of Refrig., Vol. 24, 2001, pp. 809-822. [36] K. A. R. Ismail, R. Stuginsky Jr. A parametric study on possible fixed bed models for pcm and sensible heat storage. Appl. Therm. Eng., Vol. 19, 1999, pp. 757-788. [37] K. Cho, S. H. Choi. Thermal characteristics of paraffin in a spherical capsule during freezing and melting processes. Int. J. of Heat and Mass Transfer, Vol. 43, 2000, pp. 3183-3196. [38] K. A. R. Ismail, R. Stuginsky Jr. A parametric study on possible fixed bed models for pcm and sensible heat storage. Appl. Therm. Eng., Vol. 19, 1999, pp. 757-788. [39] A. Castell, C. Solé, M. Medrano, J. Roca, L. F. Cabeza, D. García. Natural convection heat transfer coefficients in phase change material (PCM) modules with external vertical fins. Appl. Therm. Eng., Vol. 28, 2008, pp. 1676-1686. [40] M. Lacroix. Study of the heat transfer behavior of a latent heat thermal energy storage unit with a finned tube. Int. J. of Heat and Mass Transfer, Vol. 36, 1993, pp. 2083-2092. [41] K. Ermis, A. Erek, I. Dincer. Heat transfer analysis of phase change process in a finned-tube thermal energy storage system using artificial neural network. Int. J. of Heat and Mass Transfer, Vol. 50, 2007, pp. 3163-3175. [42] E. M. A. Mokheimer. Performance of annular fins with different profiles subject to variable heat transfer coefficient. Int. J. of Heat and Mass Transfer, Vol. 45, pp. 3631–3642. [43] Y. Zhang, A. Faghri. Heat transfer enhancement in latent heat thermal energy storage system by using the internally finned tube. Int. J. of Heat and Mass Transfer, Vol. 39, 1996, pp. 3165-3173. [44] R. Velraj, R. V. Seeniraj, B. Hafner, C. Faber, K. Schwarzer. Heat transfer enhancement in a latent heat storage system. Sol. Energy, Vol. 65, 1999, pp. 171-180. [45] J. C. Choi, S. D. Kim, G. Y. Han. Heat transfer characteristics in low-temperature latent heat storage systems using salt-hydrates at heat recovery stage. Sol. Energy Mater. Sol. Cells, Vol. 40, 1996, pp. 71-87. [46] K. A. R Ismail, C. L. F Alves, M. S. Modesto. Numerical and experimental study on the solidification of PCM around a vertical axially finned isothermal cylinder. Appl. Therm. Eng., Vol. 21, 2001, pp. 53-77. [47] W. Wang, X. Yang, Y. Fang, J. Ding, J. Yan. Enhanced thermal conductivity and thermal performance of form-stable composite phase change materials by using β-Aluminum nitride. Appl. Energy, In Press, Corrected Proof, Available online December 2008. [48] S S. Pincemin, R. Olives, X. Py, M. Christ. Highly conductive composites made of phase change materials and graphite for thermal storage. Sol. Energy Mater. Sol. Cells, Vol. 92, 2008, pp. 603-613. [49] S. Kim, L. T. Drzal. High latent heat storage and high thermal conductive phase change materials using exfoliated graphite nanoplatelets. Sol. Energy Mater. Sol. Cells, Vol. 93, 2009, pp. 136-142. [50] H. Yin, X. Gao, J. Ding, Z. Zhang. Experimental research on heat transfer mechanism of heat sink with composite phase change materials. Energy Convers. Manage., Vol. 49, 2008, pp. 1740-1746. [51] T. R. Knowles and G.W. Webb. AIAA 22nd Thermophysics Conference Honolulu, Hawaii, AIAA Paper 87-1489 June 1987. [52] E. Mettawee, G. Assassa. Thermal conductivity enhancement in a latent heat storage system. Sol. Energy, Vol. 81, 2007, pp. 839-845. [53] A. Karaipekli, A. Sarı. Capric–myristic acid/expanded perlite composite as form-stable phase change material for latent heat thermal energy storage. Renew Eng. 33, 2008, pp. 2599– 2605. [54] A. Karaipekli, A. Sarı. Capric–myristic acid/vermiculite composite as form-stable phase change material for thermal energy storage. Sol. Energy, 2008. Article in Press. [55] A. Karaipekli, A. Sarı, K. Kaygusuz. Thermal conductivity improvement of stearic acid using expanded graphite and carbon fiber for energy storage Applications. Renew Eng., Vol. 32, 2007, pp. 2201-2210. [56] J. M. Marín, B. Zalba, L. F. Cabeza, H. Mehling. Improvement of a thermal energy storage using plates with paraffin–graphite composite. Int. J. of Heat and Mass Transfer, Vol. 48, 2005, pp. 2561-2570. [57] A. Mills, M. Farid, J.R. Selman, S. Al-Hallaj. Thermal conductivity enhancement of phase change materials using a graphite matrix. Appl. Therm. Eng. Vol. 26, 2006, pp. 1652–1661. [58] X. Py, R. Olives, S. Mauran. Paraffin/porous-graphite-matrix composite as a high and constant power thermal storage material. Int. J. of Heat and Mass Transfer, Vol. 44, 2001, pp. 2727-2737. [59] W. Streicher, J. M. Schultz, C. Solé & L. F. Cabeza, J. Bony & S. Citherlet, A. Heinz. Final report of Subtask C “Phase Change Materials”, IEA Solar Heating and Cooling programme - Task 32 Advanced storage concepts for solar and low energy buildings, 2008. [60] S. Cantor. DSC study of melting and solidification of salt hydrates. Thermochimica Acta, Vol. 26, 1978, pp. 39-47. [61] B. Shin, S. Kim, W.-H. Park. Phase separation and supercooling of a latent heat-storage material. Energy, Vol. 14, 1989, pp. 921-930. [62] M. Telkes, Thixotropic mixture and method of making same. U.S. Pat No. 3,986,969, 19 Oct. 1976. [63] H. W. Ryu, S. W. Woo, B. C. Shin, S. D. Kim. Prevention of supercooling and stabilization of inorganic salt hydrates as latent heat storage materials. Sol. Energy Mater. Sol. Cells, Vol. 27, 1992, pp. 161-172. [64] L. F. Cabeza, G. Svensson, S. Hiebler, H. Mehling. Thermal performance of sodium acetate trihydrate thickened with different materials as phase change energy storage material. Appl. Therm. Eng., Vol. 23, 2003, pp. 1697-1704. [65] S. Marks. An investigation of the thermal energy storage capacity of Glauber's salt with respect to thermal cycling. Sol. Energy, Vol. 25, 1980, pp. 255-258. [66] S. B.Marks. The effect of crystal size on the thermal energy storage capacity of thickened Glauber's salt. Sol. Energy, Vol. 30, 1983, pp. 45-49. [67] V. V. Tyagi, D. Buddhi. Thermal cycle testing of calcium chloride hexahydrate as a possible PCM for latent heat storage. Sol. Energy Mater. Sol. Cells, Vol. 92, 2008, pp. 891-899. [68] C. S. Herrick. Melt-freeze-cycle life-testing of Glauber's salt in a rolling cylinder heat store. Sol. Energy, Vol. 28, 1982, Pages 99-104. [69] A. Abhat. Low temperature latent heat thermal energy storage: Heat storage materials. Sol. Energy, Vol. 30, 1983, pp. 313-332. [70] A. Elgafy, K. Lafdi. Effect of carbon nanofiber additives on thermal behavior of phase change materials. Carbon, Vol. 43, 2005, pp. 3067-3074. [71] G. A. Lane. Phase change materials for energy storage nucleation to prevent supercooling. Sol. Energy Mater. Sol. Cells, Vol. 27, 1992, pp. 135-160. [72] C. Onwubiko, L. D. Russell. Experimental investigation of physical characteristics of Glauber's salt as a storage medium. Sol. Energy, Vol. 33, 1984, pp. 465-467. [73] J. Candanedo and A. K. Athienitis. Modelling of Predictive Control Strategies in a Net Zero Energy House with Active and Passive Thermal Storage. Eurosun international congress, October 7-10 2008, Lisbon, Portugal. [74] G. P. Henze, C. Felsmann, G. Knabe. Evaluation of optimal control for active and passive building thermal storage. Int. J. of Thermal Sciences, Vol. 43, 2004, pp. 173-183. [75] M. Stadler, W. Krause, M. Sonnenschein, U. Vogel. Modelling and evaluation of control schemes for enhancing load shift of electricity demand for cooling devices. Envir. Modelling & Software, Vol. 24, 2009, pp. 285-295. [76] K. Liu, H. Güven, A. Beyene, P. Lowrey. A comparison of the field performance of thermal energy storage (TES) and conventional chiller systems. Energy, Vol. 19, 1994, pp. 889-900. [77] S. M. Hasnain, S. H. Alawaji, A. M. Al-Ibrahim, M. S. Smiai. Prospects of cool thermal storage utilization in Saudi Arabia. Energy Convers. Manage., Vol. 41, 2000, pp. 1829-1839. [78] S. M. Vakilaltojjar, W. Saman. Analysis and modelling of a phase change storage system for air conditioning Applications. Appl. Therm. Eng., Vol. 21, 2001, pp. 249-263. [79] C. Arkar, S. Medved. Influence of accuracy of thermal property data of a phase change material on the result of a numerical model of a packed bed latent heat storage with spheres. Thermochimica Acta, Vol. 438, 2005, pp. 192-201. [80] B. He, V. Martin, F. Setterwall. Liquid–solid phase equilibrium study of tetradecane and hexadecane binary mixtures as phase change materials (PCMs) for comfort cooling storage. Fluid Phase Equilibria, Vol. 212, 2003, pp. 97-109. [81] Z. Yinping, J.Yi, J. Yi. A simple method, the T-history method, of determining the heat of fusion, specific heat and thermal conductivity of phase-change materials. Meas. Sci. Technol. Vol. 10, 1999, pp. 201-205. [82] J. M., B. Zalba, L. F. Cabeza, H. Mehling. Determination of enthalpy–temperature curves of phase change materials with the temperature-history method: improvement to temperature dependent properties. Meas. Sci. Technol., Vol. 14, 2003, pp. 184-189. [83] A. Saito, S. Okawa, T. Shintani, R. Iwamoto. On the heat removal characteristics and the analytical model of a thermal energy storage capsule using gelled Glauber's salt as the PCM. Int. J. of Heat and Mass Transfer, Vol. 44, 2001, pp. 4693-4701. [84] A. M. Tayeb. A simulation model for a phase-change energy storage system: Experimental and verification. Energy Convers. Manage., Vol. 34, 1993, pp. 243-250. [85] L. Bilir, Z. İlken. Total solidification time of a liquid phase change material enclosed in cylindrical/spherical containers. Appl. Therm. Eng., Vol. 25, 2005, pp. 1488-1502. [86] S. A. Fomin, T. S. Saitoh. Melting of unfixed material in spherical capsule with non-isothermal wall. Int. J. of Heat and Mass Transfer, Vol. 42, 1999, pp. 4197-4205. [87] K. A. R. Ismail, A. B. de Jesus. Parametric study of solidification of PCM around a cylinder for ice-bank Applications. Int J. of Refrig., Vol. 24, 2001, pp. 809-822. [88] L.E. Bourdeau, Study of two passive solar systems containing phase change materials for thermal storage. Proceedings of fifth national passive solar conference, October 19–26, Amherst, American Sol. Energy Society, Newark, Delaware, 1980, pp. 297–301. [89] L. F. Cabeza, C. Castellón, M. Nogués, M. Medrano, R. Leppers, O. Zubillaga. Use of microencapsulated PCM in concrete walls for energy savings. Energy and Buildings, Vol. 39, 2007, pp. 113-119. [90] C. Castellón, M. Medrano, L. F. Cabeza1, M. E. Navarro, I. Fernandez, A. Lázaro, B. Zalba. Increase of thermal inertia of sandwich panels due to the inclusion of phase change materials. Eurosun international congress, October 7-10 2008, Lisbon, Portugal. [91] X. Xu, Y. Zhang, K. Lin, H. Di, R. Yang. Modeling and simulation on the thermal performance of shape-stabilized phase change material floor used in passive solar buildings. Energy and Buildings, Vol. 37, 2005, pp. 1084-1091. [92] J. R. Turnpenny, D. W. Etheridge, D.A. Reay. Novel ventilation cooling system for reducing air conditioning in buildings. Part I: Testing and theoretical modeling. Appl. Therm. Eng., Vol. 20, 2000, pp.1019–1037. [93] F. Kuznik, J. Virgone, J. Noel. Optimization of a phase change material wallboard for building use. Appl. Therm. Eng., Vol. 28, 2008, pp. 1291-1298. [94] H. Mehling. Strategic project ‘‘Innovative PCM-Technology’’ results and future perspectives. 8th expert meeting and work shop, Kizkalesi, Turkey, April 18–20, 2004. [95] A. M. Khudhair, M. M. Farid. A review on energy conservation in building Applications with thermal storage by latent heat using phase change materials. Energy Convers. Manage., Vol. 45, 2004, pp. 263-275. [96] R.V. Seeniraj, N. Lakshmi Narasimhan. The thermal response of a cold LHTS unit with heat leak through side walls. International Communications in Heat and Mass Transfer, Vol. 32, 2005, pp. 1375-1386. [97] M. M. Farid and A. Kanzawa, Thermal performance of a heat storage module using PCM's with different melting temperatures: mathematical modeling. J. Sol. Energy Eng., Vol. 111, 1989, pp. 152-157. [98] M. M. Farid, Y. Kim and A. Kanzawa, Thermal performance of a heat storage module using PCM's with different melting temperatures: experimental. J. Sol. Energy Eng. Vol. 112, 1990, pp. 125-131. [99] T. Watanabe, H. Kikuchi, A. Kanzawa. Enhancement of charging and discharging rates in a latent heat storage system by use of PCM with different melting temperatures. Heat Recov. Sys. and CHP, Vol. 13, 1993, pp. 57-66. [100] T. Watanabe, A. Kanzawa. Second law optimization of a latent heat storage system with PCMS having different melting points. Heat Recov. Sys. and CHP, Vol. 15, 1995, pp. 641-653.
© Copyright 2026 Paperzz