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IRJET- Nano Enhanced Phase Change Material for Thermal Energy Storage Application
1.
International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 05 Issue: 03 | Mar-2018 www.irjet.net p-ISSN: 2395-0072 © 2018, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 564 Nano Enhanced Phase Change Material for Thermal Energy Storage Application Selva prabhu1, Vijay2, Chermakani3,Gopalasubramanian4, Heric5, Beniyel6 1,5 Research Scholar, Dept. of Mechanical Engineering, PSN College of Engineering and Technology 2 PG Student, M.E Cryogenic Engineering, PSN College of Engineering and Technology 3,4 UG Student, B.E Mechanical Engineering, PSN College of Engineering and Technology, India 6Research scholar, Dept. of Mechanical Engineering, VV College of Engineering ---------------------------------------------------------------------***--------------------------------------------------------------------- Abstract - In past few decades usage of phase change materials (PCMs) in thermal energy storage is considered to be an effective way of absorbing and releasingthermalenergy. The storage of thermal energy is a major area in todayâs advanced research. In thermal energy storage the PCM are used to store the thermal energy. Due to the less thermal conductivity of PCMâs, nano particles are introduced to enhance the thermal performance of base PCM. In present work, thermo physical properties of the paraffin wax usedasa PCM (58ËC -60ËC) with Al2O3 (nanoparticles) were analyzed. The effect of dispersion of nanoparticle in base PCM increase the thermal conductivity of the paraffin wax. In this experiment the thermal storage capacity of paraffin wax and the combined thermal storage capacity of paraffin wax with alumina (nano PCM) are compared in a shell and tube heat exchanger. The results shows that there is an improved performance in the thermal storage capacity using nanoPCM (paraffin wax with alumina) than using paraffin wax as PCM. Key Words: Phase change materials, Paraffin wax, Thermal energy storage, Alumina. 1. INTRODUCTION Energy demands in the commercial, industrial, and utility sectors vary on daily, weekly, and seasonal bases. These demands can be matched with the help of thermal energy storage (TES) systems that operate synergistically. The use of TES for thermal applications such as space and water heating, cooling, air-conditioning, and so on has recently received much attention. A variety of TES techniques have developed over the past four or five decades as industrial countries have become highly electrified. Such TES systems have an enormous potential to make the use of thermal energy equipment more effective and for facilitating large- scale energy substitutions from an economic perspective. In general, a coordinated set of actions in several sectorsof the energy system is needed if the potential benefits of thermal storage are to be fully realized. TES deals with the storage of energy by cooling, heating, melting, solidifying, or vaporizing a material; the thermal energy becomes available when the process is reversed. Storage by causing a material to raise or lower in temperature is called sensible heat storage; its effectiveness depends on the specific heat of the storage material and, if volume is important, on itsdensity. Storage by phasechange (the transition from solid to liquid or from liquid to vapor with no change in temperature) is a mode of TES known as latent heat storage. Sensible storage systemscommonly use rocks, ground, or water as the storage medium, and the thermal energy is stored by increasing the storage-medium temperature. Latent heat storage systems store energy in phase change materials (PCMs), with the thermal energy stored when the material changesphase, usuallyfromasolid to a liquid. The specific heat of solidification/fusion or vaporization and the temperature at whichthephasechange occurs are of design importance. Both sensible and latent TES also may occur in the same storage material. Latent heat thermal energy storage technique hasproved to be a better engineering option primarily duetoitsadvantage of providing higher energy storage density with the smaller temperature difference between storage and retrieval. Thermal energy can be stored in the form of sensible heat in which the energy is stored by raising the temperature of the storage material solid or liquid. Rock or water is the best example. Alternatively thermal energy can be stored as latent heat in which energy is stored when a substance changes from one phase to another by either melting or freezing. The temperature of the substanceremainsconstant during phase change. In order to enhance the effective thermal conductivity usually highlyconductingmaterialsare added to the paraffin wax. Aluminiumoxide nano particle is mixed with phase change material andexperimentalanalysis has been carried out to investigate the performance enhancement due to the addition of nano alumina (Al2O3) particles in paraffin wax in a shell and tube heat exchanger by both the cyclic as well as individual charging and discharging. 1.1 Phase Change Materials When a material melts or vaporizes, it absorbs heat; when it changes to a solid (crystallizes) or to a liquid (condenses), it releases this heat. This phase change is used for storing thermal energy in PCMs. Also, the PCM hasbeen subjectedto accelerated life cycling equivalent to 12 years of performance with no loss of capacity. With the physical equilibrium of the PCM established after the first few cycles, the phase change appears to be stable and the TES capacity constant indefinitely, or at least as long as the life of chiller equipment used to freeze the PCM. Latent TES in the temperature range 0â120 âŠC is of interest for a variety of
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International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 05 Issue: 03 | Mar-2018 www.irjet.net p-ISSN: 2395-0072 © 2018, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 565 low-temperature applications, such as space heating, domestic hot water production, heat-pump-assisted space heating, and greenhouse heating and solar cooling. The melting and freezing characteristics of PCMs, and their ability to undergo thermal cycling, and their compatibility with construction materials is essential for assessing the short and long-term performance of a latent TES. Using two different measurement techniques(e.g.,differentialscanning calorimetry and thermal analysis), the melting and freezing behavior of PCMs can be determined. Thermal cycling and corrosion behavior are also of importance intheappropriate choice of materials as they affect the life of a latent heat storage. 1.2 Characteristics and ThermophysicalProperties of PCMs Thermo physical propertiesof paraffinâs generallychange monotonously as a function of melting temperature, homogeneous mixtures can be readily prepared. However, properties of mixtures cannot be calculated from simple interpolation of properties of pure components, and therefore experimental characterization is required. Paraffinâs generally have higher specific heats in both the solid and liquid states than salt hydrates. When the conductivity is high, the heat transfer for a given design will be more efficient .The density of a PCM is important,because it affects its storage effectiveness per unit volume. Salt hydrates are generally denser than paraffinâs,butareslightly more effective on a per volume basis, despiteaslightlylower heat of fusion. The rate of crystallization of a salt hydratecan below, and can become the limiting factor in the rate of heat storage and restitution. Crystallization is generally more rapid for paraffinâs, and heat-transfer mechanisms are then the limiting factors. In addition, paraffins exhibit little or no supercooling, which is frequent and often significant in magnitude with salt hydrates. Paraffins have very lowvapor pressures, which leadsto low long-term lossof material and flammability. Salt hydrates have significantly higher vapor pressures, which induce water lossand progressivechanges of thermal behaviour. The vapor pressure of salt hydrates increases with the degree of hydration, and salt hydrates exhibit variable chemical stability and can be subject to long term degradation by oxidization, hydrolysis, thermal decomposition, and other reactions. Some salt hydrates are very corrosive in the presence of water. Paraffins are very stable and unreactive, but slow oxidization may occur when they are exposed to air at elevated temperatures over extended periods. Paraffins are not corrosive Latent TES using PCMs provides an effective way to store thermal energy from a range of sources, high storage capacity, and heat recovery at almost constant temperatures. 2. Paraffin wax as PCM Paraffin are selected due to their availability, inexpensive nature and melt at different temperatures relating to their carbon chain length with the generalformulaCnH2n+2.They are chemically stable, their volume increase upon melting is in the order of 10% of their volume. Paraffin are safe and non-reactive. They do not react with mostcommonchemical agents. They are economical, having a high heat of fusion, a low vapour pressure in the melt, exhibit negligible super cooling and no phase segregation, and are chemically stable and inert. Commercially available paraffinâsfrom Rubiherm RT21 and RT27 were investigated. Melting temperature of the PCM 58-60ËC Latent heat of fusion 216 kg/m3 Density of the PCM (liquid phase) 760 kg/m3 Density of the PCM (solid phase) 818 kg/m3 Specific heat of the PCM (solid phase) 2.95 kJ/kgk Specific heat of the PCM (liquid phase) 2.51 kJ/kgk Thermal conductivity 0.24 w/mK Table -1: Thermo physical properties of paraffin wax 2.1 Dispersion of high conductivity particles in the PCM Using graphite made composite PCMs has been proven as efficient and successful way in enhancing the performanceof LHTS systems. However, graphite composites can be prepared only through various mechanical/chemical processes like heat treatment, drying, mixing, grinding/compression, etc., which are time and energy consuming processes. The porosityofgraphite isverycrucial in deciding the effectiveness of the composites. If graphite of small mean pore size is used, then there may be decrease in latent heat value as small mean pore size hinders the molecular motion and thus very difficult to impregnate the porous media with the PCM. On the other hand, increasing pore size reduces the capillary force resulting in leakage of liquid PCM. Since the high conductivity metal particles are free fromthese shortcomings, dispersionofhighconductivity particles into the PCM is relatively simpler technique to enhance the thermal conductivity of PCM. 2.2 Use of high conductivity and low density materials Due to relatively high density, the metal particles/metal structuresmay settle on the bottom surface of the container and add considerable weight to the system.Besides,allmetal particlesare not compatible with allPCMs.Forexample,with paraffin, aluminium is compatible, whereas copper and nickel are not compatible. Similarly, aluminium and copper are not compatible with some salt hydrates. Hence,therehas been a search for low-density high conductivity additives, which should be compatible with all PCMs. Since the densities of carbon fibers are relatively lower than those of metals and the thermal conductivities are almost equal to that of aluminium and copper, these can be better
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of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 05 Issue: 03 | Mar-2018 www.irjet.net p-ISSN: 2395-0072 © 2018, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 566 alternatives to enhance the thermal performance of LHTS systems. Moreover, carbon fibers possess high corrosive resistance and hence compatible with most of the PCMs. In a cylindrical capsule, carbon fibers were added in the PCM in two ways. In the first case fiberswere randomly distributed, where as in the second case brush type fiberswereused.The two cases of distribution of carbon fibers in cylindrical capsule can be seen in fig below. The effective thermal conductivity with brush type was found to be three times higher than that with random type. This is because in brush type the fibers were distributed uniformly in such a way all the fibers were arranged in radial direction, which was the heat flow direction. For lower mass fraction of fibers, the randomly distributed arrangement could not presenthigher melting rate than that with pure paraffin, even though the effective thermal conductivity of former is greater than that of latter. This is due to the loss in natural convection in case of randomly distributed arrangement. Ontheotherhand,the lossin natural convection could not affect the highermelting rate in case of brush type. This shows that the fibers should be arranged in such a way that they are oriented in the direction of heat flow. They could achieve 30% and 20% higher solidification rate and melting rate respectively with 1% mass fraction carbon brush type fibers as compared to those with pure PCM. 2.3 Mathematical modeling of LHTS systems employing performance enhancement techniques Phase change problems are examples of what are closely referred to as moving boundary problems and their study presents one of the most exciting and challenging areas of current applied mathematical research. The existence of a moving boundary generally meansthattheproblemdoesnot admit a simple closed form analytical solution and accordingly much research has focused on approximate solution techniques. In general, phase change problems involve a transient, non-linear phenomenon with a moving liquidâsolid interface whose position is unknown a priori and also flow problems associated with HTF. In addition, the two phases of PCM may have different properties and configuration of the LHTS unit may differ with the applications. Substantial number of numerical based studies on LHTS units employing enhancement techniques and on their performance measurement is available in the literature. The numerical formulations widely implemented so far are enthalpy method and effective heat capacity method. In the enthalpy method, the enthalpy which is a function of temperature is consideredas a dependent variable along with temperature. Thus the enthalpy based conduction equation is valid for both solid and liquid phases. Besides, it is valid for solidâliquid interface. Therefore, there is no need to track the interface which makes this formulation attractive. In theeffectiveheat capacity method, the heat capacity of the PCM during phase change process (effective heat capacity) is introduced. The effective heat capacity is directly proportional to the stored/released energy during the phase change and the specific heat. Therefore, with effective heat capacity itisalso possible to describe the non-isothermal phase change in the PCM. For the details of these two formulations, readers are referred to for enthalpy method and for effective heat capacity method. Besides these two formulations there is another method called alternate thermal resistancemethod. The numerical studies on LHTS units employing performance enhancement technique have mainly focused on evaluation of melting/solidification time, heat transfer rate and amount of energy stored/retrieved in comparison with those of system without enhancement techniques. 3 NANOPARTICLES 3.1 Introduction of nanotechnology Nanotechnology deals with nanometer scale of natural and artificial structures, i.e. in the range from 1 ÎŒm down to . one nanometer, 1 nm=10-9 m, Generally nanotechnology deals with structures sized between 1 to100 nm. 3.2 Nanotechnology Enhancement of convective heat transfer and thermal conductivity of liquids was earlier made possible by mixing micron sized particleswith a base fluid. A very smallamount of nanoparticles, when dispersed uniformly and suspended stably in base fluids, can provide impressive improvements in the thermal properties of base fluids. Nanofluids, which are a colloidal mixture of nano particles (1-100 nm) and a base liquid (nanoparticle fluid suspension). Nano particles often possess unexpected optical properties and as they are small enough to confine their electrons and produce quantum effects. For example gold nanoparticles appear deep-red to black in solution. Nanoparticles of yellow gold and grey silicon are red in color. Gold nanoparticles melt at much lower temperature (300 ËC for 2.5 nm size) than the gold slabs (1064 ËC). Absorption of solar radiation is much higher in materials composed of nanoparticles than it is in thin films of continuous seeds of material for example, thermal conductivity of copper at roomtemperatureisabout 700 times greater than that of water and about 3000 times greater than that of engine oil. Nanotechnology, a particle is defined as a small object that behaves as a whole unit in terms of its transport and properties. Nano particles are the particles of size between 1 nm to 100 nm. It is further classified according to size in terms of diameter, fine particles cover a range between100and2500 nm, while ultrafine particles, on the other hand, are sized between 1 and 100 nm. Similar to ultrafine particles, nanoparticles are sized between 1 and 100 nm. Nanoparticlesmay or may not exhibit size relatedproperties that differ significantly from those observed I fine particles or bulk materials. Nanoparticles are the simplest form of structures with sizes in the nm range. In principle any collection of atomsbonded together with a structural radius of < 100 nm can be considered a nanoparticles
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International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 05 Issue: 03 | Mar-2018 www.irjet.net p-ISSN: 2395-0072 © 2018, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 567 Specific heat capacity of Al2O3 765 kJ/kg K Thermal conductivity of Al2O3 36 W/m K Density of Al2O3 3600 kg/m3 Diameter of Al2O3 20-30 nm Weight of Al2O3 30g Table-2 thermo physical properties of nanoparticle Al2O3 3.3 Calculation of volumetric concentration of Al2O3 nanoparticle Volumetric concentration = weight/density =30/3600 Volumetric concentration = 0.833% 3.4 Preparation methods of nanoPCM Initially, Al2O3 nanoparticle of 30g are divided approximately 6 g each needed for the addition to the paraffin wax of 1.37 kg. Then the paraffin wax of 250g is filled in a small tank. The tank with paraffin wax immersed in another tank in which the water is maintained at 85 ËC. By the convection process the heat from the hot water is transferred to the paraffin wax material. Asthe temperature increase, the paraffin wax starts changing itsphase from the normal. Once the paraffin wax increases above 45 ËC, Al2O3 nanoparticles of 6 g are added to the paraffin wax of 250 g, before its melting temperature. After preparing it, the tank with nano PCM is cooled by water at 35 ËC to get nano PCM in solid phase the same procedure is repeated for the remaining nanoparticles which is further added to the annulus side of concentric tube heat exchanger. 4 EXPERIMENTATION 4.1 Methodology To enhance the effective thermal conductivity of the system, the copper tube is formed in coil form. 10 number of coil are used with the distance of 5 cm between the coils. 2 mm thick circular fin has been fitted with spiral coil. The inner tube is made of copper. The outer tube is made of mild steel. The outside of the outer pipe was insulated with 3 mm thick asbestos rope to reduce the heat loss during charging and discharging process of the PCM. The outer tube inner side was filled with 1.374 kg commercial grade paraffin wax being used as latent heat storage media. Type T-copper constantan thermocoupleswere usedformeasuringtheinlet and outlet temperature of heat transfer fluid (HTF) and the PCM temperature at two locations in the PCM tank. A two tank system are used form maintaining a constant pressure head for inlet water to maintain nearly constant flow rate. Heaters with thermocouple were also provided in the water tanks for constant inlet water temperature during charging mode. Flowing hot water through inner tube started the energy charging test, and the stored energy wasextractedby passing cold water in the inner tube. The temperature of water at inlet and outlet of the heat exchanger at four axial locations were measured simultaneously at an intervalof15 min. 4.2 Charging Process-Heat Stored The temperature distribution of HTF and the PCM intheTES tank for different mass flow rates are recorded during charging and discharging processes. The cumulative heat stored and system efficiency of process is studied in detail during the charging process. The first experiment was conducted with flowrate 5 lt/hr and the inlettemperatureof the hot water was kept 88 oC and the atmospheric temperature is 320C. During the charging process, theHTFis circulated through the TES tank continuously. Initially, temperature of PCM is 32 oC and as HTF exchanges its heat energy to PCM, the PCM gets heated up to melting temperature (storing the energy as sensible heat).Laterheat is stored as latent heat once the PCM melts and becomes liquid. The energy is then stored as sensible heat in liquid PCM. The temperature of PCM and HTF are recorded at interval of 15 min. the charging process is continued until the PCM temperature reaches maximum temperature. The graph represented hot water outlet temperature (HTF) and mean PCM temperature with respect to the time. Like that the flow rate changed to 15 lt/hr, the inlet temperature of hot water waskept at 88ËC and the atmospherictemperature is 320C. During the charging process the HTF is circulated through the TES tank continuously. The temperature of the PCM and HTF are recorded at intervals of 15 min. the charging process is continued until the PCM temperature reaches maximum temperature. The charging process has been completed for PCM with two mass flow rates (5 lt/hr, 15 lt/hr). After that, I have taken the charging process was conducted with flow rate 5 lt/hr, 15 lt/hr for nanoPCM and the inlet temperature of the hot water waskept 88ËC andthe atmospheric temperature is 32ËC. During the charging process, the HTF is circulated through the TES tank continuously. Initially the temperature of the nano PCM is 32ËC and as the HTF exchanges its heat energy to nano PCM. The nanoPCM gets heated up to melting temperature (storing the energy as sensible heat). Later heat is stored as latent heat once the nanoPCM melts and becomesliquid.The energy is then stored as sensible heat inliquidnanoPCM.The temperature of nanoPCM and HTF are recorded at intervals of 15 min. The charging process is continued until the nanoPCM temperature reaches maximum temperature. 4.3 Discharging Process â heat released At the beginning of the solidification period the temperature of the paraffin wax decreased rapidly by transferring the sensible heat stored to the cooling water. Duringthisperiod, the temperature of the paraffin wax is high, and the paraffin wax is in liquid state. This is mainly because heat transfer inside the molten paraffin wax is by natural convection and the temperature gap between PCM tube and the cooling water is large.
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International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 05 Issue: 03 | Mar-2018 www.irjet.net p-ISSN: 2395-0072 © 2018, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 568 Then the paraffin wax adjacent to the PCM tube begins to freeze and discharge its latent heat. Hence we find that the PCM releases its sensible heat very rapidlyand,thenalonger time is needed to transfer the latent heat during the phase change. Since the paraffin wax is basically in a liquid state, the major portion of heat dissipated from the PCM is its latent heat. However towards the final period of solidification, the amount of latent heat transfer to the heat transfer fluid is becoming smaller and smaller, and the heat dissipation from the PCM is again mainly the sensibleheatof the solid paraffin wax. The discharging processthe first experiment wasconducted with flow rate 5 lt/hr and the inlet temperature of the cold water kept at the atmospheric temperature is 32ËC. During the discharging processthe cold water is circulated through the TES tank continuously. Now that heat energy stored in PCM is transferred to the cold water, so the cold water temperature is increased. The temperature of the PCM and cold water outlet temperature are recordedatintervalsof15 min. The discharging process is continued until the PCM temperature reduced to atmospheric temperature. The graph represented the values of cold water outlet temperature (HTF) and PCM temperature respectwithtime. Like that the flow rate changed to 15 lt/hr the inlet temperature of cold water kept at the atmospheric temperature is 320C. The temperature of the PCM and cold water outlet temperature (HTF) are recorded at intervals of 15 min. The discharging processof nanoPCM wasconducted with flow rate 5 lt/hr and the inlet temperature of the cold water kept at the atmospheric temperature is 320C. During the discharging processthe cold water is circulated through the TES tank continuously. Now the heat energy stored in nanoPCM is transferred to the cold water, so the cold water temperature is increased. Temperature of the nanoPCM and cold water temperature (HTF) are recorded at intervals of 15 min. The discharging process is continued until the nanoPCM temperature reduced toatmospherictemperature. The graph represented the values of cold water outlet temperature (HTF) and nanoPCM temperature respect with time. Like that the flow rate changed to 15 lt/hr the inlet temperature of cold water kept at the atmospheric temperature is 32oC. The temperature of the PCM and cold water outlet temperature (HTF) are recorded at intervals of 15 min. 4.4 Calculation 4.5 Loading calculation of PCM VPCM = [(đ/4) x (0.06)2] x 0.06 = 1.169 x10-3 m3 Vcopper tube = [(đ/4) x (0.006)2] x 1.7 = 4.806 x 10-5 m3 MPCM = (VPCM - Vcopper tube) x ÏPCM = (1.169 x10-3 - 4.806 x 10-5) x 818 MPCM =1.3480 kg 4.6 Performance During Charging Process In charging process, the HTF entered LHSS at high temperature. It cause melting of PCM Heat stored QS = MW * CpW *(T hi âT ho) * t Heat available QA = MW * CpW *(T hi âT ci) *t Charging Efficiency È = (QS /QA) * 100 4.7 Performance during Discharging Process In discharge process, the HTF entered at low temperatureto the LHSS. It cause solidification of PCM Heat Released QR = MW x CpW x (T co âT ci) x t Heat available QA = m pcm x Cp pcm x (T pcm â T ci) + (m pcm x L pcm) Charging Efficiency È = (QR /QA) * 100 5 RESULT AND DISCUSSION Thus the experimental analysis on the latent heat thermal energy storage system has been done using Al2O3 nanoparticle. The effect of 0.833%volumetricconcentration of nanoparticles on the melting and solidification performance is examined and compared between nanoPCM and pure paraffin wax. The reading were tabulated for PCM as well as nanoPCM. From the experimental results, it is found that the use of nanoparticles with paraffin wax reduces the melting and solidification time. It is also observed that there is almost 50% reduction in charging time and discharging time of the PCM for a volume concentration of 0.833%. 6 Graphical Representation 6.1 Charging process for PCM (5L/hr, 15L/hr) Variation of PCM mean temperature and HTF outlet temperature with time during charging mode with average flow rate of 5L/hr
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International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 05 Issue: 03 | Mar-2018 www.irjet.net p-ISSN: 2395-0072 © 2018, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 569 Variation of PCM mean temperature and HTF outlet temperature with time during charging mode with average flow rate of 15L/hr 6.2 Discharging process for PCM (5L, 15L/hr) Variation of PCM mean temperature and HTF outlet temperature with time during discharging mode with average flow rate of 5L/hr Variation of PCM mean temperature and HTF outlet temperature with time during discharging mode with average flow rate of 15L/hr 6.3 Charging process for nano PCM (5L/hr,15L/hr) Variation of nano PCM mean temperature and HTF outlet temperature with time during charging mode with average flow rate of 5L/hr Variation of Nano PCM mean temperature and HTF outlet temperature with time during charging mode with average flow rate of 15L/hr 6.4 Discharging process for nano PCM (5L, 15L/hr) Variation of nano PCM mean temperature and HTF outlet temperature with time during discharging mode with average flow rate of 5L/hr
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International Research Journal
of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 05 Issue: 03 | Mar-2018 www.irjet.net p-ISSN: 2395-0072 © 2018, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 570 Variation of nano PCM mean temperature and HTF outlet temperature with time during discharging mode with average flow rate of 15L/hr 6.5 Charging process for PCM vs nano PCM (5L/hr, 15L/hr) Charging process for Time vs Efficiency of PCM & nanoPCM with for 5L/hr Charging process for Time vs Efficiency of PCM & nano PCM with for 15L/hr 6.6 Discharging process for PCM vs nano PCM (5L/hr,15L/hr Discharging process for Time vs Efficiency of PCM & nanoPCM with for 5L/hr Discharging process for Time vs Efficiency of PCM & nano PCM with for 15L/hr 3. CONCLUSIONS In this work, the experimental analysis has been carried out to study the performance enhancement of paraffin wax with nano alumina (Al2O3) particles in comparison with simple paraffin wax in a shell and tube heat exchanger in latentheat thermal energy storage system. It isconcludedthattheusage of Al2O3 nanoparticle with paraffin wax reduces the melting and solidification time by 50% as compared to that of paraffin wax. It was found that the use of Al2O3 with paraffin wax enhance the charging efficiency by 6% to that of the pure paraffin wax. It was also found that the use of Al203 with paraffin wax enhance the discharging efficiency by 4% as compared to that of the pure paraffin wax.
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of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 05 Issue: 03 | Mar-2018 www.irjet.net p-ISSN: 2395-0072 © 2018, IRJET | Impact Factor value: 6.171 | ISO 9001:2008 Certified Journal | Page 571 REFERENCES [1] G. Lamberg P, Siren K. Analytical model for melting in a semi-infinite PCM storage with an internal fin. Heat Mass Transf 2003. [2] Jellouli Y, Chouikh R, Guizani A, Belghith A. Numerical study of the moving boundary problem during melting process in a rectangular cavity heated from below. Am J ApplSci 2007. [3] Regin AF, Solanki SC, Saini JS. Latent heat thermal storage using cylindrical capsule: numerical and experimental investigations. Renew Energy 2006. [4] AkgunM, Aydin O, Kaygusuz K. Experimental study on melting/solidification characteristics of a paraffin as PCM. Energy Convers Manage 2007. [5] Pinelli M, Piva S. Solid/liquid phase change in presence of natural convection: a thermal energy storage case study. ASME J Energy Res Tech 2003. [6] Gharebaghi M, Sezai I. Enhancement of heat transfer in latent heat storage modules with internal fins. Numer Heat Transf Part A 2008. [7] Shatikian V, Ziskind G, Letan R. Numerical investigation of a PCM-based heat sink with internal fins. Int J Heat Mass Transf 2005. [8] Seeniraj RV, Velraj R, Narasimhan NL. Thermal analysis of a finned-tube LHTS module for a solardynamicpower system. Heat Mass Transf 2002. [9] Velraj R, Seeniraj RV, Hafner B, Faber C, Schwarzer K. Experimental analysis and numerical modeling of inward solidification on a finned vertical tube for a latent heat storage unit. Sol Energy 1997. [10] Wang J, Chen G, Jiang H. Theoretical study on a novel phase change process. Int J Energy Res 1999. [11] Fiedler T, Ochsner A, Belova IV, Murch GE. Thermal conductivity enhancement of compositeheatsinksusing cellular materials. Defect Diffus Forum 2008. [12] Cabeza LF, Ibanez M, Sole C, Roca J, Nogues M. Experimentation with water tank including a PCM module. Sol Energy Mater Sol Cells 2006. [13] Pincemin S, Py X, Olives R, Christ M, Oettinger O. Elaboration of conductivethermal storage composites made of phase change materials and graphite for solar power plant. ASME J Sol Energy Eng 2008. [14] Zeng JL, Sun LX, Xu F, Tan ZC, Zhang ZH, Zhang J, et al. Study of a PCM based energy storage system containing Ag nanoparticles. J Therm Anal Calorimetry2007. [15] Hamada Y, Ohtsu W, Fugai J. Thermal response in thermal energy storage material around heat transfer tubes: effect of additives on heat transfer rates. Sol Energy 2003. [16] Alkan C, Sari A, Karaipekli A, Uzun O. Preparation, characterization, and thermal properties of microencapsulated phase change material for thermal energy storage. Sol Energy Mater Sol Cells 2009. [17] Zho GL, Tan ZC, Lan XZ, Sun LX, Zhang T. Preparation and characterization of microencapsulated hexadecane used for thermal energy storage. Chin ChemLett 2004. [18] Hawlader MNA, Uddin MS, Zhu HJ. Encapsulated phase change materials for thermal energy storage: experiments and simulation. Int J Energy Res 2002. [19] nica Trp, Kristian Lenic, Bernard Frankovic. â nalysis of the Influence of Operating Conditions and Geometric Parameters on Heat Transfer inWater-ParaffinShelland Tube Latent Thermal Energy Storage Unitâ. 5 Feb 2006. [20] Mehmet Esen. âThermal Performance of a Solar ided Latent Heat Store Used for Space Heating by Heat Pumpâ. 30 Nov 1999. [21] M. Conti and Ch. Charach. âThermodynamics of Heat Storage in a PCM Shell and Tube Heat Exchanger in Parallel or in Series With a Heat Engineâ. [22] Robynne Murray, Louis Desgrosseilliers, Jeremy Stewart, Nick Osbourne, Gina Marin, Alex Safatli, Domynic Grouix, Mary nne White. âDesign Of Latent Heat Energy Storage System Coupled With A Domestic Hot Water Solar Thermal Systemâ. World Renewable Energy Congress 2011 Sweden 8-13 May 2011. [23] nish R, S. R. Karale. Vol.1, Issue 8 Oct 2012. âEnergy Storage System for Passive Cooling, a Reviewâ. PP:
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