City University of New York (CUNY) CUNY Academic Works Master's Theses City College of New York 2012 Exploration of the Endothermic and Exothermic Reactions of Calcium Oxide and Magnesium Oxide and Design of a Vessel for a Thermochemical Heat Storage System Jorge Pulido CUNY City College How does access to this work benefit you? Let us know! Follow this and additional works at: http://academicworks.cuny.edu/cc_etds_theses Part of the Mechanical Engineering Commons Recommended Citation Pulido, Jorge, "Exploration of the Endothermic and Exothermic Reactions of Calcium Oxide and Magnesium Oxide and Design of a Vessel for a Thermochemical Heat Storage System" (2012). CUNY Academic Works. http://academicworks.cuny.edu/cc_etds_theses/621 This Thesis is brought to you for free and open access by the City College of New York at CUNY Academic Works. It has been accepted for inclusion in Master's Theses by an authorized administrator of CUNY Academic Works. For more information, please contact [email protected]. Exploration of the Endothermic and Exothermic Reactions of Calcium Oxide and Magnesium Oxide and Design of a Vessel for a Thermochemical Heat Storage System THESIS Submitted in partial fulfillment of the requirement for the degree Master of Engineering (Mechanical) at The City College of New York of the City University of New York By Jorge Pulido August, 2012 Approved: Professor Masahiro Kawaji, Thesis Advisor CUNY Energy institute Professor Feridun Delale, Chairman Department of Mechanical Engineering 1 2 ABSTRACT A high temperature Thermal Energy Storage (TES) system has been investigated for use in solar thermal power plants or in vehicles to preheat the engine and/or the cabin in cold weather. The idea is to store surplus thermal energy and then release it on demand to heat a working fluid. The stored heat can be used to generate electricity after sunset or to meet the peak loads. These would lead to an improvement in energy efficiency, reductions in energy imports from foreign sources and total energy-related emissions. The basic operating principle involved in the TES system is a thermochemical reaction involving metal oxides such the calcium oxide (CaO) or magnesium oxide (MgO) and water. In the output mode, an exothermic reaction is initiated when liquid water or steam is injected into the metal oxide particle bed to produce Ca(OH)2 or Mg(OH)2. The heat generated in this process can then be used to heat up a secondary flow of water or other heat transfer fluid that passes through the TES system. In the charging phase, the bed will be heated to dehydrate Ca(OH)2 or Mg(OH)2 in an endothermic reaction inside the TES vessel. This research investigates the integration of thermal storage and heat transfer technologies into a working system. Efficient heat exchange is vital as porous solid particles of metal oxides have low values of thermal conductivity. i Acknowledgement In first place I want to thank my advisor Professor Masahiro Kawaji of the CUNY’s Energy Institute and Mechanical Engineering Department at City College of New York, for his guidance, patience and for the opportunity he gave me. To Professor Yiannis Andreopoulos who let me use part of his lab to do the experiments and for his always amiable attitude. Also to master students Ravi Ramnanan-Singh, Randy Samaroo and Han Yi who helped me in numerous facets of the experimental setup. Finally to my brother, who always found a way to help me. ii General Index ABSTRACT ......................................................................................................................... i 1 Introduction ...................................................................................................................... 1 1.1 Theoretical Framework ......................................................................................................... 2 1.2 State of the art ........................................................................................................................ 6 1.3 objectives ............................................................................................................................... 7 2 Construction of the experimental setup ........................................................................... 8 2.1 Material .................................................................................................................................. 8 2.2 Furnace................................................................................................................................... 9 2.3 Temperature measurement ..................................................................................................... 9 2.4 First container ...................................................................................................................... 10 2.5 Second container .................................................................................................................. 12 2.6 Container for test with steam ............................................................................................... 15 2.7 General purpose container ................................................................................................... 17 2.7.2 Sprinkler ........................................................................................................................ 18 2.7.3 Coil ................................................................................................................................ 19 2.7.4 Heater ........................................................................................................................... 19 3 Experimental Procedure ................................................................................................. 20 3.1 Dehydration ......................................................................................................................... 20 3.1.2 Dehydration with the general purpose container ........................................................ 21 3.2 Hydration ............................................................................................................................. 23 3.2.2 Hydration with the general purpose container ............................................................ 23 4 Results for Calcium hydroxide and magnesium hydroxide ........................................... 24 4.1 Calcium Hydroxide .............................................................................................................. 24 4.1.2 Dehydration .................................................................................................................. 24 4.1.3 Hydration ...................................................................................................................... 26 4.1.3.1 Hydrations with cold water........................................................................................ 29 4.1.4 Hydration with steam ................................................................................................... 29 4.1.5 Dehydration in the general purpose reactor ................................................................ 30 4.1.6 Hydration general purpose reactor .............................................................................. 31 4.2 Magnesium Oxide ................................................................................................................ 32 iii 4.2.2 Dehydration .................................................................................................................. 32 4.2.3 Hydration ...................................................................................................................... 33 4.2.4 Hydration with steam ................................................................................................... 36 5 Conclusions .................................................................................................................... 37 Annex 1: Blueprints of the second container……...…………………………………….39 Annex 2: Blueprints of the general purpose container………………….……………...50 Annex 3: Steps to assemble the attachment to the upper cover for the general purpose container………………………………………………………………………………….59 References ......................................................................................................................... 62 Figures index Figure 1: Energy flows (TWh) in the global electricity system.......................................... 2 Figure 2: Classification of thermochemical storage reactions ............................................ 4 Figure 3: Hydration/dehydration cycle for the calcium ...................................................... 5 Figure 4: Glass reactor ........................................................................................................ 6 Figure 5: Cooper and polyurethane..................................................................................... 6 Figure 6: Close loop reactor ................................................................................................ 7 Figure 7: Jewerly furnace.................................................................................................... 9 Figure 8: Thermocouple type K ........................................................................................ 10 Figure 9: Data acquisition board with USB carrier .......................................................... 10 Figure 10: Sugar shaker .................................................................................................... 11 Figure 11 Wire basket ....................................................................................................... 11 Figure 12: Base with insulation ........................................................................................ 12 Figure 13: Second container ............................................................................................. 13 Figure 14: Distribution of the holes .................................................................................. 13 Figure 15: Cap of the second container ............................................................................ 14 Figure 16: Configurations of the second container ........................................................... 14 Figure 17: Characteristic behavior of the small furnace ................................................... 15 Figure 18: Sugar shaker divided by mesh ......................................................................... 15 Figure 19: Container for test with steam........................................................................... 16 Figure 20: General purpose container ............................................................................... 17 Figure 21: Furnace Omegalux LMF-A550 ....................................................................... 18 Figure 22: Sprinkler .......................................................................................................... 18 Figure 23: Inner and outer coil.......................................................................................... 19 Figure 24: Electric heater .................................................................................................. 19 Figure 25: Jumps in the temperature reading .................................................................... 20 iv Figure 26: Gas heater ........................................................................................................ 22 Figure 27: Hydration with steam ...................................................................................... 23 Figure 28: Funnel .............................................................................................................. 24 Figure 29: First successful dehydration ............................................................................ 25 Figure 30: Dehydration for two different sizes of lumps .................................................. 26 Figure 31: Typical hydration reaction for the CaO ........................................................... 27 Figure 32: Fast and slow reactions in the CaO ................................................................. 28 Figure 33: Super-hot hydrations ....................................................................................... 29 Figure 34: CaO hydration with steam ............................................................................... 30 Figure 35: Dehydration with the general purpose reactor ................................................ 31 Figure 36: Hydration with the general purpose reactor .................................................... 32 Figure 37: Magnesium dehydration .................................................................................. 33 Figure 38: Magnesium hydration ...................................................................................... 34 Figure 39: Slow magnesium hydration ............................................................................. 35 Figure 40: Steam magnesium hydration ........................................................................... 36 Tables Index Table 1Insulation properties .......................................................................................................... 21 Table 2: Characteristics of the pipe and heater of the gas dehydrator ........................................... 22 v vi 1 Introduction Some statistics that indicate the current situation of fuels, energy consumption and production have been reported by the International Energy Agency (IEA). For example, 81% of energy production in 2009 was from fossil fuels; the price per barrel of oil today is 7 times higher than 25 years ago, the amounts of CO2 emissions as well as the rate of energy consumption have doubled since the 70’s. Every day, it is more evident that processes with higher energy efficiency are needed and that research in new technology to produce energy is urgent. The two most used types of energy are electricity and heat. In the case of electric energy, the power plants are about 30 to 40% efficient depending on the thermodynamic cycles used. In some energy systems where one can find low efficiencies; in a combustion engine, only 20% of the fuel’s energy is used to generate work, while the rest is wasted in the form of heat. Thermal Energy Storage Devices (TESD) can help to recover part of this heat making the thermal cycles more efficient. In figure 1, we can see that 63% of the thermal energy is lost in the generation of electricity. Generally, the waste heat is released to the environment by cooling towers, cooling water or flue gases. This surplus energy can be used with TESD in the production of electricity in power plants fed by fossil fuels, nuclear fuels or even in solar thermal plants. TESD can also be applied on a smaller scale in vehicles where the cabin needs to be heated or to preheat the engine. The chemicals used in thermal storage, do not lose the capacity of storage over time, so this concept can be used to supply energy after hours or even months of storage. 1 Figure 1: Energy flows (TWh) in the global electricity system 1.1 Theoretical Framework The thermal energy storage devices can be classified into three groups, sensible, latent and chemical, according to the physical principles used. Each group has particular characteristics that will be explained below. Sensible Heat Storage: This kind of device is most popular commercially due to its relative simplicity. The principle used is the sensible heat, defined as the heat received or sensed by a body or a substance which does not change the molecular state of the material. Generally this kind of storage consists of a solid or fluid, usually water, that is heated, stored in a thermally isolated container or reservoir and then released to heat or cool a space or pipe system. The amount of heat that can be stored depends on the thermal characteristics of the fluid and the efficiency of the insulation used in the reservoir. One of the problems of this system is that the difference between the fluid and environment temperatures must be high. This represents bulky and expensive systems. A second inconvenience is seen in the storage duration, that is not longer that two or three days. The energy density storage is around 100 kJ/kg [1]. 2 Latent Heat Storage: The operating principle of these devices is the heat absorbed or released when a substance changes its phase (gas, liquid or solid). There are two ways to store the heat: the first in which Phase Change Material (PCM) is kept in such way that the phase change occurs as the environment’s temperature drops; in the second method the PCM is maintained in a phase (gas or liquid), and when needed it is compressed or decompressed freely or with a pump. Because the PCM also needs to be thermally insulated, this energy storage lasts about the same period of time as the sensible heat devices. The working fluid needs to be confined inside the device, so the presence of heat exchangers is a must in this method. The stored energy density goes up to 250-330 kJ/kg [1]. Chemical Heat Storage: Thermal energy is released or absorbed when new chemical bonds are formed or broken between two or more molecules. Although in theory all the new bonds generate heat, only a few generate enough heat to be useful. The principal advantage is that the heat released is not a function of external conditions and the heat can be stored indefinitely without any loss. Desirable characteristics of this technology would be practical forward and backward reaction temperatures, fast reaction rates and low cost of the components. These characteristics are what make chemical energy storage so promising and are why this method is the subject of this work. In figure 2, we can see a general classification of the most common chemical reactions used for heat storage. The stored energy density goes up to 2 MJ/kg [1]. 3 Figure 2: Classification of thermochemical storage reactions (from W. Wongsuwan at al. Applied Thermal Engineering 21 (2001) 1489-1519) 4 CaO/ Ca(OH)2 Cycle The reactions of CaO and MgO are classified as a solid-fluid reaction, monovariant and inorganic, where the solid is a metal oxide. CaO is a white powder with a consistency very similar to talcum powder and its theoretical density is 3350 kg/m3 but in the powder form used in most experiments, the density is 508.6 kg/m3. The typical reaction cycle is shown in figure 3. Figure 3: Hydration/dehydration cycle for the calcium For one mol of Ca(OH)2 at room temperature, it is necessary to add 148.6 kJ of energy to decompose it into CaO and H2O; this reaction occurs at a temperature over 500ºC. This energy can come from exhaust gases from a boiler, an engine, or a solar thermal power plant. This part of the cycle can be considered as the charging process. Then the calcium oxide can be hydrated with water at room temperature, releasing 63.6 kJ/mol. The energy efficiency in this particular cycle would be 42.8%, but one can increase this efficiency using 23.5 kJ/mol and the 61.5 kJ/mol lost in the cooling of the CaO and in the condensation of the water. Furthermore, if the hydration reaction is done at a higher temperature instead of at 25ºC, the energy efficiency could also be improved. The use of nickel oxide as a dopant for the dehydration reaction could be considered another way to increase the efficiency, but its effect on the hydration is unknown as of now. The efficiency could be reduced after many cycles because of the reaction between CaO and CO2, which forms calcium carbonate, CaCO3. The calcium carbonate can be eliminated by increasing the temperature and the pressure of the dehydration every several cycles. Most of this work is conducted with CaO; nevertheless some experiments with magnesium oxide (MgO) were performed. An energy balance of the reaction shows that less energy is released with magnesium oxide, only 81 kJ/mol in comparison with 148.6 kJ/mol released by the calcium oxide reaction. 5 1.2 State of the art A Azpiazu et al. [2] used two configurations for the analysis of the reaction. One of them, maybe the simplest design, was a device made of glass beakers, as shown in figure 4. The smallest beaker had the calcium oxide to be tested. Then this container was immersed in a second beaker with liquid antifreeze used as thermal media to measure the heat delivery of the exothermal reaction. Finally, this assembly was positioned in a bigger beaker that worked as a thermal isolation chamber to avoid air currents which would cool down the reactor. A Differential Scanning Calorimetry (DSC), was used to measure the heat of reaction, calculate the specific heat changes, enthalpies and the kinetics of the reaction. CaO/Ca(OH)2 Aqueous antifreeze Air insulation Figure 4: Glass reactor The second prototype was similar to a heat exchanger and was made of a copper box with copper fins inside that are in contact with the calcium oxide bed and connected to a space with antifreeze as shown in figure 5. Then this box was then placed inside a second box made of polyurethane. Figure 5: Cooper and polyurethane 6 Thermocouples are used to measure the temperatures of the calcium bed and the antifreeze. With this configuration, not only is the behavior of the hydration/dehydration evaluated, but also calculated is the usable energy that can be extracted from the reaction. With thermo-gravimetry or differential calorimetry, it is possible only to evaluate the behavior of the reaction. As previously shown, a very simple device can demonstrate how easily energy from exothermic reactions can be used. But this device was not designed to achieve several cycles or manipulate variables that have an influence over the reaction. Ogura et al. [3] proposed a configuration of two containers connected with pipes as shown in Figure 6: one was a high temperature reactor and contained the CaO/Ca(OH)2; the other container was the low temperature reactor that acted as a condenser and evaporator for water. Figure 6: Close loop reactor The dehydration is done in the high temperature reactor by the heaters and the resulting water vapor goes to the low temperature reactor where it is condensed. For the hydration reaction, the water was heated to the boiling point and due to a difference in pressure the vapor flowed to the calcium oxide container. The temperature at which the water reacts could be controlled by the vacuum pump. The last configuration is the most commonly used. It is common to see variations like a second set of high and low temperature reactors, coils or fins in the reactors to heat or cool a thermal fluid (like an antifreeze) or to achieve dehydration. Also several trays or levels are in the high temperature reactors. The common characteristic is the manipulation of the pressure to increase or reduce the boiling point of the water from 100ºC. 1.3 objectives The objective of the present study is to explore the behavior of the dehydration and hydration reactions with calcium oxide and magnesium oxide in order to understand 7 which variables can be controlled to produce several thermal charge and discharge cycles. A consequence of this exploration will be the development of a device that works with liquid water or steam at atmospheric pressure. This device could be considered as a prototype of a TESD that will be used for further investigations. 2 Construction of the experimental setup The project is divided into three different stages. The first stage is an exploration of the dehydration and hydration reactions. In the second stage, the aim is to find a way to perform as many thermal cycles as possible and to explore the effect of different variables. In the last stage, the goal is to see how a TESD can be constructed. In all the stages, the conditions are extreme, with temperatures up to 900ºC (1652ºF); also a very detailed monitoring of the temperature is important. For these reasons the design of the container represents an important part of this project. 2.1 Material The experiment needs a container that does not react with water, CaO/Ca(OH)2 or MgO/ Mg(OH)2, does not leak particles and also tolerates the high temperatures of the dehydration and hydration reactions. Other important consideration is that the container must be as light as possible, since a heavy container will require a lot of energy just to heat the container material; a similar situation occurs when measuring the heating and cooling times, as the thermal inertia of the container would give a false impression of the speed of the chemical reactions. The best material is stainless steel. It has a melting point of around 1,510ºC (2,750ºF) so the temperatures reached in the present experiment will not affect the structural integrity of the container. This also allows a light design, and this material is innocuous to the reaction of the MgO or the CaO and water. It is important to say, however, that the thermal conductivity of steel is not the best for this experiment in comparison with aluminum, copper, or other materials as shown in table 1. Table 1: Thermal conductivity for different metallic materials W/(mºK) Aluminum 250 Brass 109 Copper 401 Steel, Carbon 1% 43 Stainless Steel 16 8 BTU/(fthr*ºF) 144 63 232 25 9.2 This low thermal conductivity is compensated by the high yield strength of the stainless steel, that allows the construction of a light container of thin walls and hence a low thermal mass. 2.2 Furnace The best option was an electric jewelry furnace shown in figure 7; as it could reach temperatures above the dehydration limit 550ºC (1022ºF) for a long period of time, necessitated by mind the low thermal conductivity of the magnesium and calcium oxide and hydroxide. The furnace selected for the exploratory stage was the model MPM1C from Wenesco. Figure 7: Jewelry furnace 2.3 Temperature measurement For temperature reading a type K thermocouple was used, which has the components chromel (90 percent nickel and 10 percent chromium) and Alumel (95% nickel, 2% manganese, 2% aluminum and 1% silicon). It has a temperature range of 0º to 927ºC (32º to 1700ºF), with a sensitivity of approximately 41 µV/°C. The thermocouple is inside an immersion probe made of 316 stainless steel with a grounded tip as shown in the figure 8; this means that the thermocouple wires are physically attached to the inside of the probe wall. This results in good heat transfer from the outside, through the probe wall to the thermocouple junction. 9 Figure 8: Thermocouple type K The thermocouples (fig 8) were connected to a pc using a data acquisition board from National Instruments with 16 channels, model NI 9213 and its USB carrier model 9162 shown in figure 9. Labview was used to configure the data sampling frequency of the readings and export the file to Microsoft Excel. Figure 9: Data acquisition board with USB carrier 2.4 First container In the first part of the project a container that fits inside a small furnace was necessary. To meet all the constraints mentioned before, it must be made of stainless steel. Furthermore, to manufacture a container to do the first experiments without having any experience could be expensive, so a very simple and commercial container, was need, a sugar shaker, was selected as shown in figure 10. 10 A A Mass: 127g 90 mm 1 mm 50,4 mm Figure 10: Sugar shaker This container would be used for most cycles. This particular model comes with a cap and a pipe that later would be used to make the container for the tests with steam injection. It was necessary to remove the plastic parts of the container and then burn the epoxy glue. In figure 11 it can be seen one of the wire baskets that were made to safely manipulate the container when hot. This is not a stainless steel wire, but it would not be in contact with the calcium oxide at any moment. The configuration of the basket was a strong structure even at high temperatures, but if it breaks the container could hit the chamber of the furnace and damage it or spill out the powder. Figure 11 Wire basket In the hydration process, the thermocouple tends to rotate the container when it is inserted into the bed; to solve this and also reduce heat losses, a stable, heavy and thermally isolated base was built, shown in figure 12. 11 Figure 12: Base with insulation 2.5 Second container Using the first container some important characteristics of the reactions, processes and methodology were identified. In chapter 3, it will be explained that it is necessary to add more water than the stoichiometric amount, but too much water would cool down the powder, so a proper distribution of the water will be important. It would be easier to track the behavior of a large quantity of CaO or MgO, because a large mass of powder will be less sensitive to fluctuations in the dehydration temperature, the amount of water added for the hydration reaction and the thermal influence of the container’s steel wall. In the dehydration process, the possibility to collect the steam coming from the container was considered. The stainless steel is expensive and as the experiment progresses, the container will undergo design changes, so the container must have the possibility to be updated and have as little welding and as few permanent parts as possible. In response to these requirements, a second container was designed. It is shown in figure 13. 12 Figure 13: Second container Some of the parts deserve a short explanation. First the water injection attachment; it is composed of a disk that holds three small pipes that spread water. To do this it has holes that are not aligned as shown in figure 14. Figure 14: Distribution of the holes Figure 13 shows one green and one purple pipe. The green pipe is for the thermocouple, and the purple pipe injects water. In the figure they appear to be cut off, but their length can be checked on the plans in Appendix 1. There is also a green ring in the image. This ring acts as a spacer, with two purposes: In the hydration reaction, it forms a “pool”, giving time to the calcium or magnesium to absorb the water; second, this is where the steam is going to accumulate before exiting by the same pipe that is used to pour the water in, avoiding condensation inside the chamber. The cap shown in figure 15 has a shoulder to hold the different attachments together; the cap also has a groove with space for a wire that allows manipulating the container when hot. 13 Shoulder Thread Groove Figure 15: Cap of the second container The threads on the container and the cap are standard for a commercial pipe of that size, and its length allows adjusting the cap without any accessory, giving the possibility for different configurations. For example, we can see the container without connectors in the first picture of figure 16, and without the spacer in the second figure. This design made a versatile tool. Figure 16: Configurations of the second container Some problems were detected while the container was in use. The design does not use any standard parts; everything must be machined from raw materials, generating difficulties and delays for modifications or repairs. Even though the container was designed to fit inside the small furnace, the two long pipes for the injection of water and the thermocouple did not allow the furnace lid to fully close, so this increased the time to complete a reaction. Furthermore, the furnace presented an oscillatory behavior in the temperature as the control system tried to maintain it constant. This can be seen in figure 17. 14 Temperature (ºC) Temperature furnace curve 800 700 600 500 400 300 200 100 0 0 20 40 Time (min) 60 80 Figure 17: Characteristic behavior of the small furnace When the top lid of the furnace is open, the temperature is less stable and the peaks and valleys are more frequent. Hence the plateau, characteristic of the dehydration, is more difficult to identify. Finally, the container needs a lot of steel, reducing the usable space, which is in contradiction with the requirements that were initially mentioned about the low thermal mass the container should have. 2.6 Container for test with steam For the test with steam, it is necessary to boil the water in a separate compartment and then inject the vapor into the container that has the calcium or magnesium oxide powder. The initial concept was to divide the sugar shaker in two chambers using a mesh, as shown in figure 18. The lower compartment will have liquid water and after applying heat the water would begin to boil and the vapor would cause a reaction. A A Powder Mesh Water . Figure 18: Sugar shaker divided by mesh This design has some problems; first regardless of how fine the mesh is, there will always be calcium or magnesium oxide that passes through the mesh, reacting with water, 15 resulting in a loss of control of when and in what quantity the reaction occurs. Another problem the reduced sizes of the chambers, so the amount of water is restricted to the small space under the mesh. However, the principal problem is that it would be necessary to extract the powder, then refill the container with water after each experiment and that is another source of error. The solution to these obstacles was a second sugar shaker. Using the cap and the pipe that comes with the container, it is possible to make a separate chamber for the water and connect it to the container with the calcium or the magnesium oxide, this configuration as shown in figure 19. Figure 19: Container for test with steam The two caps (blue) and the pipe (red) are a single piece to avoid any loss of vapor; we can see that the container has two holes, one for the thermocouple and the other is the hole where the excess of vapor escapes. This design also has some limitations. The piece composed by the caps and the pipe was not easy to weld so only a single welded point was joinined each cap to the pipe. This, plus the fact that between the caps and the containers is a pressure fitting, ended with rupture of both joints. The daily manipulation made that the mouth of the water container got deformed, breaking the delicate seal that keeps the vapor in the chambers. Moreover, in the manipulation some powder escapes through the holes of the pipe in very small quantities; but with several cycles the amount of powder that reacts could be significantly reduced. 16 2.7 General purpose container The biggest problem with previous designs was the size. Any kind of system to spray the water, cool down the container, take readings in more than one point, division of the chambers, etc, is very hard to design in such small dimensions. The goal of the next design was to maximize the size of the container, taking into account the conditions we established before and what was learned with the last designs. The result was a container made of a thin stainless steel sheet, with a simple flange system to attach different accessories by only replacing the caps, as it can be seen in figure 20. Figure 20: General purpose container In figure 20, one of the multiple configurations can be seen, which in particular shows a helical heating element, with a single pipe for water injection. The space that contains the powder is composed by the flanges (blue) and a cylinder (black); without any attachment inside, the capacity is 2513.7 cm3 (more than 15 times the capacity of the biggest container until then). Due to the fact that the container can work with water or with low pressure steam it is important to guarantee a tight seal, hence a high temperature-high pressure material was found; it is made of laminated vermiculite core with carbon steel, that tolerates temperatures up to 982.2ºC (1800ºF) and can be cut with sheet metal shears. It is important to remember that that a high repeatability of the thermal cycling is desired, thus the methodology must be less manual and more automated. The first step in this direction was to maximize the size of the container in coordination with the size of the chamber of the new furnace (Omegalux LMF-A550), shown in figure 21. This furnace has a chimney that could be used to pass small pipes to the container; there is a space of 47.6 mm between the furnace’s roof and the container for any accessory. This gives the possibility to make the hydration and dehydration reactions inside the furnace, and also allow the automation of the furnace operation. 17 Figure 21: Furnace Omegalux LMF-A550 The initial configuration for the experiments with this container has a sprinkler for the water, an electric heater and a cooper coil. The coil can be used as a heat exchanger to cool down the container, to warm up the thermal fluid or also for the dehydration. Here each of them is explained briefly. 2.7.2 Sprinkler The sprinkler, shown in figure 22, is made of copper, which has a high fusion point 1084.62 °C (1984.32 °F) and is very easy to bend or form. The spiral shape allows us to cover most of the container’s diameter without couplings or Swagelok. It has 20 holes with a 1.1mm in diameter to spray the water. Figure 22: Sprinkler 18 2.7.3 Coil The coil is composed of two copper tubes, whose size was selected with the condition that the areas inside the small coil and the ring outside of it were the same. A similar norm was applied in its length. They are attached together by a Yor-Lok compression fitting made of stainless steel. The surface area in contact with the powder is 462 cm2. Its assembly can be checked in figure 23. Figure 23: Inner and outer coil 2.7.4 Heater The heater is a single phase electric heater that works with 120 V.AC. It is not commercially available, so it was manufactured specifically for this experiment. The helical shape, in figure 24, gives a lot of surface with minimum of volume. Figure 24: Electric heater 19 3 Experimental Procedure For the first three containers the procedure was almost the same. The general purpose container used a particular method depending on the accessories that were used. 3.1 Dehydration For the sugar shaker, we use the wire basket to put it inside the furnace; the wire basket is not needed for the second container because it has a groove for its own wire. The dehydration is characterized by a change in the slope in the graph of the temperature vs time. The change of the slope is produced by the absorption of heat and to a lesser extent by the change in the thermal conductivity of the bed. The dehydration was usually done at 700 ºC, at which temperature the inflection point is still visible, within the range of the thermocouple. The reaction is fast enough to do several experiments in a day. Other temperatures were explored; lower temperatures allow to see a more evident plateau, but consumes more time. In the case of higher temperatures, it is hard to find the exact point where the dehydration begins, and the thermocouple can shows jumps in the readings, as it was showed in figure 25. Apparently, these jumps happen because the metallic probe of the thermocouple begins to bend under the high temperature and its own weight. Dehydration 700 Temperature (ºC) 600 500 400 300 200 100 0 0 20 40 60 Time (min) 80 Figure 25: Jumps in the temperature reading 20 100 This can be avoided if the thermocouple is hung, even though the lifetime of the sensor is reduced, so either way it is suggested not to go over 700ºC frequently. After the dehydration process is finished it is necessary to wait until the container cools down, which can take up to one hour in the case of the second container; when the purpose is to make as many cycles as possible, this is not efficient. To accelerate the process, the container is submerged in water, holding it with some pliers from the basket or the wire in the case of the second container. It is important to highlight that this is safe as long as we are using small containers and the water does not get inside the container. If water touches the powder at this temperature, particles will jump out of the container (if it is open) becoming a safety hazard. This process generates a dark scale, or very brittle flake on the exterior of the containers. Keeping in mind that the container is stainless steel and that the oxidation of the steel is a slow process, the corrosion can be disregarded. On the other hand, based on the color of the material, how brittle it is (observable when the basket wire is then bended) and noting that it is almost exclusively present in the exterior of the container, it could be inferred that the material is one of the crystal structures formed in a tempering or quenching processes (martensite, austenite, pearlite). The problem with the flakes is that it falls very easily from the container, so in several cycles the thickness of the container would be reduced. Until now this has not represented a considerable problem, but it should be kept in mind in the future. 3.1.2 Dehydration with the general purpose container The dehydration can be achieved by three different methods. With the large furnace, just put the container inside the chamber and set the temperature; as with the small furnace, 700ºC is the temperature recommended. If the hydration process is going to be done inside the furnace, the pipes for the water injection and the coil need to be placed through the chimney before the container is installed. The second method is to use the helical heater inside the container, which can be hung from the upper cover of the container that also holds the coil and the sprinkler; with a Variac transformer the temperature can be set. For this setup we need to cover the container with high temperature thermal insulation to reduce the heating time, the power consumption and the risk of accidents. The characteristics of this material is presented on table 2. Table 1Insulation properties Material Alumina silica Heat Flow Rate (K-factor) @ 426.6 ºC (800ºF): Density 21 0.65 128.14 Kg/m3 Thickness Maximum temperature 50.8 mm 1093.3ºC The heater has a temperature limit of 871ºC, because it is submerged in the calcium oxide powder, a low conductive material. The powder temperature can increase really fast and burn the heater. It is necessary to have a thermocouple in contact with the heater and reduce the voltage when the temperature gets closer to that limit. The electric power supplied to the heating coil is one of the principal parameters to be automated. A third way to achieve dehydration is by injecting hot gas; for this a flexible heating tape is wrapped around a nickel-chromium(or copper) tubing, as shown in figure 26, where air from a compressor is heated and then passed through the copper coil inside the container. Some characteristics of the heater and the pipe appear in table 3. Figure 26: Gas heater maximum heat output of 760ºC Heater 1/8" thick, 1/2" wide 10' Length, 520 Watts, 120 VAC with Plug 3/4" OD, .620" ID, .065" Wall, 3' Length 72% nickel, 14-17% chromium, and 6Tubing 10% iron Temperature Range: -200° to 650° C Table 2: Characteristics of the pipe and heater of the gas dehydrator 22 3.2 Hydration As was mentioned before, the sugar shaker is placed into the heavy base (figure 12); 60 mL of water is added to 50 g of calcium. The reaction takes several seconds and the temperature rises to around 200ºC. The second container is heavy so it is not necessary to put it inside the base; this container is not as versatile as the sugar shaker, so it was used only a few times. For the hydration with steam the reactor in figure 19 is used; one of the containers is filled with water, then the container with calcium oxide closes the first container and the entire device is then placed on a hot plate, as shown in figure 27, where water boils and the vapor reaches the powder in the upper chamber. In the test with vapor, the reaction takes several minutes, in part because it takes a long time for the water to boil. Figure 27: Hydration with steam 3.2.2 Hydration with the general purpose container The sprinkler in figure 22 is used with a funnel, a hose and a small ball valve to inject the water, shown in figure 28. With the valve closed, the funnel is filled with water and then raised to increase the potential energy of the fluid; in this way the speed of the injection can be controlled with the height of the funnel. 23 Figure 28: Funnel This simple system allows full control in the amount of water without using a pump, but it will be hard to automate in the future; a future design for this system needs to recover the water from the dehydration and store it a bladder-pressure tank that will be pressurized at the moment of the injection with a compressor that can be automated. 4 Results for Calcium hydroxide and magnesium hydroxide 4.1 Calcium Hydroxide 4.1.2 Dehydration The experiment began with 50 grams of Ca(OH)2; it is known that the dehydration starts at a temperature higher than 512ºC [1], so the furnace was initially set at 550ºC. However, the oscillatory behavior of the furnace, prevented us from recognizing if and when the reaction took place. It was when the furnace temperature reached 600ºC that a change in the temperature gradient became appreciable. 24 Dehydration 800 700 Temperature (ºC) 600 532.3 500 Bed temperature 400 Furnace temperature 300 200 100 0 0 20 40 60 80 100 120 140 Time (min) Figure 29: First successful dehydration In figure 29, 532.3ºC appears to be the point where the dehydration reaction begins, while at 100ºC there is a plateau that corresponds to the vaporization of remaining moisture in the Ca(OH)2 bed. The next step was to conduct experiments with different sizes of Ca(OH)2 lumps. To prepare the lumps, an aluminum container was filled with approximately 250 grams of Ca(OH)2. Then water was added forming mud that is heated at 200ºC (a temperature high enough to vaporize the water) to form a hard bed that could be broken and separated into different sizes. The dry shell was very brittle, in fact it was easier to make small lumps than big ones; then with the help of three sieves the particles were separated into four sizes: bigger than 12.5 mm, between 6.3 and 12.5 mm, between 2 and 6.3 mm and smaller than 2mm. Several hydration-dehydration cycles were repeated with all sizes, but there were not an appreciable difference in the dehydration process, as can be seen in the dehydration processes for two different lumps sizes in figure 30. 25 Dehydration 800 700 Temperature (ºC) 600 500 6.3<Lumps size<12.5 2<Lumps size<6.3 400 300 200 100 0 0 10 20 30 40 50 Time (min) Figure 30: Dehydration for two different sizes of lumps 4.1.3 Hydration In the first test of hydration, 18 mL of water were added to 50 grams of calcium oxide, the stoichiometric quantity. But that amount of water did not produce a temperature increase that could be interpreted as an undeniable exothermic chemical reaction. Hence, the amount of water was increased until it was seen that with 60 ml of water all the calcium was hydrated almost at the same time. The CaO and the Ca(OH)2 beds are very porous, able to store a lot of water beyond the stoichiometric quantity necessary for the reaction. When water reaches the CaO, even parts at the same depth as layers that have already reacted could stay dry; this explains why even when the thermocouple was at the bottom, the temperature rise was small. For this reason it was necessary to inundate the container just enough to hydrate the most external stratum and ensure that all the calcium reacts and produces heat. Due to the porosity of the CaO bed, the water takes a little time to be absorbed by the solid bed. On the other hand we see that it is important that the bed reacts at the same time to avoid that the unreacted calcium absorbs heat already generated. This gives importance to a system or device to spread water in the reactors. The sugar shaker was the container most used for the cycles; because of its size, it was very hard to design a 26 sprinkler, but this was achieved in the general purpose reactor. It can be said that the speed at which the water reacts with the CaO, depends on the absorption speed and mostly the water pouring speed. Thirty four hydration tests were done with liquid water and only with a few exceptions the behavior was almost the same as shown in figure 31. First, there is an almost vertical line that shows a very fast temperature increase, then a peak in temperature after which a typical cooling curve descends to 100ºC. Hydration 200 180 174.77 Temperature (ºC) 160 140 120 100 80 60 40 20 0 0 20 40 60 80 100 Time (sec) Figure 31: Typical hydration reaction for the CaO It is seen that in only a few seconds the temperature reaches a peak 70% higher than the boiling point. The subsequent cooling curve and plateau are a result of the cooling effect of the vapor leaving the Ca(OH)2 bed. The speed of the reaction, the speed of the cooling and the maximum temperature reached varied a little among the experiments. 27 Hydration 180 160 Temperature (ºC) 140 120 100 80 Series1 60 Series2 40 20 0 0 50 100 150 200 Time (sec) 250 300 350 Figure 32: Fast and slow reactions in the CaO bed The hypothesis that the reaction degrades over several thermal cycles, making the reactions slower and cooler can be discarded. One slow and cool hydration curve, like the series 2 in figure 32, can be followed in the next cycle by a fast and hot hydration curve, like the series 1 in the same figure; the opposite is also true. One hypothesis that explains slow and cool reactions is related with how fast the water is poured into the container. Moreover, even when the cycles are done with a relatively homogeneous powder bed, there are smaller particles, that with the manipulation are decanted and dragged by the water to the bottom, forming a more dense and less porous base; this affects the speed of absorption and therefore the speed of the reaction. With a slower reaction, it is logical to think that there will be a lower peak; in turn, a lower peak means fewer vapors cooling the bed and a flatter cooling curve. The presence of this more dense bed at the bottom can be confirmed when the container is emptied and the dense layer is exposed. In the experiments with the CaO lumps, no relation between the reaction behavior and the presence of the lumps could be established. No lump size survived beyond the fourth cycle. Trying to maintain the stone consistency of the lumps, the hydrations began with 35 ml of water, but again it was found that there was not a full reaction in the calcium 28 oxide bed. Thus, the amount of water was increased in several tests up to 60 ml, but the more water was used, the fewer cycles the lumps lasted. 4.1.3.1 Hydrations with cold water Some of the cycles presented a peak in temperature almost twice higher than most experiments. At the beginning there was not a clear cause for these super-hot hydrations. Then, 10 cycles with water that was close to the freezing point offered a hint: the tests with cold water resulted in peak temperatures from 280ºC to 400ºC. This result was unexpected and although it is sure that the low temperature water is the cause, it is still not clear why this happened, In figure 33, the behavior of two of this super-hot reactions can be seen. Hydration 450 400.9 400 343.03 Temperature (ºC) 350 300 250 200 150 100 50 0 0 100 200 300 400 500 Time (sec) Figure 33: Super-hot hydrations 4.1.4 Hydration with steam The reaction with steam was found to be slower than with water. The steam took more time to reach and react with the bed, but the peak temperatures were in the same range as with the hydration with liquid water. Because there is steam inside the container, the cooling process after the peak reaches only 100ºC, where the temperature is maintained due to the continuous injection of vapor. Other new situation in some hydration tests was the presence of secondary temperature peaks after the highest peak. This can be explained 29 by the rupture of lumps formed through several cycles. These lumps reacted with the vapor that still flowed through the reactor. These smaller peaks can be seen in figure 34. Hydration 160 140 Temperature (ºC) 120 100 80 60 40 20 0 0 10 20 30 40 50 Tíme ( min) 60 70 80 Figure 34: CaO hydration with steam In some experiments, once the 100ºC plateau was reached, the hot plate was turned off to check the amount of water that remained in the container; it can be seen that it took as little as 30ml of water to produce a reaction. This could be explained because the vapor (as any gas) tends to expand and fill its container regardless of its amount, and we could fill the sugar shaker with only 30 ml of steam instead of 60 ml of liquid water. This was a situation that could compensate for the slow reaction. It is important to say that in 28 cycles with steam, 2 cycles did not go beyond 100ºC. It is not easy to give an explanation for that until the process is automated, where hundreds of thermal cycles could produce a good statistical data. 4.1.5 Dehydration in the general purpose reactor In figure 35, the start of the hydration reaction when is in the furnace took around three hours. It is expected that with other methods this time can be reduced. 30 Dehydration 800 700 Temperature ()ºC 600 500 400 300 200 100 0 0 50 100 150 200 Time (min) 250 300 350 400 Figure 35: Dehydration with the general purpose reactor 4.1.6 Hydration general purpose reactor In the hydration plot (figure 36) we find that the reaction was slower than in the smaller containers. Due to the bigger mass, the cooling curve is also less steep. The blue line confirms how important a water injection system is, even when 1300ml of water was used. Since no reaction took place in the peripheral region. It is important to mention that the first hydration test in this container yielded a peak temperature of 442ºC in the central region and 373.5ºC in the peripheral, suggesting that other water injection systems should be tested. 31 Hydration 180 160 Temperature (ºC) 140 Peripheral thermocouple Central thermocouple 120 100 80 60 40 20 0 0 10 20 30 40 50 Time (min) 60 70 80 90 Figure 36: Hydration with the general purpose reactor 4.2 Magnesium Oxide 4.2.2 Dehydration For magnesium oxide tests, 50 grams were used again and the temperature of the furnace was kept at 700ºC. The dehydration reaction occurred at 400ºC in accordance with the available literature on this process. Figure 37 is a record of this dehydration reaction. 32 Dehydration 700 600 500 Temperature (ºC) 407.3 400 Bed temperatue Furnace temperature 300 200 100 0 0 10 20 30 40 50 Time (min) Figure 37: Magnesium dehydration The consistency of the magnesium oxide after several cycles was less porous, more compact and the particles attached to the walls of the container, in an almost diametrically opposite behavior to the CaO or the Ca(OH)2. 4.2.3 Hydration The hydration test began with 60 ml of water without any reaction. Considering that probably too much water was added, cycles with 50 and 40 ml were done until 10 repetitions were completed without obtaining a positive result. It was considered that an initial high temperature is necessary to start the reaction, so tests with warm water were made. The first test was with 60 ml of water at 60ºC and the result is shown in figure 38; the water warmed up the magnesium until the first peak, then it cooled relatively slowly until it reached a minimum, but then the temperature increased again until it reached 100ºC where it stayed for a long time. After which, the bed cooled down back to the room temperature. 33 Hydration 120 Temperature (ºC) 100 80 70.5 65.1 60 40 20 0 0 5 10 15 20 25 Time (min) Figure 38: Magnesium hydration The temperatures in the peak and valley, as well as the speed of the reaction, changed for each cycle. At the beginning it seemed that there was a minimum temperature necessary for the reaction, but the cycle with 60 ml of water at 60ºC was done again, showing a different result that contradicted this hypothesis (figure 39). 34 Hydration 60 Temperature (ºC) 50 40 30 20 10 0 0 50 100 150 Time (min) 200 250 300 Figure 39: Slow magnesium hydration After one hour it was possible to see an indication of a reaction, evidenced by a change in the slope. It seems the different curve shapes in the hydration cycles are related with the low porosity of the bed, rather than with temperature of the water. This is coherent with the different peaks, valleys and durations of the reaction; if a specific water temperature would be necessary, the range of these temperature in the reactions would be closer in different hydrations tests. A hypothesis similar to that of the Ca(OH)2 where finer particles were decanted, is proposed to explain this effect. However, the slower absorption speed effect is accentuated by the naturally higher density of the magnesium oxide. The temperature never exceeded 100ºC, even when water at 95ºC was added. In the experiments, it was seen that 40 ml is the proper quantity for the hydration reaction with the magnesium oxide. When more water is added, after the 100ºC plateau the remaining water stayed on the bed and was not absorbed as in the Ca(OH)2. This pool over the bed boiled and a lot of steam emanating from the container was observed; in one particular hydration test with 50 grams of magnesium oxide and 100 ml of water, 20 ml were left in the container and considering the relatively low absorptivity of the bed, it can be said that around 40 ml of water was transformed into steam. This can be a good situation despite the low temperatures reached in the reaction. 35 4.2.4 Hydration with steam With steam the behavior was different as shown in figure 40. The MgO bed temperatures exceed 100ºC in 5 min, then there was a very drastic change in the slope, from very vertical to almost horizontal; the temperature rose to 107.8ºC rapidly and then began a very slow cooling that ended again at 100ºC. Hydration 120 107.8 Temperature (ºC) 100 80 60 40 20 0 0 10 20 30 Tíme (min) Figure 40: Steam magnesium hydration 36 40 50 5 Conclusions The amount of water and how it is added is probably the most important variable. The temperature, amount, water phase, and the speed at which it is poured, determines the peak temperature that can be reached. The porosity of the bed material is not a negligible characteristic. However, in the case of CaO the porosity is very high, but for MgO, it is less, to the point that the water can form a pool over the bed. The best method to achieve high temperatures in hydration reaction could be a topic for a separate investigation. According to the present results, the use of lumps of any size in the dehydration or hydration steps for the tests with steam water is innocuous. Between the MgO and CaO, it is the latter that offers higher temperatures, indicating that this reaction could be more promising for use in thermal storage devices in power plants and in vehicles. The MgO does not offer as high temperatures as CaO; but because it is less porous, it releases steam easier than the CaO, a characteristic that also could be exploited in other applications. The use of cold water, close to the freezing point, generated higher temperatures than with room temperature water, the reason for this is unknown. Cooling the water to this point could represent an obstacle to overcome. There is still a lot to study such as, dehydration with a hot gas and electric heaters, hydration at different bed temperatures, dehydration under different pressures, hydration with cold water, and the effect of catalysts and additives in the dehydration and hydration processes for both, CaO and MgO. 37 Annex 1 Blue prints of the second container 9 7 6 8 5 3 Item Number Title 1 From Quantity 1 Internal pipe Stainless steel 1 2 Bottom Stainless steel 1 3 Spray Stainless steel 1 4 Inyector Stainless steel 3 5 Spacer Stainless steel 1 6 Colector Stainless steel 1 7 Condenser Stainless steel 1 8 External pipe Stainless steel 1 9 Thermocouple pipe Stainless steel 1 4 2 Material City College of New York Container for water Jorge Pulido Esc: 1 : 1 Mechanical Ing. Assamble To Date: 2/28/2011 39 Thesis Stainless steel Masahiro Kawaji Item#: 0 2 1 Item Number From City College of New York Container for water Jorge Pulido Esc: 2 : 1 Title Material Quantity 1 Internal pipe Stainless steel 1 2 Bottom 1 Stainless steel Thesis Mechanical Ing. Stainless steel Container Assamble To Masahiro Kawaji Date: 2/28 Item#: 0 40 3 The three holes of each pipes point to the center Item Number 4 From City College of New York Container for water Jorge Pulido Esc: 2 : 1 Title Material Quantity 3 Spray Stainless steel 1 4 Inyector Stainless steel 3 Thesis Mechanical Ing. Stainless steel Inyectors Assamble To Masahiro Kawaji Date: 2/28 Item#: 0 41 2 3 Item Number Title Material Quantity 1 Colector Stainless steel 1 2 Condenser Stainless steel 1 3 Thermocouple pipe Stainless steel 1 1 From City College of New York Container for water Jorge Pulido Esc: 2 : 1 Mechanical Ing. Conectors To Date: 2/28 42 Thesis Stainless steel Masahiro Kawaji Item#: 0 43 O 1.50 From 2.00 City College of New York Container for water Jorge Pulido Esc: 1 : 1 4.00 Thread 1 1/2-6 UNC Mechanical Ing. Thesis Stainless Steel Internal Pipe To Masahiro Kawaji Item#: 1 Date: 2/28 .020 O 1.50 From City College of New York Container for water Jorge Pulido Esc: 2 : 1 Mechanical Ing. Bottom To Date: 2/28 Thesis Stainless steel Masahiro Kawaji Item#: 2 O .148 6.39 From O3/16" City College of New York Container for water Jorge Pulido Esc: 2 : 1 Thesis Mechanical Ing. Stainless steel Thermocouple pipe To Masahiro Kawaji Date: 2/28 Item#: 9 44 45 O 1/4" O 1/4" O 1.50 From O 1/8" City College of New York Container for water Jorge Pulido Esc: 2 : 1 O 1/4" .02 Mechanical Ing. Thesis Stainless Steel Spray To Masahiro Kawaji Item#: 3 Date: 2/28 46 .73 .52 1.36 NOTE: All the holes are of the same size. Each set of holes are in faces at 90º of the adyacents faces O 3/32" .31 From .73 .52 City College of New York Container for water Jorge Pulido Esc: 1 : 1 1.36 2.000 .31 O 1/4" Mechanical Ing. Thesis Stainless Steel Inyector To Masahiro Kawaji Item#: 4 Date: 2/28 O .18 .500 O 1.500 1 1/2-6 UNC From City College of New York Container for water Jorge Pulido Esc: 2 : 1 Mechanical Ing. Spacer To Date: 2/28 Thesis Stainless steel Masahiro Kawaji Item#: 5 .020 .375 O3/16" O 1/4" O 1.500 From City College of New York Container for water Jorge Pulido Esc: 2 : 1 Mechanical Ing. Colector To Date: 2/28 47 Thesis Stainless steel Masahiro Kawaji Item#: 6 48 12.00 From City College of New York Container for water Jorge Pulido Esc: 1 : 1 Mechanical Ing. Thesis Stainless Steel Condenser To Masahiro Kawaji Item#: 7 Date: 2/28 O .180 49 .19 O 1.64 O 1.07 1/16" 1/16" From City College of New York Container for water Jorge Pulido Esc: 2 : 1 1.50 1.31 1.37 Mechanical Ing. Thesis Stainless Steel External Pipe To Masahiro Kawaji Item#: 8 Date: 2/28 1 1/2-6 UNC 50 3 8 7 From 2 City College of New York Container for water Jorge Pulido Esc: 1 : 1.11 1 6 4 9 Big Coil Injection Coil 8 9 1 1 1 1 1 1 2 2 1 Quantity Mechanical Ing. Thesis Stainless Steel General assamble To Masahiro Kawaji Item#: 0 Quantity: 1 Copper Copper Copper Small Coil Stainless steel 7 Upper cover 5 Stainless steel Heating element Stainless steel Pipe 4 Stainless steel Silicone Stainless steel Material 6 Flange Gasket Lower cap Title 3 2 1 Item Number 5 Annex 2 Blueprints of the general purpose container 51 3/8 " 60° From City College of New York Container for water Jorge Pulido Esc: 1 : 2 97,04 .062 " Mechanical Ing. Thesis Stainless Steel Lower cover To Masahiro Kawaji Piece#: 1 Quantity: 1 8.625 " 97.04 O 6.5 " 52 From 3/8" City College of New York Container for water Jorge Pulido Esc: 1 : 2 60° .062 " Mechanical Ing. Thesis Stainless Steel Flange To Masahiro Kawaji Piece#: 3 Quantity: 2 8.625 " 53 From City College of New York Container for water Jorge Pulido Esc: 1 : 2 .062 " Mechanical Ing. Thesis Stainless Steel Pipe To Masahiro Kawaji Piece#: 4 Quantity: 1 111,48 169,08 54 Heater Diameter: 0.26" Number of turns: 3 4,7 From 0,7 1,2 Mechanical Ing. Heating element To Masahiro Kawaji Piece#: 6 Quantity: 1 Extension regardless of the length of the electric terminal City College of New York Container for water Jorge Pulido Esc: 1 : 1 2,2 55 60° 7/16 " O 12,7 7/1 6" 60,56 5/16" 5/16" 2,56 From 33,56 24,56 5/16" 5/1 3/8" " 7/16 1,56 7/16" 75,56 66,56 33,06 19,9 38,5 57,1 75,7 City College of New York Container for water Jorge Pulido Esc: 1 : 2 6" 8.6 " Mechanical Ing. Thesis Stainless Steel Upper cover To Masahiro Kawaji Piece#: 5 Quantity: 1 .062 " 56 1,8 2 R1 Pipe: O.D.= 1/4" I.D.= 0.186" Number of turns: 3 left-handed O 71,93 41,46 11,82 From City College of New York Container for water Jorge Pulido Esc: 1 : 1 68,57 14,46 Mechanical Ing. Thesis Coper Small Coil To Masahiro Kawaji Piece#: 7 Quantity: 1 R 1 1,82 57 Pipe: O.D.=1/4" I.D.=0.186" Number of turns: 3 right-handed 11,83 O 138,56 From 40,13 City College of New York Container for water Jorge Pulido Esc: 1 : 2 1,82 R1 14,91 R 11,37 Mechanical Ing. Thesis Copper Big Coil To Masahiro Kawaji Piece#: 8 Quantity: 1 68,57 58 Pipe: O.D.= 1/4" I.D.= 0.19" Number of turns: 2 Parametric equation: x= 4.8xtxcos(t)+4.13 y= 4.8xtxsin(t)+9.5 157,33 From City College of New York Container for water Jorge Pulido Esc: 1 : 2 This end is closed Mechanical Ing. Thesis Copper Big Coil To Masahiro Kawaji Piece#: 9 Quantity: 1 R 11,4 8 16,17 Annex 3 Steps to assemble the attachment to the upper cover for the general purpose container. Step 0: Upper cover with compression fittings Step 1: Injection coil 59 Step 2: Small coil added Step 3: Electrical heater added 60 Step 4: External coil added 61 References [1] M.N. Azpiazu, J.M. Morquillas, A. Vazquez, Heat recovery from a thermal energy storage based on the Ca(OH)2/CaO cycle, Applied Thermal Engineering 23 (2003) 733– 741. [2] Hironao Ogura, Tetsuya Yamamoto, Hiroyuki Kage, Efficiencies of CaO/H2O/Ca(OH)2 chemical heat pump for heat storing and heating/cooling, Energy 28 (2003) 1479–1493, 2001. [3] W.Wongsuwan, S. Kumar, P.Neveu, F.Meunier, A review of chemical heat pump technology and applications, Applied Thermal Engineering 21(2003) 1489-1519. [4] F. Schaube, L. Koch, A. Wörner, H. Müller-Steinhagen, A thermodynamic and kinetic study of the de- and rehydration of Ca(OH)2 at high H2O partial pressures for thermo-chemical heat storage, Thermochimica Acta 538 (2012) 9– 20. [5] S. Fujimoto, E. Bilgen, H. Ogura, CaO/Ca(OH)2 chemical heat pump system, Energy Conversion and Management 43 (2002) 947–960. [6] S. Fujimoto, E. Bilgena, H. Ogura, Dynamic simulation of CaO/Ca(OH)2 chemical heat pump systems, Exergy, an International Journal 2 (2002) 6–14. [7] Hironao Oguraa, Energy Recycling System Using Chemical Heat Pump Container, Energy Procedia 14 (2012) 2048 – 2053 [8] Hironao Ogura, Shokrat Abliz, Hiroyuki Kage, Studies on applicability of scallop material to calcium oxide/calcium hydroxide chemical heat pump, Fuel Processing Technology 85 (2004) 1259– 1269 [9] F. Schaube, A. Wörner, H. Müller-Steinhagen, High temperature heat storage Using gas-solid eactions, Pfaffenwaldring 38-40, 70569 Stuttgart. [10] M.A. Hamdan, S.D. Rossides, R. Haj Khalil, Thermal energy storage using thermochemical heat pump, Energy Conversion and Management (2012) [11] Jaume Cot-Gores, Albert Castell, Luisa F.Cabeza, Thermochemical energy storage and conversion: A-state-of-the-art review of the experimental research under practical conditions, Renewable and Sustainable Energy Reviews 16 (2012) 5207–5224. [12] K. Darkwa, Thermochemical energy storage in inorganic oxides: an experimental evaluation, Applied Thermal Engineering Vol. 18, No. 6, pp. 387±400, 1998. [13] Yukitaka Kato, Kei Kobayashi and Yoshio Yoshizawa, Durability to repetitive reaction of magnesium oxide/water reaction system for a heat pump, Applied Thermal Engineering Vol. 18, Nos 3-4, pp. 85-92, 1998. 62 [14] BY P. J. Anderson., F. Horlcaknd, J. F. OLIVER, Interaction of Water with the Magnesium Oxide Surface, 01 January 1965 on http://pubs.rsc.org | doi:10.1039/TF9656102754, 1965 63
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