James Madison University Department of Engineering Eric J. Leaman Jack R. Cochran Faculty Advisor: Dr. Jacquelyn Nagel Overview Background Problem Statement Broader Impact Literature Review Design Approach Energy Storage Concepts Models and Calculations Model Validation and Experimental Results Conclusions Future Work 2 Background 22% of total energy consumed in the United States is used in residences Electricity accounts for 41% Only 10.6% of energy generation is from renewable resources Residential solar energy systems help to reduce dependency on fossil fuels for electrical energy If 15% of Shenandoah Valley households utilized PV systems, carbon emission would be reduced by the equivalent of removing 5,000 passenger vehicles from the road [1] 3 Problem Statement Typical small-scale solar systems use chemical batteries for energy storage Lead acid batteries account for [2] more than 2 million tons of total waste each year Comprised of regulated toxins (sulfuric acid and lead) More than 200,000 tons is nonrecyclable Off-gassing is another danger They are expensive – averaging $115 to $160 per amp-hour capacity at 12V Lifespans are short and discharge to below about 80% capacity damages battery [3] 4 Advancement of renewable energy systems and greater incentive for skeptical adopters Inexpensive, safe, and lowmaintenance system for remote and poor locations Economic Environmental Social Technical Broader Impact Reduction in waste, toxins, and emissions Improvement of costfeasibility for residential PV system 5 Pumped hydroelectric energy storage (PHES) Accounts for over 99% of worldwide bulk energy storage Up to 85% efficient Advantages Good reliability [8] Low maintenance Low environmental impact Disadvantages High start-up costs Typically used in large-scale systems such as power plants PHES Reservoir in Rönkhausen, Germany [8] 6 Compressed Air Energy Storage (CAES) Published overall efficiencies typically around 50% Highly reliable Greater complexity than comparable storage methods Typically used on very large scales [10] 7 Design Approach 8 System Architecture 9 Functional Model 10 Concept Generation 11 PHES Architecture House (Not to scale) 12 Concept Selection – High-level Analysis Published efficiency values for water turbines range from 60% to 90% Published efficiencies for generators range from 80% to 95% At minimum efficiency, this translates to a reservoir of about 5.6% the volume of an Olympic swimming pool at 62 m to meet power and energy requirements System Parameters to Provide 1 kW Power for 11.4 h Using an 11 mm Nozzle 13 Results of High-level Analysis Stored energy is a function of both reservoir height and volume 𝐸 = 𝑚𝑔ℎ = 𝜌𝑉𝑔ℎ Power is a function of height: 𝑃= 𝑑𝐸 𝑑𝑡 = 𝑚𝑔ℎ Needed Volume vs Height for 1 kW Power and 11.4 kWh Energy for No Loss, Max. Expected Efficiency, and Min. Expected Efficiency 14 Compressed Air 𝑛−1 𝑛 𝑛 𝑃𝑜𝑢𝑡 𝑤𝑜𝑣 = 𝑃𝑖𝑛 1 − 𝑛−1 𝑃𝑖𝑛 𝑤𝑜𝑣 = Specific work that can be stored n = value related to the conditions of the system 𝑃𝑜𝑢𝑡 = the pressure outside of the tank 𝑃𝑖𝑛 =denotes the pressure inside of the tank. Compressed Air 𝑤𝑜𝑢𝑣 𝑛 𝑃𝑜𝑢𝑡 = 𝑃𝑚 1 − 𝑛−1 𝑃𝑚 𝑛−1 𝑛 𝑃𝑚 = working pneumatic pressure Replacing 𝑃𝑖𝑛 with 𝑃𝑚 𝑤𝑜𝑢𝑣 = wasted energy density Tank Storage Needed 𝑤𝑜𝑒𝑣 = 𝑤𝑜𝑣 − 𝑤𝑜𝑢𝑣 𝐸𝑠𝑡 𝑉𝑖𝑛𝑡 = 𝑤𝑜𝑒𝑣 Compressed Air System Efficiency 𝜂𝑠𝑡𝑜𝑟 𝐸2 𝑊𝑡 = = 43% 𝜂𝑥,𝑡 = = 36% 𝐸1 𝐸2 𝜂𝑠𝑡𝑜𝑟 = 𝐸𝑓𝑓𝑖𝑐𝑖𝑐𝑒𝑛𝑐𝑦 𝑜𝑓 𝑡ℎ𝑒 𝑆𝑡𝑜𝑟𝑎𝑔𝑒 𝑇𝑎𝑛𝑘 𝜂𝑥,𝑡 = 𝐸𝑓𝑓𝑖𝑐𝑖𝑒𝑛𝑐𝑦 𝑜𝑓 𝑡ℎ𝑒 𝑇𝑢𝑟𝑏𝑖𝑛𝑒 𝐸1 = 𝐸𝑛𝑒𝑟𝑔𝑦 𝑓𝑟𝑜𝑚 𝑆𝑡𝑜𝑟𝑎𝑔𝑒 𝐼𝑛𝑙𝑒𝑡 𝐸2 = 𝐸𝑛𝑒𝑟𝑔𝑦 𝑓𝑟𝑜𝑚 𝑡ℎ𝑒 𝑆𝑡𝑜𝑟𝑎𝑔𝑒 𝑂𝑢𝑡𝑙𝑒𝑡 𝑊𝑡 = 𝑇𝑢𝑟𝑏𝑖𝑛𝑒 𝑊𝑜𝑟𝑘 Energy Conversion Turgo and Pelton turbines operate in air Francis and propeller turbines operate submerged (From Williamson, et al. [11]) [12] All shown practical at a small- scale 19 Dynamic System-level Model 𝐼𝑒 𝜔 = 𝑇 − 𝑇𝐿 − 𝑐𝜔 𝑇𝐿 𝑐 𝐼𝑎𝑟𝑚𝑎𝑡𝑢𝑟𝑒 𝐼𝑡𝑢𝑟𝑏𝑖𝑛𝑒 𝑇, 𝜔 𝑘𝑏 𝜔 − 𝑖𝑎 (𝑅𝐿 + 𝑅𝑎 ) = 0 𝑇𝐿 = 𝑘 𝑇 𝑖𝑎 = 𝑘𝑏 𝑘 𝑇 𝜔 𝑅𝐿 + 𝑅𝑎 𝑉𝑎 𝑅𝐿 𝐿 𝑅𝑎 𝑉𝑏 𝑖𝑎 20 The force on a vane of the turbine is: 𝐹 = 𝑚𝑏 𝑣𝑗 − 𝑣𝑏 𝛽 𝑚𝑏 = 𝜌𝐴𝑛 (𝑣𝑗 − 𝑣𝑏 ) And: Then the torque on the turbine is: 𝑇 = 𝐹𝑟 = 𝑚𝑏 𝑟 𝑣𝑗 − 𝑣𝑏 𝛽 = 𝑟𝜌𝐴𝑛 𝛽 𝑣𝑗 − 𝑟𝜔 Where: 𝑚𝑏 = mass flow rate into turbine bucket 𝑣𝑗 = velocity of jet 𝑣𝑏 = tangential velocity of turbine 𝛽 = 1 + cos(𝛾) 𝛾 = 60° (angle between center of bucket and bucket wall) 𝜌 = density of water 𝐴𝑛 = cross-sectional area of nozzle outlet 𝑟 = radius of turbine 𝑣𝑏 = 𝑟𝜔 Leading to: 𝐼𝑒 𝜔 = 𝑟𝜌𝐴𝑛𝑜𝑧𝑧𝑙𝑒 𝛽𝑣𝑗2 − 2𝑣𝑗 𝑟 2 𝜌𝐴 2 (From Thake [15]) 𝑘𝑏 𝑘 𝑇 + 𝑐 𝜔 + 𝑟 3 𝜌𝐴𝑛𝑜𝑧𝑧𝑙𝑒 𝛽𝜔2 𝑛𝑜𝑧𝑧𝑙𝑒 𝛽 + 𝑅𝐿 + 𝑅𝑎 21 Experimental Set-up The model was validated by simulating a raised reservoir using a fluid bench and pump 22 Model Validation 6, 8, 10, 12, and 16 mm nozzles tested Model accurate within 7% of results on average for 10 and 12 mm nozzles Accounting for loss due to air resistance and the support bearing brings model within 6% of results 1.2 × 10−3 Ns/m added to damping coefficient Smaller and larger nozzles less accurate: 27% average for 6 and 8 mm 14% average for 16 mm 23 Experimental Results Measured efficiency up to about 40% power output ( total kinetic jet power ) 10 mm nozzle Flow rate of 15.8 GPM Total hydraulic head of 10.4 m Max. Overall efficiency of about 32% power output ( ) power potential 24 Design of Experiments – What factors most significantly impact efficiency? Parameter Effect Gross head Flow rate Pipe diameter Frictional losses at pipe walls Pipe components Frictional losses due changes in flow direction Number of nozzles Total power input to turbine Nozzle geometry Flow rate, jet velocity Level Nozzle Size Motor Speed Load Water jet position Total power input to turbine 1 8 mm 40 Hz 35 Ω 2 10 mm 45 Hz 50 Ω Load on generator Induced torque on turbine 3 12 mm 50 Hz 65 Ω 25 Modeled efficiency for 250 W target with optimized load and nozzle diameter at 20, 30, and 40 m 26 Conclusions and Future Work Target of 1 kW power output may be difficult to achieve with great efficiency Expectation is that residence is grid-connected System is most cost effective by providing little power for a long time System could be implemented in poor or remote locations, especially where local topography permits low-cost installation of raised reservoir Further analysis and concurrent optimization of generator and turbine efficiency 27 References 1. 2. 3. 4. 5. 6. 7. 8. 9. 10. 11. 12. 13. 14. 15. Zimmerman, D. L., 2011. Residential Solar Energy in the Valley: A Feasibility Assessment and Carbon Mitigation (Master’s Thesis). Retrieved from James Madison University files database. http://www.jadoopower.com/storage.php?Energy-Storage-Solar-VRLA-Batteries-4 http://www.solarenergy.gen.in/ Nagel, J. K., (2012). Two-phase Energy System (Project proposal to Valley 25x’25). Source provided by Dr. Nagel. October 25, 2012. Basic Tutorials: Storage Batteries. http://www.freesunpower.com/batteries.php. Free Sun Power. October 25, 2012. Packing some power. http://www.economist.com/node/21548495?frsc=dg|a. The Economist. Levine, J. G., 2003. Pumped Hydroelectric Energy Storage and Spatial Diversity of Wind Resources as Methods of Improving Utilization of Renewable Energy Sources (Master’s Thesis). Retrieved from University of Colorado Boulder files database. http://large.stanford.edu/courses/2012/ph240/doshay1/ Young-Min K., Jange-Hee L., Seok-Jeon K., Favrat, D., 2012. Potential and Evolution of Compressed Air Energy Storage: Energy and Exergy Analyses. Entropy 14 (8), 1501-1521. http://www.pge.com/web/includes/images/about/environment/pge/cleanenergy/caes.jpg Williamson, S., Stark, B., Booker, J., 2014. Low head pico hydro turbine selection using a multi-criteria analysis. Renewable Energy 61, 43-50. http://images.cpbay.com/uploadfile/comimg/big/Runner-of-Francis-Turbine-200KW-271584.jpg Proczka, J., Muralidharan, K., Villela, D., Simmons, J., & Frantziskonis, G. (2013). Guidelines for the pressure and efficient sizing of pressure vessels for compressed air energy storage. Energy Conversion and Management, 65, 597605. Retrieved October 30, 2013, from the Science Direct database. Elmegaard, B., Brix, W. Efficiency of Compressed Air Energy Storage. Retrieved from http://orbit.dtu.dk/fedora/objects/orbit:72193/datastreams/file_6324034/content Thake, J., 2000. The Micro-hydro Pelton Turbine Manual. ITDG Publishing, London. 28