Review of Lecture 8 IT M n, o e • Blackbody function h lt C g r ma • Earth motion n a he n G • Solar spectra: AM0, AM1, io etc. © lar/TAM1.5 s r t • Definition of rradiative ve gh t Soproperties i n o y ec ofCsolar • Maximumopefficiency thermal engines C Dir rgy 7 9achievable 7 ne temperature • Maximum 9 9 9 E . 2. a(frequency) l • 2 Wavelength selective surfaces r ric o F ct Ele Contents of lecture 9 T I ,M n e to h • Solar hot water systems C al g n er m • Maximum solar concentration a G /Th ion • Methods for©concentration t olar ers h • Nontracking S tracking nv rig ctand o y p thermal-mechanical • Solar o re gy C i C er 7 energy 7 Dconversion n 9 9 .9 wave l E calculation of surface 2.9 •r 2EM a tric Fo properties c Ele 1 Solar Hot Water Systems IT M , You Need? nArea How Much e to h of Water l • 80C Gallon a T =15 C •g Start temperature m r n • Hot water T =60 C e temperature h n GaEnergy io © lar/T Balance s r t gh t So nA v• Je • Δt •η = mc(T − T ) i r y ec CoΔt = 5.5 hours/day p heat c= 4180 J/kg.K Co Dir rgy Specific J =1000 W/m 7 97 ne Thermal efficiency η=60% 9 9 9 E . . l 2 r 2 ca A=5.1 m Fo ctri Ele o i o f s f i 2 s 2 http://78.136.49.147/images/Solar%20Hot%20Water%20Heating %20Diagram.gif Image by EERE. Flat Panel Solar Hot Water Heaters T I M n, o e h lt C a g m r n Ga /The ion t © olar ers h g nv o C Images removed due to copyright restrictions. Please also see: http://greennav.files.wordpress.com/2008/03/solar-panel.gif http://www.mdelectric.ca/1_Pictures/Green Energies/GE-ViessmannCollector.jpg http://collector-solar.com/products/index.htm Photo by szczel on Flickr. Figure by MIT OpenCourseWare. 2 Evacuated Tube Technology IT ,M n e to h l C a n g er m a G /Th ion t © olar ers h rig ct S onv y p ire C o y C D rg 7 7 ne 9 9 9 9 2. r 2. cal E Fo ctri Ele Images removed due to copyright restrictions. Please see: http://img.diytrade.com/cdimg/194777/1624552/0/1160536024/AllGlass_Evacuated_Solar_Collector_Tube-SFVA.jpg http://img.diytrade.com/cdimg/194777/1624568/0/1160536058/AllGlass_Evacuated_Solar_Collector_Tube-SFVB.jpg http://img.diytrade.com/cdimg/194777/1624573/0/1160536136/MetalGlass_Evacuated_Solar_Collector_Tube-SFVC.jpg http://www.diytrade.com/china/4/products/1716424/All-Glass_Evacuated_Solar_Collector_Tube-SFVA.html Vacuum Tube Hot Water HeatersT I M n, o e h lt C a g m r n Ga /The ion t © olar ers h rig ct S onv y p ire C o C D rgy 7 97 ne 9 9 2. r 2.9 cal E o tri Separate Tank Collector FUnpressurized c Ele Images removed due to copyright restrictions. Please see any photos of solar water heaters, such as: http://image.made-in-china.com/2f0j00ferESMmCAVoH/Solar-Collector.jpg http://image.made-in-china.com/2f0j00VBdtYnQhIaRE/Split-Pressurized-SolarWater-Heater-CY-SP-24-.jpg 3 Efficiency Estimation---Evacuated Tubes IT M Incoming Solar Radiation n, o e t Qin = Do • L • JCs h al rm ng Radiation AbsorbedaSolar e h on G T / Qa © = Di • Lr• J s • τs•iα t la ver h o S Loss D n rigRadiation t o y c p C 4 4 e Co Dir Qlossrg=yε (πDi L )σ [Ts − T a ] e Efficiency 7D 97 Thermal n 9 9 9 E 2. r 2. cal Q − Q o tri η = a loss = Di ⎛⎜⎜ατ − πεσ [ Ts4 − Ta4 ]⎞⎟⎟ F c J Qin Do ⎝ J s e ⎠ l E in o s Efficiency Estimation---Flat Panel T I ,M R T T T n e to h C al R R g R n erm Solar In a G /Th ion r rsσT © 4 a σTamht l g t So nve i r y R e=c d ≈ 10C×o10 = 0.38 [K/W] p o ir k Ay 0.026 A A C D ed rg 0.3×10 0.00025 d 7 7 9 .99 REn= k A ≈ 1.2 A = A [K/W] 9 . 2 r 2 cal 1 1 0.2 [K/W ] ≈ = R = i o r t hA 5 A A F c J d 3 ×10 0.3 Ele [K/W ] ≈ = R = i s am Thermal Insulation Air air2 g am air1 4 s −3 air 1 air −3 g g g air 2 s −2 i i ki A 0.1A A 4 Efficiency Estimation---Flat Panel IT M T − T T −T , Q = + en + εσoA[T − T ] hR l t R + R + R C a = 5.5 A[T − Tn]g+ εσA[Trm −T ] Ga /The ion t ©Efficiency Thermal lar vers h o rig ct S on y p irQea − QlossC o C ηD= Qrgy 7 97 ne in 9 9 2. r 2.9 cal =Eατ − 1.7[Ts − Tam ] − πεσ [Ts4 − Ta4 ] o tri Js Js F c J Ele am s s 4 s am loss air 2 s Thermal Insulation Air air 1 i g am 4 am 4 s 4 am s Estimated and Experimental Results IT Thermal Efficiency 0.9 0.8 0.7 0.6 0.5 0.4 0.3 0.2 0.1 0 ,M n e to h C al g n er m a G /Th ion © t olar ers h rig ct S onv y p ire C o C D rgy 7 97 ne 9 9 . 9 al E 2. Temperature 2 r c ( C) Fo ctri Ele 40 50 60 70 80 o http://www.enviro-friendly.com/images/NSWWinter-Solar-Efficiency-graph.jpg Courtesy of Hills Solar. Used with permission. 5 Total Renewable Capacity in 2007 I T M n, o e h lt C g r ma n Ga /The ion t © olar ers h rig ct S onv y p ire C o y C D rg 7 7 ne 9 9 9 9 2. r 2. cal E Fo ctri Ele Courtesy of IEA-SHC. Used with permission. Weiss et al., Solar Heat Worldwide, 2009 Ed. Solar Heat Utilization T I ,M n e to h C al g n er m a G /Th ion © t olar ers h rig ct S onv y p ire C o C D rgy 7 97 ne 9 9 2. r 2.9 cal E Fo ctri Ele Courtesy of IEA-SHC. Used with permission. Weiss et al., Solar Heat Worldwide, 2009 Ed. 6 Earth Orbital , g an Image by Robert Simmon (NASA). Sun rec er n E 1.27 x 107 m 7900 mi 109 m 5 1.39 x 8.64 x 10 mi 32' Solar constant Gsc Distance is { al c tri c e { Earth = 1367 W/m2 2 = 433 Btu/ft hr 2 = 4.92 MJ/m hr 1011 = 1.495 x m = 9.3 x 107 mi C la ver o S on yC March equinox Mar 20/21 June solstice Jun 21/22 Aphelion July 4 152,100,000 km Sun 147,300,000 km Perihelion January 3 December solstice Dec 21/22 1.7% September equinox Sept 22/23 Figure by MIT OpenCourseWare. Figure by MIT OpenCourseWare. Maximum Concentration of Sun Light---2nd Law Limit Energy Balance θs r R G © ht Sola t rm o rsi Concentration With 4eπr 2 J sn= 4πR 2 J e CJ e = σTc ≤ σTs4 = J s 4 2 Maximum concentration C max J ⎛R⎞ = s = ⎜ ⎟ Je ⎝ r ⎠ 1 = = 46,164 sin 2 θ s 7 Maximum Concentration of Sun Light---2nd Law Limit IT M n, o e h lt Inside a medium of C a= nσT g CJ m r n refractive index n Ga /The ion t © olar erCs = n h sin θ rig ct S onv y p C e Co Dir rgy 7 97 ne 9 9 2. r 2.9 cal E Achieved C=56,000 i o r F ct Ele 4 e c 2 max 2 Image removed due to copyright restrictions Please see Fig. 1a in Gleckman, Philip, Joseph O'Gallagher, and Roland Winston. "Concentration of Sunlight to Solar-surface Levels Using Non-imaging Optics." Nature 339 (1989): 198-200. Gleckman et al., Nature, 339, 198 (1989) θs Gθas θs Concave focusing mirror r D/2 rθs gh i r y D/2 op d/2 r C Di 7 97 n 9 9 . .9 al E ic Φ F I M , 2D FlatnPanel e o h d cos Φ 2 D r sin Φ = 2 r sin θ s = D sin Φ cos Φ sin 2Φ = = d sin θ s 2sin θ s Figure by MIT OpenCourseWare. 3D Concentration Cmax = 1 4sin 2 θ s Cmax = 1 = 107 2sin θ s 8 Imaging Concentration to Cylinder T , θsn e o t h l C a Concave θ g m r n focusing θs e a mirror r G h on D/2 T / r rsi © Φ a t l ghF t So nve i r rθ o y D/2 c p C e o r i y C D rg 7 7 ne C = (D/2 π r sin θ = sin φ / sin θ 9 9 1/π sin θ (1/π) C 9 9 2. r 2. cal E Fo c ri Ele s s s s s max Figure by MIT OpenCourseWare. From Fig.4.3: R. Winston et al., Nonimaging Optics, Elsevier, 2005 Nonimaging Optics T I , Mto Flat Plate 2D Concentration n e to h C+ ABa' =l A' B + BB' AC g m an her n T ' =siAo' B / r AB ht ola ver g i n yr ect CoAC = AA'sin θ p o r i C D 7 7 9 9 AA' 1 9 9 . 2. al = = C r c BB' sin θ Fo ctri 2 ⎛ 1 ⎞ Ele Maximum when θ=θ String Method C Edge ray Wave front W θ A' A Reflector profile B' B Figure by MIT OpenCourseWare. 3D Concentration C =⎜ ⎟ ⎝ sin θ ⎠ s 9 2D Concentration to Cylinder IT M n, o e h lt C g r ma n Ga /The ion t © olar ers h rig ct S onv y p ire C o y C D rg 7 7 ne 9 9 9 9 2. r 2. cal E Fo ctri Ele Winston and Hinterberger, Solar Energy, 17, 255 (1975) Courtesy of Elsevier, Inc., http://www.sciencedirect.com. Used with permission. 23.5o (22-24.5 o) g yri p Co D 7 7 .99 2.99 r Equator Winter Summer Images from Wikimedia Commons, http://commons.wikimedia.org Earth Orbital 10 Daily Insolation Variation IT M J also varies due n, toopath length e h lt C g r ma n Ga /The ion A t © olar ers h At Noon: Q=J A ig r c t S onv y p ire C o y Cθ D rg 7 7 ne 9 9 9 9 2. r 2. cal E Fo ctri EleA Js s s 45o North Latitude http://www.eoearth.org/article/Daily_a nd_annual_cycles_of_temperature Courtesy of Michael Pidwirny. Used with permission. Q= JsAsinθ Tracking T I ,M n e to h J C al g n er m θ a G /Th ion © t olar ers h v rig ct S onQ= y JA p ire C A o y C D rg Q= J Asinθ 7 7 ne θ 9 9 9 9 E 2. r 2. cal tri Axis: Axis Along South-North Direction Fo cOne Ele s s s 11 V-Trough IT M n, o e h lt C g r ma n Ga /The ion t © olar ers h rig ct S onv y p ire C o y C D rg 7 7 ne 9 9 9 9 2. r 2. cal E Fo ctri Ele • East-West Orientation, with seasonal adjustment: 2.5-3 times • South-North tracking Holland, Solar Energy, 13, 149 (1971) http://www.electricksolutions.com/cms/temp lates/electriksolutions/IMAGES/banner1.jpg Courtesy of Elsevier, Inc., http://www.sciencedirect.com. Used with permission. Solar Thermal Energy Conversion ---Mechanical Systems T I ,M n e to h C al g n er m a G /Th ion © t olar ers h rig ct S onv y p ire C o C D rgy 7 97 ne 9 9 2. r 2.9 cal E Fo ctri Ele Images by EERE. Please also see Fig. 21-13 in Kreith, Frank, and D. Yogi Goswami. Handbook of Energy Efficiency and Renewable Energy. Boca Raton, FL: CRC Press, 2007. Handbook of Energy Efficiency and Renewable Energy 12 Solar Trough IT M n, o e h lt C g r ma n Ga /The ion t © olar ers h rig ct S onv y p ire C o y C D rg 7 7 ne 9 9 9 9 2. r 2. cal E Fo ctri Ele Courtesy of Plataforma Solar de Almería. Used with permission. Solar Trough T I ,M n e to h C al g n er m a G /Th ion © t olar ers h rig ct S onv y p ire C o C D rgy 7 97 ne 9 9 2. r 2.9 cal E Fo ctri Ele Image removed due to copyright restrictions. Please see Fig. 5.16 in Kaltschmitt, Martin, Wolfgang Streicher, and Andreas Weise. Renewable Energy: Technology, Economics, and Environment. New York, NY: Springer, 2007. Also see any photo of a commercial HCE, such as Schott's PTR 70. 13 Solar Trough with Molten Salt Storage IT M n, o e h lt C g r ma n Ga /The ion t © olar ers h rig ct S onv y p ire C o y C D rg 7 7 ne 9 9 9 9 2. r 2. cal E Fo ctri Ele Courtesy of Elsevier, Inc., http://www.sciencedirect.com. Used with permission. Price, H. Lupfert, E.“Advances in Parabolic Trough Solar Power Technology” T I ,M n e to h C al g n er m a G /Th ion © t olar ers h rig ct S onv y p ire C o C D rgy 7 97 ne 9 9 2. r 2.9 cal E Fo ctri From J. Karni Ele Photos by EERE, Sandia National Labs. Image removed due to copyright restrictions. Please see any photo of a linear Fresnel lens system, such as http://commons.wikimedia. org/wiki/File:Fresnel_reflectors_ausra.jpg http://i.i.com.com/cnwk.1d/i/ne/p/2007/910 Ausra1_550x367.jpg Courtesy of Jacob Karni. Used with permission. 14 Solar Trough: Concentration Ratio IT M n, o e h lt C g r ma n Ga /The ion t © olar ers h rig ct S onv y p ire C o y C D rg 7 7 ne 9 9 9 9 2. r 2. cal E Fo ctri Ele Table removed due to copyright restrictions. Please see Table 2 in Price, Hank, et al. "Advances in Parabolic Trough Solar Power Technology." Journal of Solar Energy Engineering 124 (May 2002): 109-125. Price, H. Lupfert, E.“Advances in Parabolic Trough Solar Power Technology” Solar Trough: Cost T I ,M n e to h C al g n er m a G /Th ion © t olar ers h rig ct S onv y p ire C o C D rgy 7 97 ne 9 9 2. r 2.9 cal E Fo ctri Ele Table removed due to copyright restrictions. Please see Table 8 in Price, Hank, et al. "Advances in Parabolic Trough Solar Power Technology." Journal of Solar Energy Engineering 124 (May 2002): 109-125. Price, H. Lupfert, E.“Advances in Parabolic Trough Solar Power Technology” 15 Trough Efficiency IT M n, o e h lt C g r ma n Ga /The ion t © olar ers h rig ct S onv y p ire C o y C D rg 7 7 ne 9 9 9 9 2. r 2. cal E Fo ctri Ele “Assessment of Parabolic Trough and Power Tower Solar Technology Cost and Performance Forecasts” NREL, 2003 Trough Cost Breakdown T I ,M n e to h C al g n er m a G /Th ion © t olar ers h rig ct S onv y p ire C o C D rgy 7 97 ne 9 9 2. r 2.9 cal E Fo ctri Ele “Assessment of Parabolic Trough and Power Tower Solar Technology Cost and Performance Forecasts” NREL, 2003 16 Heliostat / Power Tower T I ,M n e to h C al g n erm a G /Th ion t © olar ers h rig ct S onv y p ire C o y 7 C 97 D nerg 9 2.9 r 2.9 al E Fo ctric Ele Photo by Koza1983 on Wikipedia. T I ,M n e to h C al g n er m a G /Th ion © t olar ers h rig ct S onv y p ire C o C D rgy 7 97 ne 9 9 2. r 2.9 cal E Fo ctri Ele Images by EERE and Sandia National Laboratory. Courtesy of Jacob Karni. Used with permission. From J. Karni 17 Heliostat Receiver IT M n, o e h lt C g r ma n Ga /The ion t © olar ers h rig ct S onv y p ire C o y C D rg 7 7 ne 9 9 9 9 2. r 2. cal E Fo ctri Ele Images removed due to copyright restrictions. Please see Fig. 21-49. 21-51, and Table 21-9 in Kreith, Frank, and D. Yogi Goswami. Handbook of Energy Efficiency and Renewable Energy. Boca Raton, FL: CRC Press, 2007. Handbook of Energy Efficiency and Renewable Energy Heliostat / Power Tower Cost T I ,M n e to h C al g n er m a G /Th ion © t olar ers h rig ct S onv y p ire C o C D rgy 7 97 ne 9 9 2. r 2.9 cal E Fo ctri Ele Image removed due to copyright restrictions. Please see Fig. 21-40 in Kreith, Frank, and D. Yogi Goswami. Handbook of Energy Efficiency and Renewable Energy. Boca Raton, FL: CRC Press, 2007. Handbook of Energy Efficiency and Renewable Energy 18 Heliostat / Power Tower Efficiency IT M n, o e h lt C g r ma n Ga /The ion t © olar ers h rig ct S onv y p ire C o y C D rg 7 7 ne 9 9 9 9 2. r 2. cal E Fo ctri Ele “Assessment of Parabolic Trough and Power Tower Solar Technology Cost and Performance Forecasts” NREL, 2003 Dish T I ,M n e to h C al g n er m a G /Th ion © t olar ers h rig ct S onv y p ire C o C D rgy 7 97 ne 9 9 2. r 2.9 cal E Fo ctri Ele Photo from Wikimedia Commons, http://commons.wikimedia.org 19 Dish and Stirling Engine IT M n, o e h lt C g r ma n Ga /The ion t © olar ers h rig ct S onv y p ire C o y C D rg 7 7 ne 9 9 9 9 2. r 2. cal E Fo ctri Ele Images removed due to copyright restrictions. Please see Fig. 5.20, 5.21, and 5.22 in Kaltschmitt, Martin, Wolfgang Streicher, and Andreas Weise. Renewable Energy: Technology, Economics, and Environment. New York, NY: Springer, 2007. Kaltschmitt, M.,Wolfgang, S. Wiese, A. “Renewable Energy, technology, Economics and Enviroment” Dish and Stirling Engine T I ,M n e to h C al g n er m a G /Th ion © t olar ers h rig ct S onv y p ire C o C D rgy 7 97 ne 9 9 2. r 2. 9 cal E Fo ctri Ele Table removed due to copyright restrictions. Please see Table 5.10 in Kaltschmitt, Martin, Wolfgang Streicher, and Andreas Weise. Renewable Energy: Technology, Economics, and Environment. New York, NY: Springer, 2007. Kaltschmitt, M.,Wolfgang, S. Wiese, A. “Renewable Energy, technology, Economics and Enviroment” 20 EM Waves IT M n, o e h Fieldl t E --- Electric Maxwell Equations: C a H ---gMagnetic Field m r n e Displacement aDB ------ Electric ∂B h Magnetic Induction n G ∇ × E = − TFree Current o / i --Density J r © s ∂t t ola er h v ig t S • Constitutive ∂D n r Relations o y + Je ∇ × H = c C e ∂t op D = ε E C Dir rgy 7= ρ e 97 ne ∇ •D 9 B = μH 9 2. r 2.9 cal E ε – Electric Permitivity ∇ •FBo= 0 tri μ – Magnetic permeability c e l E e EM Wave Propagation inside A Medium T I M , n E e to h • Plane Wave Solution C al g n ⎡erm⎛ N ˆ ⎞⎤ k a E(r,G t ) = E o exp Th⎢⎢⎣−siωio⎜⎜⎝ tn− co k • r ⎟⎟⎠⎥⎥⎦ / r © H ht Sola ve⎡ r g i yr ecHt (r, t )C= Honexp⎢− iω ⎛⎜⎜ t − cN k̂ • r ⎞⎟⎟⎤⎥ p ⎝ ⎠⎦ o ir ⎣ y ω--- angular frequency C g D r k --- Wavevector 7 97 n•ePoynting Vector (Energy Flux) 9 9 . Wavevector . 9 al E k̂ ---2Unit 2 1 r ric S (r ) = Re[E × H ] 4πκ o α= N=n+iκ, t 2 F c λ Complex refractive index Ele coefficient S = 1 n e E k̂ κ --- Extinction o o * −αx 2 μco o 2 Absorption Coefficient 21 EM Wave Reflection and Transmission at An Interface IT M • Snell Law n, h e l to θC =θ a g n sinrm n θ = n sin θ Ga /Th1 e ioi n 2 t s ar erCoefficients t © •olFresnel h rig ct S or n=vE = − n cosθ + n cosθ y p ire C E n cosθ + n cosθ Symbol Convention: o y C D rg E 2n cos θ Field Going Out of Paper 7 t = = 7 ne Field9Going Into9Paper E n cos θ + n cos θ 9 of Incidence: E l 2.9 Inrthe2.Plane E-Field a c i TM Wave = // Wave = p Wave o r t of Incidence: • Reflectivity/transmissivity F cPlane H-Field In the Re( N cos θ ) t τ = R =r Ele Ei kr n̂ Hi ki θi x θr Er i n1 r x n2 Et θt kt z // r 2 i 1 t // // i 2 i // t // // i TE Wave = Wave = s Wave t 1 2 i 2 // 1 i 1 2 // // t 2 t Re( N1 cos θ i ) // Examples T I ,M n e to h C al g n er m a G /Th ion © t olar ers h rig ct S onv y p ire C o C D rgy 7 97 ne 9 9 2. r 2.9 cal E tri as a function of the angle of incidence for a FoReflectivity c le material with n=4 and for gold with N=10.8+i51.6. Edielectric Gold (wavelength=10um, TE) 1 Gold (wavelength=10um, TM) REFLECTIVITY 0.8 Dielectric material (n=4, TE) 0.6 0.4 0.2 Dielectric material (n=4, TM) Brewster Angle 0 0 20 40 60 INCIDENT ANGLE 80 22 MIT OpenCourseWare http://ocw.mit.edu 2.997 Direct Solar/Thermal to Electrical Energy Conversion Technologies Fall 2009 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms.