Outline. Solar Photovoltaic Applications. Midterm Problem One. Midterm Results. Midterm Problem Two. Midterm Problem One II
|
|
- Ruby Stanley
- 5 years ago
- Views:
Transcription
1 Photovoltaic Solar April 6, 010 Solar Photovoltaic Application Larry Cartto Mchanical Enginring 483 Altrnativ Enrgy Enginring II April 6, 010 Outlin Midtrm xam rult Mt on Wdnday at PPM Confrnc room for photovoltaic tour Photovoltaic baic Application of photovoltaic ytm Cot and cll fficinci Concluion Midtrm Rult Numbr of tudnt: 30 Maximum poibl cor: 90 Man: 43.8 Mdian: 43 Standard Dviation: Midtrm Problm On Givn: Spctral miivity Find: Solar radiation aborbd αolar = εolar = 0.88[ f ( λ = 0.88 Emiivity μm Wavlngth (μm) T = 0,300μm K) 0] + 0.4[ 1 f ( λt = 0,300μm K) ] ( ) + 0.4( ) = For 800 W/m incoming olar radiation th aborbd radiation i (0.8710)(800 W/m) = W/m. b. If th urfac i opaqu, what happn to th radiation that i not aborbd? It i rflctd. 4 Midtrm Problm On II c. What i th miiv powr of th urfac if it tmpratur i 340 K? α340 K = ε 340 K = 0.88[ f ( λt = 1,190 μm K) 0] [ 1 f ( λt = 1,190 μm K) ] = 0.88( ) + 0.4( ) = x10 W E = εσt = ( 0.413) ( 340K ) 4 E = 18.8 W/m 4 m K d. What i th total amount of radiant nrgy laving th urfac? It i um of th miiv powr, 18.8 W/m, plu rflctd nrgy, 800 W/m W/m = 103. W/m. Total radiant nrgy laving th urfac i 86.1 W/m. 5 Q top Midtrm Problm Two Givn: problm on urfac i aborbr plat in olar collctor at 340 K. Gla plat ha T = 30 K and ε = h gap = 3.5 W/m K. Find: hat tranfr, pr unit arabtwn th aborbr plat and th lowr gla plat? 4 4 Acσ ( ) ( TP Tg ) Qtop 3.5W = hp g Ac TP Tg + = ( 340 K 30 K ) Ac m K ε P ε g x10 W 4 4 [( 340 K ) ( 30 K ) ] 4 m K 107.8W + = m ME 483 Altrnativ Enrgy Enginring II 1
2 Photovoltaic Solar April 6, 010 Midtrm Problm Two II I Q in part a l than, gratr, than or qual to Q top? It i qual Find: hat tranfr cofficint, U P-g, btwn th aborbr plat and th lowr gla plat? Qtop 107.8W Qtop A c m 5.39W U P g = = = = A T T T T 340 K 30 K m c ( ) ( ) ( ) K P g P g I U P-g l than, gratr, than or qual to U top? It i gratr; it ha th am hat flow, Q top, with a mallr tmpratur diffrnc 7 Midtrm Problm Thr Givn: olar collctor rating ht. Find: fficincy for T in = 40 o C, I = 800 W/m and ambint tmpratur = 0 o C P P 0 0 η = = = 6.1% I I Find: T out for watr uing tt flow rat from ht and prviou data 1 Qu ηia c o m W o Tout = Tin + = Tin + = 40 C + = C mc & p mc & 3 p 48mL 1000kg m o m 10 ml kg C 800W ( 6.1% ) (.411m ) 8 Midtrm Problm Thr II Find: fraction of 90 thrm/month from collctor for olar radiation = 4 kwh/m /day for 30-day month with τα/(τα)n = 0.94, T a = 17.8 o C, and F R /F R = F R U c = ngativ lop = W/m o C and F R (τα)n = intrcpt = 0.715; 90 thrm/mo = (90x10 5 Btu/thrm)(1.055 k/btu)(g/10 6 k) = G/mo. H total = (30 day) (4 kwh/m /day) ( G/kWh) = 0.43 G/m /month. F R U c = (3.975 W/m o C)(10-9 G/W )(3600 /hr)(4 hr/day)(30 day/mo) = G/m /mo, 9 Midtrm Problm Thr III G mo o o ( T T ) = (.411m ) ( 0.97) ( 100 C 17.8 ) = ' F Δt X = A F U R c R c rf a C FR D m mo G ' F τα H, Y = A F ( τα) R i total c R n = FR ( τα) n D 0.43G (.411m ) ( 0.715)( 0.97)( 0.94) m mo = G mo f = 1.09Y 0.065X 0.45Y X Y 3 = 1.09(0.0715) 0.065(0.086) 0.45( ) (0.086) (0.0715) 3 = 5.89% of th monthly hating load i 10 upplid by olar Wdnday Cla Mting Mt in PPM Confrnc room Entranc from Lot C6 Nar cornr of Haltd and Etiwanda 11 Slid with NIST logo hown hr takn from thi prntation 1 ME 483 Altrnativ Enrgy Enginring II
3 Photovoltaic Solar April 6, 010 Cll in Modul in Array Solar cll Solar modul Solar array Baic Concpt Dirct convrion of light nrgy into lctrical currnt Bad on adorption of light photon with nrgy E = hν = hc/λ Planck contant: h = x10-3 Light pd: c = 99,79,458 m/ frquncy( -1 ) = ν wavlngth (m) = λ E = hν alo bai for pctrum of blackbody radiation 15 Smiconductor Conductor hav lot of fr lctron to conduct hat and lctricity Inulator hav almot no fr lctron Pur miconductor can produc om fr lctron laving lctrondficint atom known a hol Dopd miconductor add matrial with diffrnt numbr of valnc lctron 16 Smiconductor II Silicon ha 4 lctron in valnc band Adding phophoru with 5 lctron in it valanc band mak it air for th dopd matrial to rla fr lctron Thi i calld an n-typ matrial Adding aluminum with 3 lctron in it valanc band mak it air for th dopd matrial to produc hol Thi i calld a p-typ matrial 17 Smiconductor III oining n-typ and p-typ matrial rult in a pn junction Elctron and hol flow acro junction to rjoin Extrnal circuit i mor fficint mchanim for lctron to rjoin hol Solar cll i pn junction whr photon provid nrgy for lctron to bcom fr lctron 18 ME 483 Altrnativ Enrgy Enginring II 3
4 Photovoltaic Solar April 6, 010 Smiconductor to Solar Cll Phyic of olid viualiz valanc band whr lctron ar linkd to atom and conduction band for fr lctron Fr lctron hav highr nrgy Band gap i nrgy diffrnc btwn valanc band and conduction band Photon from unlight mut hav nough nrgy to mov lctron from valanc to conduction band 19 Silicon Band Gap = 1.11 V E = 1.11 V = hc/λ giv λ = 1.1 μm L nrgtic photon (λ > 1.1 μm) will not rla an lctron Highr nrgy photon (λ < 1.1 μm) will rla lctron and produc hat Radiant nrgy not rlaing lctron will b rflctd or aborbd For λt (1.1 μm)(5800 K) = μm K olar fraction i 77.5% (not all ud) 0 Link to Dmo olarcll/javaolarcllfigur1.jpg 1 Solar Cll Currnt Dnity L = + o o S Hodg pp 31-3 for drivation Currnt dnity L = I L /A dlivrd to load Intrnal currnt dniti acro p-n junction: p-to-n, 0, and n-to-p, r, nt j = r o Cll output currnt dnity ; L = j 0 = lctron charg = x10-19 /V k = Boltzmann contant = 1.381x10-3 /K V = cll voltag Solar Cll Output L = 0 giv opn circuit voltag = + = 0 = L o o Voc 1 0 o V = 0 giv hort circuit currnt 00 L = + o o = + o o = L = + o o L o = 1+ o 3 Solar Cll Output II For givn opn circuit voltag, 0 and tmpratur, T, find 0 / 0 1 = 1 = 0 o oc + 1 U thi 0 / to plot L / vru V L o 1 = 1 1 = 1 oc ME 483 Altrnativ Enrgy Enginring II 4
5 Photovoltaic Solar April 6, 010 dp dv Solar Cll Powr P = I L V = L AV L 1 P = L AV = AV = AV 1 oc + 1 dp/dv = 0 giv P max V 0 1 = A1 + AV = A 0Voc 0Voc V Voc + 1 oc 0 0 oc P max dp max = P 1 = 0 dv Solv numrically Iload/Ihort circuit and P/Pmax Solar Cll Paramtr Currnt P/Pmax V at Pma I at Pmax for V Pmax = V at P max 5 V/V opn circuit ME 483 Altrnativ Enrgy Enginring II 5
6 Photovoltaic Solar April 6, ME 483 Altrnativ Enrgy Enginring II 6
7 Photovoltaic Solar April 6, 010 Photovoltaic Shipmnt 37 Modul Typ Crytallin ilicon from a wdg of ingl-crytal or polycrytallin ilicon Cat, thin-film, or ribbon Thin-film from layr of miconductor matrial, uch a amorphou ilicon (a- Si), cadmium tllurid (CdT), or coppr indium gallium lnid (CIGS) Concntrator u ln that gathr and concntrat unlight onto th cll 38 Typ of Modul Shippd Cll and Modul Cot From manufacturr urvy ME 483 Altrnativ Enrgy Enginring II 7
8 Photovoltaic Solar April 6, 010 SF Vally Photovoltaic Cot From Supply 5% of avrag 860 kwh/mo 1.49 kw (pak) 148 ft ara Cot $10,416 ($,531 aftr incntiv) $7000/kW(pak) for ntir ytm Saving $/month, $10,995 for 5 yar with 4%/yar cot incra Rturn on invtmnt = 9.3% with incntiv, 3.4% without incntiv ME 483 Altrnativ Enrgy Enginring II 8
9 Photovoltaic Solar April 6, 010 I Efficincy Important? Y and no Solar nrgy i fr What i cot pr quar mtr of olar photovoltaic cll? Solar cll cot mot xpniv Low fficincy, low cot could b bttr Auxiliary cot for tructur High fficincy will alway b bttr hr Organic Photovoltaic η < 6% Lowr cot than Silicon Liftim a fw 1000 hour Goal: 10% and 10,000 h Solar Concluion Promi of larg amount of pollutionfr nrgy with ignificant limitation Low nrgy flux rquir larg ara Cot for currnt olar matrial ar not jutifid by cot aving Solar pak match lctricity dmand and thrmal torag xtnd gnration tim Scinc of olar nrgy wll undrtood, but problm with prviou commrcial Still nd ignificant cot rduction to mak olar PV cot ffctiv x300_nit-organic-photovoltaic.jpg 51 5 ME 483 Altrnativ Enrgy Enginring II 9
Solid State Device Fundamentals
Solid Stat vic Fundamntal ES 345 Lctur Cour by landr M. Zaitv alandr.zaitv@ci.cuny.du Tl: 718 98 81 4101b Collg of Statn Iland / CUY p-n Junction p-n junction i a phyical contact of p- and n-typ miconductor.
More informationThe pn junction: 2 Current vs Voltage (IV) characteristics
Th pn junction: Currnt vs Voltag (V) charactristics Considr a pn junction in quilibrium with no applid xtrnal voltag: o th V E F E F V p-typ Dpltion rgion n-typ Elctron movmnt across th junction: 1. n
More informationExam 2 Thursday (7:30-9pm) It will cover material through HW 7, but no material that was on the 1 st exam.
Exam 2 Thursday (7:30-9pm) It will covr matrial through HW 7, but no matrial that was on th 1 st xam. What happns if w bash atoms with lctrons? In atomic discharg lamps, lots of lctrons ar givn kintic
More informationCalculation of electromotive force induced by the slot harmonics and parameters of the linear generator
Calculation of lctromotiv forc inducd by th lot harmonic and paramtr of th linar gnrator (*)Hui-juan IU (**)Yi-huang ZHANG (*)School of Elctrical Enginring, Bijing Jiaotong Univrity, Bijing,China 8++58483,
More informationStochastic Heating in RF capacitive discharges
Stochatic Hating in RF capacitiv dicharg PTSG Sminar Emi Kawamura Thr ar two main mchanim for hating lctron in RF capacitiv dicharg: ohmic and tochatic hating. Plama ritivity du to lctron-nutral colliion
More informationQuantitative Model of PV Cells The Illuminated Diode. G.R. Tynan UC San Diego MAE 119 Lecture Notes
Quantitativ Modl of PV Clls T Illuminatd Diod G.R. Tynan UC San Digo MAE 119 ctur Nots WE FOUND WHAT WE SEEK: JJ(V) Currnt Dnsity vs Voltag Across Diod: J total qdn p qd pn J + J kt ( xp( qv / ) 1) 0 0
More informationVoltage, Current, Power, Series Resistance, Parallel Resistance, and Diodes
Lctur 1. oltag, Currnt, Powr, Sris sistanc, Paralll sistanc, and Diods Whn you start to dal with lctronics thr ar thr main concpts to start with: Nam Symbol Unit oltag volt Currnt ampr Powr W watt oltag
More informationWhere k is either given or determined from the data and c is an arbitrary constant.
Exponntial growth and dcay applications W wish to solv an quation that has a drivativ. dy ky k > dx This quation says that th rat of chang of th function is proportional to th function. Th solution is
More informationPHYS ,Fall 05, Term Exam #1, Oct., 12, 2005
PHYS1444-,Fall 5, Trm Exam #1, Oct., 1, 5 Nam: Kys 1. circular ring of charg of raius an a total charg Q lis in th x-y plan with its cntr at th origin. small positiv tst charg q is plac at th origin. What
More informationMath 34A. Final Review
Math A Final Rviw 1) Us th graph of y10 to find approimat valus: a) 50 0. b) y (0.65) solution for part a) first writ an quation: 50 0. now tak th logarithm of both sids: log() log(50 0. ) pand th right
More informationINTRODUCTION TO AUTOMATIC CONTROLS INDEX LAPLACE TRANSFORMS
adjoint...6 block diagram...4 clod loop ytm... 5, 0 E()...6 (t)...6 rror tady tat tracking...6 tracking...6...6 gloary... 0 impul function...3 input...5 invr Laplac tranform, INTRODUCTION TO AUTOMATIC
More informationAtomic energy levels. Announcements:
Atomic nrgy lvls Announcmnts: Exam solutions ar postd. Problm solving sssions ar M3-5 and Tusday 1-3 in G-140. Will nd arly and hand back your Midtrm Exam at nd of class. http://www.colorado.du/physics/phys2170/
More informationLecture Outline. Skin Depth Power Flow 8/7/2018. EE 4347 Applied Electromagnetics. Topic 3e
8/7/018 Cours Instructor Dr. Raymond C. Rumpf Offic: A 337 Phon: (915) 747 6958 E Mail: rcrumpf@utp.du EE 4347 Applid Elctromagntics Topic 3 Skin Dpth & Powr Flow Skin Dpth Ths & Powr nots Flow may contain
More informationElectromagnetism Physics 15b
lctromagntism Physics 15b Lctur #8 lctric Currnts Purcll 4.1 4.3 Today s Goals Dfin lctric currnt I Rat of lctric charg flow Also dfin lctric currnt dnsity J Charg consrvation in a formula Ohm s Law vryon
More informationPhysics 312 First Pledged Problem Set
Physics 31 First Pldgd Problm St 1. Th ground stat of hydrogn is dscribd by th wavfunction whr a is th Bohr radius. (a) Comput th charg dnsity à (r) = 1 p ¼ µ 1 a 3 r=a ; ½ (r) = jã (r)j : and plot 4¼r
More informationHigh Energy Physics. Lecture 5 The Passage of Particles through Matter
High Enrgy Physics Lctur 5 Th Passag of Particls through Mattr 1 Introduction In prvious lcturs w hav sn xampls of tracks lft by chargd particls in passing through mattr. Such tracks provid som of th most
More informationPrinciples of Humidity Dalton s law
Principls of Humidity Dalton s law Air is a mixtur of diffrnt gass. Th main gas componnts ar: Gas componnt volum [%] wight [%] Nitrogn N 2 78,03 75,47 Oxygn O 2 20,99 23,20 Argon Ar 0,93 1,28 Carbon dioxid
More informationSupplementary Materials
6 Supplmntary Matrials APPENDIX A PHYSICAL INTERPRETATION OF FUEL-RATE-SPEED FUNCTION A truck running on a road with grad/slop θ positiv if moving up and ngativ if moving down facs thr rsistancs: arodynamic
More informationSeebeck and Peltier Effects
Sbck and Pltir Effcts Introduction Thrmal nrgy is usually a byproduct of othr forms of nrgy such as chmical nrgy, mchanical nrgy, and lctrical nrgy. Th procss in which lctrical nrgy is transformd into
More informationTitle: Vibrational structure of electronic transition
Titl: Vibrational structur of lctronic transition Pag- Th band spctrum sn in th Ultra-Violt (UV) and visibl (VIS) rgions of th lctromagntic spctrum can not intrprtd as vibrational and rotational spctrum
More informationCS 152 Computer Architecture and Engineering
CS 152 Computr Architctur and Enginring Lctur 11 VLSI I 2005-2-22 John Lazzaro (www.cs.brkly.du/~lazzaro) TAs: Td Hong and David Marquardt www-inst.cs.brkly.du/~cs152/ Last Tim: Piplin Hazard Rsolution
More informationEngineering Differential Equations Practice Final Exam Solutions Fall 2011
9.6 Enginring Diffrntial Equation Practic Final Exam Solution Fall 0 Problm. (0 pt.) Solv th following initial valu problm: x y = xy, y() = 4. Thi i a linar d.. bcau y and y appar only to th firt powr.
More information[ ] 1+ lim G( s) 1+ s + s G s s G s Kacc SYSTEM PERFORMANCE. Since. Lecture 10: Steady-state Errors. Steady-state Errors. Then
SYSTEM PERFORMANCE Lctur 0: Stady-tat Error Stady-tat Error Lctur 0: Stady-tat Error Dr.alyana Vluvolu Stady-tat rror can b found by applying th final valu thorm and i givn by lim ( t) lim E ( ) t 0 providd
More informationorbiting electron turns out to be wrong even though it Unfortunately, the classical visualization of the
Lctur 22-1 Byond Bohr Modl Unfortunatly, th classical visualization of th orbiting lctron turns out to b wrong vn though it still givs us a simpl way to think of th atom. Quantum Mchanics is ndd to truly
More informationDetermination of Vibrational and Electronic Parameters From an Electronic Spectrum of I 2 and a Birge-Sponer Plot
5 J. Phys. Chm G Dtrmination of Vibrational and Elctronic Paramtrs From an Elctronic Spctrum of I 2 and a Birg-Sponr Plot 1 15 2 25 3 35 4 45 Dpartmnt of Chmistry, Gustavus Adolphus Collg. 8 Wst Collg
More information2. Background Material
S. Blair Sptmbr 3, 003 4. Background Matrial Th rst of this cours dals with th gnration, modulation, propagation, and ction of optical radiation. As such, bic background in lctromagntics and optics nds
More informationQuantitative Model of Unilluminated Diode part II. G.R. Tynan UC San Diego MAE 119 Lecture Notes
Quantitativ Modl of Unilluminatd Diod part II G.R. Tynan UC San Digo MAE 119 Lctur Nots Minority Carrir Dnsity at dg of quasinutral rgion incrass EXPONENTIALLY forward bias p nb n pa = p n0 xp qv a kt
More informationElectrochemistry L E O
Rmmbr from CHM151 A rdox raction in on in which lctrons ar transfrrd lctrochmistry L O Rduction os lctrons xidation G R ain lctrons duction W can dtrmin which lmnt is oxidizd or rducd by assigning oxidation
More informationDefinition1: The ratio of the radiation intensity in a given direction from the antenna to the radiation intensity averaged over all directions.
Dirctivity or Dirctiv Gain. 1 Dfinition1: Dirctivity Th ratio of th radiation intnsity in a givn dirction from th antnna to th radiation intnsity avragd ovr all dirctions. Dfinition2: Th avg U is obtaind
More informationph People Grade Level: basic Duration: minutes Setting: classroom or field site
ph Popl Adaptd from: Whr Ar th Frogs? in Projct WET: Curriculum & Activity Guid. Bozman: Th Watrcours and th Council for Environmntal Education, 1995. ph Grad Lvl: basic Duration: 10 15 minuts Stting:
More informationElectrochemical Energy Systems Spring 2014 MIT, M. Z. Bazant. Midterm Exam
10.66 Elctrochmical Enrgy Systms Spring 014 MIT, M. Z. Bazant Midtrm Exam Instructions. This is a tak-hom, opn-book xam du in Lctur. Lat xams will not b accptd. You may consult any books, handouts, or
More informationExam 1. It is important that you clearly show your work and mark the final answer clearly, closed book, closed notes, no calculator.
Exam N a m : _ S O L U T I O N P U I D : I n s t r u c t i o n s : It is important that you clarly show your work and mark th final answr clarly, closd book, closd nots, no calculator. T i m : h o u r
More informationA central nucleus. Protons have a positive charge Electrons have a negative charge
Atomic Structur Lss than ninty yars ago scintists blivd that atoms wr tiny solid sphrs lik minut snookr balls. Sinc thn it has bn discovrd that atoms ar not compltly solid but hav innr and outr parts.
More informationVntilation 4 Natural Vntilation Vladimír Zmrhal (room no. 814) http://ur.f.cvut.cz/~zmrhavla/indx.htm Útav tchniky protřd dí 1 Natural vntilation Th air flow i drivn by prur diffrnc acro th building nvlop.
More information22/ Breakdown of the Born-Oppenheimer approximation. Selection rules for rotational-vibrational transitions. P, R branches.
Subjct Chmistry Papr No and Titl Modul No and Titl Modul Tag 8/ Physical Spctroscopy / Brakdown of th Born-Oppnhimr approximation. Slction ruls for rotational-vibrational transitions. P, R branchs. CHE_P8_M
More informationBrief Introduction to Statistical Mechanics
Brif Introduction to Statistical Mchanics. Purpos: Ths nots ar intndd to provid a vry quick introduction to Statistical Mchanics. Th fild is of cours far mor vast than could b containd in ths fw pags.
More informationRadiation Physics Laboratory - Complementary Exercise Set MeBiom 2016/2017
Th following qustions ar to b answrd individually. Usful information such as tabls with dtctor charactristics and graphs with th proprtis of matrials ar availabl in th cours wb sit: http://www.lip.pt/~patricia/fisicadaradiacao.
More informationWhy is a E&M nature of light not sufficient to explain experiments?
1 Th wird world of photons Why is a E&M natur of light not sufficint to xplain xprimnts? Do photons xist? Som quantum proprtis of photons 2 Black body radiation Stfan s law: Enrgy/ ara/ tim = Win s displacmnt
More informationIntroduction to Condensed Matter Physics
Introduction to Condnsd Mattr Physics pcific hat M.P. Vaughan Ovrviw Ovrviw of spcific hat Hat capacity Dulong-Ptit Law Einstin modl Dby modl h Hat Capacity Hat capacity h hat capacity of a systm hld at
More information(1) Then we could wave our hands over this and it would become:
MAT* K285 Spring 28 Anthony Bnoit 4/17/28 Wk 12: Laplac Tranform Rading: Kohlr & Johnon, Chaptr 5 to p. 35 HW: 5.1: 3, 7, 1*, 19 5.2: 1, 5*, 13*, 19, 45* 5.3: 1, 11*, 19 * Pla writ-up th problm natly and
More informationLast time. Resistors. Circuits. Question. Quick Quiz. Quick Quiz. ( V c. Which bulb is brighter? A. A B. B. C. Both the same
Last tim Bgin circuits Rsistors Circuits Today Rsistor circuits Start rsistor-capacitor circuits Physical layout Schmatic layout Tu. Oct. 13, 2009 Physics 208 Lctur 12 1 Tu. Oct. 13, 2009 Physics 208 Lctur
More informationPart 7: Capacitance And Capacitors
Part 7: apacitanc And apacitors 7. Elctric harg And Elctric Filds onsidr a pair of flat, conducting plats, arrangd paralll to ach othr (as in figur 7.) and sparatd by an insulator, which may simply b air.
More informationAn Inventory Model with Change in Demand Distribution
Autralian Journal of Baic and Applid cinc, 5(8): 478-488, IN 99-878 An Invntory Modl with Chang in Dmand Ditribution P.. hik Uduman,. rinivaan, 3 Dowlath Fathima and 4 athyamoorthy, R. Aociat Profor, H.O.D
More informationOutline. Heat Exchangers. Heat Exchangers. Compact Heat Exchangers. Compact Heat Exchangers II. Heat Exchangers April 18, ME 375 Heat Transfer 1
Hat Exangr April 8, 007 Hat Exangr Larry artt Manial Engrg 375 Hat ranfr April 8, 007 Outl Bai ida f at xangr Ovrall at tranfr ffiint Lg-man tmpratur diffrn mtd Efftivn NU mtd ratial nidratin Hat Exangr
More informationOptoelectronics EE/OPE 451, OPT 444 Fall 2009 Section 1: T/Th 9:30 10:55 PM
Optolctronics EE/OPE 451, OPT 444 Fall 009 Sction 1: T/Th 9:30 10:55 PM John D. Williams, Ph.D. Dpartmnt of Elctrical and Computr Enginring 406 Optics uilding UAHuntsvill, Huntsvill, AL 35899 Ph. (56)
More information2. Laser physics - basics
. Lasr physics - basics Spontanous and stimulatd procsss Einstin A and B cofficints Rat quation analysis Gain saturation What is a lasr? LASER: Light Amplification by Stimulatd Emission of Radiation "light"
More informationSpatial channeling of energy and momentum of energetic ions by destabilized Alfvén eigenmodes
Spatial channling of nrgy and momntum of nrgtic ions by dstabilizd Alfvén ignmods Ya.I. Kolsnichnko 1,V.V. Lutsnko 1, R.B. Whit, Yu.V. Yakovnko 1 1 Institut for Nuclar Rsarch, Kyiv, Ukrain Princton Plasma
More informationOptoelectronics EE/OPE 451, OPT 444 Fall 2009 Section 1: T/Th 9:30-10:55 PM
Optolctronics EE/OPE 451, OPT 444 Fall 2009 Sction 1: T/Th 9:30-10:55 PM John D. illiams, Ph.D. Dpartmnt of Elctrical and Computr Enginring 406 Optics Building - UAHuntsvill, Huntsvill, AL 35899 Ph. (256)
More informationPair (and Triplet) Production Effect:
Pair (and riplt Production Effct: In both Pair and riplt production, a positron (anti-lctron and an lctron (or ngatron ar producd spontanously as a photon intracts with a strong lctric fild from ithr a
More informationSeptember 23, Honors Chem Atomic structure.notebook. Atomic Structure
Atomic Structur Topics covrd Atomic structur Subatomic particls Atomic numbr Mass numbr Charg Cations Anions Isotops Avrag atomic mass Practic qustions atomic structur Sp 27 8:16 PM 1 Powr Standards/ Larning
More informationOptics and Non-Linear Optics I Non-linear Optics Tutorial Sheet November 2007
Optics and Non-Linar Optics I - 007 Non-linar Optics Tutorial Sht Novmbr 007 1. An altrnativ xponntial notion somtims usd in NLO is to writ Acos (") # 1 ( Ai" + A * $i" ). By using this notation and substituting
More informationPHA 5127 Answers Homework 2 Fall 2001
PH 5127 nswrs Homwork 2 Fall 2001 OK, bfor you rad th answrs, many of you spnt a lot of tim on this homwork. Plas, nxt tim if you hav qustions plas com talk/ask us. Thr is no nd to suffr (wll a littl suffring
More informationMath-3. Lesson 5-6 Euler s Number e Logarithmic and Exponential Modeling (Newton s Law of Cooling)
Math-3 Lsson 5-6 Eulr s Numbr Logarithmic and Eponntial Modling (Nwton s Law of Cooling) f ( ) What is th numbr? is th horizontal asymptot of th function: 1 1 ~ 2.718... On my 3rd submarin (USS Springfild,
More informationCh. 24 Molecular Reaction Dynamics 1. Collision Theory
Ch. 4 Molcular Raction Dynamics 1. Collision Thory Lctur 16. Diffusion-Controlld Raction 3. Th Matrial Balanc Equation 4. Transition Stat Thory: Th Eyring Equation 5. Transition Stat Thory: Thrmodynamic
More informationElements of Statistical Thermodynamics
24 Elmnts of Statistical Thrmodynamics Statistical thrmodynamics is a branch of knowldg that has its own postulats and tchniqus. W do not attmpt to giv hr vn an introduction to th fild. In this chaptr,
More informationContemporary, atomic, nuclear, and particle physics
Contmporary, atomic, nuclar, and particl physics 1 Blackbody radiation as a thrmal quilibrium condition (in vacuum this is th only hat loss) Exampl-1 black plan surfac at a constant high tmpratur T h is
More informationImpedance Transformation and Parameter Relations
8/1/18 Cours nstructor Dr. Raymond C. Rumpf Offic: A 337 Phon: (915) 747 6958 E Mail: rcrumpf@utp.du EE 4347 Applid Elctromagntics Topic 4 mpdanc Transformation and Paramtr Rlations mpdanc Ths Transformation
More informationUniversity of Illinois at Chicago Department of Physics. Thermodynamics & Statistical Mechanics Qualifying Examination
Univrsity of Illinois at Chicago Dpartmnt of hysics hrmodynamics & tatistical Mchanics Qualifying Eamination January 9, 009 9.00 am 1:00 pm Full crdit can b achivd from compltly corrct answrs to 4 qustions.
More informationChemical Physics II. More Stat. Thermo Kinetics Protein Folding...
Chmical Physics II Mor Stat. Thrmo Kintics Protin Folding... http://www.nmc.ctc.com/imags/projct/proj15thumb.jpg http://nuclarwaponarchiv.org/usa/tsts/ukgrabl2.jpg http://www.photolib.noaa.gov/corps/imags/big/corp1417.jpg
More informationLecture 18 - Semiconductors - continued
Lctur 18 - Smiconductors - continud Lctur 18: Smiconductors - continud (Kittl C. 8) + a - Donors and accptors Outlin Mor on concntrations of lctrons and ols in Smiconductors Control of conductivity by
More informationHuman vision is determined based on information theory:
Human vision is dtrmind basd on information thory: Supplmntary Information Alfonso Dlgado-Bonal,2 and F. Javir Martn Torrs,3 [] Instituto Andaluz d Cincias d la Tirra CSIC-UGR, Avda. d Las Palmras n 4,
More informationContinuous probability distributions
Continuous probability distributions Many continuous probability distributions, including: Uniform Normal Gamma Eponntial Chi-Squard Lognormal Wibull EGR 5 Ch. 6 Uniform distribution Simplst charactrizd
More informationChapter 4. It s all about e -
Chatr 4 Major Goal of Chatr 4:. Fining th xact location (hom) for th lctron in an atom 2. Dicu hyical an chmical xrimntal vinc which uort a) lctronic tructur & b) th rioic trn in th rorti of atom. Bfor
More informationElectric (Rocket) Propulsion. EP Overview
Elctric (Rockt) Propulsion EP Ovrviw Elctric Propulsion-1 Basics Rockt Propulsion Elmnts Propllant Enrgy Sourc Storag Fd Systm sam in chmical rockts Storag Convrsion Acclrator Elctric Propulsion- 1 Elctric
More informationPHYS-333: Problem set #2 Solutions
PHYS-333: Problm st #2 Solutions Vrsion of March 5, 2016. 1. Visual binary 15 points): Ovr a priod of 10 yars, two stars sparatd by an angl of 1 arcsc ar obsrvd to mov through a full circl about a point
More informationMCB137: Physical Biology of the Cell Spring 2017 Homework 6: Ligand binding and the MWC model of allostery (Due 3/23/17)
MCB37: Physical Biology of th Cll Spring 207 Homwork 6: Ligand binding and th MWC modl of allostry (Du 3/23/7) Hrnan G. Garcia March 2, 207 Simpl rprssion In class, w drivd a mathmatical modl of how simpl
More informationMultiple Short Term Infusion Homework # 5 PHA 5127
Multipl Short rm Infusion Homwork # 5 PHA 527 A rug is aministr as a short trm infusion. h avrag pharmacokintic paramtrs for this rug ar: k 0.40 hr - V 28 L his rug follows a on-compartmnt boy mol. A 300
More informationBasics about radiative transfer
aic about radiativ tranfr runo Carli Day Lctur aic about radiativ tranfr - runo Carli Tabl of Contnt Th radiativ tranfr quation. Th radiativ tranfr quation in a impl ca Analytical olution of th intgral
More informationREGISTER!!! The Farmer and the Seeds (a parable of scientific reasoning) Class Updates. The Farmer and the Seeds. The Farmer and the Seeds
How dos light intract with mattr? And what dos (this say about) mattr? REGISTER!!! If Schrödingr s Cat walks into a forst, and no on is around to obsrv it, is h rally in th forst? sourc unknown Phys 1010
More informationCompact Polymeric Optical Attenuator Using Laser Writing Asymmetric Y-Junction
Compact Polymric Optical Attnuator Uing Lar Writing Aymmtric Y-Junction Alok K Da a, H.P.Chan b a Elctronic and Tl-Communication Enginring Dpartmnt, Jadavpur Univrity, Calcutta-700 032, INDIA, -mail: alok_kumar_da@yahoo.com
More informationPipe flow friction, small vs. big pipes
Friction actor (t/0 t o pip) Friction small vs larg pips J. Chaurtt May 016 It is an intrsting act that riction is highr in small pips than largr pips or th sam vlocity o low and th sam lngth. Friction
More informationConstants and Conversions:
EXAM INFORMATION Radial Distribution Function: P 2 ( r) RDF( r) Br R( r ) 2, B is th normalization constant. Ordr of Orbital Enrgis: Homonuclar Diatomic Molculs * * * * g1s u1s g 2s u 2s u 2 p g 2 p g
More informationAPP-IV Introduction to Astro-Particle Physics. Maarten de Jong
APP-IV Introduction to Astro-Particl Physics Maartn d Jong 1 cosmology in a nut shll Hubbl s law cosmic microwav background radiation abundancs of light lmnts (H, H, ) Hubbl s law (199) 1000 vlocity [km/s]
More informationChapter 8: Electron Configurations and Periodicity
Elctron Spin & th Pauli Exclusion Principl Chaptr 8: Elctron Configurations and Priodicity 3 quantum numbrs (n, l, ml) dfin th nrgy, siz, shap, and spatial orintation of ach atomic orbital. To xplain how
More informationSAFE HANDS & IIT-ian's PACE EDT-15 (JEE) SOLUTIONS
It is not possibl to find flu through biggr loop dirctly So w will find cofficint of mutual inductanc btwn two loops and thn find th flu through biggr loop Also rmmbr M = M ( ) ( ) EDT- (JEE) SOLUTIONS
More informationModule 8 Non equilibrium Thermodynamics
Modul 8 Non quilibrium hrmodynamics ctur 8.1 Basic Postulats NON-EQUIIRIBIUM HERMODYNAMICS Stady Stat procsss. (Stationary) Concpt of ocal thrmodynamic qlbm Extnsiv proprty Hat conducting bar dfin proprtis
More informationSearch sequence databases 3 10/25/2016
Sarch squnc databass 3 10/25/2016 Etrm valu distribution Ø Suppos X is a random variabl with probability dnsity function p(, w sampl a larg numbr S of indpndnt valus of X from this distribution for an
More informationDavisson Germer experiment Announcements:
Davisson Grmr xprimnt Announcmnts: Homwork st 7 is du Wdnsday. Problm solving sssions M3-5, T3-5. Th 2 nd midtrm will b April 7 in MUEN E0046 at 7:30pm. BFFs: Davisson and Grmr. Today w will go ovr th
More informationCollisionless anisotropic electron heating and turbulent transport in coronal flare loops
Collisionlss anisotropic lctron hating and turbulnt transport in coronal flar loops K.-W. L and J. Büchnr 5 April 2011 Outlin: 1. HXR obsrvation and standard flar modl 2. Linar stability analysis (multi-fluid
More informationNARAYANA I I T / P M T A C A D E M Y. C o m m o n P r a c t i c e T e s t 1 6 XII STD BATCHES [CF] Date: PHYSIS HEMISTRY MTHEMTIS
. (D). (A). (D). (D) 5. (B) 6. (A) 7. (A) 8. (A) 9. (B). (A). (D). (B). (B). (C) 5. (D) NARAYANA I I T / P M T A C A D E M Y C o m m o n P r a c t i c T s t 6 XII STD BATCHES [CF] Dat: 8.8.6 ANSWER PHYSIS
More informationSCALING OF SYNCHROTRON RADIATION WITH MULTIPOLE ORDER. J. C. Sprott
SCALING OF SYNCHROTRON RADIATION WITH MULTIPOLE ORDER J. C. Sprott PLP 821 Novmbr 1979 Plasma Studis Univrsity of Wisconsin Ths PLP Rports ar informal and prliminary and as such may contain rrors not yt
More informationFr Carrir : Carrir onntrations as a funtion of tmpratur in intrinsi S/C s. o n = f(t) o p = f(t) W will find that: n = NN i v g W want to dtrmin how m
MS 0-C 40 Intrinsi Smiondutors Bill Knowlton Fr Carrir find n and p for intrinsi (undopd) S/Cs Plots: o g() o f() o n( g ) & p() Arrhnius Bhavior Fr Carrir : Carrir onntrations as a funtion of tmpratur
More informationIVE(TY) Department of Engineering E&T2520 Electrical Machines 1 Miscellaneous Exercises
TRANSFORMER Q1 IE(TY) Dpartmnt of Enginring E&T50 Elctrical Machins 1 Miscllanous Exrciss Q Q3 A singl phas, 5 ka, 0/440, 60 Hz transformr gav th following tst rsults. Opn circuit tst (440 sid opn): 0
More informationMAE 110A. Homework 4: Solutions 10/27/2017
MAE 0A Homwork 4: Solution 0/27/207 MS 4.20: Th figur blow provid tady-tat data for watr vapor flowing through a piping configuration. At ach xit, th volumtric flow rat, prur, and tmpratur ar qual. Dtrmin
More informationElectronic Supplementary Information (ESI)
Elctronic Supplmntary Matrial (ESI) for RSC Advancs. This journal is Th Royal Socity of Chmistry 2015 Elctronic Supplmntary Information (ESI) Bouqut-lik calcium sulfat dihydrat: a highly fficint adsorbnt
More informationY 0. Standing Wave Interference between the incident & reflected waves Standing wave. A string with one end fixed on a wall
Staning Wav Intrfrnc btwn th incint & rflct wavs Staning wav A string with on n fix on a wall Incint: y, t) Y cos( t ) 1( Y 1 ( ) Y (St th incint wav s phas to b, i.., Y + ral & positiv.) Rflct: y, t)
More informationDetailed analysis of the energy yield of systems with covered sheet-and-tube PVT collectors
Availabl onlin at www.scincdirct.com Solar Enrgy 84 (2010) 867 878 www.lsvir.com/locat/solnr Dtaild analysis of nrgy yild of systms wi covrd sht-and-tub PVT collctors R. Santbrgn a, C.C.M. Rindt a, *,
More informationDerivation of Electron-Electron Interaction Terms in the Multi-Electron Hamiltonian
Drivation of Elctron-Elctron Intraction Trms in th Multi-Elctron Hamiltonian Erica Smith Octobr 1, 010 1 Introduction Th Hamiltonian for a multi-lctron atom with n lctrons is drivd by Itoh (1965) by accounting
More informationde/dx Effectively all charged particles except electrons
de/dx Lt s nxt turn our attntion to how chargd particls los nrgy in mattr To start with w ll considr only havy chargd particls lik muons, pions, protons, alphas, havy ions, Effctivly all chargd particls
More informationSPH4U Electric Charges and Electric Fields Mr. LoRusso
SPH4U lctric Chargs an lctric Fils Mr. LoRusso lctricity is th flow of lctric charg. Th Grks first obsrv lctrical forcs whn arly scintists rubb ambr with fur. Th notic thy coul attract small bits of straw
More informationElectrons and Conductors
Elctrons and Conductors Atoms consist primarily of lctrons, protons, and nutrons. A modifid Bohr modl of th atom is shown blow. nuclus composd of a clustr of protons and nutrons orbital lctrons lctron
More informationPhysics 43 HW #9 Chapter 40 Key
Pysics 43 HW #9 Captr 4 Ky Captr 4 1 Aftr many ours of dilignt rsarc, you obtain t following data on t potolctric ffct for a crtain matrial: Wavlngt of Ligt (nm) Stopping Potntial (V) 36 3 4 14 31 a) Plot
More informationText: WMM, Chapter 5. Sections , ,
Lcturs 6 - Continuous Probabilit Distributions Tt: WMM, Chaptr 5. Sctions 6.-6.4, 6.6-6.8, 7.-7. In th prvious sction, w introduc som of th common probabilit distribution functions (PDFs) for discrt sampl
More informationAlpha and beta decay equation practice
Alpha and bta dcay quation practic Introduction Alpha and bta particls may b rprsntd in quations in svral diffrnt ways. Diffrnt xam boards hav thir own prfrnc. For xampl: Alpha Bta α β alpha bta Dspit
More informationHow can I control light? (and rule the world?)
How can I control light? (and rul th world?) "You know, I hav on simpl rqust. And that is to hav sharks with frickin' lasr bams attachd to thir hads! - Dr. Evil Phys 230, Day 35 Qustions? Spctra (colors
More informationFinite element discretization of Laplace and Poisson equations
Finit lmnt discrtization of Laplac and Poisson quations Yashwanth Tummala Tutor: Prof S.Mittal 1 Outlin Finit Elmnt Mthod for 1D Introduction to Poisson s and Laplac s Equations Finit Elmnt Mthod for 2D-Discrtization
More informationSolutions to Supplementary Problems
Solution to Supplmntary Problm Chaptr 5 Solution 5. Failur of th tiff clay occur, hn th ffctiv prur at th bottom of th layr bcom ro. Initially Total ovrburn prur at X : = 9 5 + = 7 kn/m Por atr prur at
More informationChapter 6 Current and Resistance
Chaptr 6 Currnt and Rsistanc 6.1 Elctric Currnt... 1 6.1.1 Currnt Dnsity... 1 6. Ohm s Law... 3 6.3 Elctrical Enrgy and Powr... 6 6.4 Summary... 6.5 Solvd Problms... 8 6.5.1 Rsistivity of a Cabl... 8 6.5.
More informationExploitation of density of states and mobility difference between holes and electrons for high efficiency solar cells
Exloitation of dity of stats and mobility diffrnc btwn hols and lctro for high fficincy solar clls KEE HME PVE*, M. REZW KH** *artmnt of Comutr Scinc and Enginring East Wst Univrsity, haka, Bangladsh **artmnt
More informationHigher order derivatives
Robrto s Nots on Diffrntial Calculus Chaptr 4: Basic diffrntiation ruls Sction 7 Highr ordr drivativs What you nd to know alrady: Basic diffrntiation ruls. What you can larn hr: How to rpat th procss of
More information