Experience from PV system performence including comparison of on-roof and façade systems. (Case study on BIPV systems.)

Size: px
Start display at page:

Download "Experience from PV system performence including comparison of on-roof and façade systems. (Case study on BIPV systems.)"

Transcription

1 Expeience fom PV system pefomence including compaison of on-oof and façade systems. (Case study on BIPV systems.) Vitezslav Benda CTU Pague, Faculty of Electical Engineeing

2 Intelligent enegy management in the household Zeo enegy house cannot opeate without PV system

3 PV systems may be integated into building constuction PV system output powe depens on Iadiance Opeating tempeatue

4 ε v ϕ α β P ad ε h ) ( )cos ( cos ) ( ) ( sin 1 t t t B h v t ε ε ϕ = dt t t W h v t SS SR u ) ( )cos ( cos ) ( sin 1 ε ε ϕ = S J V Z , ,5

5 Radiation aiving on PV module Clea sky Cloudy sky inceases potion of diffuse adiation Reality:

6 In the yea 2001, a 3kW p demonstation, on-gid connected photovoltaic system has been built at the Czech Technical Univesity in Pague on the oof of the Faculty of Electical Engineeing.

7 Installed peak powe: 3320 W p Total module aea: 26 m 2 Numbe of modules: 30 (3 fields of 10) Latitude: N Altitude: 205 m

8 PV field Tilt angle Module type P m (W p ) 1 45 RADIX vaiable RADIX RADIX Paametes of individual PV fields Invetes: Fonius Sunice Mini

9 Enegy poduced by individual PV fields in peiod fom Januay 2002 to May 2009

10 A compaison of estimated and measued enegy poduction in peiod fom Januay 2002 to May 2007

11 Compaison of on-oof and façade PV field in the yea 2006

12 The module efficiency depends on iadiance and sola cell opeating tempeatue Both fill facto and efficiency decease with tempeatue FF T < 0 η < 0 T 1 At cystalline silicon cells % K η T η

13 Tempeatue dependece of enegy convesion efficiency Efficiency (%) 15,0 14,0 13,0 12,0 11,0 10,0 Tempeatue Efficiency 35,0 30,0 25,0 20,0 15,0 10,0 5,0 0,0 PV field tempeatue ( C) 9,0 Febuay Mach Apil May June July August Septembe Octobe Novembe -5,0 This gives the efficiency decease of about 0.6% pe 1K, which is highe than supposed decease of cell efficiency (about 0.4% pe 1K). It means that an incease of losses with inceasing tempeatue in othe pats of system cannot be neglected.

14 August Januay

15 PV modules ubbe sealing Cell opeating tempeatue hadened glass EVA thca thcaf = thcaf thcaf d + thcab thcab 1 T = T + c a d = λ thca G f b = + thcab λ f h f b hb Module tempeatue T mod can be measued on the ea of the module + 1 ab Al fame back coveing foil (tedla) PV cells T c = T mod + T G G SCT

16 Influence of tempeatue Open cicuit voltage V OC depends on the cell tempeatue T c T c Geff = Tm + * G T Tempeatue of the back suface T m vw T G [ T exp( bv T ] eff m = Ta + * 1 W ) + G is the wind velocity 2

17 The cell tempeatue incese depends on the ambient temeatue, the iadiance and the wind speed w thcab d b = λ b + 1 h b thcaf d f = λ f + 1 h f h k = A k ( w) 3/ 4

18 Tempeatue distibution ove the PV field aeas 45 90

19 Tempeatue distibution ove the PV field aeas 30 (oof) The module tempeatue distibution is position sensitive

20 The cell opeating tempeatue in the case of building integation The building suface should be themally isolated Placing PV modules diectly on the themally isolated suface esults in one-side cooling and consequently, in a highe opeating tempeatue thcaf d T = T + c 1 a thca G d ab 1 thca = thcaf thcaf >> + f b = + thcab thcab = + thcaf thca thcaf λ f h f λ b hb thcab thcab Cooling the back suface of PV modules is vey impotant

21 Non-unifom tempeatue distibution on a backventilated PV façade south-west oiented, 3 independent PV fields (E1, E2, E3), 2 sepaated pats 176 c-si PV modules Solatec SI W p / 24 V, kw p in total, m mm wide natually ventilated ai gap between PV modules and insulated wall - geomety of the PV facade - - photo of the PV facade -

22 Tempeatue distibution daily peak tempeatues at (30 min afte iadiance peak) ambient conditions (G ho =675 W/m 2, G in-plane =644 W/m 2, amb. temp C) the tempeatue distibution is highly non-unifom along the height

23 The sting is opeating at MPP I = I mp Expeimentally found I mp pactically independent on tempeatue n P mp = Imp Vmp( Ti ) = nimpvmp( TAV ) i=1 T AV is aveage cell tempeatue in the sting

24 Stings in paallel It is impossible to opeate both in paallel connected cells (stings) of diffeent tempeatues in maximal powe points (MPP) at the same time The efficiency decease due to in paallel connection of cells with diffeent tempeatue was about 0.15% pe C in compaison with cells opeated on the same (aveage) tempeatue

25 Measued vs. calculated pofiles of convesion efficiency and DC output powe fo the façade PV field in the peiod of the highest tempeatue non-unifomity. η conv = η STC. (1 + γ(t cell T cell,stc )) η conv = η STC. (1 + αi(t cell T cell,stc ).( 1 + c 1. ln(g/g STC ) + + c 2. (ln(g/g STC )) 2 + β V (T cell T cell,stc )) 16% 14% DC output powe Efficiency (%) 12% 10% 8% 6% 4% convesion efficiency DC output powe (W) 2% 500 0% Euopean Summe Time (hous) EFF measued EFF calc - simple EFF calc - Huld P measued P calc - simple P calc - Huld

26 100 mm wide natually ventilated ai gap between PV modules and the oof themal isolation

27 Conclusions Facade PV system applications can poduce about 66% of electical enegy poduced by the oof (45 tilted) one Efficiency of PV systems is stongly influenced by tempeatue PV field constuctions should allow an effective cooling of PV modules In paallel should be connected the module stings with the same aveage tempeatue

One-Dimensional, Steady-State. State Conduction with Thermal Energy Generation

One-Dimensional, Steady-State. State Conduction with Thermal Energy Generation One-Dimensional, Steady-State State Conduction with Themal Enegy Geneation Implications of Enegy Geneation Involves a local (volumetic) souce of themal enegy due to convesion fom anothe fom of enegy in

More information

Photovoltaic cell and module physics and technology. Vitezslav Benda, Prof Czech Technical University in Prague

Photovoltaic cell and module physics and technology. Vitezslav Benda, Prof Czech Technical University in Prague Photovoltaic cell and module physics and technology Vitezslav Benda, Prof Czech Technical University in Prague benda@fel.cvut.cz www.fel.cvut.cz 1 Outlines Photovoltaic Effect Photovoltaic cell structure

More information

11) A thin, uniform rod of mass M is supported by two vertical strings, as shown below.

11) A thin, uniform rod of mass M is supported by two vertical strings, as shown below. Fall 2007 Qualifie Pat II 12 minute questions 11) A thin, unifom od of mass M is suppoted by two vetical stings, as shown below. Find the tension in the emaining sting immediately afte one of the stings

More information

1) Emits radiation at the maximum intensity possible for every wavelength. 2) Completely absorbs all incident radiation (hence the term black ).

1) Emits radiation at the maximum intensity possible for every wavelength. 2) Completely absorbs all incident radiation (hence the term black ). Radiation laws Blackbody adiation Planck s Law Any substance (solid, liquid o gas) emits adiation accoding to its absolute tempeatue, measued in units of Kelvin (K = o C + 73.5). The efficiency at which

More information

Black Body Radiation and Radiometric Parameters:

Black Body Radiation and Radiometric Parameters: Black Body Radiation and Radiometic Paametes: All mateials absob and emit adiation to some extent. A blackbody is an idealization of how mateials emit and absob adiation. It can be used as a efeence fo

More information

Coupled Electromagnetic and Heat Transfer Simulations for RF Applicator Design for Efficient Heating of Materials

Coupled Electromagnetic and Heat Transfer Simulations for RF Applicator Design for Efficient Heating of Materials Coupled Electomagnetic and Heat Tansfe Simulations fo RF Applicato Design fo Efficient Heating of Mateials Jeni Anto 1 and Raj C Thiagaajan 2 * 1 Reseache, Anna Univesity, Chennai, 2 ATOA Scientific Technologies

More information

Review for Midterm-1

Review for Midterm-1 Review fo Midtem-1 Midtem-1! Wednesday Sept. 24th at 6pm Section 1 (the 4:10pm class) exam in BCC N130 (Business College) Section 2 (the 6:00pm class) exam in NR 158 (Natual Resouces) Allowed one sheet

More information

Electromagnetism Physics 15b

Electromagnetism Physics 15b lectomagnetism Physics 15b Lectue #20 Dielectics lectic Dipoles Pucell 10.1 10.6 What We Did Last Time Plane wave solutions of Maxwell s equations = 0 sin(k ωt) B = B 0 sin(k ωt) ω = kc, 0 = B, 0 ˆk =

More information

EKT 345 MICROWAVE ENGINEERING CHAPTER 2: PLANAR TRANSMISSION LINES

EKT 345 MICROWAVE ENGINEERING CHAPTER 2: PLANAR TRANSMISSION LINES EKT 345 MICROWAVE ENGINEERING CHAPTER : PLANAR TRANSMISSION LINES 1 Tansmission Lines A device used to tansfe enegy fom one point to anothe point efficiently Efficiently minimum loss, eflection and close

More information

ANALYSIS OF GLOBAL WARMING MITIGATION BY WHITE REFLECTING SURFACES

ANALYSIS OF GLOBAL WARMING MITIGATION BY WHITE REFLECTING SURFACES Intenational Confeence CO Summit: Technology and Oppotunity Vail, Coloado June 6-10 010 ANALYSIS OF GLOBAL WARMING MITIGATION BY WHITE REFLECTING SURFACES Fedeico Rossi, Andea Nicolini Univesity of Peugia,

More information

B. Spherical Wave Propagation

B. Spherical Wave Propagation 11/8/007 Spheical Wave Popagation notes 1/1 B. Spheical Wave Popagation Evey antenna launches a spheical wave, thus its powe density educes as a function of 1, whee is the distance fom the antenna. We

More information

Chemical Engineering 412

Chemical Engineering 412 Chemical Engineeing 41 Intoductoy Nuclea Engineeing Lectue 16 Nuclea eacto Theoy III Neuton Tanspot 1 One-goup eacto Equation Mono-enegetic neutons (Neuton Balance) DD φφ aa φφ + ss 1 vv vv is neuton speed

More information

Experiment I Voltage Variation and Control

Experiment I Voltage Variation and Control ELE303 Electicity Netwoks Expeiment I oltage aiation and ontol Objective To demonstate that the voltage diffeence between the sending end of a tansmission line and the load o eceiving end depends mainly

More information

EKT 356 MICROWAVE COMMUNICATIONS CHAPTER 2: PLANAR TRANSMISSION LINES

EKT 356 MICROWAVE COMMUNICATIONS CHAPTER 2: PLANAR TRANSMISSION LINES EKT 356 MICROWAVE COMMUNICATIONS CHAPTER : PLANAR TRANSMISSION LINES 1 Tansmission Lines A device used to tansfe enegy fom one point to anothe point efficiently Efficiently minimum loss, eflection and

More information

ELECTROSTATICS::BHSEC MCQ 1. A. B. C. D.

ELECTROSTATICS::BHSEC MCQ 1. A. B. C. D. ELETROSTATIS::BHSE 9-4 MQ. A moving electic chage poduces A. electic field only. B. magnetic field only.. both electic field and magnetic field. D. neithe of these two fields.. both electic field and magnetic

More information

, and the curve BC is symmetrical. Find also the horizontal force in x-direction on one side of the body. h C

, and the curve BC is symmetrical. Find also the horizontal force in x-direction on one side of the body. h C Umeå Univesitet, Fysik 1 Vitaly Bychkov Pov i teknisk fysik, Fluid Dynamics (Stömningsläa), 2013-05-31, kl 9.00-15.00 jälpmedel: Students may use any book including the textbook Lectues on Fluid Dynamics.

More information

Photovoltaic cell and module physics and technology

Photovoltaic cell and module physics and technology Photovoltaic cell and module physics and technology Vitezslav Benda, Prof Czech Technical University in Prague benda@fel.cvut.cz www.fel.cvut.cz 6/21/2012 1 Outlines Photovoltaic Effect Photovoltaic cell

More information

Research Article EXPERIMENTAL STUDY OF HEAT TRANSFER CHARACTERISTICS OF STAINLESS STEEL FIBROUS FLOW INSULATOR

Research Article EXPERIMENTAL STUDY OF HEAT TRANSFER CHARACTERISTICS OF STAINLESS STEEL FIBROUS FLOW INSULATOR Tansactions of the TSME (16) Vol. 4, No. 2, 148 155 Jounal of seach and Applications in Mechanical Engineeing Copyight 16 by TSME ISSN 2229-2152 pint DOI: 1.14456/jame.16.15 seach Aticle EXPERIMENTAL STUDY

More information

Insulated Bearings MEGAOHM TM Series

Insulated Bearings MEGAOHM TM Series Fo ew Technology etwok copoation R Insulated eaings MEGAOHM TM Seies Insulated eaings MEGAOHM TM Seies : Offeing Enhanced Safety and Reliability eaings used in electical equipment such as motos and powe

More information

15 B1 1. Figure 1. At what speed would the car have to travel for resonant oscillations to occur? Comment on your answer.

15 B1 1. Figure 1. At what speed would the car have to travel for resonant oscillations to occur? Comment on your answer. Kiangsu-Chekiang College (Shatin) F:EasteHolidaysAssignmentAns.doc Easte Holidays Assignment Answe Fom 6B Subject: Physics. (a) State the conditions fo a body to undego simple hamonic motion. ( mak) (a)

More information

Thermal-Fluids I. Chapter 17 Steady heat conduction. Dr. Primal Fernando Ph: (850)

Thermal-Fluids I. Chapter 17 Steady heat conduction. Dr. Primal Fernando Ph: (850) emal-fluids I Capte 7 Steady eat conduction D. Pimal Fenando pimal@eng.fsu.edu P: (850 40-633 Steady eat conduction Hee we conside one dimensional steady eat conduction. We conside eat tansfe in a plane

More information

Chapter 2 ONE DIMENSIONAL STEADY STATE CONDUCTION. Chapter 2 Chee 318 1

Chapter 2 ONE DIMENSIONAL STEADY STATE CONDUCTION. Chapter 2 Chee 318 1 hapte ONE DIMENSIONAL SEADY SAE ONDUION hapte hee 38 HEA ONDUION HOUGH OMPOSIE EANGULA WALLS empeatue pofile A B X X 3 X 3 4 X 4 Χ A Χ B Χ hapte hee 38 hemal conductivity Fouie s law ( is constant) A A

More information

Calculation of Temperature Rise in Dry-type Air-core Reactors Using Strong Coupling of Fluid-Temperature Field

Calculation of Temperature Rise in Dry-type Air-core Reactors Using Strong Coupling of Fluid-Temperature Field Reseach Jounal of Applied Sciences, Engineeing and Technology 5(10: 941-945, 013 ISSN: 040-7459; e-issn: 040-7467 Maxwell Scientific Oganization, 013 Submitted: Septembe 15, 01 Accepted: Octobe 4, 01 Published:

More information

Phys102 Second Major-182 Zero Version Monday, March 25, 2019 Page: 1

Phys102 Second Major-182 Zero Version Monday, March 25, 2019 Page: 1 Monday, Mach 5, 019 Page: 1 Q1. Figue 1 shows thee pais of identical conducting sphees that ae to be touched togethe and then sepaated. The initial chages on them befoe the touch ae indicated. Rank the

More information

Effect of drag on the performance for an efficient wind turbine blade design

Effect of drag on the performance for an efficient wind turbine blade design Available online at www.sciencediect.com Enegy Pocedia 18 (01 ) 404 415 Abstact Effect of dag on the pefomance fo an efficient wind tubine blade design D. Eng. Ali H. Almukhta Univesity of Technology Email-

More information

Physics 313 Practice Test Page 1. University Physics III Practice Test II

Physics 313 Practice Test Page 1. University Physics III Practice Test II Physics 313 Pactice Test Page 1 Univesity Physics III Pactice Test II This pactice test should give you a ough idea of the fomat and oveall level of the Physics 313 exams. The actual exams will have diffeent

More information

Foundations of Chemical Kinetics. Lecture 9: Generalizing collision theory

Foundations of Chemical Kinetics. Lecture 9: Generalizing collision theory Foundations of Chemical Kinetics Lectue 9: Genealizing collision theoy Mac R. Roussel Depatment of Chemisty and Biochemisty Spheical pola coodinates z θ φ y x Angles and solid angles θ a A Ω θ=a/ unit:

More information

Determining solar characteristics using planetary data

Determining solar characteristics using planetary data Detemining sola chaacteistics using planetay data Intoduction The Sun is a G-type main sequence sta at the cente of the Sola System aound which the planets, including ou Eath, obit. In this investigation

More information

Gauss s Law Simulation Activities

Gauss s Law Simulation Activities Gauss s Law Simulation Activities Name: Backgound: The electic field aound a point chage is found by: = kq/ 2 If thee ae multiple chages, the net field at any point is the vecto sum of the fields. Fo a

More information

High precision computer simulation of cyclotrons KARAMYSHEVA T., AMIRKHANOV I. MALININ V., POPOV D.

High precision computer simulation of cyclotrons KARAMYSHEVA T., AMIRKHANOV I. MALININ V., POPOV D. High pecision compute simulation of cyclotons KARAMYSHEVA T., AMIRKHANOV I. MALININ V., POPOV D. Abstact Effective and accuate compute simulations ae highly impotant in acceleatos design and poduction.

More information

COMPARISON OF METHODS FOR SOLVING THE HEAT TRANSFER IN ELECTRICAL MACHINES

COMPARISON OF METHODS FOR SOLVING THE HEAT TRANSFER IN ELECTRICAL MACHINES POZNAN UNIVE RSITY OF TE CHNOLOGY ACADE MIC JOURNALS No 75 Electical Engineeing 2013 Zbynek MAKKI* Macel JANDA* Ramia DEEB* COMPARISON OF METHODS FOR SOLVING THE HEAT TRANSFER IN ELECTRICAL MACHINES This

More information

M.M.A HIGHER SECONDARY SCHOOL - PAPPANADU 12 TH PHYSICS - HALF YEARLY EXAM ANSWER KEY

M.M.A HIGHER SECONDARY SCHOOL - PAPPANADU 12 TH PHYSICS - HALF YEARLY EXAM ANSWER KEY http://www.tbtnpsc.com/07//plus-two-th-half-yealy-exam-questions-pape-answe-key-download-07.html M.M.A HIGHER SEONDARY SHOOL - PAPPANADU TH PHYSIS - HALF YEARLY EXAM ANSWER KEY 07-08 STD : XII - EM PART

More information

Physics 122, Fall September 2012

Physics 122, Fall September 2012 Physics 1, Fall 1 7 Septembe 1 Today in Physics 1: getting V fom E When it s best to get V fom E, athe than vice vesa V within continuous chage distibutions Potential enegy of continuous chage distibutions

More information

18.1 Origin of Electricity 18.2 Charged Objects and Electric Force

18.1 Origin of Electricity 18.2 Charged Objects and Electric Force 1 18.1 Oigin of lecticity 18. Chaged Objects and lectic Foce Thee ae two kinds of electic chage: positive and negative. The SI unit of electic chage is the coulomb (C). The magnitude of the chage on an

More information

Basic Bridge Circuits

Basic Bridge Circuits AN7 Datafoth Copoation Page of 6 DID YOU KNOW? Samuel Hunte Chistie (784-865) was bon in London the son of James Chistie, who founded Chistie's Fine At Auctionees. Samuel studied mathematics at Tinity

More information

The second law of thermodynamics - II.

The second law of thermodynamics - II. Januay 21, 2013 The second law of themodynamics - II. Asaf Pe e 1 1. The Schottky defect At absolute zeo tempeatue, the atoms of a solid ae odeed completely egulaly on a cystal lattice. As the tempeatue

More information

17.1 Electric Potential Energy. Equipotential Lines. PE = energy associated with an arrangement of objects that exert forces on each other

17.1 Electric Potential Energy. Equipotential Lines. PE = energy associated with an arrangement of objects that exert forces on each other Electic Potential Enegy, PE Units: Joules Electic Potential, Units: olts 17.1 Electic Potential Enegy Electic foce is a consevative foce and so we can assign an electic potential enegy (PE) to the system

More information

LECTURER: PM DR MAZLAN ABDUL WAHID PM Dr Mazlan Abdul Wahid

LECTURER: PM DR MAZLAN ABDUL WAHID   PM Dr Mazlan Abdul Wahid M 445 LU: M D MZL BDUL WID http://www.fkm.utm.my/~mazlan hapte teady-tate tate One Dimensional eat onduction M bdul Wahid UM aculty of Mechanical ngineeing Univesiti eknologi Malaysia www.fkm.utm.my/~mazlan

More information

20-9 ELECTRIC FIELD LINES 20-9 ELECTRIC POTENTIAL. Answers to the Conceptual Questions. Chapter 20 Electricity 241

20-9 ELECTRIC FIELD LINES 20-9 ELECTRIC POTENTIAL. Answers to the Conceptual Questions. Chapter 20 Electricity 241 Chapte 0 Electicity 41 0-9 ELECTRIC IELD LINES Goals Illustate the concept of electic field lines. Content The electic field can be symbolized by lines of foce thoughout space. The electic field is stonge

More information

OSCILLATIONS AND GRAVITATION

OSCILLATIONS AND GRAVITATION 1. SIMPLE HARMONIC MOTION Simple hamonic motion is any motion that is equivalent to a single component of unifom cicula motion. In this situation the velocity is always geatest in the middle of the motion,

More information

Lab #4: Newton s Second Law

Lab #4: Newton s Second Law Lab #4: Newton s Second Law Si Isaac Newton Reading Assignment: bon: Januay 4, 1643 Chapte 5 died: Mach 31, 1727 Chapte 9, Section 9-7 Intoduction: Potait of Isaac Newton by Si Godfey Knelle http://www.newton.cam.ac.uk/at/potait.html

More information

Gauss Law. Physics 231 Lecture 2-1

Gauss Law. Physics 231 Lecture 2-1 Gauss Law Physics 31 Lectue -1 lectic Field Lines The numbe of field lines, also known as lines of foce, ae elated to stength of the electic field Moe appopiately it is the numbe of field lines cossing

More information

Chapter 5 Page 5.1 CHAPTER 5. r Force times distance has units of energy. Therefore, fxr=u, or f / is dimensionless.

Chapter 5 Page 5.1 CHAPTER 5. r Force times distance has units of energy. Therefore, fxr=u, or f / is dimensionless. Chapte 5 Page 5.1 CHAPTER 5 Poblem 5.1: 1 (a) u () 4 0.90.93 3.0 (b) Foce times distance has units of enegy. Theefoe, fx=u, o f/ is dimensionless. d f = d u 1 d f 4ε 1 = f = 4 ε1 d 13 f = 4 ε 1 f ε = 4

More information

Electrostatics (Electric Charges and Field) #2 2010

Electrostatics (Electric Charges and Field) #2 2010 Electic Field: The concept of electic field explains the action at a distance foce between two chaged paticles. Evey chage poduces a field aound it so that any othe chaged paticle expeiences a foce when

More information

m1 m2 M 2 = M -1 L 3 T -2

m1 m2 M 2 = M -1 L 3 T -2 GAVITATION Newton s Univesal law of gavitation. Evey paticle of matte in this univese attacts evey othe paticle with a foce which vaies diectly as the poduct of thei masses and invesely as the squae of

More information

PES 3950/PHYS 6950: Homework Assignment 6

PES 3950/PHYS 6950: Homework Assignment 6 PES 3950/PHYS 6950: Homewok Assignment 6 Handed out: Monday Apil 7 Due in: Wednesday May 6, at the stat of class at 3:05 pm shap Show all woking and easoning to eceive full points. Question 1 [5 points]

More information

General Railgun Function

General Railgun Function Geneal ailgun Function An electomagnetic ail gun uses a lage Loentz foce to fie a pojectile. The classic configuation uses two conducting ails with amatue that fits between and closes the cicuit between

More information

Physics 2212 GH Quiz #2 Solutions Spring 2016

Physics 2212 GH Quiz #2 Solutions Spring 2016 Physics 2212 GH Quiz #2 Solutions Sping 216 I. 17 points) Thee point chages, each caying a chage Q = +6. nc, ae placed on an equilateal tiangle of side length = 3. mm. An additional point chage, caying

More information

Gaia s Place in Space

Gaia s Place in Space Gaia s Place in Space The impotance of obital positions fo satellites Obits and Lagange Points Satellites can be launched into a numbe of diffeent obits depending on thei objectives and what they ae obseving.

More information

Algebra-based Physics II

Algebra-based Physics II lgebabased Physics II Chapte 19 Electic potential enegy & The Electic potential Why enegy is stoed in an electic field? How to descibe an field fom enegetic point of view? Class Website: Natual way of

More information

RAO IIT ACADEMY / NSEP Physics / Code : P 152 / Solutions NATIONAL STANDARD EXAMINATION IN PHYSICS SOLUTIONS

RAO IIT ACADEMY / NSEP Physics / Code : P 152 / Solutions NATIONAL STANDARD EXAMINATION IN PHYSICS SOLUTIONS RAO ACADEMY / NSEP Physics / Code : P 5 / Solutions NAONAL SANDARD EXAMNAON N PHYSCS - 5 SOLUONS RAO ACADEMY / NSEP Physics / Code : P 5 / Solutions NSEP SOLUONS (PHYSCS) CODE - P 5 ANSWER KEY & SOLUONS.

More information

Search for a Critical Electron Temperature Gradient in DIII-D L-mode Discharges

Search for a Critical Electron Temperature Gradient in DIII-D L-mode Discharges Seach fo a Citical Electon Tempeatue Gadient in DIII-D L-mode Dischages.C. Deoo, S. Ciant 1, T.C. Luce, A. Manini, C.C. Petty, F. Ryte, M.E. Austin 3, D.R. ake, K.W. Gentle 3, C.M. Geenfield,.E. Kinsey

More information

Predicting Cone-in-Cone Blender Efficiencies from Key Material Properties

Predicting Cone-in-Cone Blender Efficiencies from Key Material Properties Pedicting Cone-in-Cone Blende Efficiencies fom Key Mateial Popeties By: D. Key Johanson Mateial Flow Solutions, Inc. NOTICE: This is the autho s vesion of a wok accepted fo publication by Elsevie. Changes

More information

Phys-272 Lecture 17. Motional Electromotive Force (emf) Induced Electric Fields Displacement Currents Maxwell s Equations

Phys-272 Lecture 17. Motional Electromotive Force (emf) Induced Electric Fields Displacement Currents Maxwell s Equations Phys-7 Lectue 17 Motional Electomotive Foce (emf) Induced Electic Fields Displacement Cuents Maxwell s Equations Fom Faaday's Law to Displacement Cuent AC geneato Magnetic Levitation Tain Review of Souces

More information

The nature of electromagnetic radiation.

The nature of electromagnetic radiation. Lectue 3 The natue of electomagnetic adiation. Objectives: 1. Basic intoduction to the electomagnetic field: Definitions Dual natue of electomagnetic adiation lectomagnetic spectum. Main adiometic quantities:

More information

Today in Physics 122: getting V from E

Today in Physics 122: getting V from E Today in Physics 1: getting V fom E When it s best to get V fom E, athe than vice vesa V within continuous chage distibutions Potential enegy of continuous chage distibutions Capacitance Potential enegy

More information

Gauss s Law: Circuits

Gauss s Law: Circuits Gauss s Law: Cicuits Can we have excess chage inside in steady state? E suface nˆ A q inside E nˆ A E nˆ A left _ suface ight _ suface q inside 1 Gauss s Law: Junction Between two Wies n 2

More information

Physics 211: Newton s Second Law

Physics 211: Newton s Second Law Physics 211: Newton s Second Law Reading Assignment: Chapte 5, Sections 5-9 Chapte 6, Section 2-3 Si Isaac Newton Bon: Januay 4, 1643 Died: Mach 31, 1727 Intoduction: Kinematics is the study of how objects

More information

Fields and Waves I Spring 2005 Homework 4. Due 8 March 2005

Fields and Waves I Spring 2005 Homework 4. Due 8 March 2005 Homewok 4 Due 8 Mach 005. Inceasing the Beakdown Voltage: This fist question is a mini design poject. You fist step is to find a commecial cable (coaxial o two wie line) fo which you have the following

More information

Analysis and Optimization of a Special Type of Dielectric Loaded Resonant Cavity for Mobile Communication Filters

Analysis and Optimization of a Special Type of Dielectric Loaded Resonant Cavity for Mobile Communication Filters 328 Analysis and Optimization of a Special Type of Dielectic Loaded Resonant Cavity fo Mobile Communication Filtes Haold S. Showes, Banmali S. Rawat *, Syam S. Challa Depatment of Electical and Biomedical

More information

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007 School of Electical and Compute Engineeing, Conell Univesity ECE 303: Electomagnetic Fields and Waves Fall 007 Homewok 8 Due on Oct. 19, 007 by 5:00 PM Reading Assignments: i) Review the lectue notes.

More information

(Sample 3) Exam 1 - Physics Patel SPRING 1998 FORM CODE - A (solution key at end of exam)

(Sample 3) Exam 1 - Physics Patel SPRING 1998 FORM CODE - A (solution key at end of exam) (Sample 3) Exam 1 - Physics 202 - Patel SPRING 1998 FORM CODE - A (solution key at end of exam) Be sue to fill in you student numbe and FORM lette (A, B, C) on you answe sheet. If you foget to include

More information

Electric Field, Potential Energy, & Voltage

Electric Field, Potential Energy, & Voltage Slide 1 / 66 lectic Field, Potential negy, & oltage Wok Slide 2 / 66 Q+ Q+ The foce changes as chages move towads each othe since the foce depends on the distance between the chages. s these two chages

More information

1 Spherical multipole moments

1 Spherical multipole moments Jackson notes 9 Spheical multipole moments Suppose we have a chage distibution ρ (x) wheeallofthechageiscontained within a spheical egion of adius R, as shown in the diagam. Then thee is no chage in the

More information

The Combined Effect of Chemical reaction, Radiation, MHD on Mixed Convection Heat and Mass Transfer Along a Vertical Moving Surface

The Combined Effect of Chemical reaction, Radiation, MHD on Mixed Convection Heat and Mass Transfer Along a Vertical Moving Surface Available at http://pvamu.edu/aam Appl. Appl. Math. ISSN: 93-966 Vol. 5, Issue (Decembe ), pp. 53 53 (Peviously, Vol. 5, Issue, pp. 63 6) Applications and Applied Mathematics: An Intenational Jounal (AAM)

More information

1) Consider an object of a parabolic shape with rotational symmetry z

1) Consider an object of a parabolic shape with rotational symmetry z Umeå Univesitet, Fysik 1 Vitaly Bychkov Pov i teknisk fysik, Fluid Mechanics (Stömningsläa), 01-06-01, kl 9.00-15.00 jälpmedel: Students may use any book including the tetbook Lectues on Fluid Dynamics.

More information

V G. In this class, we will look at a possible hypothesis for way the time dependence is t

V G. In this class, we will look at a possible hypothesis for way the time dependence is t ECE65R : Reliability Physics of anoelectonic Devices Lectue : CI Time Exponents Date : Dec. 4, 6 Classnote : Saakshi Gangwal Review : Lutfe A Siddiqui. Review We have spent seveal weeks discussing discussing

More information

Lecture 8 - Gauss s Law

Lecture 8 - Gauss s Law Lectue 8 - Gauss s Law A Puzzle... Example Calculate the potential enegy, pe ion, fo an infinite 1D ionic cystal with sepaation a; that is, a ow of equally spaced chages of magnitude e and altenating sign.

More information

6 PROBABILITY GENERATING FUNCTIONS

6 PROBABILITY GENERATING FUNCTIONS 6 PROBABILITY GENERATING FUNCTIONS Cetain deivations pesented in this couse have been somewhat heavy on algeba. Fo example, detemining the expectation of the Binomial distibution (page 5.1 tuned out to

More information

Current Balance Warm Up

Current Balance Warm Up PHYSICS EXPERIMENTS 133 Cuent Balance-1 Cuent Balance Wam Up 1. Foce between cuent-caying wies Wie 1 has a length L (whee L is "long") and caies a cuent I 0. What is the magnitude of the magnetic field

More information

Phys-272 Lecture 18. Mutual Inductance Self-Inductance R-L Circuits

Phys-272 Lecture 18. Mutual Inductance Self-Inductance R-L Circuits Phys-7 ectue 8 Mutual nductance Self-nductance - Cicuits Mutual nductance f we have a constant cuent i in coil, a constant magnetic field is ceated and this poduces a constant magnetic flux in coil. Since

More information

Dynamic Performances of Self-Excited Induction Generator Feeding Different Static Loads

Dynamic Performances of Self-Excited Induction Generator Feeding Different Static Loads SERBIAN JOURNAL OF ELECTRICAL ENGINEERING Vol. 3, No. 1, June 2006, 63-76 Dynamic Pefomances of Self-Excited Induction Geneato Feeding Diffeent Static Loads Ali Nesba 1, Rachid Ibtiouen 2, Oma Touhami

More information

IN SITU SOUND ABSORPTION COEFFICIENT MEASUREMENT OF VARIOUS SURFACES

IN SITU SOUND ABSORPTION COEFFICIENT MEASUREMENT OF VARIOUS SURFACES IN SITU SOUND ABSORPTION COEFFICIENT MEASUREMENT OF VARIOUS SURFACES PACS REFERENCES : 43.20.El, 43.20.Ye, 43.55.Ev, 43.58.Bh Michel Béengie 1 ; Massimo Gaai 2 1 Laboatoie Cental des Ponts et Chaussées

More information

STUDY INTO THE INFLUENCE OF TEMPERATURE AND TIME FACTORS (160 C, 1-7 DAYS) ON HMX STRUCTURE (#254)

STUDY INTO THE INFLUENCE OF TEMPERATURE AND TIME FACTORS (160 C, 1-7 DAYS) ON HMX STRUCTURE (#254) STUDY INTO THE INFLUENCE OF TEMPERATURE AND TIME FACTORS (160 C, 1-7 DAYS) ON HMX STRUCTURE (#254) T.Ye. Kisanova, V.N. Geman, A.M. Zlobin, T.G. Kiianova, Ye.S. Kozlova, V.N. Kolesnikova, S.P. Lobanova,

More information

A scaling-up methodology for co-rotating twin-screw extruders

A scaling-up methodology for co-rotating twin-screw extruders A scaling-up methodology fo co-otating twin-scew extudes A. Gaspa-Cunha, J. A. Covas Institute fo Polymes and Composites/I3N, Univesity of Minho, Guimaães 4800-058, Potugal Abstact. Scaling-up of co-otating

More information

CHAPTER 10 ELECTRIC POTENTIAL AND CAPACITANCE

CHAPTER 10 ELECTRIC POTENTIAL AND CAPACITANCE CHAPTER 0 ELECTRIC POTENTIAL AND CAPACITANCE ELECTRIC POTENTIAL AND CAPACITANCE 7 0. ELECTRIC POTENTIAL ENERGY Conside a chaged paticle of chage in a egion of an electic field E. This filed exets an electic

More information

Force between two parallel current wires and Newton s. third law

Force between two parallel current wires and Newton s. third law Foce between two paallel cuent wies and Newton s thid law Yannan Yang (Shanghai Jinjuan Infomation Science and Technology Co., Ltd.) Abstact: In this pape, the essence of the inteaction between two paallel

More information

II. MRI Technology. B. Localized Information. Lorenz Mitschang Physikalisch-Technische Bundesanstalt, 29 th June 2009

II. MRI Technology. B. Localized Information. Lorenz Mitschang Physikalisch-Technische Bundesanstalt,   29 th June 2009 Magnetic Resonance Imaging II. MRI Technology A. Limitations to patial Infomation B. Localized Infomation Loenz Mitschang Physikalisch-Technische Bundesanstalt, www.ptb.de 9 th June 009 A. Limitations

More information

Mathematisch-Naturwissenschaftliche Fakultät I Humboldt-Universität zu Berlin Institut für Physik Physikalisches Grundpraktikum.

Mathematisch-Naturwissenschaftliche Fakultät I Humboldt-Universität zu Berlin Institut für Physik Physikalisches Grundpraktikum. Mathematisch-Natuwissenschaftliche Fakultät I Humboldt-Univesität zu Belin Institut fü Physik Physikalisches Gundpaktikum Vesuchspotokoll Polaisation duch Reflexion (O11) duchgefüht am 10.11.2009 mit Vesuchspatne

More information

Revision of Lecture Eight

Revision of Lecture Eight Revision of Lectue Eight Baseband equivalent system and equiements of optimal tansmit and eceive filteing: (1) achieve zeo ISI, and () maximise the eceive SNR Thee detection schemes: Theshold detection

More information

Plasma heating in reversed field pinches at the fundamental ion cyclotron frequency

Plasma heating in reversed field pinches at the fundamental ion cyclotron frequency PHYSICS OF PLASMAS VOLUME 9, NUMBER 4 APRIL 2002 Plasma heating in evesed field pinches at the fundamental ion cycloton fequency V. A. Svidzinski and S. C. Page Univesity of Wisconsin-Madison, Madison,

More information

Astronomy 111, Fall October 2011

Astronomy 111, Fall October 2011 Astonomy 111, Fall 011 4 Octobe 011 Today in Astonomy 111: moe details on enegy tanspot and the tempeatues of the planets Moe about albedo and emissivity Moe about the tempeatue of sunlit, adiation-cooled

More information

ELECTRON ENERGY DISTRIBUTIONS AND NON-COLLISIONAL HEATING IN MAGNETICALLY ENHANCED INDUCTIVELY COUPLED PLASMAS*

ELECTRON ENERGY DISTRIBUTIONS AND NON-COLLISIONAL HEATING IN MAGNETICALLY ENHANCED INDUCTIVELY COUPLED PLASMAS* ELECTRON ENERGY DISTRIUTIONS AND NON-COLLISIONAL HEATING IN MAGNETICALLY ENHANCED INDUCTIVELY COUPLED PLASMAS* Ronald L. Kinde and Mak J. Kushne Depatment of Electical and Compute Engineeing Ubana, IL

More information

rect_patch_cavity.doc Page 1 of 12 Microstrip Antennas- Rectangular Patch Chapter 14 in Antenna Theory, Analysis and Design (4th Edition) by Balanis

rect_patch_cavity.doc Page 1 of 12 Microstrip Antennas- Rectangular Patch Chapter 14 in Antenna Theory, Analysis and Design (4th Edition) by Balanis ect_patch_cavit.doc Page 1 of 1 Micostip Antennas- Rectangula Patch Chapte 14 in Antenna Theo, Analsis and Design (4th dition) b Balanis Cavit model Micostip antennas esemble dielectic-loaded cavities

More information

V7: Diffusional association of proteins and Brownian dynamics simulations

V7: Diffusional association of proteins and Brownian dynamics simulations V7: Diffusional association of poteins and Bownian dynamics simulations Bownian motion The paticle movement was discoveed by Robet Bown in 1827 and was intepeted coectly fist by W. Ramsay in 1876. Exact

More information

PART- A 1. (C) 2. (D) 3. (D) 4. (B) 5. (D) 6. (C) 7. (D) 8. (B) 9. (D) 10. (B) 11. (B) 12. (B) 13. (A) 14. (D)

PART- A 1. (C) 2. (D) 3. (D) 4. (B) 5. (D) 6. (C) 7. (D) 8. (B) 9. (D) 10. (B) 11. (B) 12. (B) 13. (A) 14. (D) PRACTICE TEST-4 KISHORE VAIGYANIK PROTSAHAN YOJANA (KVPY) 7 STREAM (SA)_ DATE : -9-7 ANSWER KEY PART- A. (C). (D) 3. (D) 4. (B) 5. (D) 6. (C) 7. (D) 8. (B) 9. (D). (B). (B). (B) 3. (A) 4. (D) 5. (C) 6.

More information

763620SS STATISTICAL PHYSICS Solutions 2 Autumn 2012

763620SS STATISTICAL PHYSICS Solutions 2 Autumn 2012 763620SS STATISTICAL PHYSICS Solutions 2 Autumn 2012 1. Continuous Random Walk Conside a continuous one-dimensional andom walk. Let w(s i ds i be the pobability that the length of the i th displacement

More information

Proceedings of the 11th WSEAS International Conference on Automatic Control, Modelling and Simulation

Proceedings of the 11th WSEAS International Conference on Automatic Control, Modelling and Simulation Tempeatue measuement in contact pantogaph - AC contact line Constantin-Floin OCOLEANU *, Ioan POPA *, Gheoghe MANOLEA **, Alin-Iulian DOLAN * Electical Appaatus and Technologies *, Electomechanical **

More information

Steady State and Transient Performance Analysis of Three Phase Induction Machine using MATLAB Simulations

Steady State and Transient Performance Analysis of Three Phase Induction Machine using MATLAB Simulations Intenational Jounal of Recent Tends in Engineeing, Vol, No., May 9 Steady State and Tansient Pefomance Analysis of Thee Phase Induction Machine using MATAB Simulations Pof. Himanshu K. Patel Assistant

More information

Circular Orbits. and g =

Circular Orbits. and g = using analyse planetay and satellite motion modelled as unifom cicula motion in a univesal gavitation field, a = v = 4π and g = T GM1 GM and F = 1M SATELLITES IN OBIT A satellite is any object that is

More information

HINDCASTING OF WIND AND WAVE CLIMATE OF SEAS AROUND RUSSIA

HINDCASTING OF WIND AND WAVE CLIMATE OF SEAS AROUND RUSSIA Leonid J. Lopatoukhin, Alexande V. Boukhanovsky, Ecateina S. Chenysheva, Segey V. Ivanov HINDCASTING OF WIND AND WAVE CLIMATE OF SEAS AROUND RUSSIA St. Petesbug State Univesity, Institute fo High Pefomance

More information

ANALYSIS OF SURF ZONE RADAR BACKSCATTER MEASUREMENTS

ANALYSIS OF SURF ZONE RADAR BACKSCATTER MEASUREMENTS ANALYSIS OF SURF ZONE RADAR BACKSCATTER MEASUREMENTS LONG-TERM GOAL David R. Lyzenga Naval Achitectue and Maine Engineeing Dept. Univesity of Michigan Ann Abo, MI 48109-2145 phone: (734) 764-3216 fax:

More information

Lecture 1a: Satellite Orbits

Lecture 1a: Satellite Orbits Lectue 1a: Satellite Obits Outline 1. Newton s Laws of Mo3on 2. Newton s Law of Univesal Gavita3on 3. Calcula3ng satellite obital paametes (assuming cicula mo3on) Scala & Vectos Scala: a physical quan3ty

More information

MEASUREMENT AND MODELING OF SPACE CHARGE ACCUMULATION IN POLYMERIC HVDC CABLE SYSTEMS

MEASUREMENT AND MODELING OF SPACE CHARGE ACCUMULATION IN POLYMERIC HVDC CABLE SYSTEMS MEASUREMENT AND MODELING OF SPACE CHARGE ACCUMULATION IN POLYMERIC HVDC CABLE SYSTEMS Riccado BODEGA, Pysmian Cables and Systems, The Nethelands, iccado.bodega@pysmian.com Pete MORSHUIS, Delft Univesity

More information

PREDICTION OF THERMAL BREAKTHROUGH FROM TRACER TESTS. G. Michael Shook

PREDICTION OF THERMAL BREAKTHROUGH FROM TRACER TESTS. G. Michael Shook PROCEEDINGS, Tenty-Fouth Wokshop on Geothemal Resevoi Engineeing Stanfod Univesity, Stanfod, Califonia, Januay 25-27, 1999 SGP-TR-162 PREDICTION OF THERMAL BREAKTHROUGH FROM TRACER TESTS G. Michael Shook

More information

Stellar Structure and Evolution

Stellar Structure and Evolution Stella Stuctue and Evolution Theoetical Stella odels Conside each spheically symmetic shell of adius and thickness d. Basic equations of stella stuctue ae: 1 Hydostatic equilibium π dp dp d G π = G =.

More information

Supplementary Figure 1. Circular parallel lamellae grain size as a function of annealing time at 250 C. Error bars represent the 2σ uncertainty in

Supplementary Figure 1. Circular parallel lamellae grain size as a function of annealing time at 250 C. Error bars represent the 2σ uncertainty in Supplementay Figue 1. Cicula paallel lamellae gain size as a function of annealing time at 50 C. Eo bas epesent the σ uncetainty in the measued adii based on image pixilation and analysis uncetainty contibutions

More information

Numerical Integration

Numerical Integration MCEN 473/573 Chapte 0 Numeical Integation Fall, 2006 Textbook, 0.4 and 0.5 Isopaametic Fomula Numeical Integation [] e [ ] T k = h B [ D][ B] e B Jdsdt In pactice, the element stiffness is calculated numeically.

More information

Chapter 3 Optical Systems with Annular Pupils

Chapter 3 Optical Systems with Annular Pupils Chapte 3 Optical Systems with Annula Pupils 3 INTRODUCTION In this chapte, we discuss the imaging popeties of a system with an annula pupil in a manne simila to those fo a system with a cicula pupil The

More information

Chapter 23: GAUSS LAW 343

Chapter 23: GAUSS LAW 343 Chapte 23: GAUSS LAW 1 A total chage of 63 10 8 C is distibuted unifomly thoughout a 27-cm adius sphee The volume chage density is: A 37 10 7 C/m 3 B 69 10 6 C/m 3 C 69 10 6 C/m 2 D 25 10 4 C/m 3 76 10

More information