FYS 3028/8028 Solar Energy and Energy Storage. Calculator with empty memory Language dictionaries

Similar documents
PHOTOVOLTAICS Fundamentals

1 Name: Student number: DEPARTMENT OF PHYSICS AND PHYSICAL OCEANOGRAPHY MEMORIAL UNIVERSITY OF NEWFOUNDLAND. Fall :00-11:00

n N D n p = n i p N A

EE 5611 Introduction to Microelectronic Technologies Fall Tuesday, September 23, 2014 Lecture 07

Appendix 1: List of symbols

Electrons are shared in covalent bonds between atoms of Si. A bound electron has the lowest energy state.

Chemistry Instrumental Analysis Lecture 8. Chem 4631

Semiconductor Physics and Devices

Spring Semester 2012 Final Exam

Semiconductor Devices and Circuits Fall Midterm Exam. Instructor: Dr. Dietmar Knipp, Professor of Electrical Engineering. Name: Mat. -Nr.

For the following statements, mark ( ) for true statement and (X) for wrong statement and correct it.

Chapter 7. Solar Cell

Semiconductor Physics fall 2012 problems

Chapter 7. The pn Junction

Semiconductor Junctions

Solar cells operation

Solid State Electronics. Final Examination

Final Examination EE 130 December 16, 1997 Time allotted: 180 minutes

3.003 Principles of Engineering Practice

Quiz #1 Practice Problem Set

UNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences. EECS 130 Professor Ali Javey Fall 2006

Lecture 2. Introduction to semiconductors Structures and characteristics in semiconductors

Photovoltaic cell and module physics and technology

Comparison of Ge, InGaAs p-n junction solar cell

Charge Carriers in Semiconductor

( )! N D ( x) ) and equilibrium

Qualitative Picture of the Ideal Diode. G.R. Tynan UC San Diego MAE 119 Lecture Notes

smal band gap Saturday, April 9, 2011

Stanford University MatSci 152: Principles of Electronic Materials and Devices Spring Quarter, Final Exam, June 8, 2010

ET3034TUx Utilization of band gap energy

Lecture 2. Introduction to semiconductors Structures and characteristics in semiconductors

Lecture 5 Junction characterisation

Classification of Solids

Fundamentals of Photovoltaics: C1 Problems. R.Treharne, K. Durose, J. Major, T. Veal, V.

UNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences. Professor Chenming Hu.

OPTI510R: Photonics. Khanh Kieu College of Optical Sciences, University of Arizona Meinel building R.626

EECS130 Integrated Circuit Devices

Photovoltaic Energy Conversion. Frank Zimmermann

PN Junction

KATIHAL FİZİĞİ MNT-510

ECE 305 Exam 3: Spring 2015 March 6, 2015 Mark Lundstrom Purdue University

Organic Electronic Devices

Consider a uniformly doped PN junction, in which one region of the semiconductor is uniformly doped with acceptor atoms and the adjacent region is

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

ECE 606 Homework Week 7 Mark Lundstrom Purdue University (revised 2/25/13) e E i! E T

Lecture 15: Optoelectronic devices: Introduction

ECE 440 Lecture 20 : PN Junction Electrostatics II Class Outline:

Lecture 1. OUTLINE Basic Semiconductor Physics. Reading: Chapter 2.1. Semiconductors Intrinsic (undoped) silicon Doping Carrier concentrations

5. Semiconductors and P-N junction

Lecture 6 PN Junction and MOS Electrostatics(III) Metal-Oxide-Semiconductor Structure

Chapter 1 Overview of Semiconductor Materials and Physics

Electronic Supplementary Information. Recombination kinetics in silicon solar cell under low-concentration: Electroanalytical

February 1, 2011 The University of Toledo, Department of Physics and Astronomy SSARE, PVIC

Lab #5 Current/Voltage Curves, Efficiency Measurements and Quantum Efficiency

Semiconductor Physics fall 2012 problems

Semiconductor Physics Problems 2015

ECE 305 Exam 2: Spring 2017 March 10, 2017 Muhammad Alam Purdue University

Lecture 15 - The pn Junction Diode (I) I-V Characteristics. November 1, 2005

UNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences. Professor Ali Javey. Spring 2009.

THE UNIVERSITY OF NEW SOUTH WALES SCHOOL OF PHYSICS FINAL EXAMINATION JUNE/JULY PHYS3080 Solid State Physics

UNIVERSITY OF CALIFORNIA College of Engineering Department of Electrical Engineering and Computer Sciences. EECS 130 Professor Ali Javey Fall 2006

Solar Cell Physics: recombination and generation

Midterm I - Solutions

Engineering 2000 Chapter 8 Semiconductors. ENG2000: R.I. Hornsey Semi: 1

Paper Review. Special Topics in Optical Engineering II (15/1) Minkyu Kim. IEEE Journal of Quantum Electronics, Feb 1985

Solar Photovoltaics & Energy Systems

Supplementary Figure 1. Supplementary Figure 1 Characterization of another locally gated PN junction based on boron

Due to the quantum nature of electrons, one energy state can be occupied only by one electron.

Basic Physics of Semiconductors

UNIVERSITY OF CALIFORNIA, BERKELEY College of Engineering Department of Electrical Engineering and Computer Sciences

6.012 Electronic Devices and Circuits

This is the 15th lecture of this course in which we begin a new topic, Excess Carriers. This topic will be covered in two lectures.

Solar Photovoltaics & Energy Systems

3.1 Absorption and Transparency

EE 446/646 Photovoltaic Devices I. Y. Baghzouz

Toward a 1D Device Model Part 1: Device Fundamentals

collisions of electrons. In semiconductor, in certain temperature ranges the conductivity increases rapidly by increasing temperature

Electronics The basics of semiconductor physics

e - Galvanic Cell 1. Voltage Sources 1.1 Polymer Electrolyte Membrane (PEM) Fuel Cell

Section 12: Intro to Devices

ECE 340 Lecture 21 : P-N Junction II Class Outline:

The Role of doping in the window layer on Performance of a InP Solar Cells USING AMPS-1D

EXAMINATION QUESTION PAPER

EE105 Fall 2015 Microelectronic Devices and Circuits: Semiconductor Fabrication and PN Junctions

pn JUNCTION THE SHOCKLEY MODEL

MODELING THE FUNDAMENTAL LIMIT ON CONVERSION EFFICIENCY OF QD SOLAR CELLS

V BI. H. Föll: kiel.de/matwis/amat/semi_en/kap_2/backbone/r2_2_4.html. different electrochemical potentials (i.e.

EECS130 Integrated Circuit Devices

Semiconductor Detectors

6.012 Electronic Devices and Circuits

16EC401 BASIC ELECTRONIC DEVICES UNIT I PN JUNCTION DIODE. Energy Band Diagram of Conductor, Insulator and Semiconductor:

Free Electron Model for Metals

Review Energy Bands Carrier Density & Mobility Carrier Transport Generation and Recombination

A SEMICONDUCTOR DIODE. P-N Junction

Schottky Rectifiers Zheng Yang (ERF 3017,

Photodiodes and other semiconductor devices

Lecture 2. Introduction to semiconductors Structures and characteristics in semiconductors. Fabrication of semiconductor sensor

3.1 Introduction to Semiconductors. Y. Baghzouz ECE Department UNLV

CLASS 12th. Semiconductors

Junction Diodes. Tim Sumner, Imperial College, Rm: 1009, x /18/2006

Transcription:

Faculty of Science and Technology Exam in: FYS 3028/8028 Solar Energy and Energy Storage Date: 11.05.2016 Time: 9-13 Place: Åsgårdvegen 9 Approved aids: Type of sheets (sqares/lines): Number of pages incl. cover page: Calculator with empty memory Language dictionaries Lines The exam contains 7 pages included this cover page Observe that your answer has to be written in English. Contact person during the exam: Observe that the questions weigh differently, from 1-12 points. Useful data and formulas can be found in the appendix. Tobias Boström Phone: Cell: 4124 8485 PO Box 6050 Langnes, NO-9037 Tromsø / +47 77 64 40 00 / postmottak@uit.no / uit.no

1. You have a pn-junction under illumination. The pn-junction is exposed to three different cases 1) No bias 2) forward bias and 3) reverse bias. For each case, draw the following sketches: a. (3p) Model circuit showing the pn-junction, depletion region with charges and the connection circuit between p and n side b. (3p) Band diagram over the pn-junction, with the conduction and valence band (Fermi level not needed) c. (3p) Illustrate the direction and quantitatively the size (if it is larger, smaller or equal) of the different electron currents present d. (3p) IV-curve and make a X where the working point is 2. (2p) What is conductivity dependent on, and how does temperature affect the conductivity in an intrinsic semiconductor, and what is the conductivity at zero Kelvin? 3. (2p) What is the optimal band gap value for a one band gap solar cell? Also, calculate the equivalent wavelengths the cell can absorb. 4. (2p) What is plasmon resonance and give an example of where it is used in the solar energy field? 5. (4p) Name four major efficiency losses in a crystalline silicon solar cell? Explain them briefly. 6. (2p) In the design of a crystalline silicon solar cell, which are the major material parameters that determine the thickness of the solar cell? 7. (3p) You are designing a solar cell system for the roof on the Realfagsbygget at UiT. The solar cell modules need to be placed in two rows facing south, the modules are fixed at a 40ᵒ angle. The modules are of a standard 60 cell type on 1.0 x 1.5 m 2. What distance should the rows be separated with in order to avoid shading on the second row when the sun is 15ᵒ or higher above the horizon? Should the modules be placed in a portrait or landscape position and why? 8. Draw an IV curve for an ideal diode solar cell in the dark and under illumination. a. (2p) Mark, in your figure, the saturation current and the illumination current for both cases. b. (1p) State the equation each curve is obeying (derived from) 9. (2p) What is the fill factor definition of a solar cell and what is a good fill factor number? 10. (1p) Thin film solar cells often do not have metal front contacts but instead the use transparent conductive oxides. How can TCO s be transparent and still conduct current? 11. (3p) What is a shunt in a solar cell, how can the shunt be created and how can you detect it? 12. A 160-micrometer thick crystalline silicon wafer is doped with 5.0 10 16 acceptors per cubic centimeter. A 1 micrometer thick emitter layer is formed at the surface of this wafer with a uniform concentration of 3.0 10 19 donors per cubic centimeter. Assume that all doping atoms are ionized. The intrinsic carrier concentration in silicon at 27 ᵒC is n i =1.5 x 10 10 cm -3. The effective density of states at the valence UiT / PO Box 6050 Langnes, NO-9037 Tromsø / 77 64 40 00 / postmottak@uit.no / uit.no 2

band N v and at the conduction band N c are respectively 1.0 x 10 19 cm -3 and 3.0 x 10 19 cm -3. The wafer is 27 ᵒC and in thermal equilibrium. a. (2p) How large is the electron and hole concentration in the p-type region and n-type region? Which charge carriers are the majority carriers in the p- type region and what is their concentration? b. (3p) What is the position of the Fermi level (in ev) in respect to the conduction band in the p-type and n-type region, respectively? c. (1p) What is the built-in voltage of the p-n junction? 13. (3p) In this question you should show your reasoning skills (there is no correct answer). Max ½ an A4 page is allowed for your answer. What will be the winning (dominating) electric energy storage technology in the year 2025 for; a. electric grid energy storage? b. electric vehicles? 14. (4p) How does V oc and I sc change when varying the band gap of your semiconductor? Explain by using (and modifying) suitable equations from the appendix. UiT / PO Box 6050 Langnes, NO-9037 Tromsø / 77 64 40 00 / postmottak@uit.no / uit.no 3

Appendix Useful Equations Reflectance from an interface: Anti-reflection optics: n 1 = n 0 n 2 (2) d 1 = λ (3) 4n 1 n 1 = refractive index of ARC n 2 = refractive index of underlying material n 0 = refractive index of the surrounding medium d 1 = thickness of ARC Ideal diode equation: I = I 0 (e (qv/kt) 1) (4) Current from a solar cell: I = I L I 0 (e qv/kt) 1) (5) Lambert Beers Law: I = I initial e αl (6) Light generated current from a solar cell: I L = qag carrier (L p + W + L n ) (7) W = width of the space charge region L = diffusion length of holes and electrons A = Area G carrier = carrier generation term (1) Saturation current: I 0 = qa Dn i 2 LN D D = minority carrier diffusivity N D = doping concentration (8) Intrinsic carrier concentration: n i 2 = np = N c N v e E g kt (9) n = electron concentration p = hole concentration N v = effective density of states at the valence band N c = effective density of states at the conduction band E g = bandgap energy Minority carrier concentration equals to n i 2 divided on the doping concentration (10) UiT / PO Box 6050 Langnes, NO-9037 Tromsø / 77 64 40 00 / postmottak@uit.no / uit.no 4

Width of depletion region: W SCR = 2ε 0ε r ψ 0 q N A = acceptor doping concentration N D = donor doping concentration Built in voltage: ( 1 N A + 1 N D ) (11) ψ 0 = kt q ln (N AN D n i 2 ) (12) Fermi function: Carrier concentration in equilibrium: (13) (14) E F = Fermi level energy E C = Conduction band energy E V = Valence band energy (15) UiT / PO Box 6050 Langnes, NO-9037 Tromsø / 77 64 40 00 / postmottak@uit.no / uit.no 5

Energy of a photon: E = hc λ (16) σ = 1 = qµn ρ (17) σ = Conductivity ρ = Resistivity µ = Mobility η = Efficiency V oc = Open Circuit Voltage I sc = Short Circuit Current FF = Fill Factor P rad = incoming radiation on your solar cell (18) Useful info Figure 1. Absorption coefficient (α) of semiconductor materials. UiT / PO Box 6050 Langnes, NO-9037 Tromsø / 77 64 40 00 / postmottak@uit.no / uit.no 6

ε r (of silicon at RT) = 11.7 UiT / PO Box 6050 Langnes, NO-9037 Tromsø / 77 64 40 00 / postmottak@uit.no / uit.no 7