Lesson 23: Introduction to Solar Energy and Photo Cells ET 332a Dc Motors, Generators and Energy Conversion Devices 1Lesson 23 332a.pptx.

Slides:



Advertisements
Similar presentations
ELECTRICAL CONDUCTIVITY
Advertisements

ECE G201: Introductory Material Goal: to give you a quick, intuitive concept of how semiconductors, diodes, BJTs and MOSFETs work –as a review of electronics.
Physics of Semiconductor Devices. Formation of PN - Junction When a P-type Semiconductor is joined together with an N-type Semiconductor a PN junction.
Course: ETE 107 Electronics 1 Course Instructor: Rashedul Islam
MALVINO Electronic PRINCIPLES SIXTH EDITION.
Introduction to electronics (Syllabus)
Conduction in Metals Atoms form a crystal Atoms are in close proximity to each other Outer, loosely-bound valence electron are not associated with any.
Semiconductor Physics - 1Copyright © by John Wiley & Sons 2003 Review of Basic Semiconductor Physics.
Doped Semiconductors Group IVA semiconductors can be “doped” by adding small amounts of impurities with more or fewer than 4 valence electrons. e.g. add.
Department of Aeronautics and Astronautics NCKU Nano and MEMS Technology LAB. 1 Chapter I Introduction June 20, 2015June 20, 2015June 20, 2015.
Ideal Diode Model.
Department of Information Engineering256 Semiconductor Conduction is possible only if the electrons are free to move –But electrons are bound to their.
1 Renewable Energy Sources. Solar Cells SJSU-E10 S-2008 John Athanasiou.
P and n type semiconductors. Semiconductors Semiconductors are also referred to as metalloids. Metalloids occur at the division between metals and non-metals.
Main detector types Scintillation Detector Spectrum.
EE580 – Solar Cells Todd J. Kaiser Lecture 05 P-N Junction 1Montana State University: Solar Cells Lecture 5: P-N Junction.
PV Panels and P N Junctions How PV Panels work Or An Introduction to the World of Microelctronics.
Lesson 24: Photocell Electrical Characteristic and Circuit Model ET 332a Dc Motors, Generators and Energy Conversion Devices 1Lesson a.pptx.
WEEK ONE TOPIC: ELECTRONICS SOLID STATE MATERIALS  CONDUCTORS  INSULATORS  SEMICONDUCTORS.
1 SEMICONDUCTOR Diodes PN junction and diode biasing Diodes PN junction and diode biasing.
Introduction to Semiconductor Materials
Solar Cells Early development of solar tech. starts in the 1960s Conversion of sunlight to electricity – by photovoltaic effect In 1974 only.
ECE 3336 Introduction to Circuits & Electronics Dr. Dave Shattuck Associate Professor, ECE Dept. Lecture Set #17 Diodes W326-D3.
Case Study: Solar cells
Higher Physics Semiconductor Diodes. Light Emitting Diode 1  An LED is a forward biased diode  When a current flows, electron-hole pairs combine at.
Electronic Devices and Circuit Theory
Electric Current. Current Rate at which charge flows through a surface. Ex. If the charge on a capacitor changes by the function Q(t)=6(1-e  0.1t ),
Semiconductors. A semiconductor is a material whose resistance is between that of a conductor and an insulator. Eg Silicon.
Electronics 1 Lecture 2 Ahsan Khawaja Lecturer Room 102 Department of Electrical Engineering.
Fresnel Lens Seen in lighthouses- used to form a concentrated beam of light.
Presentation on: ELECTROMAGNETISM Topic: SEMICONDUCTORS Presented to: SIR.TARIQ BHATTI Program: BsIT-3rd Department of Computer Science.
Semiconductor Introduction ENGI 242 ELEC 222. January 2004ENGI 242/ELEC 2222 Specification Symbol Notation Standard Type of valueSymbolSubscript Instantaneous.
29-1Bonding in Molecules *When atoms cling together as a single unit to achieve lower energy levels, this is a chemical bond. *Bonds occur as ionic an.
Detectors (UV-Vis) 1. Phototube 2. Photomultiplier Tube (PMT) 3. Si Photodiode 4. Photodiode Array (PDA) 5. Charge Coupled Device (CCD) 6. Charge Injection.
P-N JUNCTION DIODE Electronics. OBJECTIVE 1. describe the electrical properties of semiconductors and distinguish between p-type and n-type material;
ELECTRONIC PROPERTIES OF MATTER - Semi-conductors and the p-n junction -
Introduction to Semiconductor Materials
Band Theory of Solids In isolated atoms the electrons are arranged in energy levels.
Extended Questions- The Answers
By Squadron Leader Zahid Mir CS&IT Department, Superior University PHY-BE -13 Light Emitting Diode & Tunnel Diode.
Conductors – many electrons free to move
1. Unit I: Semiconductor Diodes and Applications Before we start with Electronics Let us review the Basics of Electricity Q. What are the two main quantities.
1 Higher Physics Unit 3 Optoelectronics Semiconductors.
Introduction to Semiconductors
UNIT- IV SOLID STATE PHYSICS. 1)Electrical conductivity in between conductors & insulators is a) high conductors b) low conductors c) Semiconductors d)
Introduction to Solar Photovoltaic (PV) Systems – Part 2
Optoelectronics.
Problems All problems up to p.28 Q 4 can be done.
Solar Cell Semiconductor Physics
1 Semiconductor Devices  Metal-semiconductor junction  Rectifier (Schottky contact or Schottky barrier)  Ohmic contact  p – n rectifier  Zener diode.
Based on current conduction, materials are classifieds as 1)Insulators Ex: Wood, Mica, Diamond 2) Conductors Ex: Copper, Aluminium 3) Semiconductors Ex:
Semiconductors – Learning Outcomes
Properties of metals Metals (75% of elements) Lustrous (reflect light)
Semiconductors. O A Semiconductor is a material whose resistivity is between that of a good conductor and a good insulator. O Examples of materials which.
Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. MALVINO & BATES SEVENTH EDITION Electronic PRINCIPLES.
Electronics Technology Fundamentals Chapter 17 Introduction to Solid State Components: Diodes.
ELECTRONICS. FUNDAMENTALS OF ELECTRONICS ELECTRONICS Electronics is the branch of physics which deals with development of electron-emitting devices, there.
ELECTONICS & COMMUNICATION SEM-3 YEAR SUBJECT-ELECTCTRONICS DEVICE &CIRCUIT SUBJECT CODE ACTIVE LEARING ASSIGNMENT.
Band Theory of Electronic Structure in Solids
INTRODUCTION TO SEMICONDUCTORS
COURSE NAME: SEMICONDUCTORS Course Code: PHYS 473.
Physics of Semiconductor Devices
Application of photodiodes
Multiple choise questions related to lecture PV2
Parul Institute of Engineering & Technology
Semiconductors. Silicon crystal Types of semiconductors
Semiconductor Fundamentals
Semiconductors Chapter 25.
Higher Physics Electricity.
Presentation transcript:

Lesson 23: Introduction to Solar Energy and Photo Cells ET 332a Dc Motors, Generators and Energy Conversion Devices 1Lesson a.pptx

2 Learning Objectives After this presentation you will be able to:  Identify the solar spectrum  Determine the angle that captures the maximum solar energy  Explain the atomic difference between conductor, insulators, and semiconductors  Explain physics behind the photoelectric effect  Compute the open circuit voltage and short circuit current of a photocell

Lesson a.pptx3 Solar Energy and Photocells Solar Spectrum AM0 =1.36 kW/m 2 Incident on Atmosphere AM kW/m 2 Passing through Atmosphere Incident to 48 0 angle to vertical Includes absorption of water vapor, C0 2, methane.

Lesson a.pptx4 Solar Energy Conversion Direct Radiation depends on season, location, cloudiness. Yearly average 30% Average Intensity (W/m 2 ) 10% in lower Canada to 50% in tropics Solar Array Sun Defuse Radiation unfocusable. Long wavelengths scatter more color sky blue. Solar Radiation perpendicular to Array Surface

Lesson a.pptx5 Solar Intensity

Lesson a.pptx6 Solar Intensity

Lesson a.pptx7 Conductors, Insulators and Semiconductors Semiconductors – Valence electrons exist Bonded to other atoms Bonds broken by external energy like heat or light Examples: Silicon, Germanium Conductors – Free electrons in atomic structure Valence electrons form current when electric potential applied. Examples: copper, silver Insulators – No free electrons in valence band Examples: glass, plastics.

Lesson a.pptx8 Semiconductors Doped Semiconductors – Impurities added to increase conductance P-type semiconductor - excess holes (absent electrons) N-type semiconductor – excess electrons Charge drift forms Depletion Zone PN Junction

Lesson a.pptx9 Forward Biased PN Junction V lowers potential barrier for electrons upsets balance I flows Forward Bias

Lesson a.pptx10 Solar.ppt10 PN Junction-Diode Operation PN Junction Characteristic V  = cut-in voltage 0.6 V for silicon Junction conducts when forward biased V T = Voltage-equivalent of Temperature = V at room temperature I s = saturation current depends on junction area and doping

Lesson a.pptx11 Photoelectric Effect Photon E >1.1 eV I C = cell current I L = reverse current Light striking a PN junction creates currents. Photons must have sufficient energy increase electron energy and create Electron/hole pairs

Lesson a.pptx12 Open Circuit Voltage/Short Circuit Current Open circuit means R= ∞ and I C =0, so open circuit voltage is V T = V at room temperature I s = saturation current I L = reverse current Cell power output given by

END LESSON 23 ET 332a Dc Motors, Generators and Energy Conversion Devices Lesson a.pptx13