4/10/06 Transistors, Analog, and Digital Wednesday’s Reading: Section 13.1: Radio (pp. 423 – 431) Upcoming Reading Assignments: Section 13.2: Microwave.

Slides:



Advertisements
Similar presentations
TOC 1 Physics 212 and 222 Circuit Elements and Electric Power Resistors Capacitors Inductors.
Advertisements

PN Junction ES230 Jack Ou. Review What if we introduce n-type and p-type dopants into two adjacent sections of a piece of silicon?
1 Slides taken from: A.R. Hambley, Electronics, © Prentice Hall, 2/e, 2000 A. Sedra and K.C. Smith, Microelectronic Circuits, © Oxford University Press,
Course: ETE 107 Electronics 1 Course Instructor: Rashedul Islam
ELECTRONICS P.MUNIREDDY GOVT.H.S, SANTHIPURAM BAND THEORY OF SOLIDS INTRINSIC and EXTRINSIC SEMICONDUCTORS JUNCTION DIODE –PROPERTIES AND USES TRANSISTORS.
Semiconductor basics 1. Vacuum tubes  Diode  Triode 2. Semiconductors  Diode  Transistors Bipolar Bipolar Field Effect Field Effect 3. What’s next?
Basic Electricity and Electronics Mr. McClean Concepts of Engineering and Technology Copyright © Texas Education Agency, All rights reserved.
4/7/06 Capacitors & Diodes Monday’s Reading: Section 12.2: Audio Players (pp. 404 – 411); stop at “The Audio Player’s Computer”. Upcoming Reading Assignments:
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.
4/14/06 More Electromagnetic Waves Monday’s Reading: Section 14.1: Sunlight (pp. 443 – 453) Upcoming Reading Assignments: Section 14.2: Discharge Lamps.
What We’ve Learned So Far A Review of Topics on Test 2.
Lecture 11: MOS Transistor
Announcements Assignment 1 solutions posted Assignment 2 due Thursday First mid-term Thursday October 27 th (?)
Circuits Resistors, Capacitors and Inductors 1 Resistors Capacitors Inductors.
PN-Junction Diode Characteristics
Department of Information Engineering256 Semiconductor Conduction is possible only if the electrons are free to move –But electrons are bound to their.
4/12/06 Electromagnetic Waves and Radio Friday’s Reading: Section 13.2: Microwave Ovens (pp. 432 – 438) Upcoming Reading Assignments: Section 14.1: Sunlight.
4/17/06 Sunlight Wednesday’s Reading: Section 14.2: Discharge Lamps (pp. 454 – 463) This afternoon: Lab #10 Upcoming Reading Assignments: Section 14.3:
Lecture 101 Capacitors (5.1); Inductors (5.2); LC Combinations (5.3) Prof. Phillips March 7, 2003.
Putting Electrons to Work Doping and Semiconductor Devices.
WEEK ONE TOPIC: ELECTRONICS SOLID STATE MATERIALS  CONDUCTORS  INSULATORS  SEMICONDUCTORS.
Power Adapters 1 Power Adapters. Power Adapters 2 Introductory Question If you install a pocket radio’s batteries backward, it won’t work because its.
1 SEMICONDUCTOR Diodes PN junction and diode biasing Diodes PN junction and diode biasing.
Unit 7, Chapter 24 CPO Science Foundations of Physics.
Depletion Region ECE Depletion Region As electrons diffuse from the n region into the p region and holes diffuse from the p region into the n region,
Lecture 25: Semiconductors
Alternating Current Circuits
EMT111 CHAPTER 1 Introduction to Semiconductor By Pn
A semiconductor material is one which conducts only when excited.
Higher Physics Semiconductor Diodes. Light Emitting Diode 1  An LED is a forward biased diode  When a current flows, electron-hole pairs combine at.
Audio Amplifiers. Question: If you install a pocket radio’s batteries backward, it won’t work because its 1.speaker will move the wrong direction. 2.parts.
Drift and Diffusion Current
General Licensing Class Oscillators & Components Your organization and dates here.
Electric Components. Basics 1 Current: electrons moving together in same direction (electrons are always moving in materials like metals but in a random.
P-N Junctions Physical aspects of pn junctions Mathematical models Depletion capacitance Breakdown characteristics Basis for other devices Circuit Symbol.
PN Junction Section
Basic Circuit Components
Kristin Ackerson, Virginia Tech EE Spring The diode is the simplest and most fundamental nonlinear circuit element. Just like resistor, it has.
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 ),
1 Metal-Oxide-Semicondutor FET (MOSFET) Copyright  2004 by Oxford University Press, Inc. 2 Figure 4.1 Physical structure of the enhancement-type NMOS.
Semiconductors. A semiconductor is a material whose resistance is between that of a conductor and an insulator. Eg Silicon.
CHAPTER 1 Introduction To Diodes. OBJECTIVES Describe and Analyze: Function of Diodes Some Physics of Diodes Diode Models.
Lecture 7.0 Device Physics. Electronic Devices Passive Components Resistance (real #) –Conductor –Resistor –Battery Active Components Reactance (Imaginary.
Review for Exam 2 Spring, 2002 Charges in Conductors  Electric fields are created when positive charges and negative charges are separated  A uniform.
Chapter Intrinsic: -- case for pure Si -- # electrons = # holes (n = p) Extrinsic: -- electrical behavior is determined by presence of impurities.
Field Effect Transistor. What is FET FET is abbreviation of Field Effect Transistor. This is a transistor in which current is controlled by voltage only.
Semiconductor Introduction ENGI 242 ELEC 222. January 2004ENGI 242/ELEC 2222 Specification Symbol Notation Standard Type of valueSymbolSubscript Instantaneous.
Electronics The Seventh and Eighth and Lectures Eighth week 28 / 12/ 1436 هـ - 1 / 1/ 1437 هـ أ / سمر السلمي.
MOSFET Placing an insulating layer between the gate and the channel allows for a wider range of control (gate) voltages and further decreases the gate.
Conductors – many electrons free to move
PN-Junction Diode Characteristics
1 Higher Physics Unit 3 Optoelectronics Semiconductors.
Putting Electrons to Work Doping and Semiconductor Devices.
Introduction to Semiconductors
Ohm’s Law Resistance in Series Circuits
PRACTICAL # 11 Introduction to light emitting diode (LED), its working principle and terminal identification By:Engr.Irshad Rahim Memon.
Lab Experiment: 3 Objectives: To understand the Transistor’s characteristics. Construct the Transistor circuit ( Common base and common emitter connection.
Problems All problems up to p.28 Q 4 can be done.
CHAPTER 6: MOSFET & RELATED DEVICES CHAPTER 6: MOSFET & RELATED DEVICES Part 2.
Semiconductors – Learning Outcomes
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.
Basic Circuit Components Name: gohel khushbu dilipbhai. Enrollment no: Subject : Basic electronics Branch : Co(Shift -1)
WARM UP Two negative charges, one twice as large as the other, are located 0.05 m apart and experience a repulsive force of 5 N. What is the magnitude.
Introduction Semiconductors are materials whose electrical properties lie between Conductors and Insulators. Ex : Silicon and Germanium.
Intrinsic. N-Type P-Type The Diode and PN Junction.
INTRODUCTION TO SEMICONDUCTORS
Intro to Semiconductors and p-n junction devices
Semiconductors Chapter 25.
Higher Physics Electricity.
Chapter 1 – Semiconductor Devices – Part 2
Presentation transcript:

4/10/06 Transistors, Analog, and Digital Wednesday’s Reading: Section 13.1: Radio (pp. 423 – 431) Upcoming Reading Assignments: Section 13.2: Microwave Ovens (pp. 432 – 438) Section 14.1: Sunlight (pp. 445 – 453) Section 14.2: Discharge Lamps (pp. 454 – 463) Section 14.3: Lasers and LEDs (pp. 464 – 470) Section 15.1: Cameras (pp. 478 – 488) Section 15.2: Optical Recording and Communication (pp. 489 – 497) Poster Session Meetings Schedule appointment Change/Modify your topic Plan your poster Etc. Lab #9 this afternoon Bring N pole marked magnet

Capacitors Two closely spaced conducting plates Separated by a thin insulating layer Holds charge (equal and opposite, overall neutral) Potential difference between plates (charge, geometry) Applications: “Slows” things down “Stores” Charge, Potential Difference Memory Keyboards

Start with good insulator Add small impurity that “opens” up some “space” in the valence band; P(ositive)-type or p-type Add small impurity that “add” some electrons to conduction band; N(egative)-type or n-type Semi-conductors and p-n junction Taken from howstuffworks.com

Biasing the Junction

Diodes p-type semi-conductor joined to n-type semi-conductor p-n junction Results in “depletion” region Apply a potential difference across junction (like hooking up battery) “Reverse bias”  increases depletion region “Forward bias”  enough potential shrinks depletion region to nothing No depletion region means current can flow. So results in current flow in one direction! Resistors Resistance Rule (Ohm’s Law): Current proportional to voltage drop

Power Adapter

Transistors

n-channel MOSFET Metal-Oxide-Semiconductor Field Effect Transistor

Analog and Digital

Memory RAM vs. ROM Volatile vs. Non-Volatile