CHAPTER 1 Voltage Amplifier Amplifier Characteristics

Slides:



Advertisements
Similar presentations
Chapter1: Diodes 1.
Advertisements

3.1 Ideal Diodes Forward bias (on) Reverse bias (off)
Chapter 2 AC to DC CONVERSION (RECTIFIER)
Diodes 1.
Zener effect and Zener diode –When a Zener diode is reverse-biased, it acts at the breakdown region, when it is forward biased, it acts like a normal PN.
Course Outline 1. Chapter 1: Signals and Amplifiers
Electronic Instrumentation Experiment 6: Diodes * Part A: Diode I-V Characteristics * Part B: Rectifiers Part C: PN Junction Voltage Limitation Part D:
Rectification – transforming AC signal into a signal with one polarity – Half wave rectifier Recall Lecture 6 Full Wave Rectifier – Center tapped – Bridge.
C H A P T E R 4 Diodes (non-linear devices)
Diode Theory and Application
Chapter 4. Diodes. Copyright  2004 by Oxford University Press, Inc. Diode Simple non-linear device 2 terminal device, uni- or bi-directional current.
CHAPTER 2 Materials Insulator Conductor Semiconductor Semiconductor: Group 4 eg. Silicon and Germanium Intrinsic Extrinsic N-type P-type Group 5Group 3PN.
Mechatronics 1 Filters & Regulators.
Recall-Lecture 5 Zener effect and Zener diode Avalanche Effect
EE 348: Lecture Supplement Notes SN2 Semiconductor Diodes: Concepts, Models, & Circuits 22 January 2001.
0 Chap. 3 Diodes Simplest semiconductor device Nonlinear Used in power supplies Voltage limiting circuits.
1 © Unitec New Zealand APTE 5601 &DE4401 S EMICONDUCTORS A TOMIC S TRUCTURE DIODES.
Recall Lecture 6 Rectification – transforming AC signal into a signal with one polarity Half wave rectifier Full Wave Rectifier Center tapped Bridge Rectifier.
Physics of Semiconductor Devices
Schottky Barrier Diode One semiconductor region of the pn junction diode can be replaced by a non-ohmic rectifying metal contact.A Schottky.
Example Determine η, FF, RF, TUF, PIV of the diode, CF of the input current, input PF.
Chapter 3 – Diode Circuits – Part 3
DIODES AND APPLICATIONS
Microelectronic Circuit Design McGraw-Hill Chapter 3 Solid-State Diodes and Diode Circuits Microelectronic Circuit Design Richard C. Jaeger Travis N. Blalock.
Chapte r 2 Diode applications Ir. Dr. Rosemizi Abd Rahim 1 Ref: Electronic Devices and Circuit Theory, 10/e, Robert L. Boylestad and Louis Nashelsky.
Application of photodiodes
Recall Lecture 8 Full Wave Rectifier Rectifier Parameters
Recall Lecture 7 Voltage Regulator using Zener Diode
Recall-Lecture 5 DC Analysis Representation of diode into three models
Recall Last Lecture Biasing of BJT Applications of BJT
CHAPTER 2 Forward Biased, DC Analysis AC Analysis Reverse Biased
Chapter 2: Diode Applications
Chapter 1 Introduction to Electronics
Recall-Lecture 3 Atomic structure of Group IV materials particularly on Silicon Intrinsic carrier concentration, ni.
Recall-Lecture 6 Zener effect and Zener diode Avalanche Effect
Recall Last Lecture Biasing of BJT Three types of biasing
Recall Last Lecture Biasing of BJT Three types of biasing
Operational Amplifier
Recall-Lecture 3 Atomic structure of Group IV materials particularly on Silicon Intrinsic carrier concentration, ni.
Recall-Lecture 4 Current generated due to two main factors
Recall Lecture 17 MOSFET DC Analysis
Recall-Lecture 4 Current generated due to two main factors
Semiconductors Principles
Diodes Introduction Textbook CD
Introduction to the pn-junction Diode
Recall-Lecture 5 DC Analysis Representation of diode into three models
EE141 Microelectronic Circuits Chapter 10. Semiconductors, Diodes, and Power Supplies School of Computer Science and Engineering Pusan National University.
PRALLEL CLIPPER The parallel configuration is defined as while the parallel variety has the diode in a branch parallel to the load.
Recall Lecture 7 Voltage Regulator using Zener Diode
Recall-Lecture 6 Diode AC equivalent circuit – small signal analysis
EE141 Microelectronic Circuits Chapter 10. Semiconductors, Diodes, and Power Supplies School of Computer Science and Engineering Pusan National University.
Recall-Lecture 3 Atomic structure of Group IV materials particularly on Silicon Intrinsic carrier concentration, ni.
Diode Theory Chap - 3 Release 1-Sep-2010 Jetking Infotrain Ltd.
Recall Lecture 13 Biasing of BJT Voltage Divider Biasing Circuit.
Electronics Fundamentals
PRESENTATION OF ELECTRONICS-I
Practice #13—RC Circuits Mr. Burleson
دیود دکتر سعید شیری فصل سوم از: & کتابMICROELECTRONIC CIRCUITS 5/e
Recall Lecture 8 Standard Clipper Circuit Clipper in series
Diode Applications.
Recall Lecture 8 Full Wave Rectifier Rectifier Parameters
Review Half Wave Full Wave Rectifier Rectifier Parameters
ChapTer TwO DIODE APPLICATIONS
ELL100: INTRODUCTION TO ELECTRICAL ENGG.
CHAPTER 3 Range of power supply Voltage Regulator VRi = VPS - VZ
Recall-Lecture 5 DC Analysis Representation of diode into three models
Semiconductor Diodes Introduction Diodes
Review Half Wave Full Wave Rectifier Rectifier Parameters
Recall-Lecture 6 Diode AC equivalent circuit – small signal analysis
Review Half Wave Full Wave Rectifier Rectifier Parameters
Presentation transcript:

CHAPTER 1 Voltage Amplifier Amplifier Characteristics AV = Open circuit voltage gain AV vi = Open circuit voltage Ri = input resistance of the amplifier Ro = output resistance of the amplifier Voltage Amplifier Ai = short circuit current gain Ai ii = short circuit current Amplifier Characteristics Current Amplifier Passive and Active Components Analog and Digital Signals CHAPTER 1

Operational Amplifier Inverting Amplifier Op Amp Configurations Summing Amplifier Non - Inverting Amplifier If you don’t remember the formulas, remember these two characteristics and perform nodal analysis vo = Aod ( v2 – v1) Operational Amplifier Open loop mode v1 = v2 to create Aod =  Two main characteristics CHAPTER 8 No current going into the op-amp

CHAPTER 2 Forward Biased, DC Analysis AC Analysis Reverse Biased Model 1 V = 0 Model 2 V Model 3 V and rf Load Line  ID vs VD At 300K VT = 0.026 V Forward Biased, DC Analysis AC Analysis Thermal equilibrium, depletion region Reverse Biased Must perform DC Analysis first to get DC diode current, ID PN junction Group 5 N-type P-type Group 3 Calculate rd = VT / ID Insulator Conductor Semiconductor Extrinsic Semiconductor: Group 4 eg. Silicon and Germanium photodiode Intrinsic Other types of diode Solar cells Materials Bandgap Energy LED CHAPTER 2 Zener Diode

Vm is the peak value of the output voltage Half Wave V r = V m T P RC If the ripple is very small, we can approximate T’ = Tp where Tp is the period of the cycle VC = Vme – t / RC Full Wave V r = V m T P 2RC Vm is the peak value of the output voltage Capacitor Discharge V r = V m T ′ RC Ripple Voltage, Vr Vo = Vs - V Filter Vo = Vs - 2V PIV = 2Vspeak - V Center-tapped Duty Cycle Bridge PIV = Vspeak - V Full Wave Vo = Vs - V CHAPTER 3 Rectifier Half Wave PIV = Vspeak

Consider a silicon pn junction Consider a silicon pn junction. The n-region is doped to a value of Nd = 1016 cm-3. The built in potential barrier is 0.712 V. Determine the required p-doping You need to calculate ni  the required constants will be given 0.712 = 0.026 ln [(Na )(1016) / (1.5 x 1010)2] e (0.712/0.026) = [(Na )(1016) / (1.5 x 1010)2] Na = 1.76 x 1016 cm-3

A diode is biased at ID = 1mA A diode is biased at ID = 1mA. The peak to peak of its sinusoidal current is 0.05 ID. Find the value of the diode sinusoidal voltage, vd (peak-to-peak) AC analysis only since ID already calculated rd = VT / ID = 0.026 / 1mA = 26  vd = idrd = 0.05 mA (26) = 1.3 mV (peak to peak) rd id

Full wave rectifier with iDpeak = 0. 2 A and vOpeak = 12 V Full wave rectifier with iDpeak = 0.2 A and vOpeak = 12 V. Ripple voltage is to be limited to 0.25 V. The input signal is 120 V (rms) at 60 Hz. Assume V = 0.7 V Determine the required turns ratio Find the required value of the capacitor What is the PIV rating of the diode

Part (i) 0.7 + VO – VS = 0 VS peak = 12.7V Change to rms 8.98 V (rms) Turns ratio = 120 / 8.98 = 13.36 Part (ii) For full wave: V r = V m T P 2RC Vr is given as 0.25V R? vOpeak = 12 V R = 12 / 0.2 = 60  0.25 (2)(60)(C) = 12 (1/60) C = 6667 µF Part (iii) PIV for center-tapped: 2VSpeak - V = 2(12.7) – 0.7 = 24.7 V

Full wave battery charger circuit Full wave battery charger circuit. Given that VB = 9V and vs = 15 sin ( 2ᴨ60t) (V). Assume V = 0.7 V Determine R such that the peak current is 1.2 A Determine the fraction of time that each diode is conducting

Part (i) 0.7 + IDR + 9 – 15 = 0 R = (15 – 9 – 0.7) / 1.2 R = 4.42  Part (ii) VS must be at least 9.7 V 15 sin ( 2ᴨ60t) = 9.7 sin ( 2ᴨ60t) = 0.64667 2ᴨ60t = 40.29 and 139.7 Duty cycle for each diode = ( 139.7 – 40.29) / 360 ) = 27.6%