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ECE 255, MOSFET Basic Configurations
ECE 255, MOSFET Basic Configurations 8 March 2018 In this lecture, we will go back to Section 7.3, and the basic configurations of MOSFET amplifiers will be studied similar to that of BJT. Previously, it has been shown that with the transistor DC biased at the appropriate point (Q point or operating point), linear relations can be derived between the small voltage signal and current signal. We will continue this analysis with MOSFETs, starting with the common-source amplifier. 1 Common-Source (CS) Amplifier The common-source (CS) amplifier for MOSFET is the analogue of the common- emitter amplifier for BJT. Its popularity arises from its high gain, and that by cascading a number of them, larger amplification of the signal can be achieved. 1.1 Chararacteristic Parameters of the CS Amplifier Figure 1(a) shows the small-signal model for the common-source amplifier. Here, RD is considered part of the amplifier and is the resistance that one measures between the drain and the ground. The small-signal model can be replaced by its hybrid-π model as shown in Figure 1(b). Then the current induced in the output port is i = −gmvgs as indicated by the current source. Thus vo = −gmvgsRD (1.1) By inspection, one sees that Rin = 1; vi = vsig; vgs = vi (1.2) Thus the open-circuit voltage gain is vo Avo = = −gmRD (1.3) vi Printed on March 14, 2018 at 10 : 48: W.C. Chew and S.K. Gupta. 1 One can replace a linear circuit driven by a source by its Th´evenin equivalence. -
Thyristors.Pdf
THYRISTORS Electronic Devices, 9th edition © 2012 Pearson Education. Upper Saddle River, NJ, 07458. Thomas L. Floyd All rights reserved. Thyristors Thyristors are a class of semiconductor devices characterized by 4-layers of alternating p and n material. Four-layer devices act as either open or closed switches; for this reason, they are most frequently used in control applications. Some thyristors and their symbols are (a) 4-layer diode (b) SCR (c) Diac (d) Triac (e) SCS Electronic Devices, 9th edition © 2012 Pearson Education. Upper Saddle River, NJ, 07458. Thomas L. Floyd All rights reserved. The Four-Layer Diode The 4-layer diode (or Shockley diode) is a type of thyristor that acts something like an ordinary diode but conducts in the forward direction only after a certain anode to cathode voltage called the forward-breakover voltage is reached. The basic construction of a 4-layer diode and its schematic symbol are shown The 4-layer diode has two leads, labeled the anode (A) and the Anode (A) A cathode (K). p 1 n The symbol reminds you that it acts 2 p like a diode. It does not conduct 3 when it is reverse-biased. n Cathode (K) K Electronic Devices, 9th edition © 2012 Pearson Education. Upper Saddle River, NJ, 07458. Thomas L. Floyd All rights reserved. The Four-Layer Diode The concept of 4-layer devices is usually shown as an equivalent circuit of a pnp and an npn transistor. Ideally, these devices would not conduct, but when forward biased, if there is sufficient leakage current in the upper pnp device, it can act as base current to the lower npn device causing it to conduct and bringing both transistors into saturation. -
First-Order Circuits
CHAPTER SIX FIRST-ORDER CIRCUITS Chapters 2 to 5 have been devoted exclusively to circuits made of resistors and independent sources. The resistors may contain two or more terminals and may be linear or nonlinear, time-varying or time-invariant. We have shown that these resistive circuits are always governed by algebraic equations. In this chapter, we introduce two new circuit elements, namely, two- terminal capacitors and inductors. We will see that these elements differ from resistors in a fundamental way: They are lossless, and therefore energy is not dissipated but merely stored in these elements. A circuit is said to be dynamic if it includes some capacitor(s) or some inductor(s) or both. In general, dynamic circuits are governed by differential equations. In this initial chapter on dynamic circuits, we consider the simplest subclass described by only one first-order differential equation-hence the name first-order circuits. They include all circuits containing one 2-terminal capacitor (or inductor), plus resistors and independent sources. The important concepts of initial state, equilibrium state, and time constant allow us to find the solution of any first-order linear time-invariant circuit driven by dc sources by inspection (Sec. 3.1). Students should master this material before plunging into the following sections where the inspection method is extended to include linear switching circuits in Sec. 4 and piecewise- linear circuits in Sec. 5. Here,-the important concept of a dynamic route plays a crucial role in the analysis of piecewise-linear circuits by inspection. l TWO-TERMINAL CAPACITORS AND INDUCTORS Many devices cannot be modeled accurately using only resistors. -
Robust Wireless Power Transfer Using a Nonlinear Parity–Time-Symmetric Circuit Sid Assawaworrarit1, Xiaofang Yu1 & Shanhui Fan1
LETTER doi:10.1038/nature22404 Robust wireless power transfer using a nonlinear parity–time-symmetric circuit Sid Assawaworrarit1, Xiaofang Yu1 & Shanhui Fan1 Considerable progress in wireless power transfer has been made in PT-symmetric systems are invariant under the joint parity and the realm of non-radiative transfer, which employs magnetic-field time reversal operation14,15. In optical systems, where the symmetry coupling in the near field1–4. A combination of circuit resonance conditions can be met by engineering the gain/loss regions and and impedance transformation is often used to help to achieve their coupling, PT-symmetric systems have exhibited unusual efficient transfer of power over a predetermined distance of about properties16–20. A linear PT-symmetric system supports two phases, the size of the resonators3,4. The development of non-radiative depending on the magnitude of the gain/loss relative to the coupling wireless power transfer has paved the way towards real-world strength. In the unbroken or exact phase, eigenmode frequencies applications such as wireless powering of implantable medical remain real and energy is equally distributed between the gain and devices and wireless charging of stationary electric vehicles1,2,5–8. loss regions; in the broken phase, one of the eigenmodes grows expo- However, it remains a fundamental challenge to create a wireless nentially while the other decays exponentially. Recently, the concept power transfer system in which the transfer efficiency is robust of PT symmetry has been extensively explored in laser structures21–24. against the variation of operating conditions. Here we propose Theoretically, the inclusion of nonlinear gain saturation in the analysis theoretically and demonstrate experimentally that a parity–time- of a PT-symmetric system causes that system to reach a steady state symmetric circuit incorporating a nonlinear gain saturation element in a laser-like fashion that still contains the following PT symmetry provides robust wireless power transfer. -
Basic Electrical Engineering
BASIC ELECTRICAL ENGINEERING V.HimaBindu V.V.S Madhuri Chandrashekar.D GOKARAJU RANGARAJU INSTITUTE OF ENGINEERING AND TECHNOLOGY (Autonomous) Index: 1. Syllabus……………………………………………….……….. .1 2. Ohm’s Law………………………………………….…………..3 3. KVL,KCL…………………………………………….……….. .4 4. Nodes,Branches& Loops…………………….……….………. 5 5. Series elements & Voltage Division………..………….……….6 6. Parallel elements & Current Division……………….………...7 7. Star-Delta transformation…………………………….………..8 8. Independent Sources …………………………………..……….9 9. Dependent sources……………………………………………12 10. Source Transformation:…………………………………….…13 11. Review of Complex Number…………………………………..16 12. Phasor Representation:………………….…………………….19 13. Phasor Relationship with a pure resistance……………..……23 14. Phasor Relationship with a pure inductance………………....24 15. Phasor Relationship with a pure capacitance………..……….25 16. Series and Parallel combinations of Inductors………….……30 17. Series and parallel connection of capacitors……………...…..32 18. Mesh Analysis…………………………………………………..34 19. Nodal Analysis……………………………………………….…37 20. Average, RMS values……………….……………………….....43 21. R-L Series Circuit……………………………………………...47 22. R-C Series circuit……………………………………………....50 23. R-L-C Series circuit…………………………………………....53 24. Real, reactive & Apparent Power…………………………….56 25. Power triangle……………………………………………….....61 26. Series Resonance……………………………………………….66 27. Parallel Resonance……………………………………………..69 28. Thevenin’s Theorem…………………………………………...72 29. Norton’s Theorem……………………………………………...75 30. Superposition Theorem………………………………………..79 31. -
Eimac Care and Feeding of Tubes Part 3
SECTION 3 ELECTRICAL DESIGN CONSIDERATIONS 3.1 CLASS OF OPERATION Most power grid tubes used in AF or RF amplifiers can be operated over a wide range of grid bias voltage (or in the case of grounded grid configuration, cathode bias voltage) as determined by specific performance requirements such as gain, linearity and efficiency. Changes in the bias voltage will vary the conduction angle (that being the portion of the 360° cycle of varying anode voltage during which anode current flows.) A useful system has been developed that identifies several common conditions of bias voltage (and resulting anode current conduction angle). The classifications thus assigned allow one to easily differentiate between the various operating conditions. Class A is generally considered to define a conduction angle of 360°, class B is a conduction angle of 180°, with class C less than 180° conduction angle. Class AB defines operation in the range between 180° and 360° of conduction. This class is further defined by using subscripts 1 and 2. Class AB1 has no grid current flow and class AB2 has some grid current flow during the anode conduction angle. Example Class AB2 operation - denotes an anode current conduction angle of 180° to 360° degrees and that grid current is flowing. The class of operation has nothing to do with whether a tube is grid- driven or cathode-driven. The magnitude of the grid bias voltage establishes the class of operation; the amount of drive voltage applied to the tube determines the actual conduction angle. The anode current conduction angle will determine to a great extent the overall anode efficiency. -
Chapter 2: Kirchhoff Law and the Thvenin Theorem
Chapter 3: Capacitors, Inductors, and Complex Impedance Chapter 3: Capacitors, Inductors, and Complex Impedance In this chapter we introduce the concept of complex resistance, or impedance, by studying two reactive circuit elements, the capacitor and the inductor. We will study capacitors and inductors using differential equations and Fourier analysis and from these derive their impedance. Capacitors and inductors are used primarily in circuits involving time-dependent voltages and currents, such as AC circuits. I. AC Voltages and circuits Most electronic circuits involve time-dependent voltages and currents. An important class of time-dependent signal is the sinusoidal voltage (or current), also known as an AC signal (Alternating Current). Kirchhoff’s laws and Ohm’s law still apply (they always apply), but one must be careful to differentiate between time-averaged and instantaneous quantities. An AC voltage (or signal) is of the form: V(t) =Vp cos(ωt) (3.1) where ω is the angular frequency, Vp is the amplitude of the waveform or the peak voltage and t is the time. The angular frequency is related to the freguency (f) by ω=2πf and the period (T) is related to the frequency by T=1/f. Other useful voltages are also commonly defined. They include the peak-to-peak voltage (Vpp) which is twice the amplitude and the RMS voltage (VRMS) which is VVRMS = p / 2 . Average power in a resistive AC device is computed using RMS quantities: P=IRMSVRMS = IpVp/2. (3.2) This is important enough that voltmeters and ammeters in AC mode actually return the RMS values for current and voltage. -
Shults Robert D 196308 Ms 10
AN INVESTIGATION OF THE INFLUENCE OF CIRCUIT PARAMETERS ON THE OUTPUT WAVESHAPE OF A TUNNEL DIODE OSCILLATOR A THESIS Presented to The Faculty of the Graduate Division by Robert David Shults In Partial Fulfillment of the Requirements for the Degree Master of Science in Electrical Engineering Georgia Institute of Technology June, I963 AN INVESTIGATION OF THE INFLUENCE OF CIRCUIT PARAMETERS ON THE OUTPUT WAVESHAPE OF A TUNNEL DIODE OSCILLATOR Approved: —VY -w/T //'- Dr. W. B.l/Jonesj UJr. (Chairman) _A a t~l — Dry 3* L. Hammond, Jr. V ^^ __—^ '-" ^^ *• Br> J. T. Wang * Date Approved by Chairman: //l&U (A* l/j^Z) In presenting the dissertation as a partial, fulfillment of the requirements for an advanced degree from the Georgia Institute of Technology, I agree that the Library of the Institution shall make it available for inspection and circulation in accordance witn its regulations governing materials of this type. I agree -chat permission to copy from, or to publish from, this dissertation may be granted by the professor under whose direction it was written^ or, in his absence, by the dean of the Graduate Division when luch copying or publication is solely for scholarly purposes ftad does not involve potential financial gain. It is under stood that any copying from, or publication of, this disser tation which involves potential financial gain will not be allowed without written permission. _/2^ d- ii ACKNOWLEDGMEBTTS The author wishes to thank his thesis advisor, Dr. W. B„ Jones, Jr., for his suggestion of the problem and for his continued guidance and encouragement during the course of the investigation. -
Linear Electronic Circuits and Systems Graham Bishop Beginning Basic P.E
Linear Electronic Circuits andSystems Macmillan Basis Books in Electronics General Editor Noel M. Morris, Principal Lecturer, North Staffordshire Polytechnic Linear Electronic Circuits and Systems Graham Bishop Beginning Basic P.E. Gosling Continuing Basic P.E.Gosling Microprocessors and Microcomputers Eric Huggins Digital Electronic Circuits and Systems Noel M. Morris Electrical Circuits and Systems Noel M. Morris Microprocessor and Microcomputer Technology Noel M. Morris Semiconductor Devices Noel M. Morris Other related books Electrical and Electronic Systems and Practice Graham Bishop Electronics for Technicians Graham Bishop Digital Techniques Noel M. Morris Electrical Principles Noel M. Morris Essential Formulae for Electronic and Electrical Engineers: New Pocket Book Format Noel M. Morris Mastering Electronics John Watson Linear Electronic Circuits andSystems SECOND EDITION Graham Bishop Vice Principal Bridgwater College M MACMI LLAN PRESS LONDON © G. D. Bishop 1974, 1983 All rights reserved. No part of this publication may be reproduced or transmitted, in any form or by any means, without permission First edition 1974 Second edition 1983 Published by THE MACMILLAN PRESS LTD London and Basingstoke Companies and representatives throughout the world ISBN 978-0-333-35858-0 ISBN 978-1-349-06914-9 (eBook) DOI 10.1007/978-1-349-06914-9 Contents Foreword viii Preface to the First Edition ix Preface to the Second Edition xi 1 Signal processing 1 1.1 Voltages and currents 1 1.2 Transient responses 4 1.3 R-L-C transients 6 1.4 The d.c. restorer -
Effect of Load Impedance on the Performance of Microwave Negative Resistance Oscillators
Effect of Load Impedance on the Firas M. Ali , Suhad H. Jasim Issue No. 39/2016 Performance of Microwave… Effect of Load Impedance on the Performance of Microwave Negative Resistance Oscillators Firas Mohammed Ali Al-Raie [email protected] University of Technology - Department of Electrical Engineering - Baghdad - Iraq Suhad Hussein Jasim [email protected] University of Technology - Department of Electrical Engineering - Baghdad - Iraq Abstract: In microwave negative resistance oscillators, the RF transistor presents impedance with a negative real part at either of its input or output ports. According to the conventional theory of microwave negative resistance oscillators, in order to sustain oscillation and optimize the output power of the circuit, the magnitude of the negative real part of the input/output impedance should be maximized. This paper discusses the effect of the circuit’s load impedance on the input negative resistance and other oscillator performance characteristics in common base microwave oscillators. New closed-form relations for the optimum load impedance that maximizes the magnitude of the input negative resistance have been derived analytically in terms of the Z- parameters of the RF transistor. Furthermore, nonlinear CAD simulation is carried out to show the deviation of the large-signal Journal of Al Rafidain University College 427 ISSN (1681-6870) Effect of Load Impedance on the Firas M. Ali , Suhad H. Jasim Issue No. 39/2016 Performance of Microwave… optimum load impedance from its small-signal value. It has been shown also that the optimum load impedance for maximum negative input resistance differs considerably from its value required for maximum output power under large-signal conditions. -
Capacitors, Inductors, and First-Order Linear Circuits Overview
EECE251 Circuit Analysis I Set 4: Capacitors, Inductors, and First-Order Linear Circuits Shahriar Mirabbasi Department of Electrical and Computer Engineering University of British Columbia [email protected] SM 1 EECE 251, Set 4 Overview • Passive elements that we have seen so far: resistors. We will look into two other types of passive components, namely capacitors and inductors. • We have already seen different methods to analyze circuits containing sources and resistive elements. • We will examine circuits that contain two different types of passive elements namely resistors and one (equivalent) capacitor (RC circuits) or resistors and one (equivalent) inductor (RL circuits) • Similar to circuits whose passive elements are all resistive, one can analyze RC or RL circuits by applying KVL and/or KCL. We will see whether the analysis of RC or RL circuits is any different! Note: Some of the figures in this slide set are taken from (R. Decarlo and P.-M. Lin, Linear Circuit Analysis , 2nd Edition, 2001, Oxford University Press) and (C.K. Alexander and M.N.O Sadiku, Fundamentals of Electric Circuits , 4th Edition, 2008, McGraw Hill) SM 2 EECE 251, Set 4 1 Reading Material • Chapters 6 and 7 of the textbook – Section 6.1: Capacitors – Section 6.2: Inductors – Section 6.3: Capacitor and Inductor Combinations – Section 6.5: Application Examples – Section 7.2: First-Order Circuits • Reading assignment: – Review Section 7.4: Application Examples (7.12, 7.13, and 7.14) SM 3 EECE 251, Set 4 Capacitors • A capacitor is a circuit component that consists of two conductive plate separated by an insulator (or dielectric). -
The Bipolar Junction Transistor (BJT)
The Bipolar Junction Transistor (BJT) Introduction he transistor, derived from transfer resistor, is a three terminal device whose resistance between two terminals is controlled by the third. The term bipolar reflects the fact that T there are two types of carriers, holes and electrons which form the currents in the transistor. If only one carrier is employed (electron or hole), it is considered a unipolar device like field effect transistor (FET). The transistor is constructed with three doped semiconductor regions separated by two pn junctions. The three regions are called Emitter (E), Base (B), and Collector (C). Physical representations of the two types of BJTs are shown in Figure (1–1). One type consists of two n -regions separated by a p-region (npn), and the other type consists of two p-regions separated by an n- region (pnp). Figure (1-1) Transistor Basic Structure The outer layers have widths much greater than the sandwiched p– or n–type layer. The doping of the sandwiched layer is also considerably less than that of the outer layers (typically, 10:1 or less). This lower doping level decreases the conductivity of the base (increases the resistance) due to the limited number of “free” carriers. Figure (1-2) shows the schematic symbols for the npn and pnp transistors 1 College of Electronics Engineering - Communication Engineering Dept. Figure (1-2) standard transistor symbol Transistor operation Objective: understanding the basic operation of the transistor and its naming In order for the transistor to operate properly as an amplifier, the two pn junctions must be correctly biased with external voltages.