Bipolar Junction Transistor (Bjt)
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Navy Electricity and Electronics Training Series
NONRESIDENT TRAINING COURSE SEPTEMBER 1998 Navy Electricity and Electronics Training Series Module 7—Introduction to Solid-State Devices and Power Supplies NAVEDTRA 14179 DISTRIBUTION STATEMENT A: Approved for public release; distribution is unlimited. Although the words “he,” “him,” and “his” are used sparingly in this course to enhance communication, they are not intended to be gender driven or to affront or discriminate against anyone. DISTRIBUTION STATEMENT A: Approved for public release; distribution is unlimited. PREFACE By enrolling in this self-study course, you have demonstrated a desire to improve yourself and the Navy. Remember, however, this self-study course is only one part of the total Navy training program. Practical experience, schools, selected reading, and your desire to succeed are also necessary to successfully round out a fully meaningful training program. COURSE OVERVIEW: To introduce the student to the subject of Solid-State Devices and Power Supplies who needs such a background in accomplishing daily work and/or in preparing for further study. THE COURSE: This self-study course is organized into subject matter areas, each containing learning objectives to help you determine what you should learn along with text and illustrations to help you understand the information. The subject matter reflects day-to-day requirements and experiences of personnel in the rating or skill area. It also reflects guidance provided by Enlisted Community Managers (ECMs) and other senior personnel, technical references, instructions, etc., and either the occupational or naval standards, which are listed in the Manual of Navy Enlisted Manpower Personnel Classifications and Occupational Standards, NAVPERS 18068. THE QUESTIONS: The questions that appear in this course are designed to help you understand the material in the text. -
Equivalent Circuit of Unsymmetrical Inductance Diode Using Linvill Lumped Model
Scholars' Mine Masters Theses Student Theses and Dissertations 1965 Equivalent circuit of unsymmetrical inductance diode using Linvill lumped model Donald Lawrence Willyard Follow this and additional works at: https://scholarsmine.mst.edu/masters_theses Part of the Electrical and Computer Engineering Commons Department: Recommended Citation Willyard, Donald Lawrence, "Equivalent circuit of unsymmetrical inductance diode using Linvill lumped model" (1965). Masters Theses. 5235. https://scholarsmine.mst.edu/masters_theses/5235 This thesis is brought to you by Scholars' Mine, a service of the Missouri S&T Library and Learning Resources. This work is protected by U. S. Copyright Law. Unauthorized use including reproduction for redistribution requires the permission of the copyright holder. For more information, please contact [email protected]. EQUIV ALBNT CJ.RCUIT OF UNSYMMETRICAL INDUCTANCE DIODE USDJG LINVJLL LUMPED MODEL BY AP'/ r· ol~'- t'\.)J} - / OONALD L~ vJILLYARD J V~ ~~ :;> A THESIS submitted to the faculty of the UNIVERSITY OF MISSOURI AT ROLLA in partial fulfillment of the requirements for the ~gree of 1-W3TER OF SCIENCE IN ELECTRICAL ENGINEERING Rolla, Missouri 1965 Approved By ~/}/)/~~) ~~ ii ABSTRACT Integrated circuit techniques and applications are rapidJ.y changing the electronics industry. A problem common to both state of-the-art approaches to integrated circuit fabrication is that of miniaturizing and intGgrating inductors. It is found that, for a certain range of injection current levels, certain unsymmetrically doped junction diodes have an inductive small-signal impedance. This thesis discusses the theor,y of inductance diodes and applies finite difference equations and the Linvill lumped model to the differential equations that describe their carrier nov.r processes. -
Multivibrator Circuits
Multivibrator Circuits Bistable multivibrators Multivibrators Circuits characterized by the existence of some well defined states, amongst which take place fast transitions, called switching processes. A switching process is a fast change in value of a current or a voltage, the fast process implying the existence of positive reaction loops, or negative resistances. The switching can be triggered from outside, by means of command signals, or from inside, by slow charge accumulation and the reaching of a critical state by certain electrical quantities in the circuit. Circuits have two, well defined states, which can be either stable or unstable A stable state is a state, in which the circuit, in absence of a driving signal, can remain for an unlimited period of time The circuit can remain in an unstable state only for a limited period of time, after which, in the absence of any exterior command signals, it switches into the other state. The multivibrator circuits can be grouped, according to their number of stable (steady) states, into: - flip-flops (bistable circuits) with both states being stable - monostable circuits , having a stable and an unstable state - astable circuits , with both states being unstable Flip-flop circuits The main feature of the flip-flop circuits is the existence of two stable states, in which the circuit may remain for a long time. The switching from one state to the other is triggered by command signals Flip flop: an example for a sequential circuit (a circuit with outputs that present logical values depending on a certain sequence of signals, that have previously existed in the circuit). -
Npn Transistor Pnp Transistor
ELL 100 - Introduction to Electrical Engineering LECTURE 23: BIPOLAR JUNCTION TRANSISTOR (BJT) 1 CONTENTS • Introduction • Construction & working principle of BJT • Common-base and common-emitter circuits 2 BJT INTRODUCTION • Bipolar: Both electrons and holes (positively charged quasi- particles, absence of electron) contribute to current flow • Junction: Consists of an n- (or p-) type silicon sandwiched between two p- (or n-) type silicon regions • Transistor: 3-terminal device (Base, Emitter, Collector) Two types: npn & pnp 3 Bipolar Junction Transistor (BJT) 4 Various Types of General-Purpose or Switching Transistors: (a) Low Power (b) Medium Power (c) Medium to high power 5 First Working Transistor, Invented in 1947. Earliest Raytheon Blue transistors, Replica of 1st device made by first appearing in 1955 Shockley, Bardeen & Brattain at Bell Labs 6 Applications: Transistor As Switch 7 Applications: Transistor As Relay (Switch) Single channel 5V relay breakout board 8 Applications: Transistor As Amplifier TDA7297 Power Amplifier & Audio amplifier Module 9 Applications: Transistors in Radio 10 Applications: Transistor in Oscillator Colpitts Oscillator 11 Applications: Transistor in Oscillator Astable Multivibrator 12 Transistors in Timer Circuits 13 Transistor As NOT Gate 14 Transistors in NAND Gate 15 Bipolar Junction Transistor (BJT) The three terminals of the BJT are called the Base (B), the Collector (C) and the Emitter (E). n p p n n p npn transistor pnp transistor 16 Bipolar Junction Transistor (BJT) npn pnp 17 p-n-p Transistor IE, IB, IC – Emitter, Base and Collector currents VEB, VCB, VCE – Emitter-Base, Collector-Base and Collector-Emitter voltages 18 n-p-n Transistor IE, IB, IC – Emitter, Base and Collector currents VEB, VCB, VCE – Emitter-Base, Collector-Base and Collector-Emitter voltages 19 BJT Construction 20 Bipolar Junction Transistor (BJT) Basic Principle The voltage between two terminals (B and E) controls the current through the third terminal (C). -
Automatic Gain Control of Transistor Amplifiers
Calhoun: The NPS Institutional Archive Theses and Dissertations Thesis Collection 1955 Automatic gain control of transistor amplifiers Bryan, William L. http://hdl.handle.net/10945/13960 M«nl«ey, California AUTOMATIC GAIN CONTROL OF TRANSISTOR AMPLIFIERS William L* Bxyan 1^ AUTOMATIC GAIN CONTROL OF TRANSISTOR AMPLIFIERS by William Littell Bryan Lieutenant, United States Navy Submitted in partial fulfillment of the requirements for the degree of MASTER OF SCIENCE IN ENGINEERING ELECTRONICS United States Naval Postgraduate School Monterey, California 19 5 5 Tlicsls " •'-'»i;;.;„;'"''"^"'«j This work is accepted as fulfilling the thesis requirements for the degree of * MASTER OF SCIENCE IN ENGINEERING ELECTRONICS from th« United States Naval Postgraduate School PREFACE The rapid progress made in the field of semiconduc- tors since the invention of the transistor seven years ago has widely broadened our theoretical knowledge in the field and greatly increased the potentialities of these devices. Particularly our increasing ability to manxifac- ture reproducible transistors has brought us to the point of designing circuits for specific application to tran- sistors, not just to illustrate the application but rathei* •ngineered to rigid specifications. This paper treats Just such a design, that of obtaining automatic gain control of a transistor amplifier. There has been as yet little published about this difficult problem, and much of the work here presented is believed to be original* The majority of the experimental work connected with this thesis was performed during the author's Industrial Experience Tour while at Lenkurt Electric Company, San Carlos, California, and he is indebted to them for their cooperation and assistance. -
Low Noise Dual Gate Enhancement Mode MOSFET with Quantum Valve in the Channel
Proceedings of the World Congress on Electrical Engineering and Computer Systems and Science (EECSS 2015) Barcelona, Spain, July 13-14, 2015 Paper No. 153 Low Noise Dual Gate Enhancement Mode MOSFET with Quantum Valve in the Channel Sam Halilov, Anass Dahany, Sam Mil’shtein University Ave 1, University of Massachusetts Department of Electrical and Computer Engineering Lowell, MA 01854, USA Abstract- A proposed Si-based series multi-gate E-MOSFET is discussed in terms of its design, static and dynamic transport properties and noise figure. In its simplest realization, the design involves two gates in series comprising an extra n(p)-doped junction in the p(n)-channel. The role of the nano-scale junction is twofold: to minimize the Miller effect in the enhancement mode to improve the frequency response and to create a quantum well to quench the current noise associated with the carrier velocity fluctuations. While dual-gate depletion structure results in a reduced carrier transition time along the entire channel path, the quantization effects serve as a current noise filter. Similar quantum valve can be realized in the form of a well both in n- and p-channel enhancement mode FET, whereas the majority carriers experience a tunneling through a similar shape barrier. Doping concentration and size of the middle junction are free parameters and can be adjusted to the required figures of merit. AC device simulations confirm the expectations based on the along-the-channel potential profile: enhanced cutoff frequency and higher saturation current are the signatures of the reduced transition and RC-time, whereas the minimum noise figure and transfer functions demonstrate noise filtering capabilities of the state quantization. -
Chapter 3: Oscillators and Waveform-Shaping Circuits
mywbut.com CHAPTER3:OSCILLATORSANDWAVEFORM-SHAPING CIRCUITS Inthedesignofelectronicsystems,theneed frequentlyarises forsignals havingprescribed standardwaveforms(e.g.,sinusoidal, square,triangle,pulse,etc).Thesewaveformsarecommonly usedincomputers,controlsystems,communicationsystemsandtestmeasurementsystems. Therearetwocommonwaysforgeneratingsinusoids: 1. Positivefeedbackloopwithnon-lineargainlimiting 2. Appropriatelyshapingotherwaveformssuchasatrianglewaves. Circuitsthatdirectlygeneratesquare,triangleandpulsewaveformsgenerallyemploycircuit blocksknownasmultivibrators.Threebasictypesarebistable,astableandmonostable. I.SINUSOIDALOSCILLATORS: Commonly referred to as linear sine-wave oscillators although some forms of non-linearity havetobeemployedtolimittheoutputamplitude.Analysisofthecircuitsismoredifficultass-plane analysis cannot be directly applied to the non-linear part of the circuit. The basic structure of a sinusoidal oscillator consists of an amplifier and a frequency selective network connected in a positivefeedbackloop. AmplifierA xS + Σ xO + xf Freq.Selective networkβ Figure1:Basicstructureofasinusoidaloscillator. Apositive-feedbackloopisformedbyanamplifierandafrequency-selectivenetwork.Inan actualoscillatorcircuit,noinputsignalwillbepresent;hereaninputsignalxsisemployedtohelp explaintheprincipleofoperation.NotethatthefeedbacksignalXFissummedwithapositivesign: A(s) A (s) = f 1− A(s) β (s) Theloopgainis: )s(L =A(s) β (s) Andthecharacteristicequationcanbewrittenas: 1-L(s)=0 If at a specific frequency -
900000 102 03.Pdf
ELECTRONIC URCUlTS 0.WO.IM SEMICONDUCTOR SECTION 3 alphhtical list of oll letter syntnls used herein is GENERAL INFORMATION ON SEMICONDUCTOR CIRCUITS presented below for easy reference. Symbol D.Hmltion 3.1 DEFINITIONS OF LETTER SYMBOLS USED. a Current mnpllficotlon factor (common The letter symbols used in the diagrams ond discus- boa. current gain - Alpha) rims on semiomductor circuits throughout this technicul a FB, a FC, a FE Short-&cult forward current V-afsr manual me those proposed as standard for use in industry by rotlo, atottc volvs the Institute of Rodio Engineers, or ore speciai syrr~hla uib, riic, iio ~,=d!-&~d~h=rt-c!.~t?!+ forwmd not included in the stmdmd. Since some of these symbols currsnc rrrrnsior rviio chmqe from time to time, md new symbols are develop2 to AG AvoUoble qoln cover new devices as the mt changes, m alphabetical Al Current gal- listing of the symbols used herein is wesmted below. It AP Power Goln is rwmmended that this listing be used to obtain the Av Voltoqa goln proper definitions of the symbols employed in this manuol, B ar b Base electrode I"!!?? thcm to assume on erroneous meming. vR common-amlttsr cunent qah - Beta 3.1.1 Con.nuola of symbls. Semiconductm synSc!s ZL' or 'Jbn ~reakdownvoltaqe are made up of c basic letter with subscripts, either lformarly PIE or TIV) alphabetical or numbericol, or bath, in accordmcc with BZ ~m~ss~gnczlbreakdown impedance the fo!!owinq rules: br snnll-algnd breakdown impedance o. A capitol (upper case) letter designates enemoi C or c CO,I.CtOl siocrrcde or curaiiiii circuit wrameters and compcnents, largesignal aevlce CB, CC, CE common boa-, coliecloi, m.2 em:??=:. -
Experiment No: 14 ASTABLE MULTIVIBRATOR USING IC
Experiment No: 14 ASTABLE MULTIVIBRATOR USING IC 555 AIM To design and set up astable multivibrator of 1000 Hz frequency and 60% duty cycle using IC 555 THEORY IC 555 timer is an analog IC used for generating accurate time delay or oscillations. The entire circuit is usually housed in an 8-pin package as specified in figures 1 & 2 below. A series connection of three resistors inside the IC sets the reference voltage levels to the two 2 1 comparators at V and V , the output of these comparators setting or resetting the flip- 3 CC 3 CC flop unit. The output of the flip-flop circuit is then brought out through an output buffer stage. In the stable state the 푄 output of the flip-flop is high (ie Q low). This makes the output (pin 3) low because of the buffer which basically is an inverter.The flip-flop circuit also operates a transistor inside the IC, the transistor collector usually being driven low to discharge a timing capacitor connected at pin 7. The description of each pin s described below, Pin 1: (Ground): Supply ground is connected to this pin. Pin 2: (Trigger): This pin is used to give the trigger input in monostable multivibrator. When trigger of amplitude greater than (1/3)Vcc is applied to this terminal circuit switches to quasi-stable state. Pin 3: (Output) Pin 4 (Reset): This pin is used to reset the output irrespective of input. A logic low at this pin will reset output. For normal operation pin 4 is connected to Vcc. -
An Electronic Switch ?Or Transient Studies
AN ELECTRONIC SWITCH ?OR TRANSIENT STUDIES A THESIS Presented to the Faculty of the Division of Graduate Studies Georgia Institute of Technology In Partial Fulfillment of the Requirements for the Degree Master of Science in Slectrical Engineering by Marshall Joseph McCann September 1949 107545 ii AN ELECTRONIC SWITCH FOR TRANSIENT STUDIES Approved: zf r ~~v Bate Approved by Chairman A up. d±, f^4f ACKNOWLEDGMENTS I wish to express my sincerest thanks to Prof. M. A. Honnell for his patient guidance and assistance, which were an immense aid in the prosecution of this work. I am also indebted to the Photographic and Repro duction Laboratory at the State Engineering Experiment Station of the Georgia Institute of Technology for their splendid cooperation with the photographic work herein. iv TABLE 0? CONTENTS PAGE Acknowledgments iii List of figures vi I- Introduction 1 II- A Survey of the Literature 3 Mechanical Systems.. • 3 Electronic Systems 4 III- Design Considerations for an Electronic Switch 8 General , , 8 Possible Approaches 8 IV- The Switch 12 V- The Square Wave Generator 16 Design Requirement s 16 Symmetrical Multivibrator 16 Improvement of Waveform 22 VI- The Synchronizing Section 37 General 37 Phase Shifting 27 Amplification and V/ave shaping 29 Synchronization of the Multivibrator 39 Summary of the Synchronizing Action 31 VII- Operation 34 VIII- Siamples of Operation 37 Lumped Constant Circuits 37 V P-4GE VIII- Examples of Operation (continued) Transmission Line Transients 41 IX- Summary • 46 appendix I, Analysis of Plate-Inductance Compensation of the Multivibrator 47 appendix II, Scaling of Circuits for A-C Transients 50 appendix III, Parts List 55 Bibliography ... -
The Transistor
Chapter 1 The Transistor The searchfor solid-stateamplification led to the inventionof the transistor. It was immediatelyrecognized that majorefforts would be neededto understand transistorphenomena and to bring a developedsemiconductor technology to the marketplace.There followed a periodof intenseresearch and development, duringwhich manyproblems of devicedesign and fabrication, impurity control, reliability,cost, and manufacturabilitywere solved.An electronicsrevolution resulted,ushering in the eraof transistorradios and economicdigital computers, alongwith telecommunicationssystems that hadgreatly improved performance and that were lower in cost. The revolutioncaused by the transistoralso laid the foundationfor the next stage of electronicstechnology-that of silicon integratedcircuits, which promised to makeavailable to a massmarket infinitely more complexmemory and logicfunctions that could be organizedwith the aid of softwareinto powerfulcommunications systems. I. INVENTION OF THE TRANSISTOR 1.1 Research Leading to the Invention As World War II was drawing to an end, the research management of Bell Laboratories, led by then Vice President M. J. Kelly (later president of Bell Laboratories), was formulating plans for organizing its postwar basic research activities. Solid-state physics, physical electronics, and mi crowave high-frequency physics were especially to be emphasized. Within the solid-state domain, the decision was made to commit major research talent to semiconductors. The purpose of this research activity, according -
How to Configure a 555 Timer IC 555 Timer Tutorial
How To Configure a 555 Timer IC 555 Timer Tutorial By Philip Kane The 555 timer was introduced over 40 years ago. Due to its relative simplicity, ease of use and low cost it has been used in literally thousands of applications and is still widely available. Here we describe how to configure a standard 555 IC to perform two of its most common functions - as a timer in monostable mode and as a square wave oscillator in astable mode. 555 Timer Tutorial Bundle Includes: Qty. Description Manufacturer P/N 1 Standard Timer Single 8-Pin Plastic Dip Tube NE555P 1 400-Point Solderless Breadboard 3.3"L x 2.1"W WBU-301-R 10 Resistor Carbon Film 10kΩ CF1/4W103JRC 1 9V Alkaline Battery ALK 9V 522 1 9V Battery Snap with 6" 26AWG Leads BC6-R 2 3-Pin SPDT Slide Switch SS-12E17 2 Radial Capacitor 0.01µF 2.54mm Bulk SS-12E17 1 Radial Capacitor 4.7µF 2.5mm Bulk TAP475K025SCS-VP 10 Resistor Carbon Film 1.0MΩ 1/4 Watt 5% CF1/4W105JRC 10 Resistor Carbon Film 220Ω 1/4 Watt 5% CF1/4W221JRC 10 LED Uni-Color Red 660nm 2-Pin T-1¾ Box UT1871-81-M1-R 100 Resistor Carbon Film 3kΩ 1/4 Watt 5% CF1/4W302JRC 10 Resistor Carbon Film 330kΩ 1/4 Watt 5% CF1/4W334JRC 1 Radial Capacitor 1µF 25 Volt 2.5mm Bulk TAP105K025SCS-VP 555 Signals and Pinout (8 pin DIP) Figure 1 shows the input and output signals of the 555 timer as they are arranged around a standard 8 pin dual inline package (DIP).