Conjugate-Image Operation of Transistor Amplifiers Wendall Cloyd Robison Iowa State College
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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. -
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. -
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:??=:. -
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 -
The MOS Tetrode Transistor Is Studied in This Project
AN ABSTRACT OF THE THESIS OF Thawee Limvorapun for the Master of Science (Name) (Degree) in Electrical and Electronics Engineering (Major) 4; -- 7 -- presented on . (Date) Title: THE MOS TETROD.° mr""TcTcm"" Redacted for Privacy Abstract approved: James C. Lodriey The MOS tetrode transistor is studied in this project. This device is ideally suited for high frequency and switching application. In effect it is the solid state analogy of a multigrid vacuum tube performing a very useful multigrid function. A new structure is developed for p-channel 10 ohm-cm. silicon substrate of (111) crystal orientation. This structure consists of an aluminum con- trol gate G1 buried in the pyrolytic SiO2, or E-gun evapo- ration SiO with thermal oxide for the control gate in- 2' sulator. An offset gate G2 produces another channel L2 and causes a longer pinchoff region in the device. The drain breakdown can be maximized so as to approach bulk breakdown as the result of the redistribution of the surfacefield. is very low, ap- The Miller feedback capacitance CGl-D proaching values similar to those of the vacuum pentodes. This paper describes the design, artwork, pyrolytic SiO and E-gun evaporation SiO process. The V-I 2 2 characteristics, dynamic drain resistance, capacitance, small signal equivalent circuit and large signal limitation, and drain breakdown voltage are also discussed. THE MOS TETRODE TRANSISTOR by Thawee Limvorapun A THESIS submitted to Oregon State University in partial fulfillment of the requirements for the degree of Master of Science June 1973 APPROVED: Redacted for Privacy Associa e rofessor of Electrical andEleC-E-Anics Engineering in charge of major Redacted for Privacy Head of Department of Electrical and Electronics Engineering Redacted for Privacy Dean of Graduate School Date thesis is presented 6- 7- 7 2 Typed by Erma McClanathan for Thawee Limvorapun ACKNOWLEDGMENTS I wish to express my sincere appreciation to my advisor, Professor James C. -
Transistor 1 Transistor
Transistor 1 Transistor A transistor is a semiconductor device used to amplify and switch electronic signals and electrical power. It is composed of semiconductor material with at least three terminals for connection to an external circuit. A voltage or current applied to one pair of the transistor's terminals changes the current through another pair of terminals. Because the controlled (output) power can be higher than the controlling (input) power, a transistor can amplify a signal. Today, some transistors are packaged individually, but many more are found embedded in integrated circuits. The transistor is the fundamental building block of modern electronic devices, and is ubiquitous in modern electronic systems. Following its development in the early 1950s, the transistor revolutionized the field of electronics, and paved the way for smaller and cheaper radios, calculators, and computers, among other Assorted discrete transistors. things. Packages in order from top to bottom: TO-3, TO-126, TO-92, SOT-23. History The thermionic triode, a vacuum tube invented in 1907, propelled the electronics age forward, enabling amplified radio technology and long-distance telephony. The triode, however, was a fragile device that consumed a lot of power. Physicist Julius Edgar Lilienfeld filed a patent for a field-effect transistor (FET) in Canada in 1925, which was intended to be a solid-state replacement for the triode.[1][2] Lilienfeld also filed identical patents in the United States in 1926[3] and 1928.[4][5] However, Lilienfeld did not publish any research articles about his devices nor did his patents cite any specific examples of a working prototype. -
Electrical Blasting Cap
electrical blasting cap electrical blasting cap [ENG] A blasting cap ig- electrical prospecting [ENG] The use of down- nited by electric current and not by a spark. hole electrical logs to obtain subsurface informa- { əlekиtrəиkəl blastиiŋkap } tion for geological analysis. { ilekиtrəиkəl pra¨s electrical breakdown See breakdown. { əlekиtrəи pekиtiŋ } kəl bra¯kdau˙ n} electrical resistance See resistance. { ilekиtrəиkəl electrical conductance See conductance. { əlekи rizisиtəns } trəиkəlkəndəkиtəns } electrical-resistance meter See resistance meter. electrical conduction See conduction. { əlekиtrəи {ilekиtrəиkəlrizisиtəns me¯dиər} kəlkəndəkиshən} electrical-resistance strain gage [ENG] A vibra- electrical conductivity See conductivity. { əlekи tion-measuring device consisting of a grid of fine trəиkəl ka¨ndəktivиədиe¯ } wire cemented to the vibrating object to measure electrical drainage [ELEC] Diversion of electric fluctuating strains. { ilekиtrəиkəlrizisиtəns currents from subterranean pipes to prevent stra¯n ga¯j} electrolytic corrosion. { ilekиtrəиkəl dra¯nиij } electrical-resistance thermometer See resistance electrical engineer [ENG] An engineer whose thermometer. { ilekиtrəиkəlrizisиtəns thər training includes a degree in electrical engi- ma¨mиədиər} neering from an accredited college or university electrical resistivity [ELEC] The electrical (or who has comparable knowledge and experi- resistance offered by a material to the flow of ence), to prepare him or her for dealing with current, times the cross-sectional area of current the generation, transmission, and utilization of flow and per unit length of current path; the electric energy. { ilekиtrəиkəl enиjənir } reciprocal of the conductivity. Also known as electrical engineering [ENG] Engineering that resistivity; specific resistance. { ilekиtrəиkəl re¯и deals with practical applications involving cur- zistivиədиe¯ } rent flow through conductors, as in motors and electrical resistor See resistor. -
Transistor from Wikipedia, the Free Encyclopedia
Transistor From Wikipedia, the free encyclopedia A transistor is a semiconductor device used to amplify and switch electronic signals and electrical power. It is composed of semiconductor material with at least three terminals for connection to an external circuit. A voltage or current applied to one pair of the transistor's terminals changes the current through another pair of terminals. Because the controlled (output) power can be higher than the controlling (input) power, a transistor can amplify a signal. Today, some transistors are packaged individually, but many more are found embedded in integrated circuits. The transistor is the fundamental building block of modern electronic devices, and is ubiquitous in modern electronic systems. Following its development in 1947 by John Bardeen, Walter Brattain, and William Shockley, the transistor revolutionized the field of electronics, and paved the way for smaller and cheaper radios, calculators, and computers, among other things. The transistor is on the Assorted discrete transistors. list of IEEE milestones in electronics, and the inventors were jointly awarded the Packages in order from top 1956 Nobel Prize in Physics for their achievement. to bottom: TO-3, TO-126, TO-92, SOT-23. Contents 1 History 2 Importance 3 Simplified operation 3.1 Transistor as a switch 3.2 Transistor as an amplifier 4 Comparison with vacuum tubes 4.1 Advantages 4.2 Limitations 5 Types 5.1 Bipolar junction transistor (BJT) 5.2 Field-effect transistor (FET) 5.3 Usage of bipolar and field-effect transistors 5.4 Other -
Transistor - Wikipedia, the Free Encyclopedia Page 1 of 13
Transistor - Wikipedia, the free encyclopedia Page 1 of 13 Transistor From Wikipedia, the free encyclopedia A transistor is a semiconductor device used to amplify and switch electronic signals and electrical power. It is composed of semiconductor material with at least three terminals for connection to an external circuit. A voltage or current applied to one pair of the transistor's terminals changes the current through another pair of terminals. Because the controlled (output) power can be higher than the controlling (input) power, a transistor can amplify a signal. Today, some transistors are packaged individually, but many more are found embedded in integrated circuits. The transistor is the fundamental building block of modern electronic devices, and is ubiquitous in modern electronic systems. Following its development in 1947 by John Bardeen, Walter Brattain, and William Shockley, the transistor revolutionized the field of electronics, and paved the way for smaller and cheaper radios, calculators, and computers, among other things. The transistor is on the list of IEEE milestones in electronics, and the inventors were jointly awarded the 1956 Nobel Prize in Physics for their achievement. Assorted discrete transistors. Packages in order from top to bottom: TO-3, TO-126, Contents TO-92, SOT-23 ◾ 1 History ◾ 2 Importance ◾ 3 Simplified operation ◾ 3.1 Transistor as a switch ◾ 3.2 Transistor as an amplifier ◾ 4 Comparison with vacuum tubes ◾ 4.1 Advantages ◾ 4.2 Limitations ◾ 5 Types ◾ 5.1 Bipolar junction transistor (BJT) ◾ 5.2 Field-effect -
Circuit and System Design for Mm-Wave Radio and Radar Applications
CIRCUIT AND SYSTEM DESIGN FOR MM-WAVE RADIO AND RADAR APPLICATIONS by IOANNIS SARKAS A thesis submitted in conformity with the requirements for the degree of Doctor of Philosophy Graduate Department of Electrical and Computer Engineering University of Toronto c Ioannis Sarkas, 2013 Circuit and System Design for mm-wave Radio and Radar Applications Ioannis Sarkas Doctor of Philosophy, 2013 Graduate Department of Electrical and Computer Engineering University of Toronto Abstract Recent advancements in silicon technology have paved the way for the development of integrated transceivers operating well inside the mm-wave frequency range (30 - 300 GHz). This band offers opportunities for new applications such as remote sensing, short range radar, active imaging and multi-Gb/s radios. This thesis presents new ideas at the circuit and system level for a variety of such applications, up to 145 GHz and in both state-of-the-art nanoscale CMOS and SiGe BiCMOS technologies. After reviewing the theory of operation behind linear and power amplifiers, a purely dig- ital, scalable solution for power amplification that takes advantage of the significant fT/fmax improvement in pFETs as a result of strain engineering in nanoscale CMOS is presented. The proposed Class-D power amplifier, features a stacked, cascode CMOS inverter output stage, which facilitates high voltage operation while employing only thin-oxide devices in a 45 nm SOI CMOS process. Next, a single-chip, 70-80 GHz wireless transceiver for last-mile point-to-point links is described. The transceiver was fabricated in a 130 nm SiGe BiCMOS technology and can operate at data rates in excess of 18 Gb/s.