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Introduction to Electronic Engineering
VALERY VODOVOZOV INTRODUCTION TO ELECTRONIC ENGINEERING DOWNLOAD FREE TEXTBOOKS AT BOOKBOON.COM Valery Vodovozov Introduction to Electronic Engineering Download free books at BookBooN.com 2 Introduction to Electronic Engineering © 2010 Valery Vodovozov & Ventus Publishing ApS ISBN 978-87-7681-539-4 Download free books at BookBooN.com 3 Introduction to Electronic Engineering Contents Contents Designations 6 Abbreviations 7 Preface 8 Introduction 9 1. Semiconductor Devices 17 1.1 Semiconductors 17 1.1.1 Current in Conductors and Insulators 17 1.1.2 Current in Semiconductors 18 1.1.3 pn Junction 21 1.2 Diodes 24 1.2.1 Rectifier Diode 24 1.2.2 Power Diode 27 1.2.3 Special-Purpose Diodes 30 1.3 Transistors 36 1.3.1 Common Features of Transistors 36 1.3.2 Bipolar Junction Transistors (BJT) 36 1.3.3 Power Bipolar Transistors 44 WHAt‘s missing in this equaTION? You could be one of our future talents Please click the advert MAERSK INTERNATIONAL TECHNOLOGY & SCIENCE PROGRAMME Are you about to graduate as an engineer or geoscientist? Or have you already graduated? If so, there may be an exciting future for you with A.P. Moller - Maersk. www.maersk.com/mitas Download free books at BookBooN.com 4 Introduction to Electronic Engineering Contents 1.3.4 Junction Field-Effect Transistors (JFET) 47 1.3.5 Metal-Oxide Semiconductor Field-Effect Transistors (MOSFET) 51 1.3.6. Insulated Gate Bipolar Transistors (IGBT) 55 1.4 Thyristors 59 1.4.1 Rectifier Thyristor (SCR) 59 1.4.2 Special-Purpose Thyristors 63 2. Electronic Circuits 66 2.1 Circuit Composition -
Chapter-2 Semiconcuctors Diodes & Transistors
Semiconcuctors and Diodes & Transistors 1 Chapter-2 Semiconcuctors Diodes & Transistors Contents Semiconcuctors and Diodes: Energy Band of Insulators, Conductors and Semi Conductors Intrinsic and extrinsic semiconductors. PN junction diode, barrier potential, V-I characteristics. Special Purpose Diodes: Zener diode, Varactor diodes ,Light Emitting Diodes (LEDs),photo diodes, Solar cell. Specification parameters of diodes and numbering. Bipolar Junction Transistors: Structure, typical doping, Principle of operation,Detailed study of input and output characteristics of common emitter configuration,Transistor specifications. 2.1 Introduction A semiconductor material is one whose electrical properties lie in between those of insulators and good conductors. Examples are: germanium and silicon. In terms of energy bands, semiconductors can be defined as those materials which have almost an empty conduction band and almost filled valence band with a very narrow energy gap (of the order of 1 eV) separating the two. Some materials are intrinsic semiconductors. An intrinsic semiconductor is one which is made of the semiconductor material in its extremely pure form. The semiconducting properties occur in these materials naturally. However, most of the semiconducting materials used in electronics are extrinsic. Those intrinsic semiconductors to which some suitable impurity or doping agent has been added in extremely small amounts are called extrinsic or impurity semiconductors. Depending on the type of doping material used, extrinsic semiconductors can be sub-divided in to N-type and P-type semiconductors. The p-n junction is a homojunction between a p-type and an n-type semiconductor. It acts as a diode, which can serve in electronics as a rectifier, logic gate, voltage regulator (Zener diode), switching or tuner (varactor diode); and in optoelectronics as a light-emitting diode (LED), photodiode or solar cell. -
Reading 24 SEMICONDUCTORS Part 1 the Objective of This Reading and the Following, Is to Provide a Basic Coverage of the Most Ge
Reading 24 Ron Bertrand VK2DQ http://www.radioelectronicschool.com SEMICONDUCTORS Part 1 The objective of this reading and the following, is to provide a basic coverage of the most generally employed solid state devices, such as diodes of various types, bipolar junction transistors (BJTs), FETs MOSFETs, SCRs, and ICs, as well as a few of the characteristic circuits in which they are used. Information that is required for examination purposes will be brought to the attention of the reader. Pay attention to highlighting. SOLID STATE DEVICES Solid state devices are much smaller physically, more rugged and lighter than vacuum types, but cannot withstand heat as well, changing their characteristics as they warm. However, many newer special solid state devices will operate at much higher frequencies than any vacuum devices can. SEMICONDUCTORS The outer orbit, or valence electrons of some atoms, such as metals (conductors), can be detached with relative ease at almost any temperature, and may be called free electrons. This is why metals are good conductors. These valence electrons are able to move outward from a normal outer orbit level into a conduction level or band, from which they can be easily dislodged. Such materials make good electrical conductors. Other substances such as glass, rubber, and plastics, have no free valence electrons in their outer conduction bands at room temperatures, and are therefore good insulators. A few materials have a limited number of electrons in the conduction level (outer orbit or valence band) at room temperatures and are called semiconductors. Applying energy in the form of photons (small packets of light or heat energy) to the valence electrons moves some of them up into the conduction band, and the semiconductors then become better electrical conductors. -
R.B.V.R.R. Women's College
R.B.V.R.R. Women's College (Autonomous) A College with Potential for Excellence Accredited by NAAC with Grade 'A' Narayanaguda, Hyderabad-500 029. t, DEPARTMENT OF ELECTRONICS CERTIFICATE Certified that this is a Bonafide record work done in this laboratory during the yeor 20 - 20 Name: H.T. No.: Batch: Date: Subject: Electronics Paper -II: Electronic Devices Lecturer Incharge External Examiner INDEX Particulars of the Experiments Performed S.No. Name of Experiment Page Date of Date of Remarks Experiment Submission I 1. JUNCTION DIODE CHARACTERISTICS of the given diodes' @: To obtain the forward and reverse bias characteristics APPARATUS: 1) Junction diode characteristics trainer 2)Voltmeter 3)Ammeter (ma, lra) 4) Cdnnecting wires I, CIRCUIT DIAGRAM: fused together to form a p-n THEORY: A diode consists of p-type and n-type impurities in one direction only' lf the junction, The p-n junction will permit current to ftow through it terminal of the supply to the n- positive terminar of a power supply to the p-side and negative p-side of the diode is connected to the negative side, the diode is to be forward biased. lf the positive terminal of the supply the terminal of the supply and the n-side of the diode to the ' diode is said to be reverse biased' potential at junction reduces' ln When the diode is forward biased, the barrier almost no current can flow through the diode' reverse bias, the barrier potential increases, and by its schematic symbol' The figure (a) shows that the p-n iunction represented Svmbol of the diode Anode Cathode (+) t) i I, the cathode' The symbol looks like The p-region of the diode is called the anode and n-region as a remainder to us that the an arrow pointing from the p-region to the n-region. -
Electronic Devices & Circuits Ii B.Tech I Semester
ELECTRONIC DEVICES & CIRCUITS II B.TECH I SEMESTER (COMMON FOR ECE/CSE/IT) DEPARTMENT OF ELECTRONICS & COMMUNICATION ENGINEERING MALLA REDDY COLLEGE OF ENGINEERING & TECHNOLOGY Autonomous Institution – UGC, Govt. of India (Affiliated to JNTU, Hyderabad, Approved by AICTE - Accredited by NBA & NAAC – ‘A’ Grade - ISO 9001:2008 Certified) Maisammaguda, Dhulapally (Post Via Hakimpet), Secunderabad – 500100 PREPARED BY Mr K.MALLIKARJUNA LINGAM, Mr R.CHINNA RAO, Mr E.MAHENDAR REDDY, Mr V SHIVA RAJKUMAR Dr.S.SRINIVASA RAO (R15A0401) ELECTRONIC DEVICES AND CIRCUITS OBJECTIVES This is a fundamental course, basic knowledge of which is required by all the circuit branch engineers .this course focuses: 1. To familiarize the student with the principal of operation, analysis and design of junction diode .BJT and FET transistors and amplifier circuits. 2. To understand diode as a rectifier. 3. To study basic principal of filter of circuits and various types UNIT-I P-N Junction diode: Qualitative Theory of P-N Junction, P-N Junction as a diode , diode equation , volt- amper characteristics temperature dependence of V-I characteristic , ideal versus practical –resistance levels( static and dynamic), transition and diffusion capacitances, diode equivalent circuits, load line analysis ,breakdown mechanisms in semiconductor diodes , zener diode characteristics. Special purpose electronic devices: Principal of operation and Characteristics of Tunnel Diode with the help of energy band diagrams, Varactar Diode, SCR and photo diode UNIT-II RECTIFIERS, FILTERS: P-N Junction as a rectifier ,Half wave rectifier, , full wave rectifier, Bridge rectifier , Harmonic components in a rectifier circuit, Inductor filter, Capacitor filter, L- section filt - section filter and comparison of various filter circuits, Voltage regulation using zener diode. -
Semiconductors Part 1.Pdf
Reading 24 Ron Bertrand VK2DQ http://www.radioelectronicschool.com SEMICONDUCTORS Part 1 The objective of this reading and the following, is to provide a basic coverage of the most generally employed solid state devices, such as diodes of various types, bipolar junction transistors (BJTs), FETs MOSFETs, SCRs, and ICs, as well as a few of the characteristic circuits in which they are used. Information that is required for examination purposes will be brought to the attention of the reader. Pay attention to highlighting. SOLID STATE DEVICES Solid state devices are much smaller physically, more rugged and lighter than vacuum types, but cannot withstand heat as well, changing their characteristics as they warm. However, many newer special solid state devices will operate at much higher frequencies than any vacuum devices can. SEMICONDUCTORS The outer orbit, or valence electrons of some atoms, such as metals (conductors), can be detached with relative ease at almost any temperature, and may be called free electrons. This is why metals are good conductors. These valence electrons are able to move outward from a normal outer orbit level into a conduction level or band, from which they can be easily dislodged. Such materials make good electrical conductors. Other substances such as glass, rubber, and plastics, have no free valence electrons in their outer conduction bands at room temperatures, and are therefore good insulators. A few materials have a limited number of electrons in the conduction level (outer orbit or valence band) at room temperatures and are called semiconductors. Applying energy in the form of photons (small packets of light or heat energy) to the valence electrons moves some of them up into the conduction band, and the semiconductors then become better electrical conductors. -
Unit 1-Semiconductors & Rectifiers
www.Vidyarthiplus.com QUESTION BANK DEPARTMENT: ME YR/ SEM:II/ III SUB CODE: ME2255 SUB NAME: ELECTRONICS & MICROPROCESSORS UNIT 1-SEMICONDUCTORS & RECTIFIERS PART A (2 Marks) 1. Define Rectification. (AUC MAY 2012) A rectifier is an electrical device that converts alternating current (AC), which periodically reverses direction, to direct current (DC), which flows in only one direction. The process is known as rectification. Rectifiers have many uses, but are often found serving as components of DC power supplies and high-voltage direct current power transmission systems. 2. Define voltage regulation. (AUC MAY 2012) voltage regulation is a measure of change in the voltage magnitude between the sending and receiving end of a component, such as a transmission or distribution line. Voltage regulation describes the ability of a system to provide near constant voltage over a wide range of load conditions. The term may refer to a passive property that result in more or less voltage drop under various load conditions, or to the active intervention with devices for the specific purpose of adjusting voltage. 3. Draw the circuit of zener voltage regulator. (AUC MAY 2010) ME2255/Electronics& Microprocessors Department of ME 1 www.Vidyarthiplus.com www.Vidyarthiplus.com 4. A half wave rectifier having a resistance load of 1KΩ rectifies an alternating voltage of 325V peak value and the diode has a forward resistance of 100Ω. Calculate its DC power output. (AUC MAY 2010) 5. What is diffusion current? (AUC MAY 2011) In a non uniformly doped semi conductor charge carriers have a tendency to move from a region of higher concentration to a region of lower concentration. -
UNIT IV SPECIAL SEMICONDUCTOR DEVICES 4.1 ZENER DIODE a Normal P-N Junction Diode Allows Electric Current Only in Forward Biased Condition
COLLEGE OF ENGINEERING AND TECHNOLOGY UNIT IV SPECIAL SEMICONDUCTOR DEVICES 4.1 ZENER DIODE A normal p-n junction diode allows electric current only in forward biased condition. When forward biased voltage is applied to the p-n junction diode, it allows large amount of electric current and blocks only a small amount of electric current. Hence, a forward biased p-n junction diode offer only a small resistance to the electric current. When reverse biased voltage is applied to the p-n junction diode, it blocks large amount of electric current and allows only a small amount of electric current. Hence, a reverse biased p-n junction diode offer large resistance to the electric current. If reverse biased voltage applied to the p-n junction diode is highly increased, a sudden rise in current occurs. At this point, a small increase in voltage will rapidly increases the electric current. This sudden rise in electric current causes a junction breakdown called zener or avalanche breakdown. The voltage at which zener breakdown occurs is called zener voltage and the sudden increase in current is called zener current. A normal p-n junction diode does not operate in breakdown region because the excess current permanently damages the diode. Normal p-n junction diodes are not designed to operate in reverse breakdown region. Therefore, a normal p-n junction diode does not operate in reverse breakdown region. A zener diode is a special type of device designed to operate in the zener breakdown region. Zener diodes acts like normal p-n junction diodes under forward biased condition.