RRB JE 2019 Electronics Materials (Conductor, Semiconductor and Insulator)

Size: px
Start display at page:

Download "RRB JE 2019 Electronics Materials (Conductor, Semiconductor and Insulator)"

Transcription

1 RRB JE 2019 Electronics Materials (Conductor, Semiconductor and Insulator) [1 ]

2 1. Nucleus is made of न भभक बन ह त ह : - a) Electrons and Protons b) Photons and neutrons c) Photons and neutrons d) Photons and electrons 2. Atom of any element is ककस तत वn क परम ण ह त ह : - a) Positively charged b) Negatively charged c) Positively or negatively charged d) Not charged 3. Conduction of electricity through conductor takes place by क डक टर क म ध यम स भबजल क स च लन ह त ह a) Protons b) Neutrons c) Bound electrons d) Free electrons 4. Intrinsic semiconductor at room temperature will have.. a) Electrons b) Holes c) Both electrons and holes d) None of the above [2 ]

3 5. Intrinsic semiconductor at 0 K will have.. available for conduction. a) Electrons b) Holes c) Both electrons and holes d) Nothing 6. At room temperature N type material will have a) More of electrons b) More of holes c) Equal number of electrons and holes d) None 7. A room temperature P type material will have. a) More of electrons b) More of holes c) Equal number of electrons and holes d) None 8. One ev of energy is equivalent to a) 2.0 ers b) joule c) Joule d) Joule [3 ]

4 9. Which of the following statements is incorrect regarding conduction band? a) It lies below the valence band b) It may be either empty or partially filled c) It is lowest unfilled energy band d) It represents the energy of conduction electrons. 10. The forbidden band in germanium at 0 K is a) 0.03 ev b) ev c) 1.5 ev d) 2.0 ev 11. Donor type semi conductor is formed by adding impurity of valency. a) 2 b) 3 c) 4 d) Fermi level represents the energy level with probability of its occupation of Fermi स तर इसक कब ज क स भ वन क स थ ऊज स तर क प रभतभनभ त व करत ह a) Zero b) 25 Percent c) 50 Percent d) 100 Percent [4 ]

5 13. Consider the energy level diagram of an intrinsic semiconductor. The Fermi level lies in the a) Valence band b) Forbidden gap c) Conduction band or d) It can be at any of the above locations depending upon the doping concentration and temperature. 14. A semiconductor has. Temperature co efficient of resistance. a) Zero b) Positive c) Negative d) None of the above 15. A semiconductor in its purest form is called. a) Insulator b) Superconductor c) Intrinsic semiconductor d) Extrinsic semiconductor 16. An electron in the conduction band a) Is always chargeless b) Has tendency to leave the atom c) Has lower energy than an electron in the valence band. d) Has higher energy than and electron in the valence band. [5 ]

6 17... has the highest mobility. a) Electron b) Positive ions c) Negative ions d) Neutrons 18. The donor impurity must have only.. valence electrons. a) Two b) Three c) Four d) Five 19. Acceptor type impurities.. a) Can be added to silicon but not to germanium b) Create excess electrons c) Must have three valence electrons. d) Must have five valence electrons. 20. Which of the following cannot exist outside a semiconductor? इनम स क न स स म क डक टuर क ब हर नह रहत ह a) Hole b) Electron c) Both (a) and (b) d) None of the above [6 ]

7 21. In a N type semiconductor, the position of the Fermi level N type अर द च लक म फम स तtर क भस थभत ह त ह : - a) Is at the centre of the energy gap b) Is lower than the centre of energy gap c) Is higher than the centre of energy gap d) Can be anywhere depending upon the doping concentration. 22. Fermi energy is the amount of energy which a) A valence electron can have at room temperature b) Must be given to a hole to move it to valence band c) A hole can have at room temperature. d) Must be given to an electron to move it to conduction band. 23. An intrinsic semiconductor has the following properties : 1. Its electron concentration equals its hole concentration. 2. Its carrier density increases with temperature. 3. Its conductivity decrease with temperature. Which of these statements are correct? a) 1,2 and 3 b) 2 and 3 only c) 1 and 3 only d) 1 and 2 only [7 ]

8 24. A hole in a semiconductor has 1. Positive charge equal to the electron charge. 2. Positive mass equal to the mass of the electron. 3. An effective mass greater than the effective mass of electron. 4. Negative mass and positive charge equal to the charge in nucleus. Which of these statements are correct? a) 1,2,3 and 4 b) 1 and 3 only c) 2 and 4 only d) 3 and 4 only 25. Medium doping in Silicon and Germanium corresponds to impurity of the order of a) 1 part in 10 6 b) 1 part in 10 5 c) 1 part in 10 4 d) 1 part in At very high temperature, an n type semiconductor behave like a) A p type semiconductor b) An intrinsic semiconductor c) A superconductor d) An n type semiconductor [8 ]

9 27. The Fermi level in a p type semiconductor lies close to a) Top of the valence band b) Bottom of the valence band c) Top of the conduction band d) Bottom of the conduction band 28. Covalent bond energy in germanium is about a) 7.4 ev b) 3.1 ev c) 3.4 ev d) 0.7 ev 29. The energy gap in the energy band structure of a material is 9 ev at room temperature. The material is a) Semiconductor b) Conductor c) Metal d) Insulator 30. By doping germanium with Gallium, the types of semiconductors formed are : 1. N type 2. P type 3. Intrinsic 4. Extrinsic [9 ]

10 Which of the above are correct : - a) 1 and 4 b) 2 and 4 c) 1 and 3 d) 2 and An n type can be formed by adding impurity of 1. Phosphorous 2. Arsenic 3. Boron 4. Aluminum Which of the above are correct? a) 1 and 2 b) 2 and 3 c) 3 and 4 d) 1 and 4 [10 ]

11 [11 ]

CLASS 12th. Semiconductors

CLASS 12th. Semiconductors CLASS 12th Semiconductors 01. Distinction Between Metals, Insulators and Semi-Conductors Metals are good conductors of electricity, insulators do not conduct electricity, while the semiconductors have

More information

First-Hand Investigation: Modeling of Semiconductors

First-Hand Investigation: Modeling of Semiconductors perform an investigation to model the behaviour of semiconductors, including the creation of a hole or positive charge on the atom that has lost the electron and the movement of electrons and holes in

More information

Lecture 1. OUTLINE Basic Semiconductor Physics. Reading: Chapter 2.1. Semiconductors Intrinsic (undoped) silicon Doping Carrier concentrations

Lecture 1. OUTLINE Basic Semiconductor Physics. Reading: Chapter 2.1. Semiconductors Intrinsic (undoped) silicon Doping Carrier concentrations Lecture 1 OUTLINE Basic Semiconductor Physics Semiconductors Intrinsic (undoped) silicon Doping Carrier concentrations Reading: Chapter 2.1 EE105 Fall 2007 Lecture 1, Slide 1 What is a Semiconductor? Low

More information

Semiconductors 1. Explain different types of semiconductors in detail with necessary bond diagrams. Intrinsic semiconductors:

Semiconductors 1. Explain different types of semiconductors in detail with necessary bond diagrams. Intrinsic semiconductors: Semiconductors 1. Explain different types of semiconductors in detail with necessary bond diagrams. There are two types of semi conductors. 1. Intrinsic semiconductors 2. Extrinsic semiconductors Intrinsic

More information

EXTRINSIC SEMICONDUCTOR

EXTRINSIC SEMICONDUCTOR EXTRINSIC SEMICONDUCTOR EXTRINSIC SEMICONDUCTOR A semiconductor in which the impurity atoms are added by doping process is called Extrinsic semiconductor. The addition of impurities increases the carrier

More information

Atoms? All matters on earth made of atoms (made up of elements or combination of elements).

Atoms? All matters on earth made of atoms (made up of elements or combination of elements). Chapter 1 Atoms? All matters on earth made of atoms (made up of elements or combination of elements). Atomic Structure Atom is the smallest particle of an element that can exist in a stable or independent

More information

ECE 250 Electronic Devices 1. Electronic Device Modeling

ECE 250 Electronic Devices 1. Electronic Device Modeling ECE 250 Electronic Devices 1 ECE 250 Electronic Device Modeling ECE 250 Electronic Devices 2 Introduction to Semiconductor Physics You should really take a semiconductor device physics course. We can only

More information

ELECTRONIC I Lecture 1 Introduction to semiconductor. By Asst. Prof Dr. Jassim K. Hmood

ELECTRONIC I Lecture 1 Introduction to semiconductor. By Asst. Prof Dr. Jassim K. Hmood ELECTRONIC I Lecture 1 Introduction to semiconductor By Asst. Prof Dr. Jassim K. Hmood SOLID-STATE ELECTRONIC MATERIALS Electronic materials generally can be divided into three categories: insulators,

More information

Introduction to Engineering Materials ENGR2000. Dr.Coates

Introduction to Engineering Materials ENGR2000. Dr.Coates Introduction to Engineering Materials ENGR2000 Chapter 18: Electrical Properties Dr.Coates 18.2 Ohm s Law V = IR where R is the resistance of the material, V is the voltage and I is the current. l R A

More information

CLASS 1 & 2 REVISION ON SEMICONDUCTOR PHYSICS. Reference: Electronic Devices by Floyd

CLASS 1 & 2 REVISION ON SEMICONDUCTOR PHYSICS. Reference: Electronic Devices by Floyd CLASS 1 & 2 REVISION ON SEMICONDUCTOR PHYSICS Reference: Electronic Devices by Floyd 1 ELECTRONIC DEVICES Diodes, transistors and integrated circuits (IC) are typical devices in electronic circuits. All

More information

DEPARTMENT OF MECHANICAL ENGINEERING MONAD UNIVERSITY, HAPUR

DEPARTMENT OF MECHANICAL ENGINEERING MONAD UNIVERSITY, HAPUR Session - (2018-2019) Programme Name: Student s Name: Father s Name: Enrollment Number: Course Name: Course Code: Assignment Number: Date of Submission: Course Faculty Signature Course: DIPME-211 Strength

More information

ECE 335: Electronic Engineering Lecture 2: Semiconductors

ECE 335: Electronic Engineering Lecture 2: Semiconductors Faculty of Engineering ECE 335: Electronic Engineering Lecture 2: Semiconductors Agenda Intrinsic Semiconductors Extrinsic Semiconductors N-type P-type Carrier Transport Drift Diffusion Semiconductors

More information

Diamond. Covalent Insulators and Semiconductors. Silicon, Germanium, Gray Tin. Chem 462 September 24, 2004

Diamond. Covalent Insulators and Semiconductors. Silicon, Germanium, Gray Tin. Chem 462 September 24, 2004 Covalent Insulators and Chem 462 September 24, 2004 Diamond Pure sp 3 carbon All bonds staggered- ideal d(c-c) - 1.54 Å, like ethane Silicon, Germanium, Gray Tin Diamond structure Si and Ge: semiconductors

More information

WORKSHEET SESSION ( ) CLASS- II ENGLISH NAME SECTION DATE

WORKSHEET SESSION ( ) CLASS- II ENGLISH NAME SECTION DATE WORKSHEET SESSION (2017-18) CLASS- II ENGLISH NAME SECTION DATE Q1 Tick the correct answer a) Mother squirrel and baby squirrel were sitting on a branch of Neem tree Apple tree Mango tree b) Did Ravi sleep

More information

Electro - Principles I

Electro - Principles I Electro - Principles I Page 10-1 Atomic Theory It is necessary to know what goes on at the atomic level of a semiconductor so the characteristics of the semiconductor can be understood. In many cases a

More information

Review of Semiconductor Fundamentals

Review of Semiconductor Fundamentals ECE 541/ME 541 Microelectronic Fabrication Techniques Review of Semiconductor Fundamentals Zheng Yang (ERF 3017, email: yangzhen@uic.edu) Page 1 Semiconductor A semiconductor is an almost insulating material,

More information

ECE 442. Spring, Lecture -2

ECE 442. Spring, Lecture -2 ECE 442 Power Semiconductor Devices and Integrated circuits Spring, 2006 University of Illinois at Chicago Lecture -2 Semiconductor physics band structures and charge carriers 1. What are the types of

More information

A semiconductor is an almost insulating material, in which by contamination (doping) positive or negative charge carriers can be introduced.

A semiconductor is an almost insulating material, in which by contamination (doping) positive or negative charge carriers can be introduced. Semiconductor A semiconductor is an almost insulating material, in which by contamination (doping) positive or negative charge carriers can be introduced. Page 2 Semiconductor materials Page 3 Energy levels

More information

Charge Carriers in Semiconductor

Charge Carriers in Semiconductor Charge Carriers in Semiconductor To understand PN junction s IV characteristics, it is important to understand charge carriers behavior in solids, how to modify carrier densities, and different mechanisms

More information

NICNET:HP Page 1 of 7 (District Collector,Kangra)

NICNET:HP Page 1 of 7 (District Collector,Kangra) 1 ब ड ठणग हर Sq. Metre National Highway 0 0 0 0 0 0 0 0 0 0 2 भ ल ग Sq. Metre National Highway 0 0 0 0 0 0 0 0 0 0 Other Road 83 69 66 55 50 41 41 34 33 28 3 बड ध र Sq. Metre National Highway 0 0 0 0 0

More information

Amar Sir One stop solution for all competitive exams Static General Knowledge: General Science (Both in English and Hindi)

Amar Sir One stop solution for all competitive exams Static General Knowledge: General Science (Both in English and Hindi) Amar Sir One stop solution for all competitive exams Static General Knowledge General Science ( Mass, Weight And Density ) By Pradeep Pradhan If You Keep Chasing Your Dreams,One day you ll Catch them यद

More information

Carriers Concentration in Semiconductors - V. Prof.P. Ravindran, Department of Physics, Central University of Tamil Nadu, India

Carriers Concentration in Semiconductors - V. Prof.P. Ravindran, Department of Physics, Central University of Tamil Nadu, India Carriers Concentration in Semiconductors - V 1 Prof.P. Ravindran, Department of Physics, Central University of Tamil Nadu, India http://folk.uio.no/ravi/semi2013 Motion and Recombination of Electrons and

More information

EE 346: Semiconductor Devices. 02/08/2017 Tewodros A. Zewde 1

EE 346: Semiconductor Devices. 02/08/2017 Tewodros A. Zewde 1 EE 346: Semiconductor Devices 02/08/2017 Tewodros A. Zewde 1 DOPANT ATOMS AND ENERGY LEVELS Without help the total number of carriers (electrons and holes) is limited to 2ni. For most materials, this is

More information

Engineering 2000 Chapter 8 Semiconductors. ENG2000: R.I. Hornsey Semi: 1

Engineering 2000 Chapter 8 Semiconductors. ENG2000: R.I. Hornsey Semi: 1 Engineering 2000 Chapter 8 Semiconductors ENG2000: R.I. Hornsey Semi: 1 Overview We need to know the electrical properties of Si To do this, we must also draw on some of the physical properties and we

More information

Lecture 2 Electrons and Holes in Semiconductors

Lecture 2 Electrons and Holes in Semiconductors EE 471: Transport Phenomena in Solid State Devices Spring 2018 Lecture 2 Electrons and Holes in Semiconductors Bryan Ackland Department of Electrical and Computer Engineering Stevens Institute of Technology

More information

A New Plus Course by Amar Sir in the Bank Exam Category is now Live!

A New Plus Course by Amar Sir in the Bank Exam Category is now Live! For 100 most important Data Interpretation Sets for SBI PO 2019, watch: https://unacademy.com/course/hindi- 100-data-interpretation-sets-for-sbipoclerk-2019/R2EJY9BM @unacademy (Hindi) 100+ Important Miscellaneous

More information

Chapter 1 Overview of Semiconductor Materials and Physics

Chapter 1 Overview of Semiconductor Materials and Physics Chapter 1 Overview of Semiconductor Materials and Physics Professor Paul K. Chu Conductivity / Resistivity of Insulators, Semiconductors, and Conductors Semiconductor Elements Period II III IV V VI 2 B

More information

Microscopic Ohm s Law

Microscopic Ohm s Law Microscopic Ohm s Law Outline Semiconductor Review Electron Scattering and Effective Mass Microscopic Derivation of Ohm s Law 1 TRUE / FALSE 1. Judging from the filled bands, material A is an insulator.

More information

ENERGY BANDS AND GAPS IN SEMICONDUCTOR. Muhammad Hafeez Javed

ENERGY BANDS AND GAPS IN SEMICONDUCTOR. Muhammad Hafeez Javed ENERGY BANDS AND GAPS IN SEMICONDUCTOR Muhammad Hafeez Javed www.rmhjaved.com rmhjaved@gmail.com Out Line Introduction Energy band Classification of materials Direct and indirect band gap of SC Classification

More information

EE495/695 Introduction to Semiconductors I. Y. Baghzouz ECE Department UNLV

EE495/695 Introduction to Semiconductors I. Y. Baghzouz ECE Department UNLV EE495/695 Introduction to Semiconductors I Y. Baghzouz ECE Department UNLV Introduction Solar cells have always been aligned closely with other electronic devices. We will cover the basic aspects of semiconductor

More information

smal band gap Saturday, April 9, 2011

smal band gap Saturday, April 9, 2011 small band gap upper (conduction) band empty small gap valence band filled 2s 2p 2s 2p hybrid (s+p)band 2p no gap 2s (depend on the crystallographic orientation) extrinsic semiconductor semi-metal electron

More information

EECS130 Integrated Circuit Devices

EECS130 Integrated Circuit Devices EECS130 Integrated Circuit Devices Professor Ali Javey 8/30/2007 Semiconductor Fundamentals Lecture 2 Read: Chapters 1 and 2 Last Lecture: Energy Band Diagram Conduction band E c E g Band gap E v Valence

More information

ECE 142: Electronic Circuits Lecture 3: Semiconductors

ECE 142: Electronic Circuits Lecture 3: Semiconductors Faculty of Engineering ECE 142: Electronic Circuits Lecture 3: Semiconductors Agenda Intrinsic Semiconductors Extrinsic Semiconductors N-type P-type Carrier Transport Drift Diffusion Semiconductors A semiconductor

More information

Due to the quantum nature of electrons, one energy state can be occupied only by one electron.

Due to the quantum nature of electrons, one energy state can be occupied only by one electron. In crystalline solids, not all values of the electron energy are possible. The allowed intervals of energy are called allowed bands (shown as blue and chess-board blue). The forbidden intervals are called

More information

ITT Technical Institute ET215 Devices I Unit 1

ITT Technical Institute ET215 Devices I Unit 1 ITT Technical Institute ET215 Devices I Unit 1 Chapter 1 Chapter 2, Sections 2.1-2.4 Chapter 1 Basic Concepts of Analog Circuits Recall ET115 & ET145 Ohms Law I = V/R If voltage across a resistor increases

More information

EE143 Fall 2016 Microfabrication Technologies. Evolution of Devices

EE143 Fall 2016 Microfabrication Technologies. Evolution of Devices EE143 Fall 2016 Microfabrication Technologies Prof. Ming C. Wu wu@eecs.berkeley.edu 511 Sutardja Dai Hall (SDH) 1-1 Evolution of Devices Yesterday s Transistor (1947) Today s Transistor (2006) 1-2 1 Why

More information

Electrons are shared in covalent bonds between atoms of Si. A bound electron has the lowest energy state.

Electrons are shared in covalent bonds between atoms of Si. A bound electron has the lowest energy state. Photovoltaics Basic Steps the generation of light-generated carriers; the collection of the light-generated carriers to generate a current; the generation of a large voltage across the solar cell; and

More information

SOLID STATE ELECTRONICS DIGITAL ELECTRONICS SOFT CONDENSED MATTER PHYSICS

SOLID STATE ELECTRONICS DIGITAL ELECTRONICS SOFT CONDENSED MATTER PHYSICS SOLID STATE ELECTRONICS DIGITAL ELECTRONICS SOFT CONDENSED MATTER PHYSICS The energy band occupied by the valence electrons is called valence band and is the highest filled band. Bnd occupied by the electrons

More information

Lecture 2. Semiconductor Physics. Sunday 4/10/2015 Semiconductor Physics 1-1

Lecture 2. Semiconductor Physics. Sunday 4/10/2015 Semiconductor Physics 1-1 Lecture 2 Semiconductor Physics Sunday 4/10/2015 Semiconductor Physics 1-1 Outline Intrinsic bond model: electrons and holes Charge carrier generation and recombination Intrinsic semiconductor Doping:

More information

A sum of money becomes ` 2016 in 2 years and ` 2124 in 3 years, at simple interest. What is the sum of money? Q2_OA ` 1700

A sum of money becomes ` 2016 in 2 years and ` 2124 in 3 years, at simple interest. What is the sum of money? Q2_OA ` 1700 COAL INDIA LIMITED RECRUITMENT OF MANAGEMENT TRAINEES 2016-17 MODEL QUESTIONS FOR PAPER-I :COMMON FOR ALL DISCIPLINES ENGLISH: Q1 What is the least number which when divided by 24, 96 and 84 leaves remainder

More information

EE 446/646 Photovoltaic Devices I. Y. Baghzouz

EE 446/646 Photovoltaic Devices I. Y. Baghzouz EE 446/646 Photovoltaic Devices I Y. Baghzouz What is Photovoltaics? First used in about 1890, the word has two parts: photo, derived from the Greek word for light, volt, relating to electricity pioneer

More information

EECS143 Microfabrication Technology

EECS143 Microfabrication Technology EECS143 Microfabrication Technology Professor Ali Javey Introduction to Materials Lecture 1 Evolution of Devices Yesterday s Transistor (1947) Today s Transistor (2006) Why Semiconductors? Conductors e.g

More information

Lecture (02) Introduction to Electronics II, PN Junction and Diodes I

Lecture (02) Introduction to Electronics II, PN Junction and Diodes I Lecture (02) Introduction to Electronics II, PN Junction and Diodes I By: Dr. Ahmed ElShafee ١ Agenda Current in semiconductors/conductors N type, P type semiconductors N Type Semiconductor P Type Semiconductor

More information

SEMICONDUCTOR PHYSICS

SEMICONDUCTOR PHYSICS SEMICONDUCTOR PHYSICS by Dibyendu Chowdhury Semiconductors The materials whose electrical conductivity lies between those of conductors and insulators, are known as semiconductors. Silicon Germanium Cadmium

More information

UNIT TEST 4 CLASS V. Recitation of poem - The Vagabond and A Winter Night. Exercise of skill book of the above chapters will be discussed.

UNIT TEST 4 CLASS V. Recitation of poem - The Vagabond and A Winter Night. Exercise of skill book of the above chapters will be discussed. UNIT TEST 4 CLASS V 1. English Active Teach- Frames Ch- 11 The Vagabond (Poem) Ch-12 Seven Wonders of the Ancient World Ch-13 A Winter Night (Poem) Ch-14 The Refund Finger reading of Chapter 11 and 13,

More information

n i exp E g 2kT lnn i E g 2kT

n i exp E g 2kT lnn i E g 2kT HOMEWORK #10 12.19 For intrinsic semiconductors, the intrinsic carrier concentration n i depends on temperature as follows: n i exp E g 2kT (28.35a) or taking natural logarithms, lnn i E g 2kT (12.35b)

More information

Electronic Devices & Circuits

Electronic Devices & Circuits Electronic Devices & Circuits For Electronics & Communication Engineering By www.thegateacademy.com Syllabus Syllabus for Electronic Devices Energy Bands in Intrinsic and Extrinsic Silicon, Carrier Transport,

More information

Lecture (02) PN Junctions and Diodes

Lecture (02) PN Junctions and Diodes Lecture (02) PN Junctions and Diodes By: Dr. Ahmed ElShafee ١ I Agenda N type, P type semiconductors N Type Semiconductor P Type Semiconductor PN junction Energy Diagrams of the PN Junction and Depletion

More information

CEMTool Tutorial. Semiconductor physics

CEMTool Tutorial. Semiconductor physics EMTool Tutorial Semiconductor physics Overview This tutorial is part of the EMWARE series. Each tutorial in this series will teach you a specific topic of common applications by explaining theoretical

More information

NICNET:HP Page 1 of 7 (District Collector,Kangra)

NICNET:HP Page 1 of 7 (District Collector,Kangra) 1 पपल थर स न हत Sq. Metre National Highway 0 0 0 0 0 0 0 0 0 0 2 व ण व ण नचल Sq. Metre National Highway 0 0 0 0 0 0 0 0 0 0 Other Road 1728 1440 1382 1152 1037 864 864 720 691 576 3 व ण उपर ल Sq. Metre

More information

Semiconductor Devices and Circuits Fall Midterm Exam. Instructor: Dr. Dietmar Knipp, Professor of Electrical Engineering. Name: Mat. -Nr.

Semiconductor Devices and Circuits Fall Midterm Exam. Instructor: Dr. Dietmar Knipp, Professor of Electrical Engineering. Name: Mat. -Nr. Semiconductor Devices and Circuits Fall 2003 Midterm Exam Instructor: Dr. Dietmar Knipp, Professor of Electrical Engineering Name: Mat. -Nr.: Guidelines: Duration of the Midterm: 1 hour The exam is a closed

More information

ESE 372 / Spring 2013 / Lecture 5 Metal Oxide Semiconductor Field Effect Transistor

ESE 372 / Spring 2013 / Lecture 5 Metal Oxide Semiconductor Field Effect Transistor Metal Oxide Semiconductor Field Effect Transistor V G V G 1 Metal Oxide Semiconductor Field Effect Transistor We will need to understand how this current flows through Si What is electric current? 2 Back

More information

वषय: 31/12/18 स 06/01/19 तक क स ह क लए आरआरएएस ल ख क ववरण. Sub: RRAS Settlement Account Statement for the week of 31/12/18 to 06/01/19

वषय: 31/12/18 स 06/01/19 तक क स ह क लए आरआरएएस ल ख क ववरण. Sub: RRAS Settlement Account Statement for the week of 31/12/18 to 06/01/19 भ रत सरक र क य व त धकरण द ण य व त स म त, र स क स स र ड ब गल र :-0 00 Government of India Central Electricity Authority Southern Regional Committee, Race Course Cross Road BENGALURU - 0 00 Phone : 00 -

More information

ECE201 Electron Devices. Presented by K.Pandiaraj ECE Kalasalingam University

ECE201 Electron Devices. Presented by K.Pandiaraj ECE Kalasalingam University ECE201 Electron Devices Presented by K.Pandiaraj ECE Kalasalingam University Atom Atoms are the main building blocks of matter. All the materials are made up of very small particles called atoms. For example

More information

EE301 Electronics I , Fall

EE301 Electronics I , Fall EE301 Electronics I 2018-2019, Fall 1. Introduction to Microelectronics (1 Week/3 Hrs.) Introduction, Historical Background, Basic Consepts 2. Rewiev of Semiconductors (1 Week/3 Hrs.) Semiconductor materials

More information

EE 346: Semiconductor Devices

EE 346: Semiconductor Devices EE 346: Semiconductor Devices Lecture - 6 02/06/2017 Tewodros A. Zewde 1 DENSTY OF STATES FUNCTON Since current is due to the flow of charge, an important step in the process is to determine the number

More information

Chemistry Instrumental Analysis Lecture 8. Chem 4631

Chemistry Instrumental Analysis Lecture 8. Chem 4631 Chemistry 4631 Instrumental Analysis Lecture 8 UV to IR Components of Optical Basic components of spectroscopic instruments: stable source of radiant energy transparent container to hold sample device

More information

Ga and P Atoms to Covalent Solid GaP

Ga and P Atoms to Covalent Solid GaP Ga and P Atoms to Covalent Solid GaP Band Gaps in Binary Group III-V Semiconductors Mixed Semiconductors Affect of replacing some of the As with P in GaAs Band Gap (ev) (nm) GaAs 1.35 919 (IR) GaP 2.24

More information

David J. Starling Penn State Hazleton PHYS 214

David J. Starling Penn State Hazleton PHYS 214 Being virtually killed by a virtual laser in a virtual space is just as effective as the real thing, because you are as dead as you think you are. -Douglas Adams, Mostly Harmless David J. Starling Penn

More information

(Ans. (i) x=3 (ii) x=8 (iii) x = 5 (iv) x = 1) Q11. If a and b are rational number then find the value of a and b in each of following : (i)

(Ans. (i) x=3 (ii) x=8 (iii) x = 5 (iv) x = 1) Q11. If a and b are rational number then find the value of a and b in each of following : (i) D.A.V. PUBLIC SCHOOL, KURUKSHETRA CLASS : IX ASSIGNMENT : MATHEMATICS (SUMMATIVE ASSESSMENT -1) CHAPTER 1 (NUMBER SYSTEM) Q1. Define rational number? Write three rational numbers equivalent to. Q2. Write

More information

Processing of Semiconducting Materials Prof. Pallab Banerji Department of Material Science Indian Institute of Technology, Kharagpur

Processing of Semiconducting Materials Prof. Pallab Banerji Department of Material Science Indian Institute of Technology, Kharagpur Processing of Semiconducting Materials Prof. Pallab Banerji Department of Material Science Indian Institute of Technology, Kharagpur Lecture - 4 Doping in Semiconductors Good morning. Let us start with

More information

Introduction to Semiconductor Physics. Prof.P. Ravindran, Department of Physics, Central University of Tamil Nadu, India

Introduction to Semiconductor Physics. Prof.P. Ravindran, Department of Physics, Central University of Tamil Nadu, India Introduction to Semiconductor Physics 1 Prof.P. Ravindran, Department of Physics, Central University of Tamil Nadu, India http://folk.uio.no/ravi/cmp2013 Review of Semiconductor Physics Semiconductor fundamentals

More information

Basic Semiconductor Physics

Basic Semiconductor Physics 6 Basic Semiconductor Physics 6.1 Introduction With this chapter we start with the discussion of some important concepts from semiconductor physics, which are required to understand the operation of solar

More information

The Semiconductor in Equilibrium

The Semiconductor in Equilibrium Lecture 6 Semiconductor physics IV The Semiconductor in Equilibrium Equilibrium, or thermal equilibrium No external forces such as voltages, electric fields. Magnetic fields, or temperature gradients are

More information

Background of Indic segmentation

Background of Indic segmentation Background of Indic segmentation (Input for UAX#29 technical report) India has large linguistic diversity with 22 constitutionally recognized languages and 12 scripts. The mapping between languages and

More information

Module - 01 Assignment - 02 Intrinsic Semiconductors. In today's assignment class, we will be looking fully at intrinsic semiconductors.

Module - 01 Assignment - 02 Intrinsic Semiconductors. In today's assignment class, we will be looking fully at intrinsic semiconductors. Electronic Materials, Devices and Fabrication Dr. S. Parasuraman Department of Metallurgical and Materials Engineering Indian Institute of Technology, Madras Module - 01 Assignment - 02 Intrinsic Semiconductors

More information

Lecture 7: Extrinsic semiconductors - Fermi level

Lecture 7: Extrinsic semiconductors - Fermi level Lecture 7: Extrinsic semiconductors - Fermi level Contents 1 Dopant materials 1 2 E F in extrinsic semiconductors 5 3 Temperature dependence of carrier concentration 6 3.1 Low temperature regime (T < T

More information

ARMY PUBLIC SCHOOL UDHAMPUR HOLIDAY HOMEWORK WORKSHEET

ARMY PUBLIC SCHOOL UDHAMPUR HOLIDAY HOMEWORK WORKSHEET ARMY PUBLIC SCHOOL UDHAMPUR HOLIDAY HOMEWORK WORKSHEET 2017-18 NAME CLASS-VIII Please complete the Holiday Home Work given below. Question Bank and extra activities of various subjects are uploaded on

More information

ABSTRACT/ स र श ४, ३०५ ह ट यर. 4,305 ha to E Longitude प व द श तर व त त म द सव. February 2018 to March 2018

ABSTRACT/ स र श ४, ३०५ ह ट यर. 4,305 ha to E Longitude प व द श तर व त त म द सव. February 2018 to March 2018 ABSTRACT/ स र श 1. सव त Survey 2. क ल म न च त तथ रप ट कय गय फल Total Mapped and Reported 3. उपय ग कय आध र न श Base map used : स द र स व दन और भ ग लक स चन ण ल क उपय ग करत ए एनट प स, सपट, बल सप र, छ सगढ़

More information

Electrical Properties

Electrical Properties Electrical Properties Electrical Conduction R Ohm s law V = IR I l Area, A V where I is current (Ampere), V is voltage (Volts) and R is the resistance (Ohms or ) of the conductor Resistivity Resistivity,

More information

A sum of money becomes ` 2016 in 2 years and ` 2124 in 3 years, at simple interest. What is the sum of money? Q2_OA ` 1700

A sum of money becomes ` 2016 in 2 years and ` 2124 in 3 years, at simple interest. What is the sum of money? Q2_OA ` 1700 COAL INDIA LIMITED RECRUITMENT OF MANAGEMENT TRAINEES 2016-17 MODEL QUESTIONS FOR PAPER-I :COMMON FOR ALL DISCIPLINES ENGLISH: Q1 What is the least number which when divided by 24, 96 and 84 leaves remainder

More information

Introduction to Semiconductor Devices

Introduction to Semiconductor Devices Physics 233 Experiment 48 Introduction to Semiconductor Devices References 1. G.W. Neudeck, The PN Junction Diode, Addison-Wesley MA 1989 2. Background notes (Appendix A) 3. Specification sheet for Diode

More information

Introduction to Electronics and Semiconductor

Introduction to Electronics and Semiconductor Introduction to Electronics and Semiconductor 1 Chapter Objectives To study and understand basic electronics. To study and understand semiconductor principles. 2 Definition Electronics is the branch of

More information

Lecture 3b. Bonding Model and Dopants. Reading: (Cont d) Notes and Anderson 2 sections

Lecture 3b. Bonding Model and Dopants. Reading: (Cont d) Notes and Anderson 2 sections Lecture 3b Bonding Model and Dopants Reading: (Cont d) Notes and Anderson 2 sections 2.3-2.7 The need for more control over carrier concentration Without help the total number of carriers (electrons and

More information

Semiconductor Device Physics

Semiconductor Device Physics 1 Semiconductor Device Physics Lecture 1 http://zitompul.wordpress.com 2 0 1 3 2 Semiconductor Device Physics Textbook: Semiconductor Device Fundamentals, Robert F. Pierret, International Edition, Addison

More information

MASTER QUESTION PAPER WITH KEY 3. य द NOCIE, और SCENT,!#%$^ क प म क ड कय ज त ह, त COIN क क ड म क स लख ज एग? A. B. D.

MASTER QUESTION PAPER WITH KEY 3. य द NOCIE, और SCENT,!#%$^ क प म क ड कय ज त ह, त COIN क क ड म क स लख ज एग? A. B. D. 1. क न स श द न च दए गए स ब ध क सबस अ छ तरह स प र कर ग? फ ल : गमल :: खल ड़ :?. ट म. क न. ख ल. ख त 2. क न स श द न च दए गए स ब ध क सबस अ छ तरह स प र कर ग? म च : चमड़ :: दज :?. पर. फ त. ध ग. कपड़ 3. य द NOIE,

More information

Electronic Circuits for Mechatronics ELCT 609 Lecture 2: PN Junctions (1)

Electronic Circuits for Mechatronics ELCT 609 Lecture 2: PN Junctions (1) Electronic Circuits for Mechatronics ELCT 609 Lecture 2: PN Junctions (1) Assistant Professor Office: C3.315 E-mail: eman.azab@guc.edu.eg 1 Electronic (Semiconductor) Devices P-N Junctions (Diodes): Physical

More information

Solutions for IBPS Clerk Pre: Expected Paper 1

Solutions for IBPS Clerk Pre: Expected Paper 1 Solutions for IBPS Clerk Pre: Expected Paper 1 1-D Rest options apart from option (4) can easily be inferred from the passage. In the passage, it is nowhere mentioned that SWIFT allows a receiver to get

More information

electronics fundamentals

electronics fundamentals electronics fundamentals circuits, devices, and applications THOMAS L. FLOYD DAVID M. BUCHLA Lesson 1: Diodes and Applications Semiconductors Figure 1-1 The Bohr model of an atom showing electrons in orbits

More information

ESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems

ESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems ESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems Lec 6: September 14, 2015 MOS Model You are Here: Transistor Edition! Previously: simple models (0 and 1 st order) " Comfortable

More information

ECE 340 Lecture 6 : Intrinsic and Extrinsic Material I Class Outline:

ECE 340 Lecture 6 : Intrinsic and Extrinsic Material I Class Outline: ECE 340 Lecture 6 : Intrinsic and Extrinsic Material I Class Outline: Effective Mass Intrinsic Material Extrinsic Material Things you should know when you leave Key Questions What is the physical meaning

More information

Dear Students Holidays are always a welcome break from the normal routine and we all look forward to them. It gives us the opportunity to pursue all

Dear Students Holidays are always a welcome break from the normal routine and we all look forward to them. It gives us the opportunity to pursue all Dear Students Holidays are always a welcome break from the normal routine and we all look forward to them. It gives us the opportunity to pursue all those activities that we enjoy but never find enough

More information

The photovoltaic effect occurs in semiconductors where there are distinct valence and

The photovoltaic effect occurs in semiconductors where there are distinct valence and How a Photovoltaic Cell Works The photovoltaic effect occurs in semiconductors where there are distinct valence and conduction bands. (There are energies at which electrons can not exist within the solid)

More information

Contents CONTENTS. Page 2 of 47

Contents CONTENTS. Page 2 of 47 J. A. Hargreaves Lockerbie Academy June 2015 Contents CONTENTS Contents... 2 CHAPTER 7 CONDUCTORS, SEMICONDUCTORS AND INSULATORS... 4 Summary of Content... 4 Summary of this chapter- notes from column

More information

Higher Physics. Electricity. Summary Notes. Monitoring and measuring a.c. Current, potential difference, power and resistance

Higher Physics. Electricity. Summary Notes. Monitoring and measuring a.c. Current, potential difference, power and resistance Higher Physics Electricity Summary Notes Monitoring and measuring a.c. Current, potential difference, power and resistance Electrical sources and internal resistance Capacitors Conductors, semiconductors

More information

Electrons in materials. (where are they, what is their energy)

Electrons in materials. (where are they, what is their energy) Electrons in materials (where are they, what is their energy) 1 Lone atoms A single atom has electrons in shells and sub shells. Each of these have a distinct energy level. The diagram shows an example

More information

SEMI- CONDUCTOR PHYSICS

SEMI- CONDUCTOR PHYSICS C H A P T E R51 Learning Objectives The Atom Bohr's Atomic Model Electron Energy Levels in Hydrogen Atom Orbital (or Azimuthal) Quantum Number Orbital Magnetic Quantum Number (m l ) Magnetic Spin Quantum

More information

ELEMENTARY BAND THEORY

ELEMENTARY BAND THEORY ELEMENTARY BAND THEORY PHYSICIST Solid state band Valence band, VB Conduction band, CB Fermi energy, E F Bloch orbital, delocalized n-doping p-doping Band gap, E g Direct band gap Indirect band gap Phonon

More information

Unit IV Semiconductors Engineering Physics

Unit IV Semiconductors Engineering Physics Introduction A semiconductor is a material that has a resistivity lies between that of a conductor and an insulator. The conductivity of a semiconductor material can be varied under an external electrical

More information

UNIVERSITY OF CAMBRIDGE INTERNATIONAL EXAMINATIONS International General Certificate of Secondary Education MARK SCHEME for the May/June 2011 question paper for the guidance of teachers 0549 HINDI AS A

More information

Time & Tense समय और य क प. Mishra English Study Centre BY M. K. Mishra

Time & Tense समय और य क प. Mishra English Study Centre BY M. K. Mishra Time & Tense समय और य क प Mishra English Study Centre BY M. K. Mishra The use of appropriate verb according to appropriate time is called Time & Tense. There are three kinds of Time in uses 1. Present

More information

LN 3 IDLE MIND SOLUTIONS

LN 3 IDLE MIND SOLUTIONS IDLE MIND SOLUTIONS 1. Let us first look in most general terms at the optical properties of solids with band gaps (E g ) of less than 4 ev, semiconductors by definition. The band gap energy (E g ) can

More information

Introduction to Semiconductor Devices

Introduction to Semiconductor Devices Physics 233 Experiment 48 Introduction to Semiconductor Devices References 1. G.W. Neudeck, The PN Junction Diode, Addison-Wesley MA 1989 2. Background notes (Appendix A) 3. Specification sheet for Diode

More information

Determination of properties in semiconductor materials by applying Matlab

Determination of properties in semiconductor materials by applying Matlab Determination of properties in semiconductor materials by applying Matlab Carlos Figueroa. 1, Raúl Riera A. 2 1 Departamento de Ingeniería Industrial. Universidad de Sonora A.P. 5-088, Hermosillo, Sonora.

More information

ELECTRONIC DEVICES AND CIRCUITS SUMMARY

ELECTRONIC DEVICES AND CIRCUITS SUMMARY ELECTRONIC DEVICES AND CIRCUITS SUMMARY Classification of Materials: Insulator: An insulator is a material that offers a very low level (or negligible) of conductivity when voltage is applied. Eg: Paper,

More information

SUMMATIVE ASSESSMENT II, 2012 II, Class X /

SUMMATIVE ASSESSMENT II, 2012 II, Class X / SUMMATIVE ASSESSMENT II, 2012 II, 2012 SCIENCE / Class X / X 67014 Time allowed : 3 hours Maximum Marks : 80 3 80 General Instructions : The question paper comprises of two Sections, A and B. You are to

More information

Note that it is traditional to draw the diagram for semiconductors rotated 90 degrees, i.e. the version on the right above.

Note that it is traditional to draw the diagram for semiconductors rotated 90 degrees, i.e. the version on the right above. 5 Semiconductors The nearly free electron model applies equally in the case where the Fermi level lies within a small band gap (semiconductors), as it does when the Fermi level lies within a band (metal)

More information

3.1 Introduction to Semiconductors. Y. Baghzouz ECE Department UNLV

3.1 Introduction to Semiconductors. Y. Baghzouz ECE Department UNLV 3.1 Introduction to Semiconductors Y. Baghzouz ECE Department UNLV Introduction In this lecture, we will cover the basic aspects of semiconductor materials, and the physical mechanisms which are at the

More information

Mat E 272 Lecture 25: Electrical properties of materials

Mat E 272 Lecture 25: Electrical properties of materials Mat E 272 Lecture 25: Electrical properties of materials December 6, 2001 Introduction: Calcium and copper are both metals; Ca has a valence of +2 (2 electrons per atom) while Cu has a valence of +1 (1

More information

Certified that the above candidate has admitted in course as a private candidate and is eligible to write the Examination.

Certified that the above candidate has admitted in course as a private candidate and is eligible to write the Examination. Application for registration to SECOND SASTRI PRIVATE (B.A.) Degree Examinations, April 2016 Name of the Father 3. Name of the Mother Candidates should 7. Subject ऋगव द श कलश ख Rigveda (Sakala Sakha) II

More information