Size: px
Start display at page:

Download ""

Transcription

1 February 6, 2015

2

3

4

5

6

7

8 According to free electron theory, the properties of a metal depends on gas of free electrons. The outer most electrons of metal atoms are also known as Valence Electrons.These valence electrons are weakly bound with the atoms. In a solid, the valence electrons interact and form a gas of electrons.the gas of electrons move with relative freedom throughout the resulting assembly of metal ions.these electrons holds the ions together.high electric and thermal conductivities, opacity, surface luster and other characteristic properties of metals can be explained on the basis of free electron theory. The alloy of different metals can be prepared because the free electrons do not belong to a particular atom-atom bonds. Formation of solid can also be explained on the basis of free electron theory.

9 When metal atoms are separate(isolated), their total energy is higher than when they are bound together.the reason for energy reduction is that each valence electron is on the average closer to one ion or another than it would be if it belonged to an isolated atom. Hence the electrons potential energy is reduced in metal crystal than in the atom.on the other hand, the kinetic energy of electron increases in the metal crystal.the valence energy levels of the metal atoms are all slightly altered by their interactions to give as many different energy levels as the total number of atoms present.the levels are so closely spaced as to form a continuous energy band. The free electrons in this band have a Fermi Dirac energy distribution in which, at 0 k, their kinetic energies range from 0K to maximum of ε F, the fermi energy.

10 H is a gas at atmospheric pressure.it can be converted into liquid or solid states.in all the states, it does not behave like metals. The reason is that both liquid and solid hydrogen at atmospheric consist of hydrogen molecules and these molecules hold their electrons so tightly and none can move freely. At high pressure, hydrogen can be converted into conducting liquid.high pressure forces H molecules so close together that their electron wave functions overlap, which allows electron to move from one molecule to another molecule. Metallic bonding occurs when the reduction in electron potential energy outbalances the increase in electron KE that accompanies it.the more valence electrons per atom, the higher the average kinetic energies of the free electrons, but without commensurate drop in their potential energy.

11 I = V R (1) Here, R is the resistance of the conductor, depends on its dimensions, composition, and temperature, but is independent of V.Ohm s law follows free electron theory of metals.

12 Assume the free electrons in a metal move in random directions and undergo frequent collisions.if λ is the mean free path between the collisions of a free electron, the average time τ between collisions is τ = λ v F (2) Where v F is the electron velocity that corresponds to the Fermi energy ε F, since only electron at or near the top of their energy distribution can be accelerated.electron velocity in copper v F = 2εF m = eV J/eV kg = m/s

13 The superimposed drift velocity v d due to an applied electric field is usually less than 1 mm/s.

14 Let a potential differential difference V be applied across a conductor of length L which produces an electric field E = V L in the conductor.the acceleration of the electron is given by a = F m = ee m (3) The electric field E provides drift velocity (v d ) to the free electron gas.when an electron undergoes a collision, it rebounds in an arbitrary direction.after each collision, the electron is accelerated for some time interval t before the next collision and at the end of the interval, the electron has traveled a t.when the electron has made many collisions, its average displacement will be X = a t, where t is the average of the squared time intervals. t = 2τ

15 Drift velocity is given by v d = X τ = aτ (4) Substituting the values of v d and τ, we have ( ) ( ) ee λ v d = aτ = m v F (5) If the conductor of cross sectional area A contains n free electrons per unit volume,current in the conductor is given by Substituting the value of v d, we have I = neav d (6) I = nae Eλ mv F (7)

16 Substituting the value of electric field E, we have ( ne ) ( ) λ A I = V (8) mv F L I = V R (9) where R = ( ) ( ) mvf L ne λ A (10) is the resistance of the metal conductor.the resistivity of the conductor is given by ρ = mv F ne (11) λ

17 The scattering of free electron waves in a metal is the reason for electric resistance.the scattering is caused by structural defects and by ions out of place as they vibrate. Structural defects do not depend on temperature but on the purity of the metal and on its history. The resistivities of of cold worked metals are lowered by annealing because the number of defects thereby decreased.with increase in temperature, lattice vibrations increase and thereby increase in resistivity.the resistivity of the metal is given by ρ = ρ i + ρ t (12) where ρ i depends on the concentration of defects and ρ t depends on temperature.

18 The ratio K/σ between thermal and electric conductivities is the same for all the metals and is a function of temperature. K σt = π k 3e = W.Ω/K (13)

19 Find the drift velocity v d of the free electrons in a copper wire whose cross-sectional area is A = 1mm when the wire carries a current of 1 A.Assume that each copper atom contributes one electron to the electron gas. HINT: m/s I = Q t = neav d The resistivity of copper at 20 C is ρ = Ω.m.Estimate the mean free path λ between collisions of the free electrons in copper at 20 C. Hint:λ = mv F ne ρ

20 Find the Fermi energy in copper on the assumption that each copper atom contributes one free electron to the electron gas.the density of copper is kg/m and its atomic mass is 63.5u. Hint:n = N V =. = electrons/m.. Fermi energy is given by ( ) ε F = h 3N / = J = 7.04eV 2m 8πV Derive the relation I = neavd. If the free electrons have so small a drift velocity, why does an electric appliances go on as soon as its switch is closed and not minutes or hours later? What do you mean by free electron gas? What is free electron theory of metals?

21 Explain the formation of solid on the basis of free electron theory? What is the condition for the formation of metallic bond. Hydrogen belong to group 1 in periodic table an still it is not conductor.why? How can you make liquid hydrogen conductor?give the reason for conductance. What is drift velocity? What do you mean by fermi energy? What d you mean by electron velocity at fermi energy? Use free electron theory to derive Ohm s law i.e.prove that ( ne ) ( ) λ A I = V mv F L

22 What are reasons for electric resistance of metals and how does it depend on temperature? What is Weidemann-Franz Law? Which energy distribution will be used to explain free electron theory?

23 You can learn more on click from my Home Page... Feel free to mail me for any type of suggestion for improvement of this lecture notes: srivastava

24

Unit III Free Electron Theory Engineering Physics

Unit III Free Electron Theory Engineering Physics . Introduction The electron theory of metals aims to explain the structure and properties of solids through their electronic structure. The electron theory is applicable to all solids i.e., both metals

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

Physics 1302W.400 Lecture 21 Introductory Physics for Scientists and Engineering II

Physics 1302W.400 Lecture 21 Introductory Physics for Scientists and Engineering II Physics 1302W.400 Lecture 21 Introductory Physics for Scientists and Engineering II In today s lecture, we will learn to: Calculate the resistance of a conductor depending on the material and shape Apply

More information

physics for you February 11 Page 68

physics for you February 11 Page 68 urrent Electricity Passage 1 4. f the resistance of a 1 m length of a given wire t is observed that good conductors of heat are also is 8.13 10 3 W, and it carried a current 1, the good conductors of electricity.

More information

In an electric field R and magnetic field B, the force on an electron (charge e) is given by:

In an electric field R and magnetic field B, the force on an electron (charge e) is given by: Lecture 17 Electric conduction Electrons motion in magnetic field Electrons thermal conductivity Brief review In solid state physics, we do not think about electrons zipping around randomly in real space.

More information

Problem Solving Section 1

Problem Solving Section 1 Problem Solving Section 1 Problem 1: Copper has a mass density ρ m 8.95 gmcm 3 and an electrical resistivity ρ 1.55 10 8 ohm m at room temperature. Calculate, (a). The concentration of the conduction electrons.

More information

Outline. Part II - Electronic Properties of Solids Lecture 13: The Electron Gas Continued (Kittel Ch. 6) E. Electron Gas in 3 dimensions

Outline. Part II - Electronic Properties of Solids Lecture 13: The Electron Gas Continued (Kittel Ch. 6) E. Electron Gas in 3 dimensions Part II - lectronic Properties of Solids Lecture 13: The lectron Gas Continued (Kittel Ch. 6) quilibrium - no field Physics 460 F 2006 Lect 13 1 Outline From last time: Success of quantum mechanics Pauli

More information

Assumptions of classical free electron model

Assumptions of classical free electron model Module 2 Electrical Conductivity in metals & Semiconductor 1) Drift Velocity :- The Velocity attain by an Electron in the Presence of applied electronic filed is Known as drift Velocity. 2) Mean free Path:-

More information

Nasser S. Alzayed.

Nasser S. Alzayed. Lecture #4 Nasser S. Alzayed nalzayed@ksu.edu.sa ELECTRICAL CONDUCTIVITY AND OHM'S LAW The momentum of a free electron is related to the wavevector by mv = ћk. In an electric field E and magnetic field

More information

Lecture ( 9 ) Chapter Three : Electric Field in Material Space

Lecture ( 9 ) Chapter Three : Electric Field in Material Space Lecture ( 9 ) Chapter Three : Electric Field in Material Space Properties of Materials, Convection and Conduction Currents, and Conductors 3.1 Properties of Materials Just as electric fields can exist

More information

Handout 5: Current and resistance. Electric current and current density

Handout 5: Current and resistance. Electric current and current density 1 Handout 5: Current and resistance Electric current and current density Figure 1 shows a flow of positive charge. Electric current is caused by the flow of electric charge and is defined to be equal to

More information

Unit 3 Lesson 4 Ionic, Covalent, and Metallic Bonding. Copyright Houghton Mifflin Harcourt Publishing Company

Unit 3 Lesson 4 Ionic, Covalent, and Metallic Bonding. Copyright Houghton Mifflin Harcourt Publishing Company Opposites Attract What is an ion? An atom has a neutral charge because it has an equal number of electrons and protons. An ion is a particle with a positive or negative charge. An ion forms when an atom

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

The Electromagnetic Properties of Materials

The Electromagnetic Properties of Materials The lectromagnetic Properties of Materials lectrical conduction Metals Semiconductors Insulators (dielectrics) Superconductors Magnetic materials Ferromagnetic materials Others Photonic Materials (optical)

More information

Chapter 6 Free Electron Fermi Gas

Chapter 6 Free Electron Fermi Gas Chapter 6 Free Electron Fermi Gas Free electron model: The valence electrons of the constituent atoms become conduction electrons and move about freely through the volume of the metal. The simplest metals

More information

3. In the adjacent figure, E 1 = 6.0 V, E 2 = 5.5 V, E 3 = 2.0 V, R 1 = 1W, and R 2 = 6W. All batteries are ideal. Find the current in resistor R 1.

3. In the adjacent figure, E 1 = 6.0 V, E 2 = 5.5 V, E 3 = 2.0 V, R 1 = 1W, and R 2 = 6W. All batteries are ideal. Find the current in resistor R 1. 1. A cylindrical copper rod of length L and cross-sectional area A is re-formed to twice its original length with no change in volume. If the resistance between its ends was originally R, what is it now?

More information

Semiconductor Physics

Semiconductor Physics Semiconductor Physics Motivation Is it possible that there might be current flowing in a conductor (or a semiconductor) even when there is no potential difference supplied across its ends? Look at the

More information

Molecules and Condensed Matter

Molecules and Condensed Matter Chapter 42 Molecules and Condensed Matter PowerPoint Lectures for University Physics, Thirteenth Edition Hugh D. Young and Roger A. Freedman Lectures by Wayne Anderson Goals for Chapter 42 To understand

More information

From Last Time Important new Quantum Mechanical Concepts. Atoms and Molecules. Today. Symmetry. Simple molecules.

From Last Time Important new Quantum Mechanical Concepts. Atoms and Molecules. Today. Symmetry. Simple molecules. Today From Last Time Important new Quantum Mechanical Concepts Indistinguishability: Symmetries of the wavefunction: Symmetric and Antisymmetric Pauli exclusion principle: only one fermion per state Spin

More information

Conducting surface - equipotential. Potential varies across the conducting surface. Lecture 9: Electrical Resistance.

Conducting surface - equipotential. Potential varies across the conducting surface. Lecture 9: Electrical Resistance. Lecture 9: Electrical Resistance Electrostatics (time-independent E, I = 0) Stationary Currents (time-independent E and I 0) E inside = 0 Conducting surface - equipotential E inside 0 Potential varies

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

DO PHYSICS ONLINE ELECTRIC CURRENT FROM IDEAS TO IMPLEMENTATION ATOMS TO TRANSISTORS ELECTRICAL PROPERTIES OF SOLIDS

DO PHYSICS ONLINE ELECTRIC CURRENT FROM IDEAS TO IMPLEMENTATION ATOMS TO TRANSISTORS ELECTRICAL PROPERTIES OF SOLIDS DO PHYSICS ONLINE FROM IDEAS TO IMPLEMENTATION 9.4.3 ATOMS TO TRANSISTORS ELECTRICAL PROPERTIES OF SOLIDS ELECTRIC CURRENT Different substances vary considerably in their electrical properties. It is a

More information

7. FREE ELECTRON THEORY.

7. FREE ELECTRON THEORY. 7. FREE ELECTRON THEORY. Aim: To introduce the free electron model for the physical properties of metals. It is the simplest theory for these materials, but still gives a very good description of many

More information

HALL EFFECT IN SEMICONDUCTORS

HALL EFFECT IN SEMICONDUCTORS Warsaw University of Technology Faculty of Physics Physics Laboratory I P Andrzej Kubiaczyk 30 HALL EFFECT IN SEMICONDUCTORS 1. ackground 1.1. Electron motion in electric and magnetic fields A particle

More information

Conduction. Metals, Semiconductors and Interconnects. Fig 2.1

Conduction. Metals, Semiconductors and Interconnects. Fig 2.1 Conduction Metals, Semiconductors and Interconnects Fig 2.1 Metal interconnects are used in microelectronics to wire the devices within the chip, the intergraded circuit. Multilevel interconnects are used

More information

Chapter 24: Electric Current

Chapter 24: Electric Current Chapter 24: Electric Current Electric current Electric current is a net flow of electric charge. Quantitatively, current is the rate at which charge crosses a given area. I = dq dt dq = q(n AL)=q(n Av

More information

Exam 2 Solutions. = /10 = / = /m 3, where the factor of

Exam 2 Solutions. = /10 = / = /m 3, where the factor of PHY049 Fall 007 Prof. Yasu Takano Prof. Paul Avery Oct. 17, 007 Exam Solutions 1. (WebAssign 6.6) A current of 1.5 A flows in a copper wire with radius 1.5 mm. If the current is uniform, what is the electron

More information

Condensed Matter Physics Prof. G. Rangarajan Department of Physics Indian Institute of Technology, Madras

Condensed Matter Physics Prof. G. Rangarajan Department of Physics Indian Institute of Technology, Madras Condensed Matter Physics Prof. G. Rangarajan Department of Physics Indian Institute of Technology, Madras Lecture - 10 The Free Electron Theory of Metals - Electrical Conductivity (Refer Slide Time: 00:20)

More information

ragsdale (zdr82) HW5 ditmire (58335) 1

ragsdale (zdr82) HW5 ditmire (58335) 1 ragsdale (zdr82) HW5 ditmire (58335) 1 This print-out should have 20 questions. Multiple-choice questions may continue on the next column or page find all choices before answering. 001 (part 1 of 2) 10.0

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

Chapter 25: Electric Current

Chapter 25: Electric Current Chapter 25: Electric Current Conductors and Charge Carriers Consider a conducting piece of metal: The valence electrons are weakly bound to the nuclei form a fluidlike sea of electrons that can move through

More information

1. Introduction of solid state 1.1. Elements of solid state physics:

1. Introduction of solid state 1.1. Elements of solid state physics: 1. Introduction of solid state 1.1. Elements of solid state physics: To understand the operation of many of the semiconductor devices we need, at least, an appreciation of the solid state physics of homogeneous

More information

EECS 117 Lecture 13: Method of Images / Steady Currents

EECS 117 Lecture 13: Method of Images / Steady Currents EECS 117 Lecture 13: Method of Images / Steady Currents Prof. Niknejad University of California, Berkeley University of California, Berkeley EECS 217 Lecture 13 p. 1/21 Point Charge Near Ground Plane Consider

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

Electrical Resistance

Electrical Resistance Electrical Resistance I + V _ W Material with resistivity ρ t L Resistance R V I = L ρ Wt (Unit: ohms) where ρ is the electrical resistivity 1 Adding parts/billion to parts/thousand of dopants to pure

More information

Materials & Properties II: Thermal & Electrical Characteristics. Sergio Calatroni - CERN

Materials & Properties II: Thermal & Electrical Characteristics. Sergio Calatroni - CERN Materials & Properties II: Thermal & Electrical Characteristics Sergio Calatroni - CERN Outline (we will discuss mostly metals) Electrical properties - Electrical conductivity o Temperature dependence

More information

Model Question Paper ENGINEERING PHYSICS (14PHY12/14PHY22) Note: Answer any FIVE full questions, choosing one full question from each module.

Model Question Paper ENGINEERING PHYSICS (14PHY12/14PHY22) Note: Answer any FIVE full questions, choosing one full question from each module. Model Question Paper ENGINEERING PHYSICS (14PHY1/14PHY) Time: 3 hrs. Max. Marks: 100 Note: Answer any FIVE full questions, choosing one full question from each module. MODULE 1 1) a. Explain in brief Compton

More information

Energy Losses in the Electrical Circuits

Energy Losses in the Electrical Circuits Energy Losses in the Electrical Circuits Motors, lighting systems, wiring, mechanical terminations, distribution panels, protective devices, transformers, switchgear, and all end of circuit equipment experience

More information

Lecture - 20 Electrical, Magnetic and Optical Properties of Nanomaterials (C4) (Refer Slide Time: 00:15)

Lecture - 20 Electrical, Magnetic and Optical Properties of Nanomaterials (C4) (Refer Slide Time: 00:15) Nanostructures and Nanomaterials Characterization and Properties Prof. Anandh Subramaniam Prof. Kantesh Balani Department of Material Science and Engineering Indian Institute of Technology, Kanpur Lecture

More information

Module 6 : PHYSICS OF SEMICONDUCTOR DEVICES Lecture 32 : Bonding in Solids

Module 6 : PHYSICS OF SEMICONDUCTOR DEVICES Lecture 32 : Bonding in Solids Module 6 : PHYSICS OF SEMICONDUCTOR DEVICES Lecture 32 : Bonding in Solids Objectives In this course you will learn the following Bonding in solids. Ionic and covalent bond. Structure of Silicon Concept

More information

Semiconductor Device Physics

Semiconductor Device Physics 1 Semiconductor Device Physics Lecture 3 http://zitompul.wordpress.com 2 0 1 3 Semiconductor Device Physics 2 Three primary types of carrier action occur inside a semiconductor: Drift: charged particle

More information

Chapter 9 Problem Solutions

Chapter 9 Problem Solutions Chapter 9 Problem Solutions. At what temperature would one in a thousand of the atoms in a gas of atomic hydrogen be in the n energy level? g( ε ), g( ε ) Then, where 8 n ( ε ) ( ε )/ kt kt e ε e ε / n(

More information

ADVANCED UNDERGRADUATE LABORATORY EXPERIMENT 20. Semiconductor Resistance, Band Gap, and Hall Effect

ADVANCED UNDERGRADUATE LABORATORY EXPERIMENT 20. Semiconductor Resistance, Band Gap, and Hall Effect ADVANCED UNDERGRADUATE LABORATORY EXPERIMENT 20 Semiconductor Resistance, Band Gap, and Hall Effect Revised: November 1996 by David Bailey March 1990 by John Pitre & Taek-Soon Yoon Introduction Solid materials

More information

3. Consider a semiconductor. The concentration of electrons, n, in the conduction band is given by

3. Consider a semiconductor. The concentration of electrons, n, in the conduction band is given by Colloqium problems to chapter 13 1. What is meant by an intrinsic semiconductor? n = p All the electrons are originating from thermal excitation from the valence band for an intrinsic semiconductor. Then

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

Theory of Electromigration

Theory of Electromigration Theory of Electromigration Electromigration is the transport of material in a conductor under the influence of an applied electric field. All conductors are susceptible to electromigration, therefore it

More information

Microwave Loss Reduction in Cryogenically Cooled Conductors R. Finger and A. R. Kerr

Microwave Loss Reduction in Cryogenically Cooled Conductors R. Finger and A. R. Kerr NATIONAL RADIO ASTRONOMY OBSERVATORY ELECTRONICS DIVISION INTERNAL REPORT NO. 321 Microwave Loss Reduction in Cryogenically Cooled Conductors R. Finger and A. R. Kerr July 3, 2008 NATIONAL RADIO ASTRONOMY

More information

FXA 2008 ELECTRIC CHARGE (Q) 1. Candidates should be able to : Electric charge is a property possessed by protons and electrons.

FXA 2008 ELECTRIC CHARGE (Q) 1. Candidates should be able to : Electric charge is a property possessed by protons and electrons. ELECTRIC CHARGE (Q) 1 Candidates should be able to : Explain that electric current is a net flow of charged particles. Explain that electric current in a metal is due to the movement of electrons, whereas

More information

Chapter 27: Current & Resistance. HW For Chapter 27: 6, 18, 20, 30, 42, 48, 52, 56, 58, 62, 68

Chapter 27: Current & Resistance. HW For Chapter 27: 6, 18, 20, 30, 42, 48, 52, 56, 58, 62, 68 Chapter 27: Current & Resistance HW For Chapter 27: 6, 18, 20, 30, 42, 48, 52, 56, 58, 62, 68 Positive Charges move from HI to LOW potential. HI V LOW V Negative Charges move from LOW to HI potential.

More information

Physics 213: General Physics Fall :30 AM Lecture

Physics 213: General Physics Fall :30 AM Lecture Physics 213: General Physics Fall 2004 9:30 AM Lecture Midterm I Solutions Tuesday, September 21, 2004 Chem-Phys 153 Name (print): Signature: Student Number: Your Seat Number (on back of chair): 1. Immediately

More information

PHY102 Electricity Course Summary

PHY102 Electricity Course Summary TOPIC 1 ELECTOSTTICS PHY1 Electricity Course Summary Coulomb s Law The magnitude of the force between two point charges is directly proportional to the product of the charges and inversely proportional

More information

ECE 440 Lecture 12 : Diffusion of Carriers Class Outline:

ECE 440 Lecture 12 : Diffusion of Carriers Class Outline: ECE 440 Lecture 12 : Diffusion of Carriers Class Outline: Band Bending Diffusion Processes Diffusion and Drift of Carriers Things you should know when you leave Key Questions How do I calculate kinetic

More information

半導體元件與物理. Semiconductor Devices and physics 許正興國立聯合大學電機工程學系 聯大電機系電子材料與元件應用實驗室

半導體元件與物理. Semiconductor Devices and physics 許正興國立聯合大學電機工程學系 聯大電機系電子材料與元件應用實驗室 半導體元件與物理 Semiconductor Devices and physics 許正興國立聯合大學電機工程學系 1. Crystal Structure of Solids 2. Quantum Theory of Solids 3. Semiconductor in Equilibrium and Carrier Transport phenomena 4. PN Junction and

More information

Session 5: Solid State Physics. Charge Mobility Drift Diffusion Recombination-Generation

Session 5: Solid State Physics. Charge Mobility Drift Diffusion Recombination-Generation Session 5: Solid State Physics Charge Mobility Drift Diffusion Recombination-Generation 1 Outline A B C D E F G H I J 2 Mobile Charge Carriers in Semiconductors Three primary types of carrier action occur

More information

3 Electric current, resistance, energy and power

3 Electric current, resistance, energy and power 3 3.1 Introduction Having looked at static charges, we will now look at moving charges in the form of electric current. We will examine how current passes through conductors and the nature of resistance

More information

PH 102 Exam I N N N N. 3. Which of the following is true for the electric force and not true for the gravitational force?

PH 102 Exam I N N N N. 3. Which of the following is true for the electric force and not true for the gravitational force? Name Date INSTRUCTIONS PH 102 Exam I 1. nswer all questions below. ll problems have equal weight. 2. Clearly mark the answer you choose by filling in the adjacent circle. 3. There will be no partial credit

More information

6 Chapter. Current and Resistance

6 Chapter. Current and Resistance 6 Chapter Current and Resistance 6.1 Electric Current... 6-2 6.1.1 Current Density... 6-2 6.2 Ohm s Law... 6-5 6.3 Summary... 6-8 6.4 Solved Problems... 6-9 6.4.1 Resistivity of a Cable... 6-9 6.4.2 Charge

More information

Electrical conduction in solids

Electrical conduction in solids Equations of motion Electrical conduction in solids Electrical conduction is the movement of electrically charged particles through a conductor or semiconductor, which constitutes an electric current.

More information

Understanding KMT using Gas Properties and States of Matter

Understanding KMT using Gas Properties and States of Matter Understanding KMT using Gas Properties and States of Matter Learning Goals: Students will be able to describe matter in terms of particle motion. The description should include Diagrams to support the

More information

Electric Force and Charge. Electric Force and Charge. Electric Force and Charge. Electric Force and Charge. Electric Force and Charge

Electric Force and Charge. Electric Force and Charge. Electric Force and Charge. Electric Force and Charge. Electric Force and Charge Hewitt/Lyons/Suchocki/Yeh Conceptual Integrated Science Chapter 7 ELECTRICITY AND MAGNETISM Electric forces can attract some objects and repel others Electric charge: the fundamental quantity that underlies

More information

Electrical Transport. Ref. Ihn Ch. 10 YC, Ch 5; BW, Chs 4 & 8

Electrical Transport. Ref. Ihn Ch. 10 YC, Ch 5; BW, Chs 4 & 8 Electrical Transport Ref. Ihn Ch. 10 YC, Ch 5; BW, Chs 4 & 8 Electrical Transport The study of the transport of electrons & holes (in semiconductors) under various conditions. A broad & somewhat specialized

More information

Electrons in metals PHYS208. revised Go to Topics Autumn 2010

Electrons in metals PHYS208. revised Go to Topics Autumn 2010 Go to Topics Autumn 010 Electrons in metals revised 0.1.010 PHYS08 Topics 0.1.010 Classical Models The Drude Theory of metals Conductivity - static electric field Thermal conductivity Fourier Law Wiedemann-Franz

More information

The Heisenberg uncertainty principle. The Pauli exclusion principle. Classical conductance.

The Heisenberg uncertainty principle. The Pauli exclusion principle. Classical conductance. John Carroll 1 The Heisenberg uncertainty principle. Some quick particle physics. Beta decay example. The Pauli exclusion principle. The existence of energy bands. Classical conductance. Why it is inaccurate.

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

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

Chapter 3: Electric Current and Direct-Current Circuit

Chapter 3: Electric Current and Direct-Current Circuit Chapter 3: Electric Current and Direct-Current Circuit n this chapter, we are going to discuss both the microscopic aspect and macroscopic aspect of electric current. Direct-current is current that flows

More information

week 6 chapter 31 Current and Resistance

week 6 chapter 31 Current and Resistance week 6 chapter 31 Current and Resistance Which is the correct way to light the lightbulb with the battery? 4) all are correct 5) none are correct 1) 2) 3) Which is the correct way to light the lightbulb

More information

Non-Continuum Energy Transfer: Phonons

Non-Continuum Energy Transfer: Phonons Non-Continuum Energy Transfer: Phonons D. B. Go Slide 1 The Crystal Lattice The crystal lattice is the organization of atoms and/or molecules in a solid simple cubic body-centered cubic hexagonal a NaCl

More information

Electric currents (primarily, in metals)

Electric currents (primarily, in metals) Electric currents (primarily, in metals) Benjamin Franklin was experimenting electricity in the mid- XVIII Century. Nobody knew if it was the positive charges or negative charges carrying the current through

More information

Physics 1502: Lecture 8 Today s Agenda. Today s Topic :

Physics 1502: Lecture 8 Today s Agenda. Today s Topic : Physics 1502: Lecture 8 Today s Agenda Announcements: Lectures posted on: www.phys.uconn.edu/~rcote/ HW assignments, solutions etc. Homework #3: On Masterphysics today: due next Friday Go to masteringphysics.com

More information

Condensed matter theory Lecture notes and problem sets 2012/2013

Condensed matter theory Lecture notes and problem sets 2012/2013 Condensed matter theory Lecture notes and problem sets 2012/2013 Dmitri Ivanov Recommended books and lecture notes: [AM] N. W. Ashcroft and N. D. Mermin, Solid State Physics. [Mar] M. P. Marder, Condensed

More information

Louisiana State University Physics 2102, Exam 2, March 5th, 2009.

Louisiana State University Physics 2102, Exam 2, March 5th, 2009. PRINT Your Name: Instructor: Louisiana State University Physics 2102, Exam 2, March 5th, 2009. Please be sure to PRINT your name and class instructor above. The test consists of 4 questions (multiple choice),

More information

Note 5: Current and Resistance

Note 5: Current and Resistance Note 5: Current and Resistance In conductors, a large number of conduction electrons carry electricity. If current flows, electrostatics does not apply anymore (it is a dynamic phenomenon) and there can

More information

Lecture 3 Semiconductor Physics (II) Carrier Transport

Lecture 3 Semiconductor Physics (II) Carrier Transport Lecture 3 Semiconductor Physics (II) Carrier Transport Thermal Motion Carrier Drift Carrier Diffusion Outline Reading Assignment: Howe and Sodini; Chapter 2, Sect. 2.4-2.6 6.012 Spring 2009 Lecture 3 1

More information

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics Physics 111.6 MIDTERM TEST #3 January 29, 2004 Time: 90 minutes NAME: (Last) Please Print (Given) STUDENT NO.: LECTURE SECTION (please

More information

Electric Currents and Simple Circuits

Electric Currents and Simple Circuits -1 Electric Currents and Simple Circuits Electrons can flow along inside a metal wire if there is an E-field present to push them along ( F= qe). The flow of electrons in a wire is similar to the flow

More information

SPH3U1 Lesson 03 Energy

SPH3U1 Lesson 03 Energy THERMAL ENERGY AND LATENT HEAT LEARNING GOALS Students will learn: Heat changes the amount of thermal energy in an object Temperature is a measure of the average thermal energy in an object Heat capacity

More information

Physics (Theory) There are 30 questions in total. Question Nos. 1 to 8 are very short answer type questions and carry one mark each.

Physics (Theory) There are 30 questions in total. Question Nos. 1 to 8 are very short answer type questions and carry one mark each. Physics (Theory) Time allowed: 3 hours] [Maximum marks:70 General Instructions: (i) All questions are compulsory. (ii) (iii) (iii) (iv) (v) There are 30 questions in total. Question Nos. to 8 are very

More information

Physics 2220 Fall 2010 George Williams SECOND MIDTERM - REVIEW PROBLEMS

Physics 2220 Fall 2010 George Williams SECOND MIDTERM - REVIEW PROBLEMS Physics 0 Fall 010 George Williams SECOND MIDTERM - REVIEW PROBLEMS The last four problems are from last years second midterm. Solutions are available on the class web site.. There are no solutions for,

More information

ELECTRIC CURRENT INTRODUCTION. Introduction. Electric current

ELECTRIC CURRENT INTRODUCTION. Introduction. Electric current Chapter 7 ELECTRIC CURRENT Introduction Electric current Charge conservation Electric conductivity Microscopic picture Electric power Electromotive force Kirchhoff s rules Summary INTRODUCTION The first

More information

CONCEPTUAL TOOLS By: Neil E. Cotter CIRCUITS OHM'S LAW Physics

CONCEPTUAL TOOLS By: Neil E. Cotter CIRCUITS OHM'S LAW Physics Physics DERIV: Ohm's law is almost always derived from basic physics with a starting assumption that the electric field inside a resistor is constant. We first investigate this assumption. The electric

More information

Valence Electrons, Bonds and Chemical Reactions 05 October 2006

Valence Electrons, Bonds and Chemical Reactions 05 October 2006 Valence Electrons, Bonds and Chemical Reactions 05 October 2006 Principles of Valence Electrons and Bonds Ionic Bonds Metallic Bonds Covalent Bonds Intermolecular Forces Common Chemical Reactions Atoms

More information

Two Dimensional Kinematics. Pre-Test

Two Dimensional Kinematics. Pre-Test 1 Two Dimensional Kinematics Pre-Test 1. The following situation is given below. Suggest two reasonable (both magnitude and direction) component velocity vectors for the resultant velocity vector given

More information

Mechanism of electric conductance in crystals

Mechanism of electric conductance in crystals Mechanism of electric conductance in crystals 1 Electric current in conductors A When the conductor is in electric field, the field accelerates free electrons Electrons moving (drifting) in electric field

More information

Class XI Exercise 6 Work, Energy And Power Physics

Class XI Exercise 6 Work, Energy And Power Physics Question 6.1: The sign of work done by a force on a body is important to understand. State carefully if the following quantities are positive or negative: (a) work done by a man in lifting a bucket out

More information

PHYSICS B SAMPLE EXAM I Time - 90 minutes 70 Questions

PHYSICS B SAMPLE EXAM I Time - 90 minutes 70 Questions Page 1 of 7 PHYSCS B SAMPLE EXAM Time - 90 minutes 70 Questions Directions:Each of the questions or incomplete statements below is followed by five suggested Solutions or completions. Select the one that

More information

Electric Currents and Resistance II

Electric Currents and Resistance II Electric Currents and Resistance II Physics 2415 Lecture 11 Michael Fowler, UVa Today s Topics First we ll mention capacitors Power usage: kwh, etc. The microscopic picture Temperature dependence of resistivity

More information

Reading from Young & Freedman: For this topic, read the introduction to chapter 25 and sections 25.1 to 25.3 & 25.6.

Reading from Young & Freedman: For this topic, read the introduction to chapter 25 and sections 25.1 to 25.3 & 25.6. PHY10 Electricity Topic 6 (Lectures 9 & 10) Electric Current and Resistance n this topic, we will cover: 1) Current in a conductor ) Resistivity 3) Resistance 4) Oh s Law 5) The Drude Model of conduction

More information

K20: Temperature, Heat, and How Heat Moves

K20: Temperature, Heat, and How Heat Moves K20: Temperature, Heat, and How Heat Moves Definition of Temperature Definition of Heat How heat flows (Note: For all discussions here, particle means a particle of mass which moves as a unit. It could

More information

Chapter 12. Magnetism and Electromagnetism

Chapter 12. Magnetism and Electromagnetism Chapter 12 Magnetism and Electromagnetism 167 168 AP Physics Multiple Choice Practice Magnetism and Electromagnetism SECTION A Magnetostatics 1. Four infinitely long wires are arranged as shown in the

More information

Electrons in a periodic potential: Free electron approximation

Electrons in a periodic potential: Free electron approximation Dr. A. Sapelin, Jan 01 Electrons in a periodic potential: ree electron approximation ree electron ermi gas - gas of non-interacting electrons subject to Pauli principle Wealy bound electrons move freely

More information

Plasma Astrophysics Chapter 1: Basic Concepts of Plasma. Yosuke Mizuno Institute of Astronomy National Tsing-Hua University

Plasma Astrophysics Chapter 1: Basic Concepts of Plasma. Yosuke Mizuno Institute of Astronomy National Tsing-Hua University Plasma Astrophysics Chapter 1: Basic Concepts of Plasma Yosuke Mizuno Institute of Astronomy National Tsing-Hua University What is a Plasma? A plasma is a quasi-neutral gas consisting of positive and negative

More information

M04M.1 Particles on a Line

M04M.1 Particles on a Line Part I Mechanics M04M.1 Particles on a Line M04M.1 Particles on a Line Two elastic spherical particles with masses m and M (m M) are constrained to move along a straight line with an elastically reflecting

More information

Electric Currents and Circuits

Electric Currents and Circuits Nicholas J. Giordano www.cengage.com/physics/giordano Chapter 19 Electric Currents and Circuits Marilyn Akins, PhD Broome Community College Electric Circuits The motion of charges leads to the idea of

More information

CME 300 Properties of Materials. ANSWERS: Homework 9 November 26, As atoms approach each other in the solid state the quantized energy states:

CME 300 Properties of Materials. ANSWERS: Homework 9 November 26, As atoms approach each other in the solid state the quantized energy states: CME 300 Properties of Materials ANSWERS: Homework 9 November 26, 2011 As atoms approach each other in the solid state the quantized energy states: are split. This splitting is associated with the wave

More information

2. Electric Current. E.M.F. of a cell is defined as the maximum potential difference between the two electrodes of the

2. Electric Current. E.M.F. of a cell is defined as the maximum potential difference between the two electrodes of the 2. Electric Current The net flow of charges through a etallic wire constitutes an electric current. Do you know who carries current? Current carriers In solid - the electrons in outerost orbit carries

More information

Physics 2020 Exam 1 Constants and Formulae

Physics 2020 Exam 1 Constants and Formulae Physics 2020 Exam 1 Constants and Formulae Useful Constants k e = 8.99 10 9 N m 2 /C 2 ɛ = 8.85 10 12 C 2 /(N m 2 ) G = 6.673 10 11 N m 2 / kg 2 e = 1.602 10 19 C m p = 1.672 10 27 kg m e = 9.110 10 31

More information

Properties of Materials

Properties of Materials Tao Deng, dengtao@sjtu.edu.cn 1 1896 1920 1987 2006 Properties of Materials Chapter 3 Electrical Properties of Materials Tao Deng Tao Deng, dengtao@sjtu.edu.cn 2 3. The electrical properties Electrical

More information

General Physics (PHY 2140)

General Physics (PHY 2140) General Physics (PHY 2140) Lecture 7 Electrostatics and electrodynamics Capacitance and capacitors capacitors with dielectrics Electric current current and drift speed resistance and Ohm s law http://www.physics.wayne.edu/~apetrov/phy2140/

More information

7.4. Why we have two different types of materials: conductors and insulators?

7.4. Why we have two different types of materials: conductors and insulators? Phys463.nb 55 7.3.5. Folding, Reduced Brillouin zone and extended Brillouin zone for free particles without lattices In the presence of a lattice, we can also unfold the extended Brillouin zone to get

More information