VV = voltage across voltmeter = 9 (Rs + 500) = VsRv Vs. (500) = 9 (Rs + 500) Case ii VV = 13V VS=? RV = 50kΩ / V 20v RV = 1000 kω by (1)

Size: px
Start display at page:

Download "VV = voltage across voltmeter = 9 (Rs + 500) = VsRv Vs. (500) = 9 (Rs + 500) Case ii VV = 13V VS=? RV = 50kΩ / V 20v RV = 1000 kω by (1)"

Transcription

1 1

2 1. A resistor has oltage drop of 110.V and current of.a. the uncertainties in the measurement of oltage and current are ± 0.V and ±0.01 respectiely calculate the uncertainty in power calculation. Ans. Power (P) oltage x current V x I w P + i P w w () i V I Where w and wi are uncertainties in calculation of oltage and current respectiely. P VI I. V V ( ii) P VI V 110. I I ( iii) By i, ii, iii ±.96 w % A PMMC oltage has a reading of 9V when it is measuring a oltage source with an internal resistance of finite alue on its scale of 10V. When scale of this is changed to 0 full scale then reading of 13 is obtained. Gien sensitiity of oltmeter to be 0 kω/v. Find alue of the oltage source and its internal resistance R. Ans. VV oltage across oltmeter Rs Vs R + R s...( i) Vs oltage of source Rs and R are resistance of source & oltmeter respectiely. Case i V 9V, Vs? Rs? RV sensitiity range 0 k Ω / V k/ω by (1) 9 VsR R s (Rs + 00) VsR Vs. (00) 9 (Rs + 00) Case ii VV 13V VS? RS? RV 0kΩ / V 0 RV 1000 kω by (1) Vs R 13 ( R ) s Vs (1000) 1. (Rs )...(iii) by (ii) & (iii) 9( Rs + 00) 13( Rs ) Rs Rs S0 Rs 000 Rs (ii) 3. Gien a meter of range 0 1mA, haing internal resistance of Ω. How do you extend the range of it to 10 ma? Ans. To extend the range of ammeter a shunt resistance is applied to ammeter to bypass excess current through this shunt resistor. Only rated current flours through ammeter. But now the dial of ammeter has to be recalibrated by multiplying the alues with multiplication factor m. by following aboe steps the range of ammeter is extended. Numerical :

3 Rm internal meter resistance Rsh external shunt resistor to bypass excess current Im meter current Ish current in shunt arm I rated current of extended range meter V Im Rm IshRsh [KVL] Im Rm [I Im] Rsh ( I Im + Ish KCL) R sh Rm I wherem ( m 1) Im m multiplication factor I 10mA, Im 1 ma, Rm Ω, I m 10 I m Rsh 10 1 Rsh 0. 9 So, by connecting shunt resistance of 0.6Ω and multiplying dial alue by m 10 the range of ammeter will be extended from 1 ma to 10 ma.. A) explain the following terms with respect to measurement system:- i) accuracy ii) precision iii) resolution i) sensitiity ) linearity B) A oltmeter is connected across 10kΩ resistor as shown in figure The oltmeter shows., but it must hae shown V. Why is his happening? Explain Ans. i) Accuracy: The closeness with which instrument alue or reading approaches the true alue or quantity being measured. It means conformity to truth. ii) Precision: It is measure of reproducibity of the measurements precision is a measure of degree of agreement within a group of measurements. iii) Resolution: The smallest increment in the quantity being measured that can be measured with certainty by an instrument. i) Sensitiity: sensitiity of an instrument is ratio of magnitude of output signal / response to the magnitude of input signal / quantity being measured. ) linearity: linearity is simply measure of maximum deiation of calibration points from the straight line. B) The reduction in measured alue of oltmeter is due to loading effect to oltmeter as oltmeter has some finite input resistance Had the internal resistance of oltmeter infinite then no loading effect will occur and alue shown by oltmeter will be true alue itself Let RV be internal resistance of oltmeter So, RV is parallel to 10kΩ resistance and is uialent Resistance 10R R e 10 q R k 10 + R oltage shown by oltmeter 0 ( KVL) R + 10K 0. R k. R 9.60k 10R R 3

4 10R R 0. R R 0k 0. Therefore R 0k and this resistance of oltmeter causes the net oltage to reduce and is called loading effect. Define gauge factor for strain gauge and derie the expression for the same. Also explain the significance of piezo resistiity in the expression. Ans. If a metal is stretched or compressed, its resistance changes on account of fact that both the length and diameter / area of conductor changes. Also there is change in alue of resistiity when strained. Gauge factor deriation: Consider a wise haing initial length L and diameter D when stress or force is applied its length increases by ΔL and diameter decreases to D L Resis tance R A resistiity L length of wire D A area of wire D diameter of wire L R A ln R ln + ln(l) ln(a) () i [taking natural log both sides] differentiate the aboe uation with respect to stress (σ) 1 dr 1 d 1 dl 1 da + R d d L d A d D A da ( D) dd D dd d d d 1 da D dd dd A d D d D d 1 da dd A d D d...( iii) by (ii) & (iii) 1 R 1 d 1 dl dd + R d d L d D d ( ii) Rearranging aboe uation for small ariation:- dr d dl dd + R L D R L D + R L D R / R D / D / 1 + L / L L / L L / L R/ R D/ D / Guage factor L / L L / L L / L D D poissons ratio L L R / R P / P Guage factor 1+ + L / L L / L for resistor made of metal resistiity is not changed so gauge factor depends on GF (1+ ) dimensions For resistor mode of semiconductors so guage factor depends mainly on / L/ L sharply.. As resistiity changes

5

Chapter 5 Solution P5.2-2, 3, 6 P5.3-3, 5, 8, 15 P5.4-3, 6, 8, 16 P5.5-2, 4, 6, 11 P5.6-2, 4, 9

Chapter 5 Solution P5.2-2, 3, 6 P5.3-3, 5, 8, 15 P5.4-3, 6, 8, 16 P5.5-2, 4, 6, 11 P5.6-2, 4, 9 Chapter 5 Solution P5.2-2, 3, 6 P5.3-3, 5, 8, 15 P5.4-3, 6, 8, 16 P5.5-2, 4, 6, 11 P5.6-2, 4, 9 P 5.2-2 Consider the circuit of Figure P 5.2-2. Find i a by simplifying the circuit (using source transformations)

More information

Electronics Resistive Sensors and Bridge Circuits

Electronics Resistive Sensors and Bridge Circuits Electronics Resistive Sensors and Bridge Circuits Wilfrid Laurier University September 27, 2012 Switches in voltage dividers One of the simplest forms of voltage divider is where one of the elements is

More information

The Digital Multimeter (DMM)

The Digital Multimeter (DMM) The Digital Multimeter (DMM) Since Physics 152 covers electricity and magnetism, the analysis of both DC and AC circuits is required. In the lab, you will need to measure resistance, potential (voltage),

More information

INSTITUTE OF AERONAUTICAL ENGINEERING (Autonomous) Dundigal, Hyderabad

INSTITUTE OF AERONAUTICAL ENGINEERING (Autonomous) Dundigal, Hyderabad INSTITUTE OF AERONAUTICAL ENGINEERING (Autonomous) Dundigal, Hyderabad - 500 043 ELECTRONICS AND COMMUNICATION ENGINEERING Course Name : Electronic Measurements and Instrumentation Course Code : A50422

More information

E E 2320 Circuit Analysis. Calculating Resistance

E E 2320 Circuit Analysis. Calculating Resistance E E 30 Circuit Analysis Lecture 03 Simple esistive Circuits it and Applications Calculating esistance l A 6 1.67 10 cm cu 6 al.7010 Area, A When conductor has uniform crosssection cm l 1 Temperature Coefficient

More information

Chapter 2. Engr228 Circuit Analysis. Dr Curtis Nelson

Chapter 2. Engr228 Circuit Analysis. Dr Curtis Nelson Chapter 2 Engr228 Circuit Analysis Dr Curtis Nelson Chapter 2 Objectives Understand symbols and behavior of the following circuit elements: Independent voltage and current sources; Dependent voltage and

More information

Chapter 2 Resistive Circuits

Chapter 2 Resistive Circuits 1. Sole circuits (i.e., find currents and oltages of interest) by combining resistances in series and parallel. 2. Apply the oltage-diision and current-diision principles. 3. Sole circuits by the node-oltage

More information

1 S = G R R = G. Enzo Paterno

1 S = G R R = G. Enzo Paterno ECET esistie Circuits esistie Circuits: - Ohm s Law - Kirchhoff s Laws - Single-Loop Circuits - Single-Node Pair Circuits - Series Circuits - Parallel Circuits - Series-Parallel Circuits Enzo Paterno ECET

More information

Chapter 2 Homework Solution P2.2-1, 2, 5 P2.4-1, 3, 5, 6, 7 P2.5-1, 3, 5 P2.6-2, 5 P2.7-1, 4 P2.8-1 P2.9-1

Chapter 2 Homework Solution P2.2-1, 2, 5 P2.4-1, 3, 5, 6, 7 P2.5-1, 3, 5 P2.6-2, 5 P2.7-1, 4 P2.8-1 P2.9-1 Chapter Homework Solution P.-1,, 5 P.4-1, 3, 5, 6, 7 P.5-1, 3, 5 P.6-, 5 P.7-1, 4 P.8-1 P.9-1 P.-1 An element ha oltage and current i a hown in Figure P.-1a. Value of the current i and correponding oltage

More information

Chapter 5. Department of Mechanical Engineering

Chapter 5. Department of Mechanical Engineering Source Transformation By KVL: V s =ir s + v By KCL: i s =i + v/r p is=v s /R s R s =R p V s /R s =i + v/r s i s =i + v/r p Two circuits have the same terminal voltage and current Source Transformation

More information

INSTITUTE OF AERONAUTICAL ENGINEERING (Autonomous) Dundigal, Hyderabad

INSTITUTE OF AERONAUTICAL ENGINEERING (Autonomous) Dundigal, Hyderabad INSTITUTE OF AERONAUTICAL ENGINEERING (Autonomous) Dundigal, Hyderabad - 500 04 ELECTRONICS AND COMMUNICATION ENGINEERING Name : Electronic Measurements and Instrumentation Code : A50422 Class : III -

More information

INSTITUTE OF AERONAUTICAL ENGINEERING Dundigal, Hyderabad DEPARTMENT OF ECE QUESTION BANK. : G.Lakshminarayana, Asst.

INSTITUTE OF AERONAUTICAL ENGINEERING Dundigal, Hyderabad DEPARTMENT OF ECE QUESTION BANK. : G.Lakshminarayana, Asst. ` INSTITUTE OF AERONAUTICAL ENGINEERING Dundigal, Hyderabad - 500 04 DEPARTMENT OF ECE QUESTION BANK Name Code Class Branch P a g e : Electronic Measurements and Instrumentation : A504 : III - B. Tech

More information

The Strain Gauge. James K Beard, Ph.D. Rowan Hall Auditorium November 2, 2006

The Strain Gauge. James K Beard, Ph.D. Rowan Hall Auditorium  November 2, 2006 The Strain Gauge James K Beard, Ph.D. Rowan Hall Auditorium beard@rowan.edu http://rowan.jkbeard.com November 2, 2006 What is Strain? Strain is elongation or deformation of a solid body due to forces applied

More information

Resistor Network Answers

Resistor Network Answers Resistor Network Answers 1. (a) pd = 3.6 1 Example of answer; p.d. = 0.24 A 15 Ω = 3.6 (b) Calculation of pd across the resistor [6.0 3.6 = 2.4 ] Recall = I R I 1 calculated from their pd / 4Ω [correct

More information

N12/4/PHYSI/SPM/ENG/TZ0/XX. Physics Standard level Paper 1. Tuesday 13 November 2012 (afternoon) 45 minutes INSTRUCTIONS TO CANDIDATES

N12/4/PHYSI/SPM/ENG/TZ0/XX. Physics Standard level Paper 1. Tuesday 13 November 2012 (afternoon) 45 minutes INSTRUCTIONS TO CANDIDATES N1/4/PHYSI/SPM/ENG/TZ0/XX 8816504 Physics Standard leel Paper 1 Tuesday 13 Noember 01 (afternoon) 45 minutes INSTRUCTIONS TO CANDIDATES Do not open this examination paper until instructed to do so. Answer

More information

Direct Current (DC) Circuits

Direct Current (DC) Circuits Direct Current (DC) Circuits NOTE: There are short answer analysis questions in the Participation section the informal lab report. emember to include these answers in your lab notebook as they will be

More information

TSOKOS CHAP 1 TEST REVIEW

TSOKOS CHAP 1 TEST REVIEW IB PHYSICS Name: DEVIL PHYSICS Period: Date: BADDEST CLASS ON CAMPUS TSOKOS CHAP TEST REVIEW ORDERS OF MAGNITUDE AND UNITS 2. The resistie force F acting on a sphere of radius r moing at speed through

More information

Chapter 20 Electric Circuits

Chapter 20 Electric Circuits Chapter 0 Electric Circuits Chevy olt --- Electric vehicle of the future Goals for Chapter 9 To understand the concept of current. To study resistance and Ohm s Law. To observe examples of electromotive

More information

INTRODUCTION TO ELECTRONICS

INTRODUCTION TO ELECTRONICS INTRODUCTION TO ELECTRONICS Basic Quantities Voltage (symbol V) is the measure of electrical potential difference. It is measured in units of Volts, abbreviated V. The example below shows several ways

More information

COURSE OF Prepared By: MUHAMMAD MOEEN SULTAN Department of Mechanical Engineering UET Lahore, KSK Campus

COURSE OF Prepared By: MUHAMMAD MOEEN SULTAN Department of Mechanical Engineering UET Lahore, KSK Campus COURSE OF Active and passive instruments Null-type and deflection-type instruments Analogue and digital instruments In active instruments, the external power source is usually required to produce an output

More information

MET 301 EXPERIMENT # 2 APPLICATION OF BONDED STRAIN GAGES

MET 301 EXPERIMENT # 2 APPLICATION OF BONDED STRAIN GAGES MET 301 EPERIMENT # 2 APPLICATION OF BONDED STRAIN GAGES 1. Objective To understand the working principle of bonded strain gauge and to study the stress and strain in a hollow cylindrical shaft under bending,

More information

Calculate the total resistance of this combination. (3)

Calculate the total resistance of this combination. (3) 1 The circuit shows a combination of three resistors. 22 Ω 47 Ω 620 Ω Calculate the total resistance of this combination. Total resistance = (Total for Question = 3 marks) 2 (a) Sketch a graph to show

More information

Chapter 2 Resistive Circuits

Chapter 2 Resistive Circuits Chapter esistie Circuits Goal. Sole circuits by combining resistances in Series and Parallel.. Apply the Voltage-Diision and Current-Diision Principles.. Sole circuits by the Node-Voltage Technique.. Sole

More information

Flow Rate is the NET amount of water passing through a surface per unit time

Flow Rate is the NET amount of water passing through a surface per unit time Electric Current An Analogy Water Flow in a Pipe H 2 0 gallons/minute Flow Rate is the NET amount of water passing through a surface per unit time Individual molecules are bouncing around with speeds of

More information

Chapter 7. Chapter 7

Chapter 7. Chapter 7 Chapter 7 Combination circuits Most practical circuits have combinations of series and parallel components. You can frequently simplify analysis by combining series and parallel components. An important

More information

3/17/2009 PHYS202 SPRING Lecture notes Electric Circuits

3/17/2009 PHYS202 SPRING Lecture notes Electric Circuits PHYS202 SPRING 2009 Lecture notes Electric Circuits 1 Batteries A battery is a device that provides a potential difference to two terminals. Different metals in an electrolyte will create a potential difference,

More information

a) (4 pts) What is the magnitude and direction of the acceleration of the electron?

a) (4 pts) What is the magnitude and direction of the acceleration of the electron? PHYSCS 22 Fall 2010 - MDTERM #3 SHOW ALL WORK & REASONNG FOR FULL PONTS Question 1. (5 pts): Accurately show or state the direction of the force that is felt by the following charges or currents. +q -q

More information

Because the third wire carries practically no current (due to the voltmeter's extremely high internal resistance), its resistance will not drop any

Because the third wire carries practically no current (due to the voltmeter's extremely high internal resistance), its resistance will not drop any Strain gauges If a strip of conductive metal is stretched, it will become skinnier and longer, both changes resulting in an increase of electrical resistance end-to-end. Conversely, if a strip of conductive

More information

Work, Energy and Power

Work, Energy and Power 1 Work, Energy and Power Work is an activity of force and movement in the direction of force (Joules) Energy is the capacity for doing work (Joules) Power is the rate of using energy (Watt) P = W / t,

More information

Lecture 5: Using electronics to make measurements

Lecture 5: Using electronics to make measurements Lecture 5: Using electronics to make measurements As physicists, we re not really interested in electronics for its own sake We want to use it to measure something often, something too small to be directly

More information

Transmission lines using a distributed equivalent circuit

Transmission lines using a distributed equivalent circuit Cambridge Uniersity Press 978-1-107-02600-1 - Transmission Lines Equialent Circuits, Electromagnetic Theory, and Photons Part 1 Transmission lines using a distributed equialent circuit in this web serice

More information

Chapter 25 Current, Resistance, and Electromotive Force

Chapter 25 Current, Resistance, and Electromotive Force Chapter 25 Current, Resistance, and Electromotive Force Lecture by Dr. Hebin Li Goals for Chapter 25 To understand current and how charges move in a conductor To understand resistivity and conductivity

More information

Physics 212. Lecture 9. Electric Current

Physics 212. Lecture 9. Electric Current Physics 212 Lecture 9 Electric Current Exam Here, Tuesday, June 26, 8 9:30 AM Will begin at 7:30 for those who must leave by 9. Office hours 1-7 PM, Rm 232 Loomis Bring your ID! Physics 212 Lecture 9,

More information

14 - CURRENT ELECTRICITY Page 1 ( Answers at the end of all questions )

14 - CURRENT ELECTRICITY Page 1 ( Answers at the end of all questions ) 14 - CURRENT ELECTRICITY Page 1 1 ) In the circuit, the galvanometer G shows zero deflection. If the batteries A and B have negligible internal resistance, the value of the resistor R will be ( a ) 100

More information

SHREE DATTA SHETKARI SAHAKARI KARKHANA LTD. CHARITABLE TRUST SHREE DATTA POLYTECHNIC COLLEGE, DATTANAGAR CLASS TEST-01

SHREE DATTA SHETKARI SAHAKARI KARKHANA LTD. CHARITABLE TRUST SHREE DATTA POLYTECHNIC COLLEGE, DATTANAGAR CLASS TEST-01 SHREE DATTA SHETKARI SAHAKARI KARKHANA LTD. CHARITABLE TRUST SHREE DATTA POLYTECHNIC COLLEGE, DATTANAGAR CLASS TEST-01 Name of subject: Elect. & electronic Measurement Mark: 25 Institute Code: 1512 Subject

More information

Electricity Answers. Current, Potential Difference, Resistor Networks, Resistance and Resistivity

Electricity Answers. Current, Potential Difference, Resistor Networks, Resistance and Resistivity Electricity Answers Current, Potential Difference, Resistor Networks, Resistance and Resistivity 1. Resistance calculations Evidence of 20 Ω for one arm 1 1 1 = + R 20 20 R = 10 Ω 3 Comment This combination

More information

Strain Gauge Application and Measurement of Unknown Load

Strain Gauge Application and Measurement of Unknown Load University Diploma Program Electronic Equipment Maintenance Lab Instructor: Muhammad Ajmal Khan EET-027, Experiment # 6 Strain Gauge Application and Measurement of Unknown Load Objectives: 1. To find the

More information

Farr High School HIGHER PHYSICS. Unit 3 Electricity. Question Booklet

Farr High School HIGHER PHYSICS. Unit 3 Electricity. Question Booklet Farr High School HIGHER PHYSICS Unit 3 Electricity Question Booklet 1 MONITORING ND MESURING.C. 1. What is the peak voltage of the 230 V mains supply? The frequency of the mains supply is 50 Hz. How many

More information

STRAIN GAUGE MEASUREMENT

STRAIN GAUGE MEASUREMENT STRAIN GAUGE MEASUREMENT INTRODUCTION There are many possible ways of measuring strain gauges using a Datascan. All methods measure the change in resistance of the gauge within a bridge circuit and the

More information

Kirchhoff's Laws and Circuit Analysis (EC 2)

Kirchhoff's Laws and Circuit Analysis (EC 2) Kirchhoff's Laws and Circuit Analysis (EC ) Circuit analysis: solving for I and V at each element Linear circuits: involve resistors, capacitors, inductors Initial analysis uses only resistors Power sources,

More information

Chapter 26 Direct-Current and Circuits. - Resistors in Series and Parallel - Kirchhoff s Rules - Electric Measuring Instruments - R-C Circuits

Chapter 26 Direct-Current and Circuits. - Resistors in Series and Parallel - Kirchhoff s Rules - Electric Measuring Instruments - R-C Circuits Chapter 26 Direct-Current and Circuits - esistors in Series and Parallel - Kirchhoff s ules - Electric Measuring Instruments - -C Circuits . esistors in Series and Parallel esistors in Series: V ax I V

More information

Copyright , R. Eckweiler & OCARC, Inc. Page 1 of 5

Copyright , R. Eckweiler & OCARC, Inc. Page 1 of 5 by Bob Eckweiler, AF6C I = E R (2) Ohm s Law (Part I of IV): Introduction Ohm's law is a simple equation that solves the relationship between voltage, current and resistance in a simple electrical circuit.

More information

Chapter 4: Methods of Analysis

Chapter 4: Methods of Analysis Chapter 4: Methods of Analysis When SCT are not applicable, it s because the circuit is neither in series or parallel. There exist extremely powerful mathematical methods that use KVL & KCL as its basis

More information

Basic Laws. Bởi: Sy Hien Dinh

Basic Laws. Bởi: Sy Hien Dinh Basic Laws Bởi: Sy Hien Dinh INTRODUCTION Chapter 1 introduced basic concepts such as current, voltage, and power in an electric circuit. To actually determine the values of this variable in a given circuit

More information

ELECTRICAL MEASUREMENTS LAB MANUAL

ELECTRICAL MEASUREMENTS LAB MANUAL ELECTRICAL MEASUREMENTS LAB MANUAL Prepared by B.SAIDAMMA R13 Regulation Any 10 of the following experiments are to be conducted 1. Calibration and Testing of single phase energy Meter 2. Calibration of

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

Electric Circuits I. Nodal Analysis. Dr. Firas Obeidat

Electric Circuits I. Nodal Analysis. Dr. Firas Obeidat Electric Circuits I Nodal Analysis Dr. Firas Obeidat 1 Nodal Analysis Without Voltage Source Nodal analysis, which is based on a systematic application of Kirchhoff s current law (KCL). A node is defined

More information

coil of the circuit. [8+8]

coil of the circuit. [8+8] Code No: R05310202 Set No. 1 III B.Tech I Semester Regular Examinations, November 2008 ELECTRICAL MEASUREMENTS (Electrical & Electronic Engineering) Time: 3 hours Max Marks: 80 Answer any FIVE Questions

More information

PhysicsAndMathsTutor.com

PhysicsAndMathsTutor.com Electricity May 02 1. The graphs show the variation with potential difference V of the current I for three circuit elements. PhysicsAndMathsTutor.com When the four lamps are connected as shown in diagram

More information

Parallel Circuits. Chapter

Parallel Circuits. Chapter Chapter 5 Parallel Circuits Topics Covered in Chapter 5 5-1: The Applied Voltage V A Is the Same Across Parallel Branches 5-2: Each Branch I Equals V A / R 5-3: Kirchhoff s Current Law (KCL) 5-4: Resistance

More information

COE. DC. Challenging MCQ questions by The Physics Cafe. Compiled and selected by The Physics Cafe

COE. DC. Challenging MCQ questions by The Physics Cafe. Compiled and selected by The Physics Cafe COE. DC Challenging MCQ questions by The Physics Cafe Compiled and selected by The Physics Cafe 1 battery of internal resistance r and e.m.f. E can supply a current of 6.0 to a resistor R as shown in Fig

More information

COOKBOOK KVL AND KCL A COMPLETE GUIDE

COOKBOOK KVL AND KCL A COMPLETE GUIDE 1250 COOKBOOK KVL AND KCL A COMPLETE GUIDE Example circuit: 1) Label all source and component values with a voltage drop measurement (+,- ) and a current flow measurement (arrow): By the passive sign convention,

More information

COPYRIGHTED MATERIAL. DC Review and Pre-Test. Current Flow CHAPTER

COPYRIGHTED MATERIAL. DC Review and Pre-Test. Current Flow CHAPTER Kybett c0.tex V3-03/3/2008 8:44pm Page CHAPTER DC Review and Pre-Test Electronics cannot be studied without first understanding the basics of electricity. This chapter is a review and pre-test on those

More information

Assignment 4 (Solutions) NPTEL MOOC (Bayesian/ MMSE Estimation for MIMO/OFDM Wireless Communications)

Assignment 4 (Solutions) NPTEL MOOC (Bayesian/ MMSE Estimation for MIMO/OFDM Wireless Communications) Assignment 4 Solutions NPTEL MOOC Bayesian/ MMSE Estimation for MIMO/OFDM Wireless Communications The system model can be written as, y hx + The MSE of the MMSE estimate ĥ of the aboe mentioned system

More information

EE40. Lec 3. Basic Circuit Analysis. Prof. Nathan Cheung. Reading: Hambley Chapter 2

EE40. Lec 3. Basic Circuit Analysis. Prof. Nathan Cheung. Reading: Hambley Chapter 2 EE40 Lec 3 Basic Circuit Analysis Prof. Nathan Cheung 09/03/009 eading: Hambley Chapter Slide Outline Chapter esistors in Series oltage Divider Conductances in Parallel Current Divider Node-oltage Analysis

More information

EE301 RESISTANCE AND OHM S LAW

EE301 RESISTANCE AND OHM S LAW Learning Objectives a. Describe the concept of resistance b. Use Ohm s law to calculate current, voltage, and resistance values in a circuit c. Discuss the difference between an open circuit and a short

More information

ELECTROMAGNETIC INDUCTION

ELECTROMAGNETIC INDUCTION hapter Si ELETROMGNETI INUTION MQ 1 6.1 square of side L meters lies in the -y plane in a region, where the magnetic field is gien by = ˆ ˆ ˆ o (2 i+ 3j+ 4 k) T, where o is constant. The magnitude of flu

More information

Physics Unit 3 Investigative and Practical Skills in AS Physics PHY3T/P09/test

Physics Unit 3 Investigative and Practical Skills in AS Physics PHY3T/P09/test Surname Other Names Leave blank Centre Number Candidate Number Candidate Signature General Certificate of Education June 2009 Advanced Subsidiary Examination Physics Unit 3 Investigative and Practical

More information

Lesson 10 Steady Electric Currents

Lesson 10 Steady Electric Currents Lesson Steady lectric Currents 楊尚達 Shang-Da Yang Institute of Photonics Technologies Department of lectrical ngineering National Tsing Hua Uniersity, Taiwan Outline Current density Current laws Boundary

More information

Physics 115. General Physics II. Session 24 Circuits Series and parallel R Meters Kirchoff s Rules

Physics 115. General Physics II. Session 24 Circuits Series and parallel R Meters Kirchoff s Rules Physics 115 General Physics II Session 24 Circuits Series and parallel R Meters Kirchoff s Rules R. J. Wilkes Email: phy115a@u.washington.edu Home page: http://courses.washington.edu/phy115a/ 5/15/14 Phys

More information

Electrical Circuits Question Paper 1

Electrical Circuits Question Paper 1 Electrical Circuits Question Paper 1 Level IGCSE Subject Physics Exam Board CIE Topic Electricity and Magnetism Sub-Topic Electrical Circuits Paper Type Alternative to Practical Booklet Question Paper

More information

Lecture 28 Field-Effect Transistors

Lecture 28 Field-Effect Transistors Lecture 8 Field-Effect Transistors Field-Effect Transistors 1. Understand MOSFET operation.. Analyze basic FET amplifiers using the loadline technique. 3. Analyze bias circuits. 4. Use small-signal equialent

More information

CHAPTER 1 ELECTRICITY

CHAPTER 1 ELECTRICITY CHAPTER 1 ELECTRICITY Electric Current: The amount of charge flowing through a particular area in unit time. In other words, it is the rate of flow of electric charges. Electric Circuit: Electric circuit

More information

Kirchhoff's Laws and Maximum Power Transfer

Kirchhoff's Laws and Maximum Power Transfer German Jordanian University (GJU) Electrical Circuits Laboratory Section Experiment Kirchhoff's Laws and Maximum Power Transfer Post lab Report Mahmood Hisham Shubbak / / 8 Objectives: To learn KVL and

More information

Wheatstone Bridge Nonlinearity

Wheatstone Bridge Nonlinearity Index: Nonlinearity Wheatstone Bridge Nonlinearity Introduction General Considerations The "Unbalanced" Circuit The Unbalanced Circuit Table of Contents Output & Nonlinearity with Various Bridge/Strain

More information

Chapter 4: Techniques of Circuit Analysis

Chapter 4: Techniques of Circuit Analysis Chapter 4: Techniques of Circuit Analysis This chapter gies us many useful tools for soling and simplifying circuits. We saw a few simple tools in the last chapter (reduction of circuits ia series and

More information

MEP 382: Design of Applied Measurement Systems Lecture 3: DC & AC Circuit Analysis

MEP 382: Design of Applied Measurement Systems Lecture 3: DC & AC Circuit Analysis Faculty of Engineering MEP 38: Design of Applied Measurement Systems Lecture 3: DC & AC Circuit Analysis Outline oltage and Current Ohm s Law Kirchoff s laws esistors Series and Parallel oltage Dividers

More information

ME411 Engineering Measurement & Instrumentation. Winter 2017 Lecture 9

ME411 Engineering Measurement & Instrumentation. Winter 2017 Lecture 9 ME411 Engineering Measurement & Instrumentation Winter 2017 Lecture 9 1 Introduction If we design a load bearing component, how do we know it will not fail? Simulate/predict behavior from known fundamentals

More information

Direct Current (DC): In a DC circuit the current and voltage are constant as a function of time. Power (P): Rate of doing work P = dw/dt units = Watts

Direct Current (DC): In a DC circuit the current and voltage are constant as a function of time. Power (P): Rate of doing work P = dw/dt units = Watts Lecture 1: Introduction Some Definitions: Current (I): Amount of electric charge (Q) moving past a point per unit time I dq/dt Coulombs/sec units Amps (1 Coulomb 6x10 18 electrons) oltage (): Work needed

More information

The Steady Current Field

The Steady Current Field Electromagnetic Fields Lecture 5 The Steady Current Field What is current? Electric current: Flow of electric charge. Electric current in metals A solid conductive metal contains free electrons. When a

More information

Industrial Instrumentation Dr. Alok Barua Department of Electrical Engineering Indian Institute of Technology Kharagpur. Lecture - 4 Strain Gauge

Industrial Instrumentation Dr. Alok Barua Department of Electrical Engineering Indian Institute of Technology Kharagpur. Lecture - 4 Strain Gauge Industrial Instrumentation Dr. Alok Barua Department of Electrical Engineering Indian Institute of Technology Kharagpur Lecture - 4 Strain Gauge Welcome to the lesson 4 of industrial instrumentation. In

More information

Strain Gages. Approximate Elastic Constants (from University Physics, Sears Zemansky, and Young, Reading, MA, 1979

Strain Gages. Approximate Elastic Constants (from University Physics, Sears Zemansky, and Young, Reading, MA, 1979 Material Strain Gages Approximate Elastic Constants (from University Physics, Sears Zemansky, and Young, Reading, MA, 1979 Young's Modulus, Y Shear Modulus, S Bulk Modulus, B Poisson's Ratio 10 11 N/m

More information

Voltage Dividers, Nodal, and Mesh Analysis

Voltage Dividers, Nodal, and Mesh Analysis Engr228 Lab #2 Voltage Dividers, Nodal, and Mesh Analysis Name Partner(s) Grade /10 Introduction This lab exercise is designed to further your understanding of the use of the lab equipment and to verify

More information

Sensors, Signals and Noise 1 COURSE OUTLINE. Introduction Signals and Noise Filtering Sensors: Strain Gauges. Signal Recovery, 2017/2018 Strain Gauges

Sensors, Signals and Noise 1 COURSE OUTLINE. Introduction Signals and Noise Filtering Sensors: Strain Gauges. Signal Recovery, 2017/2018 Strain Gauges Sensors, Signals and Noise 1 COURSE OUTLINE Introduction Signals and Noise Filtering Sensors: Strain Gauges Strain Gauges 2 Stress and strain in elastic materials Piezoresistive Effect Strain Gauge principle

More information

Lecture 5: Using electronics to make measurements

Lecture 5: Using electronics to make measurements Lecture 5: Using electronics to make measurements As physicists, we re not really interested in electronics for its own sake We want to use it to measure something often, something too small to be directly

More information

Strain Gages. Approximate Elastic Constants (from University Physics, Sears Zemansky, and Young, Reading, MA, Shear Modulus, (S) N/m 2

Strain Gages. Approximate Elastic Constants (from University Physics, Sears Zemansky, and Young, Reading, MA, Shear Modulus, (S) N/m 2 When you bend a piece of metal, the Strain Gages Approximate Elastic Constants (from University Physics, Sears Zemansky, and Young, Reading, MA, 1979 Material Young's Modulus, (E) 10 11 N/m 2 Shear Modulus,

More information

CHAPTER 13. Solutions for Exercises

CHAPTER 13. Solutions for Exercises HPT 3 Solutions for xercises 3. The emitter current is gien by the Shockley equation: i S exp VT For operation with i, we hae exp >> S >>, and we can write VT i S exp VT Soling for, we hae 3.2 i 2 0 26ln

More information

Electronic Circuits. Prof. Dr. Qiuting Huang Integrated Systems Laboratory

Electronic Circuits. Prof. Dr. Qiuting Huang Integrated Systems Laboratory Electronic Circuits Prof. Dr. Qiuting Huang 6. Transimpedance Amplifiers, Voltage Regulators, Logarithmic Amplifiers, Anti-Logarithmic Amplifiers Transimpedance Amplifiers Sensing an input current ii in

More information

R R V I R. Conventional Current. Ohms Law V = IR

R R V I R. Conventional Current. Ohms Law V = IR DC Circuits opics EMF and erminal oltage esistors in Series and in Parallel Kirchhoff s ules EMFs in Series and in Parallel Capacitors in Series and in Parallel Ammeters and oltmeters Conventional Current

More information

Electronics II. Midterm #1

Electronics II. Midterm #1 The University of Toledo EECS:3400 Electronics I su3ms_elct7.fm Section Electronics II Midterm # Problems Points. 5. 6 3. 9 Total 0 Was the exam fair? yes no The University of Toledo su3ms_elct7.fm Problem

More information

Chapter 2. Chapter 2

Chapter 2. Chapter 2 Chapter 2 The Bohr atom The Bohr atom is useful for visualizing atomic structure. The nucleus is positively charged and has the protons and neutrons. Electrons are negatively charged and in discrete shells.

More information

1 Written and composed by: Prof. Muhammad Ali Malik (M. Phil. Physics), Govt. Degree College, Naushera

1 Written and composed by: Prof. Muhammad Ali Malik (M. Phil. Physics), Govt. Degree College, Naushera ELECTROMAGNETISM Q # 1. Describe the properties of magnetic field due to current in a long straight conductor. Ans. When the heavy current is passed through a straight conductor: i. A magnetic field is

More information

PHA3/W PHYSICS (SPECIFICATION A) Unit 3 Current Electricity and Elastic Properties of Solids

PHA3/W PHYSICS (SPECIFICATION A) Unit 3 Current Electricity and Elastic Properties of Solids Surname Centre Number Other Names Candidate Number Leave blank Candidate Signature General Certificate of Education January 2005 Advanced Subsidiary Examination PHYSICS (SPECIFICATION A) PHA3/W Unit 3

More information

Lab 3: Electric Field Mapping Lab

Lab 3: Electric Field Mapping Lab Lab 3: Electric Field Mapping Lab Last updated 9/14/06 Lab Type: Cookbook/Quantitative Concepts Electrostatic Fields Equi-potentials Objectives Our goal in this exercise is to map the electrostatic equi-potential

More information

General Physics (PHY 2140)

General Physics (PHY 2140) General Physics (PHY 2140) Lecture 9 Electrodynamics Electric current temperature variation of resistance electrical energy and power http://www.physics.wayne.edu/~apetrov/phy2140/ Chapter 17-18 1 Department

More information

Tridib s Physics Tutorials visit NCERT-XII / Unit- 03 Current Electricity

Tridib s Physics Tutorials visit   NCERT-XII / Unit- 03 Current Electricity CURRENT ELECTRICITY OHM S LAW:- Let us consider a conductor through which a current I is flowing and V be the potential difference between its ends,then Ohm s law states that V I or, V = R I..(1) where

More information

Electric Charge. Electric Charge ( q ) unbalanced charges positive and negative charges. n Units Coulombs (C)

Electric Charge. Electric Charge ( q ) unbalanced charges positive and negative charges. n Units Coulombs (C) Electric Charge Electric Charge ( q ) unbalanced charges positive and negative charges n Units Coulombs (C) Electric Charge How do objects become charged? Types of materials Conductors materials in which

More information

ANNOUNCEMENT ANNOUNCEMENT

ANNOUNCEMENT ANNOUNCEMENT ANNOUNCEMENT Exam : Tuesday September 25, 208, 8 PM - 0 PM Location: Elliott Hall of Music (see seating chart) Covers all readings, lectures, homework from Chapters 2 through 23 Multiple choice (5-8 questions)

More information

Interfacing a Sensor-- use of Signal Conditioners

Interfacing a Sensor-- use of Signal Conditioners nterfacing a ensor-- use of ignal onditioners input Transducer (sensor signal conditioner -Deflection bridges -A.. arrier systems -nstrumentation Amplifiers -oltage to current onverters -urrent to voltage

More information

ECE 1311: Electric Circuits. Chapter 2: Basic laws

ECE 1311: Electric Circuits. Chapter 2: Basic laws ECE 1311: Electric Circuits Chapter 2: Basic laws Basic Law Overview Ideal sources series and parallel Ohm s law Definitions open circuits, short circuits, conductance, nodes, branches, loops Kirchhoff's

More information

AS PHYSICS. Electricity Homework Questions. moulsham high school

AS PHYSICS. Electricity Homework Questions. moulsham high school moulsham high school AS PHYSCS Electricity Homework Questions Work with other memebrs of the group to complete at least the first 5 questions using your text books and your knowledge from GCSE. 1.List

More information

Work, Energy and Power

Work, Energy and Power 1 Work, Energy and Power Work is an activity of force and movement in the direction of force (Joules) Energy is the capacity for doing work (Joules) Power is the rate of using energy (Watt) P = W / t,

More information

5. ELECTRIC CURRENTS

5. ELECTRIC CURRENTS 5. ELECTRIC CURRENTS TOPIC OUTLINE Section Recommended Time Giancoli Section 5.1 Potential Difference, Current, Resistance 5.2 Electric Circuits 3h 19.1, 19.2 6.2 Electric Field and Force 6.3 Magnetic

More information

Symbol Offers Units. R Resistance, ohms. C Capacitance F, Farads. L Inductance H, Henry. E, I Voltage, Current V, Volts, A, Amps. D Signal shaping -

Symbol Offers Units. R Resistance, ohms. C Capacitance F, Farads. L Inductance H, Henry. E, I Voltage, Current V, Volts, A, Amps. D Signal shaping - Electrical Circuits HE 13.11.018 1. Electrical Components hese are tabulated below Component Name Properties esistor Simplest passive element, no dependence on time or frequency Capacitor eactive element,

More information

Electromotive Force. The electromotive force (emf), ε, of a battery is the maximum possible voltage that the battery can provide between its terminals

Electromotive Force. The electromotive force (emf), ε, of a battery is the maximum possible voltage that the battery can provide between its terminals Direct Current When the current in a circuit has a constant magnitude and direction, the current is called direct current Because the potential difference between the terminals of a battery is constant,

More information

Kirchhoff s Rules. Kirchhoff s rules are statements used to solve for currents and voltages in complicated circuits. The rules are

Kirchhoff s Rules. Kirchhoff s rules are statements used to solve for currents and voltages in complicated circuits. The rules are Kirchhoff s Rules Kirchhoff s rules are statements used to solve for currents and voltages in complicated circuits. The rules are Rule. Sum of currents into any junction is zero. i = 0 i 1 2 = 12 Why?

More information

Module 1. Energy Methods in Structural Analysis

Module 1. Energy Methods in Structural Analysis Module 1 Energy Methods in Structural Analysis esson 5 Virtual Work Instructional Objecties After studying this lesson, the student will be able to: 1. Define Virtual Work.. Differentiate between external

More information

V. Transistors. 3.1 III. Bipolar-Junction (BJT) Transistors

V. Transistors. 3.1 III. Bipolar-Junction (BJT) Transistors V. Transistors 3.1 III. Bipolar-Junction (BJT) Transistors A bipolar junction transistor is formed by joining three sections of semiconductors with alternatiely different dopings. The middle section (base)

More information

Active Circuits: Life gets interesting

Active Circuits: Life gets interesting Actie Circuits: Life gets interesting Actie cct elements operational amplifiers (OP AMPS) and transistors Deices which can inject power into the cct External power supply normally comes from connection

More information

Magnetic Fields Part 3: Electromagnetic Induction

Magnetic Fields Part 3: Electromagnetic Induction Magnetic Fields Part 3: Electromagnetic Induction Last modified: 15/12/2017 Contents Links Electromagnetic Induction Induced EMF Induced Current Induction & Magnetic Flux Magnetic Flux Change in Flux Faraday

More information