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)

Similar documents
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

Electronics Resistive Sensors and Bridge Circuits

The Digital Multimeter (DMM)

INSTITUTE OF AERONAUTICAL ENGINEERING (Autonomous) Dundigal, Hyderabad

E E 2320 Circuit Analysis. Calculating Resistance

Chapter 2. Engr228 Circuit Analysis. Dr Curtis Nelson

Chapter 2 Resistive Circuits

1 S = G R R = G. Enzo Paterno

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 5. Department of Mechanical Engineering

INSTITUTE OF AERONAUTICAL ENGINEERING (Autonomous) Dundigal, Hyderabad

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

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

Resistor Network Answers

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

Direct Current (DC) Circuits

TSOKOS CHAP 1 TEST REVIEW

Chapter 20 Electric Circuits

INTRODUCTION TO ELECTRONICS

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

MET 301 EXPERIMENT # 2 APPLICATION OF BONDED STRAIN GAGES

Calculate the total resistance of this combination. (3)

Chapter 2 Resistive Circuits

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

Chapter 7. Chapter 7

3/17/2009 PHYS202 SPRING Lecture notes Electric Circuits

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

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

Work, Energy and Power

Lecture 5: Using electronics to make measurements

Transmission lines using a distributed equivalent circuit

Chapter 25 Current, Resistance, and Electromotive Force

Physics 212. Lecture 9. Electric Current

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

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

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

Strain Gauge Application and Measurement of Unknown Load

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

STRAIN GAUGE MEASUREMENT

Kirchhoff's Laws and Circuit Analysis (EC 2)

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

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

Chapter 4: Methods of Analysis

Basic Laws. Bởi: Sy Hien Dinh

ELECTRICAL MEASUREMENTS LAB MANUAL

physics for you February 11 Page 68

Electric Circuits I. Nodal Analysis. Dr. Firas Obeidat

coil of the circuit. [8+8]

PhysicsAndMathsTutor.com

Parallel Circuits. Chapter

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

COOKBOOK KVL AND KCL A COMPLETE GUIDE

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

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

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

EE301 RESISTANCE AND OHM S LAW

ELECTROMAGNETIC INDUCTION

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

Lesson 10 Steady Electric Currents

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

Electrical Circuits Question Paper 1

Lecture 28 Field-Effect Transistors

CHAPTER 1 ELECTRICITY

Kirchhoff's Laws and Maximum Power Transfer

Wheatstone Bridge Nonlinearity

Chapter 4: Techniques of Circuit Analysis

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

ME411 Engineering Measurement & Instrumentation. Winter 2017 Lecture 9

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

The Steady Current Field

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

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

Voltage Dividers, Nodal, and Mesh Analysis

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

Lecture 5: Using electronics to make measurements

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

CHAPTER 13. Solutions for Exercises

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

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

Electronics II. Midterm #1

Chapter 2. Chapter 2

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

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

Lab 3: Electric Field Mapping Lab

General Physics (PHY 2140)

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

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

ANNOUNCEMENT ANNOUNCEMENT

Interfacing a Sensor-- use of Signal Conditioners

ECE 1311: Electric Circuits. Chapter 2: Basic laws

AS PHYSICS. Electricity Homework Questions. moulsham high school

Work, Energy and Power

5. ELECTRIC CURRENTS

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 -

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

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

Module 1. Energy Methods in Structural Analysis

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

Active Circuits: Life gets interesting

Magnetic Fields Part 3: Electromagnetic Induction

Transcription:

1

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 110.. 606.1 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. 0. + 110. 0.01 ±.96 w.96 100 0.888% 606.1. 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 10 00 k/ω by (1) 9 VsR R s + 00 9 (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 + 1000) s Vs (1000) 1. (Rs + 1000)...(iii) by (ii) & (iii) 9( Rs + 00) 13( Rs + 1000) 00 1000 18 Rs + 9000 13 Rs + 13000 S0 Rs 000 Rs 800...(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 :

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 + 10. + 0 9.60k. R 9.60k 10R 9.60 10 + R 3

10R 96 + 9.6 R 0. R 96 96 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 1 +... 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