EE 33-Measurements and Instrumentation
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A History of Impedance Measurements
A History of Impedance Measurements by Henry P. Hall Preface 2 Scope 2 Acknowledgements 2 Part I. The Early Experimenters 1775-1915 3 1.1 Earliest Measurements, Dc Resistance 3 1.2 Dc to Ac, Capacitance and Inductance Measurements 6 1.3 An Abundance of Bridges 10 References, Part I 14 Part II. The First Commercial Instruments 1900-1945 16 2.1 Comment: Putting it All Together 16 2.2 Early Dc Bridges 16 2.3 Other Early Dc Instruments 20 2.4 Early Ac Bridges 21 2.5 Other Early Ac Instruments 25 References Part II 26 Part III. Electronics Comes of Age 1946-1965 28 3.1 Comment: The Post-War Boom 28 3.2 General Purpose, “RLC” or “Universal” Bridges 28 3.3 Dc Bridges 30 3.4 Precision Ac Bridges: The Transformer Ratio-Arm Bridge 32 3.5 RF Bridges 37 3.6 Special Purpose Bridges 38 3,7 Impedance Meters 39 3.8 Impedance Comparators 40 3.9 Electronics in Instruments 42 References Part III 44 Part IV. The Digital Era 1966-Present 47 4.1 Comment: Measurements in the Digital Age 47 4.2 Digital Dc Meters 47 4.3 Ac Digital Meters 48 4.4 Automatic Ac Bridges 50 4.5 Computer-Bridge Systems 52 4.6 Computers in Meters and Bridges 52 4.7 Computing Impedance Meters 53 4.8 Instruments in Use Today 55 4.9 A Long Way from Ohm 57 References Part IV 59 Appendices: A. A Transformer Equivalent Circuit 60 B. LRC or Universal Bridges 61 C. Microprocessor-Base Impedance Meters 62 A HISTORY OF IMPEDANCE MEASUREMENTS PART I. -
Electrical Measurements Unit-I Measurement of Voltage and Current 1
ELECTRICAL MEASUREMENTS UNIT-I MEASUREMENT OF VOLTAGE AND CURRENT 1. What is meant by galvanometer? An instrument for detecting and measuring small electric current it is also called as galvanometer. 2. What is the Use of galvanometer in measurement system? Galvanometer is used as null detector (or) zero-current detector in bridge circuit and potentiometer measurement. 3. What are the different types of galvanometer? D’Arsonval galvanometer Vibration galvanometer Ballistic galvanometer Flux meter 4. What are the following methods are adopted calibrating the galvanometer? Use of charged capacitor Use of a standard solenoid Use of a mutual inductor 5. What is meant by vibration galvanometer? Vibration galvanometer is a tuned detector and as such, it is very sensitive to Changes of frequency. 6. Differentiate between ammeter and voltmeter. S. No Ammeter Voltmeter 1 It is a current measuring device It is a Voltage measuring device which which measures current through measures potential difference between the circuit. two points of a circuit. 2 Always connected in series with Always connected in Parallel with the circuit. circuit. 3 The resistance is very very The resistance is very very high small 4 Deflecting torque is produced by Deflecting torque is produced by current current to be measured directly which is proportional to the voltage to be measured 7. What is meant by measurement? Measurement is an act or the result of comparison between the quantity and a predefined standard. 8. Mention the basic requirements of measurement. The standard used for comparison purpose must be accurately defined and should be commonly accepted.The apparatus used and the method adopted must be provable. -
Sem 6 Prac Viva Book
V.P. & R.P.T.P.SCIENCE COLLEGE PHYSICS DEPARTMENT VALLABH VIDYANAGR 6TH SEMESTER B.Sc. PHYSICS US06CPHY07/08/09 PRACTICAL VIVA VOCE BOOK DECEMBER 2017 PREPARED BY Dr. T.H.PATEL PHYSICS DEPT VP & RPTP SCIENCE COLLGE V.VIDYANAGAR Page 1 V.P. & R.P.T.P. SCIENCE COLLEGE VALLABH VIDYANAGAR B. Sc. Semester-6 Physics Practical -VIVA-VOCE No. Experiment Course Page No. 1 Searl s Goniometer (variable distance) PHY09 3 2 Power Amplifier PHY08 3 3 Determination of Planck Constant. PHY09 5 4 L - by Owen s Bridge PHY07 11 5 Light Dependent Resistor (LDR) PHY09 12 6 Wein Bridge Oscillator PHY08 14 7 Bistable Multivibrator PHY08 16 8 Hall effect Measurements (Const. Probe Current) PHY07 18 9 e/m of an Electron by Magnetron Method PHY07 19 10 Square Well Potential PHY09 20 11 Fabri-Parot Etalon PHY09 21 12 LVDT Characteristics PHY07 23 13 Characteristics of UJT PHY08 25 14 Op-Amp Applications PHY08 26 15 Op-Amp Parameters PHY08 26 16 High Resistance by Leakage PHY07 28 17 Binary Counters (4 bit) PHY08 29 18 Babinet Compensator PHY09 34 19 Carey- PHY07 36 20 e by Millikan s Oil Drop Method PHY09 38 21 MichelsonFoster Interferometer- Method ρ II PHY09 40 Determination of Lattice Parameters PHY09 22 40 (electron diffraction ring pattern) 22 GENERAL QUESTION PHY09 41 PREPARED BY Dr. T.H.PATEL PHYSICS DEPT VP & RPTP SCIENCE COLLGE V.VIDYANAGAR Page 2 1 Searl’s Goniometer PHY09 What do you mean by a coaxial system of lenses? When a number of lenses having a common principal axis are used, then this combination is called a coaxial system of lenses. -
JAWAHARLAL NEHRU TECHNOLOGICAL UNIVERSITY HYDERABAD (Established by State Act No
JAWAHARLAL NEHRU TECHNOLOGICAL UNIVERSITY HYDERABAD (Established by State Act No. 30 of 2008) Kukatpally, Hyderabad, Telangana (India). ACADEMIC REGULATIONS FOR B.TECH. REGULAR STUDENTS WITH EFFECT FROM ACADEMIC YEAR 2016-17 (R-16) 1.0 Under-Graduate Degree Programme in Engineering & Technology (UGP in E&T) 1.1 JNTUH offers a 4-year (8 semesters) Bachelor of Technology (B.Tech.) degree programme, under Choice Based Credit System (CBCS) at its non-autonomous constituent and affiliated colleges with effect from the academic year 2016-17 in the following branches of Engineering: Branch Civil Engineering Electrical and Electronics Engineering Mechanical Engineering Electronics and Communication Engineering Computer Science and Engineering Chemical Engineering Electronics and Instrumentation Engineering Bio-Medical Engineering Information Technology Mechanical Engineering (Mechatronics) Electronics and Telematics Engineering Metallurgy and Material Technology Electronics and Computer Engineering Mechanical Engineering (Production) Aeronautical Engineering Instrumentation and Control Engineering Biotechnology Automobile Engineering Mining Engineering Petroleum Engineering Civil and Environmental Engineering Mechanical Engineering (Nano Technology) Computer Science & Technology Pharmaceutical Engineering 1 2.0 Eligibility for admission 2.1 Admission to the under graduate programme shall be made either on the basis of the merit rank obtained by the qualified student in entrance test conducted by the Telangana State Government (EAMCET) or the University or on the basis of any other order of merit approved by the University, subject to reservations as prescribed by the government from time to time. 2.2 The medium of instructions for the entire under graduate programme in E&T will be English only. 3.0 B.Tech. Programme structure 3.1 A student after securing admission shall pursue the under graduate programme in B.Tech. -
Mepco Schlenk Engineering College, Sivakasi
MEPCO SCHLENK ENGINEERING COLLEGE, SIVAKASI (AUTONOMOUS) AFFILIATED TO ANNA UNIVERSITY, CHENNAI 600 025 REGULATIONS: MEPCO - R2015 (FULL TIME) (CHOICE BASED CREDIT SYSTEM) B. E. ELECTRICAL AND ELECTRONICS ENGINEERING Department Vision Department Mission To Render Services to Meet the Growing To Provide the Students a Rigorous Learning Experience in Global Challenges of Engineering Understanding Industries Basics of Electrical & Electronics Engineering Built on the by Educating Students to become Foundation of Science, Mathematics, Computing, and Exemplary Technology by Emphasizing Professional Electrical and Electronics Active Learning with Strongly Supported Laboratory Engineers of High Ethics Component and Prepare them for Professional Careers UG Programme Educational Objectives (PEOs) I. Preparation: To prepare students to excel in Industry or in Postgraduate Programmes by Educating Students along with High moral values and Knowledge. II. Core Competence: To provide students with the fundamentals of Engineering Sciences with more emphasis in Electrical and Electronics Engineering by way of analyzing and exploiting engineering challenges in disparate systems during their professional career. III. Breadth: To train students with good scientific and engineering breadth so as to comprehend, analyze, design, and create novel products and solutions for the real life problems. IV. Professionalism: To inculcate professional and ethical attitude, effective communication skills, teamwork skills, multidisciplinary approach, entrepreneurial thinking and an ability to relate engineering issues to broader social context in students. V. Learning environment: To provide students with an academic environment aware of excellence, leadership, written ethical codes and guidelines, and the self motivated life-long learning needed for a successful professional career. UG Programme Outcomes (POs) 1. Graduates will demonstrate knowledge of mathematics, science, engineering fundamentals and an engineering specialization to the conceptualization of engineering models. -
A History of Impedance Measurements
A HISTORY OF IMPEDANCE MEASUREMENTS PART I. THE EARLY EXPERIMENTERS 1775-1915 1.1 Earliest Measurements, DC Resistance It would seem appropriate to credit the first impedance measurements to Georg Simon Ohm (1788-1854) even though others may have some claim. These were dc resistance measurements, not complex impedance, and of necessity they were relative measurements because then there was no unit of resistance or impedance, no Ohm. For his initial measurements he used a voltaic cell, probably having copper and zinc plates, whose voltage varied badly under load. As a result he arrived at an erroneous logarithmic relationship between the current measured and the length of wire, which he published in 18251. After reading this paper, his editor, Poggendorff, suggested that Ohm use the recently discovered Seebeck (thermoelectric) effect to get a more constant voltage. Ohm repeated his measurements using a copper-bismuth thermocouple for a source2. His detector was a torsion galvanometer (invented by Coulomb), a galvanometer whose deflection was offset by the torque of thin wire whose rotation was calibrated (see figure 1-1). He determined "that the force of the current is as the sum of all the tensions, and inversely as the entire length of the current". Using modern notation this becomes I = E/R or E =I*R. This is now known as Ohm's Law. He published this result in 1826 and a book, "The Galvanic Circuit Mathematically Worked Out" in 1827. For over ten years Ohm's work received little attention and, what there was, was unfavorable. Finally it was made popular by Henry in America, Lenz in Russia and Wheatstone in England3.