A Dc–Dc Converter with High-Voltage Step-Up Ratio and Reduced- Voltage Stress for Renewable Energy Generation Systems
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Control Techniques Commander SK Advanced User Guide
Advanced User Guide Commander SK AC variable speed drive for 3 phase induction motors from 0.25kW to 110kW, 0.33hp to 150hp Part Number: 0472-0001-08 Issue: 8 www.controltechniques.com General Information The manufacturer accepts no liability for any consequences resulting from inappropriate, negligent or incorrect installation or adjustment of the optional operating parameters of the equipment or from mismatching the variable speed drive with the motor. The contents of this guide are believed to be correct at the time of printing. In the interests of a commitment to a policy of continuous development and improvement, the manufacturer reserves the right to change the specification of the product or its performance, or the contents of the guide, without notice. All rights reserved. No parts of this guide may be reproduced or transmitted in any form or by any means, electrical or mechanical including photocopying, recording or by an information storage or retrieval system, without permission in writing from the publisher. Drive software version This product is supplied with the latest software version. If this drive is to be connected to an existing system or machine, all drive software versions should be verified to confirm the same functionality as drives of the same model already present. This may also apply to drives returned from a Control Techniques Service Centre or Repair Centre. If there is any doubt please contact the supplier of the product. The software version of the drive can be checked by looking at Pr 11.29 and Pr 11.34. This takes the form of xx.yy.zz where Pr 11.29 displays xx.yy and Pr 11.34 displays zz. -
Power Electronics
CMR COLLEGE OF ENGINEERING & TECHNOLOGY (AUTONOMOUS) ACADEMIC REGULATIONS COURSE STRUCTURE AND DETAILED SYLLABUS POWER ELECTRONICS For M.Tech TWO YEAR DEGREE COURSE (Applicable for the batches admitted from 2015-16) CMR COLLEGE OF ENGINEERING & TECHNOLOGY (AUTONOMOUS) (Affliated to JNTU, Accredited by NAAC with “A” grade) Kandlakoya, Medchal Road, Hyderabad. CMR COLLEGE OF ENGINEERING & TECHNOLOGY (AUTONOMOUS) CMR COLLEGE OF ENGINEERING & TECHNOLOGY (An Autonomous Institution) ACADEMIC REGULATION R15 FOR CBCS BASED M. TECH. (REGULAR) DEGREE PROGRAMMES (Applicable for the students of M. Tech. programme admitted into I year from Academic Year 2015-16 and onwards) 1.0 Eligibility for Admissions Admission to the above program shall be made subject to eligibility, qualification and specialization as prescribed by Government of Telangana State from time to time. Admission shall be made on the basis of merit/rank obtained by the candidates at the qualifying Entrance Test conducted by the Government of Telangana or on the basis of any other order of merit as approved by the University, subject to reservations as laid down by the Government from time to time. 1. Award of M. Tech. degree 2.1. A student shall be declared eligible for the award of the M. Tech. Degree, if he pursues a course of study in not less than two and not more than four academic years. However, he is permitted to write the examinations for two more years after four academic years of course work, failing which he shall forfeit his seat in M.Tech programme. 2.2. The M. Tech. degree of Jawaharlal Nehru Technological University Hyderabad shall be conferred on candidates who are admitted to the program and who fulfil all the requirements for the award of the degree. -
Automatic Permanent Magnet Generator Controller
Automatic Permanent Magnet Generator Controller for Small Applications A thesis submitted in partial fulfillment of the requirements for the degree of Master of Science in Engineering By William Scott Adkins B.S.E.E., Wright State University, 2013 2015 Wright State University WRIGHT STATE UNIVERSITY GRADUATE SCHOOL January 6, 2016 I HEREBY RECOMMEND THAT THE THESIS PREPARED UNDER MY SUPERVISION BY William Scott Adkins ENTITLED Automatic PMG Controller for Small Applications BE ACCEPTED IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE DEGREE OF Master of Science in Engineering. ______________________________ Marian K. Kazimierczuk, Ph.D. Thesis Director Committee on Final Examination ______________________________ Brian Rigling, Ph.D. ______________________________ Chair Marian K. Kazimierczuk, Ph.D. Department of Electrical Engineering College of Engineering and Computer Science ______________________________ Lavern Alan Starman, Ph. D ______________________________ Saiyu Ren, Ph.D. ______________________________ Robert E. W. Fyffe, Ph.D. Vice President for Research and Dean of the Graduate School PROPRIETARY & INTECTUAL PROPERTY INFORMATION The information contained within this document is entitled as William Scott Adkins proprietary information and intellectual property and is disclosed in confidence. It is the property of William Scott Adkins and shall not be used, disclosed to others or reproduced without the express written consent of William Scott Adkins, including, but without limitation, it is not to be used in the creation, manufacture, development, or derivation of any repairs, modifications, spare parts, designs, or configuration changes or to obtain FAA or any other government or regulatory approval to do so. If consent is given for reproduction in whole or in part, this notice shall be applicable to all contents of this document or any document provide as such. -
Introduction to Direct Current (DC) Theory
PDHonline Course E235 (4 PDH) Electrical Fundamentals - Introduction to Direct Current (DC) Theory Instructor: A. Bhatia, B.E. 2012 PDH Online | PDH Center 5272 Meadow Estates Drive Fairfax, VA 22030-6658 Phone & Fax: 703-988-0088 www.PDHonline.org www.PDHcenter.com An Approved Continuing Education Provider CHAPTER 3 DIRECT CURRENT LEARNING OBJECTIVES Upon completing this chapter, you will be able to: 1. Identify the term schematic diagram and identify the components in a circuit from a simple schematic diagram. 2. State the equation for Ohm's law and describe the effects on current caused by changes in a circuit. 3. Given simple graphs of current versus power and voltage versus power, determine the value of circuit power for a given current and voltage. 4. Identify the term power, and state three formulas for computing power. 5. Compute circuit and component power in series, parallel, and combination circuits. 6. Compute the efficiency of an electrical device. 7. Solve for unknown quantities of resistance, current, and voltage in a series circuit. 8. Describe how voltage polarities are assigned to the voltage drops across resistors when Kirchhoff's voltage law is used. 9. State the voltage at the reference point in a circuit. 10. Define open and short circuits and describe their effects on a circuit. 11. State the meaning of the term source resistance and describe its effect on a circuit. 12. Describe in terms of circuit values the circuit condition needed for maximum power transfer. 13. Compute efficiency of power transfer in a circuit. 14. Solve for unknown quantities of resistance, current, and voltage in a parallel circuit. -
Academic Regulations, Course Structure and Detailed Syllabus
ACADEMIC REGULATIONS, COURSE STRUCTURE AND DETAILED SYLLABUS M.Tech (POWER ELECTRONICS AND ELECTRIC DRIVES) FOR MASTER OF TECHNOLOGY TWO YEAR POST GRADUATE COURSE (Applicable for the batches admitted from 2014-2015) R14 ANURAG GROUP OF INSTITUTIONS (AUTONOMOUS) SCHOOL OF ENGINEERING Venkatapur, Ghatkesar, Hyderabad – 500088 ANURAG GROUP OF INSTITUTIONS (AUTONOMOUS) M.TECH. (POWER ELECTRONICS AND ELECTRIC DRIVES) I YEAR - I SEMESTER COURSE STRUCTURE AND SYLLUBUS Subject Code Subject L P Credits A31058 Machine Modeling& Analysis 3 0 3 A31059 Power Electronic Converters-I 3 0 3 A31024 Modern Control Theory 3 0 3 A31060 Power Electronic Control of DC Drives 3 0 3 Elective-I 3 0 3 A31029 HVDC Transmission A31061 Operations Research A31062 Embedded Systems Elective-II A31027 Microcontrollers and Applications 3 0 3 A31063 Programmable Logic Controllers and their Applications A31064 Special Machines A31213 Power Converters Lab 0 3 2 A31214 Seminar - - 2 Total 18 3 22 I YEAR - II SEMESTER Subject Subject L P Credits Code A32058 Power Electronic Converters-II 3 0 3 A32059 Power Electronic Control of AC Drives 3 0 3 A32022 Flexible AC Transmission Systems (FACTS) 3 0 3 A32060 Neural Networks and Fuzzy Systems 3 0 3 Elective-III A32061 Digital Control Systems 3 0 3 A32062 Power Quality A32063 Advanced Digital Signal Processing Elective-IV A32064 Dynamics of Electrical Machines A32065 High-Frequency Magnetic Components A32066 3 0 3 Renewable Energy Systems A32213 Electrical Systems Simulation Lab 0 3 2 A32214 Seminar-II - - 2 Total 18 3 22 II YEAR – I SEMESTER Code Subject L P Credits A33219 Comprehensive Viva-Voce - - 2 A33220 Project Seminar 0 3 2 A33221 Project Work Part-I - - 18 Total Credits - 3 22 II YEAR – II SEMESTER Code Subject L P Credits A34207 Project Work Part-II and Seminar - - 22 Total - - 22 L P C M. -
Instructor's Guide
Instructor’s Guide Electricity: A 3-D Animated Demonstration ELECTRICITY AND MAGNETISM Introduction This instructor’s guide provides information to help you get the most out of Electricity and Magnetism, part of the eight-part series Electricity: A 3-D Animated Demonstration. The series makes the principles of electricity easier to understand and discuss. The series includes Electrostatics; Electric Current; Ohm's Law; Circuits; Power and Efficiency; Electricity and Magnetism; Electric Motors; and Electric Generators. Electricity and Magnetism traces the relationship between magnetism and electricity from the first accidental discovery of induced current. Learning Objectives After watching the video program, students will be able to: • Describe the relationship between electricity and magnetism • Explain the difference between electric and magnetic fields • Explain the construct, function, and use of solenoids • Differentiate between, explain, and apply the left-hand and right-hand rules • Demonstrate (via experiments) and explain aspects, and actions and functions of electricity, magnetism, and electromagnetism Educational Standards National Science Standards This program correlates with the National Science Education Standards from the National Academies of Science, and Project 2061, from the American Association for the Advancement of Science. Copyright © 2008 SHOPWARE® • www.shopware-usa.com • 1-800-487-3392 Electricity: A 3-D Animated Demonstration ELECTRICITY AND MAGNETISM INSTRUCTOR’S GUIDE Science as Inquiry Content Standard A: -
Faraday's Law Da
Faraday's Law dA B B r r Φ≡B •d A B ∫ dΦ ε= − B dt Faraday’s Law of Induction r r Recall the definition of magnetic flux is ΦB =B∫ ⋅ d A Faraday’s Law is the induced EMF in a closed loop equal the negative of the time derivative of magnetic flux change in the loop, d r r dΦ ε= −B∫ d ⋅= A − B dt dt Constant B field, changing B field, no induced EMF causes induced EMF in loop in loop Getting the sign EMF in Faraday’s Law of Induction Define the loop and an area vector, A, who magnitude is the Area and whose direction normal to the surface. A The choice of vector A direction defines the direction of EMF with a right hand rule. Your thumb in A direction and then your fingers point to positive EMF direction. Lenz’s Law – easier way! The direction of any magnetic induction effect is such as to oppose the cause of the effect. ⇒ Convenient method to determine I direction Heinrich Friedrich Example if an external magnetic field on a loop Emil Lenz is increasing, the induced current creates a field opposite that reduces the net field. (1804-1865) Example if an external magnetic field on a loop is decreasing, the induced current creates a field parallel to the that tends to increase the net field. Incredible shrinking loop: a circular loop of wire with a magnetic flux is shrinking with time. In which direction is the induced current? (a) There is none. (b) CW. -
Teaching H. C. Ørsted's Scientific Work in Danish High School Physics
UNIVERSITY OF COPENHAGEN FACULTY OF SCIENCE Ida Marie Monberg Hindsholm Teaching H. C. Ørsted's Scientific Work in Danish High School Physics Masterʹs thesis Department of Science Education 19 July 2018 Master's thesis Teaching H. C. Ørsted’s Scientific Work in Danish High School Physics Submitted 19 July 2018 Author Ida Marie Monberg Hindsholm, B.Sc. E-mail [email protected] Departments Niels Bohr Institute, University of Copenhagen Department of Science Education, University of Copenhagen Main supervisor Ricardo Avelar Sotomaior Karam, Associate Professor, Department of Science Education, University of Copenhagen Co-supervisor Steen Harle Hansen, Associate Professor, Niels Bohr Institute, University of Copenhagen 1 Contents 1 Introduction . 1 2 The Material: H. C. Ørsted's Work . 3 2.1 The Life of Hans Christian Ørsted . 3 2.2 Ørsted’s Metaphysical Framework: The Dynamical Sys- tem............................. 6 2.3 Ritter and the failure in Paris . 9 2.4 Ørsted’s work with acoustic and electric figures . 12 2.5 The discovery of electromagnetism . 16 2.6 What I Use for the Teaching Sequence . 19 3 Didactic Theory . 20 3.1 Constructivist teaching . 20 3.2 Inquiry Teaching . 22 3.3 HIPST . 24 4 The Purpose and Design of the Teaching Sequence . 27 4.1 Factual details and lesson plan . 28 5 Analysis of Transcripts and Writings . 40 5.1 Method of Analysis . 40 5.2 Practical Problems . 41 5.3 Reading Original Ørsted's Texts . 42 5.4 Inquiry and Experiments . 43 5.5 "Role play" - Thinking like Ørsted . 48 5.6 The Reflection Corner . 51 5.7 Evaluation: The Learning Objectives . -
Voltage Control and Braking System of a DFIG During a Fault
Journal of the Institute of Engineering Volume 16, No. 1 Published: April 2021 ISSN: 1810-3383 © TUTA j IOE j PCU Printed in Nepal Voltage Control and Braking System of a DFIG during a Fault Rabin Mahat a, Khagendra B. Thapa b, Sudip Lamichhane, Sudeep Thapaliya, Sagar Dhakal Department of Electrical Engineering, Pulchowk Campus, Institute of Engineering, Tribhuvan University, Nepal Corresponding Authors: a [email protected], b [email protected] Received: 2020-08-31 Revised: 2021-01-23 Accepted: 2021-01-30 Abstract: This paper describes a voltage control scheme of a doubly fed induction generator (DFIG) wind turbine that can inject more reactive power to the grid during a fault so as to support the grid voltage. To achieve this, the coordinated control scheme using both rotor side converter (RSC) and grid side converters (GSC) controllers of the DFIG are employed simultaneously. The RSC and GSC controllers employ PI controller to operate smoothly. In the voltage control mode, the RSC and GSC are operated. During a fault, both RSC and GSC are used simultaneously to supply the reactive power into the grid (main line) depending on voltage dip condition to support the grid voltage. The proposed system is implemented for single DFIG wind turbine using MATLAB simulation software. The results illustrate that the control strategy injects the reactive power to support the voltage stability during a fault rapidly. Also, the braking system is designed to protect the wind turbine system from over speed. For this purpose, the braking resistors are being used. Keywords: Voltage control, Braking System, DFIG, RSC, GSC 1. -
AC Vs. DC Boost Converters: a Detailed Conduction Loss Comparison
AC vs. DC Boost Converters: A Detailed Conduction Loss Comparison Daniel L Gerber Fariborz Musavi Building Technology and Urban Systems Engineering and Computer Science Lawrence Berkeley Labs Washington State University Berkeley, CA, USA Vancouver, WA, USA [email protected] [email protected] Abstract—Studies have shown the efficiency benefits of DC dis- at the same voltage. Although several previous works have tribution systems are largely due to the superior performance of analyzed and established loss models for the DC/DC [9]– DC/DC converters. Nonetheless, these studies are often based on [12] and AC/DC PFC [13]–[20] boost converters, they each product data that differs widely in manufacturer and operating have their own methods and formulae, making an analytic voltage. This work develops a rigorous loss model to theoretically comparison difficult. In addition, many of them neglect es- compare the efficiency of a DC/DC and an AC/DC PFC boost sential components such as the input bridge drop and output converter. It ensures each converter has the same components and equivalent operating voltages. The results show AC boost capacitor equivalent series resistance (ESR). This is the first converters below 500 W to have 2.9 to 4.2 times the loss of DC. work to establish a set of formulae that compare the loss between an AC and DC boost converter, both of which have the Keywords—DC microgrid, boost converter, loss model, power same components and equivalent operating voltages. Although factor correction DC/DC converters are already known to be more efficient, this work reports exactly how much more. -
Faraday's Law Da
Faraday's Law dA B B r r Φ≡B •d A B ∫ dΦ ε= − B dt Applications of Magnetic Induction • AC Generator – Water turns wheel Æ rotates magnet Æ changes flux Æ induces emf Æ drives current • “Dynamic” Microphones (E.g., some telephones) – Sound Æ oscillating pressure waves Æ oscillating [diaphragm + coil] Æ oscillating magnetic flux Æ oscillating induced emf Æ oscillating current in wire Question: Do dynamic microphones need a battery? More Applications of Magnetic Induction • Tape / Hard Drive / ZIP Readout – Tiny coil responds to change in flux as the magnetic domains (encoding 0’s or 1’s) go by. 2007 Nobel Prize!!!!!!!! Giant Magnetoresistance • Credit Card Reader – Must swipe card Æ generates changing flux – Faster swipe Æ bigger signal More Applications of Magnetic Induction • Magnetic Levitation (Maglev) Trains – Induced surface (“eddy”) currents produce field in opposite direction Æ Repels magnet Æ Levitates train S N rails “eddy” current – Maglev trains today can travel up to 310 mph Æ Twice the speed of Amtrak’s fastest conventional train! – May eventually use superconducting loops to produce B-field Æ No power dissipation in resistance of wires! Faraday’s Law of Induction r r Recall the definition of magnetic flux is ΦB =B∫ ⋅ d A Faraday’s Law is the induced EMF in a closed loop equal the negative of the time derivative of magnetic flux change in the loop, d r r dΦ ε= −B∫ d ⋅= A − B dt dt Constant B field, changing B field, no induced EMF causes induced EMF in loop in loop Getting the sign EMF in Faraday’s Law of Induction Define the loop and an area vector, A, who magnitude is the Area and whose direction normal to the surface. -
Voltage Sag Ride-Through of AC Drives: Control and Analysis
Voltage Sag Ride-Through of AC Drives: Control and Analysis Kai PietilÄainen Stockholm 2005 Electrical Machines and Power Electronics Department of Electrical Systems Royal Institute of Technology Submitted to the School of Electrical Engineering, KTH, in partial ful¯llment of the requirements for the degree of Doctor of Technology. TRITA-ETS-2005-12 ISSN 1650{674X ISRN KTH/R-0504-SE ISBN 91-7178-165-X KTH, Royal Institute of Technology Department of Electrical Systems Division of Electrical Machines and Power Electronics KTH/ETS/EME Teknikringen 33 SE-10044 Stockholm Sweden °c Kai PietilÄainen,2005 Abstract This thesis focuses on controller design and analysis for induction motor (IM) drives, flux control for electrically excited synchronous motors with damper windings (EESMs), and to enhance voltage sag ride-through ability and analy- sis for a wind turbine application with a full-power grid-connected active recti- ¯er. The goal is to be able to use the existing equipment, without altering the hardware. Further, design and analysis of the stabilization of DC-link voltage oscillations for DC systems and inverter drives is studied, for example traction drives with voltage sags in focus. The proposed IM controller is based on the ¯eld-weakening controller of Kim and Sul [31], which is further developed. Applying the proposed controller to voltage sag ride-through gives a cheap and simple ride-through system. The EESM controller is based on setpoint adjustment for the ¯eld current controller. The analysis also concerns stability for the proposed flux controller. The DC-link stabilization algorithm is designed following Mosskull [38], where a component is added to the current controller.