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Analysis on Electric Field Based on Three Dimensional Atmospheric Electric Field Apparatus
J Electr Eng Technol.2018; 13(4): 1697-1704 ISSN(Print) 1975-0102 http://doi.org/10.5370/JEET.2018.13.4.1697 ISSN(Online) 2093-7423 Analysis on Electric Field Based on Three Dimensional Atmospheric Electric Field Apparatus Hong-yan Xing†, Gui-xian He* and Xin-yuan Ji** Abstract – As a key component of lighting location system (LLS) for lightning warning, the atmospheric electric field measuring is required to have high accuracy. The Conventional methods of the existent electric field measurement meter can only detect the vertical component of the atmospheric electric field, which cannot acquire the realistic electric field in the thunderstorm. This paper proposed a three dimensional (3D) electric field system for atmospheric electric field measurement, which is capable of three orthogonal directions in X, Y, Z, measuring. By analyzing the relationship between the electric field and the relative permittivity of ground surface, the permittivity is calculated, and an efficiency 3D measurement model is derived. On this basis, a three-dimensional electric field sensor and a permittivity sensor are adopted to detect the spatial electric field. Moreover, the elevation and azimuth of the detected target are calculated, which reveal the location information of the target. Experimental results show that the proposed 3D electric field meter has satisfactory sensitivity to the three components of electric field. Additionally, several observation results in the fair and thunderstorm weather have been presented. Keywords: Three dimension electric field, Permittivity sensor, Lightning, Electric field analysis. 1. Introduction cloud, which changes with the clouds changes [8]. So, there will be an existence of horizontal components of Monitoring of the atmosphere electric field is an the electric field other than the vertical component. -
High Performance Triboelectric Nanogenerator and Its Applications
HIGH PERFORMANCE TRIBOELECTRIC NANOGENERATOR AND ITS APPLICATIONS A Dissertation Presented to The Academic Faculty by Changsheng Wu In Partial Fulfillment of the Requirements for the Degree DOCTOR OF PHILOSOPHY in the SCHOOL OF MATERIALS SCIENCE AND ENGINEERING Georgia Institute of Technology AUGUST 2019 COPYRIGHT © 2019 BY CHANGSHENG WU HIGH PERFORMANCE TRIBOELECTRIC NANOGENERATOR AND ITS APPLICATIONS Approved by: Dr. Zhong Lin Wang, Advisor Dr. C. P. Wong School of Materials Science and School of Materials Science and Engineering Engineering Georgia Institute of Technology Georgia Institute of Technology Dr. Meilin Liu Dr. Younan Xia School of Materials Science and Department of Biomedical Engineering Engineering Georgia Institute of Technology Georgia Institute of Technology Dr. David L. McDowell School of Materials Science and Engineering Georgia Institute of Technology Date Approved: [April 25, 2019] To my family and friends ACKNOWLEDGEMENTS Firstly, I would like to express my sincere gratidue to my advisor Prof. Zhong Lin Wang for his continuous support and invaluable guidance in my research. As an exceptional researcher, he is my role model for his thorough knowledge in physics and nanotechnology, indefatigable diligence, and overwhelming passion for scientific innovation. It is my great fortune and honor in having him as my advisor and learning from him in the past four years. I would also like to thank the rest of my committee members, Prof. Liu, Prof. McDowell, Prof. Wong, and Prof. Xia for their insightful advice on my doctoral research and dissertation. My sincere thanks also go to my fellow lab mates for their strong support and help. In particular, I would not be able to start my research so smoothly without the mentorship of Dr. -
Synthesis and Modelling of an Electrostatic Induction Motor Jean-Frédéric Charpentier, Yvan Lefèvre, Emmanuel Sarraute, Bernard Trannoy
Synthesis and modelling of an electrostatic induction motor Jean-Frédéric Charpentier, Yvan Lefèvre, Emmanuel Sarraute, Bernard Trannoy To cite this version: Jean-Frédéric Charpentier, Yvan Lefèvre, Emmanuel Sarraute, Bernard Trannoy. Synthesis and mod- elling of an electrostatic induction motor. IEEE Transactions on Magnetics, Institute of Electrical and Electronics Engineers, 1995, vol. 31 (n° 3), pp. 1404-1407. 10.1109/20.376290. hal-01792424 HAL Id: hal-01792424 https://hal.archives-ouvertes.fr/hal-01792424 Submitted on 15 May 2018 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Open Archive TOULOUSE Archive Ouverte ( OATAO ) OATAO is an open access repository that collects the work of Toulouse researchers and makes it freely available over the web where possible. This is an author-deposited version published in: http://oatao.univ-toulouse.fr/ Eprints ID: 19944 To link to this article : DOI: 10.1109/20.376290 URL: http://dx.doi.org/10.1109/20.376290 To cite this version : Charpentier, Jean-Frédéric and Lefèvre, Yvan and Sarraute, Emmanuel and Trannoy, Bernard Synthesis and modelling of an electrostatic induction motor . (1995) IEEE Transactions on Magnetics, vol. 31 (n° 3). pp. -
Defects and Correction Theories of Electromagnetics
Applied Physics Research; Vol. 8, No. 4; 2016 ISSN 1916-9639 E-ISSN 1916-9647 Published by Canadian Center of Science and Education Defects and Correction Theories of Electromagnetics Kexin Yao1 1 Instiute of Mechanical Engineering of Shaanxi Province, Xian Metering Institution, Xian, P.R.China Correspondence: Kexin Yao, Instiute of Mechanical Engineering of Shaanxi Province, Xian Metering Institution, Xian, P.R.China. Tel: 86-134-8462-6424. E-mail: [email protected] Received: April 27, 2016 Accepted: May 15, 2016 Online Published: July 29, 2016 doi:10.5539/apr.v8n3p154 URL: http://dx.doi.org/10.5539/apr.v8n3p154 Abstract Experiments show that, there is the electrostatic field around the permanent magnet; since the electromagnetics can not explain this phenomenon, it can be concluded that there are some defects in electromagnetics. This paper makes an analysis of the defects of electromagnetics from fourteen aspects. It is noted that, the basic defect of electromagnetics is that there is no explanation of any inherent causes and physical processes of electromagnetic induction, displacement current, Lorentz force and other surface phenomena. Moreover, it may also lead us to make incorrect inferences in the theoretical analysis of electromagnetics, e.g. the same direction of action and reaction, infinitely high kinematic velocity of magnetic field, etc. It can be seen from analysis of all electromagnetic phenomena that, all the electromagnetic phenomena will be inevitably accompanied by an electron motion; and the electron motion is bound to take effect through an electric field; therefore, the analysis of motion in an electric field is the basis for analysis of all electromagnetic phenomena. -
A Vacuum Electrostatic Generator
1465 A VACUUM ELECTROSTATIC GENERATOR B.H. Choi, H.D. Kang, W. Kim, B.H. Oh, Korea Advanced Energy Research Institute Daeduk-Danji, Choongnam, 301-353, Korea and K.H. Chung Seoul National University Shinrim-Dong, Kwanak-Ku, Seoul, 151-741, Korea Abstract insulator supports the breakdown strength is limited to about 30 kV/cm due to the flashover phenomena on A compact electrostatic generator designed with the insulator surface. the principle of vacuum insulation has been developed. The concept of vacuum insulation instead of gas It consists of a rotating insulation disk with charge- insulation for the electrostatic generator design has carrying conductors placed around the circumference some advantages, such as the capability to hold the n n ti a non-contact induction system with R” electron high voltage in narrow inductor gap, elimination cf gun. The usable voltage of 130 kV with the generating the electrical cant acr problem by utilizing the current of about 300 pA has been obtained at the oper- non-contact induction method, posstbility of fice ational pressure of 1x10-’ torr. regulation of high voltage, and reduction cf frictional wind loss and the mechanical vibration. In Introduction addition, elimination of gas handling system may enhance the compactness and the flexibilities for the The recent progress of research and industrial accelerator system. The characteristics and the applications of ion beams require very stable beams operational performance of this vacuum electrostatic with the high energy of around 1 MeV and the current generator have been described in this paper. of a few mA. A candidate of high voltage sources to produce Experimental Apparatus mono-energetic beams is electrostatic generator, which has superior features such as small voltage ripple and The schematic drawins of the vacuum electrostatic small stored energy in the state of ultra high generator is shown in Fig. -
Basic Electrostatics System Model No
Instruction Manual Manual No. 012-07227E *012-07227* Basic Electrostatics System Model No. ES-9080 Basic Electrostatics System Model No. ES-9080 Table of Contents Equipment List........................................................... 3 Introduction .......................................................... 4-5 Equipment Description .............................................. 5-11 Electrometer...................................................................................................................................5 Electrostatics Voltage Source ........................................................................................................6 Variable Capacitor .........................................................................................................................7 Charge Producers and Proof Plane............................................................................................. 7-8 Proof Plane................................................................................................................................. 8-9 Faraday Ice Pail............................................................................................................................10 Conductive Spheres......................................................................................................................11 Resistor-Capacitor Network Accessory.......................................................................................11 Electrometer Operation and Setup Requirements................12-13 -
01. Franklin Intro 9/04
Franklin and Electrostatics- Ben Franklin as my Lab Partner A Workshop on Franklin’s Experiments in Electrostatics Developed at the Wright Center for Innovative Science Teaching Tufts University Medford MA 02155 by Robert A. Morse, Ph.D. ©2004 Sept 2004 Benjamin Franklin observing his lightning alarm. Described in Section VII. Engraving after the painting by Mason Chamberlin, R. A. Reproduced from Bigelow, 1904 Vol. VII Franklin and Electrostatics version 1.3 ©2004 Robert A. Morse Wright Center for Science Teaching, Tufts University Section I- page 1 Copyright and reproduction Copyright 2004 by Robert A. Morse, Wright Center for Science Education, Tufts University, Medford, MA. Quotes from Franklin and others are in the public domain, as are images labeled public domain. These materials may be reproduced freely for educational and individual use and extracts may be used with acknowledgement and a copy of this notice.These materials may not be reproduced for commercial use or otherwise sold without permission from the copyright holder. The materials are available on the Wright Center website at www.tufts.edu/as/wright_center/ Acknowledgements Rodney LaBrecque, then at Milton Academy, wrote a set of laboratory activities on Benjamin Franklin’s experiments, which was published as an appendix to my 1992 book, Teaching about Electrostatics, and I thank him for directing my attention to Franklin’s writing and the possibility of using his experiments in teaching. I would like to thank the Fondation H. Dudley Wright and the Wright Center for Innovative Science Teaching at Tufts University for the fellowship support and facilities that made this work possible. -
FLAP Modules Where They Are Discussed More Fully
ELECTRIC CHARGE, FIELD AND POTENTIAL MODULE P3.3 F PAGE P3.3.1 Module P3.3 Electric charge, field and potential 1 Opening items 1 Ready to study? 2 Electric charge 2 2.1 A brief history of electric charge 2 Study comment In order to study this module you will need to be familiar with the following 2.2 Charging by contact and by terms: atom, Cartesian coordinates, displacement, force, kinetic energy, nucleus, potential induction 3 energy, work and be able to apply the principle of conservation of energy. Vectors are used 2.3 Coulomb’s law and electrostatic extensively in this module: you must be familiar with the use of components and with the forces 4 procedure for adding vectors (vector addition) and multiplying them by scalars (scaling). It 3 Electric fields 6 would also be useful (though not essential) to have met the notions of scalar product before. 3.1 Electric field: definition and You should also be familiar with the basic ideas of calculus, including the use of derivatives representation 6 to represent gradients of graphs, and (definite) integrals to represent certain sums. However, you will not be required to evaluate integrals for yourself, so you do not need to be familiar 3.2 The field of an electric dipole 8 with the techniques for doing so. Several of these terms are reviewed briefly in the course of 3.3 The van der Waals force 9 this module but unless you are already fairly familiar with them you should consult the 4 Electric potential and electric FLAP modules where they are discussed more fully. -
Electrostatics Lab Introductory Physics Lab Summer 2018
Washington University in St. Louis Electrostatics Lab Introductory Physics Lab Summer 2018 Electrostatics: The Shocking Truth STOP Important health warning for students with pacemakers or other electronic medical devices: This lab involves the use of a Van de Graaff generator, which produces small amounts of electrical charge. They are regularly used in elementary schools, high schools, colleges, and science centers. They pose no risk to health or safety, except to students with pacemakers or other electronic medical devices. If you use a pacemaker or other electronic medical device, please contact the Lab Manager, Merita Haxhia at [email protected], IMMEDIATELY to make other arrangements for lab. It is very unlikely that you will be affected, but safety is our top priority. As long as you do not have this type of medical device, you have absolutely nothing to worry about. However, it is not recommended that you bring sensitive electronic equipment to this experiment. Pre-Lab: The Van de Graaff Generator A Bit of History The Van de Graaff generator is an electrostatic generator, capable of producing constant electric potential differences reaching about 10 million volts. The model that you will use (thankfully) only achieves about 1% of that. The term Van de Graaff electrostatic generator may sound a little foreign, but there is one electrostatic generator that you are no doubt familiar with: earth’s atmosphere. In fact, some of the most famous experiments in the history of electrostatics were done using the atmosphere. In May of 1752, Benjamin Franklin performed his well-known kite experiment, an experiment which strongly suggested that lightning might not be so different from the sparks he produced using silk and glass. -
Electrowetting Using a Microfluidic Kelvin Water Dropper
micromachines Article Electrowetting Using a Microfluidic Kelvin Water Dropper Elias Yazdanshenas 1, Qiang Tang 1,2 and Xiaoyu Zhang 1,* 1 Department of Mechanical & Aerospace Engineering, Old Dominion University, Norfolk, VA 23529, USA; [email protected] (E.Y.); [email protected] (Q.T.) 2 State Key Lab of Mechanics and Control of Mechanical Structures, Nanjing University of Aeronautics & Astronautics, Nanjing, Jiangsu 210016, China * Correspondence: [email protected]; Tel.: +1-757-683-4913 Received: 16 December 2017; Accepted: 22 February 2018; Published: 25 February 2018 Abstract: The Kelvin water dropper is an electrostatic generator that can generate high voltage electricity through water dripping. A conventional Kelvin water dropper converts the gravitational potential energy of water into electricity. Due to its low current output, Kelvin water droppers can only be used in limited cases that demand high voltage. In the present study, microfluidic Kelvin water droppers (MKWDs) were built in house to demonstrate a low-cost but accurately controlled miniature device for high voltage generation. The performance of the MKWDs was characterized using different channel diameters and flow rates. The best performed MKWD was then used to conduct experiments of the electrowetting of liquid on dielectric surfaces. Electrowetting is a process that has been widely used in manipulating the wetting properties of a surface using an external electric field. Usually electrowetting requires an expensive DC power supply that outputs high voltage. However, in this research, it was demonstrated that electrowetting can be conducted by simply using an MKWD. Additionally, an analytic model was developed to simulate the electrowetting process. Finally, the model’s ability to well predict the liquid deformation during electrowetting using MKWDs was validated. -
Phd and Mphil Thesis Classes
5 Electric field in dielectric media 5.1 Continuous media In previous sections we were studying electrostatic field of given charge configurations or electrostatic field around some ideal conductors. All electrons that belong to conduc- tivity bands in conductors possess mobility i.e. they can move inside whole conductor and dislocate on macroscopic distances. We shall call them free charges and denote by qf . There are no free charges in insulators. All their electric charges are bounded in- side atoms or molecules. Clearly, mobility of such charges is highly restricted. Bounded charges can move only inside molecules. Such materials cannot conduct electric current, however, they respond on applied external electric field by appearance of macroscopic dipole moment. Materials with these properties are called dielectrics. Dielectrics are electrically neutral materials, however, occasionally they can contain immersed electric charges. A fundamental property of dielectrics is theirs macroscopic polarity. It leads to ap- pearance of macroscopic dipole moment in response on applied external electric field. Macroscopic polarity has origin in polarization of molecules or atoms due to interac- tion of their charges with electric field. In presence of electric field electric clouds in atoms deform, what breaks the symmetry of charge configurations and results in in- duced electric dipole moment p, see Fig.5.1. In such a case, a dipole electric moment is induced on microscopic and macroscopic level. Another group of dielectrics are polar dielectrics. In such materials there exist microscopic electric dipole moment associated which each molecule (also without external electric field). Such moments do not lead to a macroscopic electric dipole moment because they cancel out for macroscopic num- ber of molecules. -
Experiment Using Electrostatic Motor
Experiment Using Electrostatic Motor 1. Learning Outcome In this sub-unit, we will perform experiment related to the attractive and repulsive forces of static electricity (Coulomb force) using the Electrostatic Motor (Franklin Motor) and Static Genecon. As the typical principle of static electricity, we will confirm the phenomena of electrostatic induction, attractive and repulsive forces. Let’s start our experiment for the sake of analyzing this phenomenon. 2. Historical Background In this sub-unit, we use an Electrostatic Motor, namely Franklin Motor, which was first invented by Benjamin Franklin and Andrew Gordon between 1740s and 1750s. Electrostatic Motor is based on the principles of electrostatic induction, attractive and repulsive force. Electrostatic Motor feature is operation with high voltage and low current. On the contrary, other types of (normal) motors can be operated with low voltage and large current, because their principle is electromagnetic induction. 3. Electrostatic Generator: “Static Genecon” We already know that if we rub piece of plastic with felt or different kind of cloth then static electricity will be generated. And we have in various ways confirmed properties of above mentioned way of generating static electricity. As a result, we have learned among other things as well, that electrostatic charge has two kinds. Furthermore, we can store static electricity because of the invention of Leyden jar and Electrophorus. By using them we can store greater 1 © Narika Corporation 2020 amount of static electricity, thus conducting experiments with large amount of static electricity. Because of that invention research about static electricity accelerated in the past. In 1929, Robert J.