Non-Propellant Eddy Current Brake and Traction in Space Using Magnetic Pulses
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Eddy Current Braking in Automobiles Sarath G Nath1, Rohith Babu2, George Varghese Biju3, Ashin S4 , Dr
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 05 Issue: 04 | Apr-2018 www.irjet.net p-ISSN: 2395-0072 Eddy Current Braking In Automobiles Sarath G Nath1, Rohith Babu2, George Varghese Biju3, Ashin S4 , Dr. Cibu K Varghese5 1,2,3,4B Tech student, Mechanical Engineering Department Mar Athanasius college of Engineering, Kerala 5Professor, Mechanical Engineering Department, Mar Athanasius College of Engineering, Kerala ---------------------------------------------------------------------***--------------------------------------------------------------------- Abstract - Eddy Current Braking slows a moving object by through a stationary magnetic field (Jou et al, 2006) [8]. The creating eddy currents through electromagnetic induction changing magnetic flux induces eddy currents in the which create resistance. In normal case if the speed of the conductor and these currents dissipate energy and generate vehicle is very high, the brake does not provide that amount of drag force (Jou et al, 2006) [8]. Therefore, there are no high braking force and it will leads to skidding and wear& tear contacting elements by using this electromagnetic braking of the vehicle. Because of this drawbacks of ordinary brakes, system which will lead to reduce the wear of brake pad. This arises a simple and effective mechanism of braking system situation will also reduce the wear debris pollution into our ‘The eddy current brake’. Eddy current is one of the most environment. outstanding of electromagnetic induction phenomena. Even though it appear many technical problems because dissipative 1.1 Conventional Braking System nature it has some valuable contributions. It is a frictionless method for braking of vehicles including trains. As it is a Braking forms an important part of motion of any frictionless brake, periodic change of braking components are automobile or locomotive. -
Modeling and Design Optimization of Electromechanical Brake Actuator Using Eddy Currents
Modeling and Design Optimization of Electromechanical Brake Actuator Using Eddy Currents by Kerem Karakoc MASc, University of Victoria, 2007 BSc, Bogazici University, 2005 A Dissertation Submitted in Partial Fulfillment of the Requirements for the Degree of DOCTOR OF PHILOSOPHY in the Department of Mechanical Engineering. Kerem Karakoc, 2012 University of Victoria All rights reserved. This dissertation may not be reproduced in whole or in part, by photocopy or other means, without the permission of the author. ii Modeling and Design Optimization of Electromechanical Brake Actuator Using Eddy Currents by Kerem Karakoc MASc, University of Victoria, 2007 BSc, Bogazici University, 2005 Supervisory Committee Dr. Afzal Suleman, Dept. of Mechanical Engineering, University of Victoria Co-Supervisor Dr. Edward Park, Dept. of Mechanical Engineering, University of Victoria Co-Supervisor Dr. Ned Djilali, Dept. of Mechanical Engineering, University of Victoria Departmental Member Dr. Issa Traore, Dept. of Electrical and Computer Engineering, University of Victoria Outside Member iii Supervisory Committee Dr. Afzal Suleman, Dept. of Mechanical Engineering, University of Victoria Co-Supervisor Dr. Edward Park, Dept. of Mechanical Engineering, University of Victoria Co-Supervisor Dr. Ned Djilali, Dept. of Mechanical Engineering, University of Victoria Departmental Member Dr. Issa Traore, Dept. of Electrical and Computer Engineering, University of Victoria Outside Member Abstract A novel electromechanical brake (EMB) based on the eddy current principle is proposed for application in electrical vehicles. The proposed solution is a feasible replacement for the current conventional hydraulic brake (CHB) systems. Unlike CHBs, eddy current brakes (ECBs) use eddy currents and their interaction with an externally applied magnetic field to generate braking torque. -
The Mathematical Modeling of Magnetostriction
THE MATHEMATICAL MODELING OF MAGNETOSTRICTION Katherine Shoemaker A Thesis Submitted to the Graduate College of Bowling Green State University in partial fulfillment of the requirements for the degree of MASTERS OF ART May 2018 Committee: So-Hsiang Chou, Advisor Kit Chan Tong Sun c 2018 Katherine Shoemaker All rights reserved iii ABSTRACT So-Hsiang Chou, Advisor In this thesis, we study a system of differential equations that are used to model the material deformation due to magnetostriction both theoretically and numerically. The ordinary differential system is a mathematical model for a much more complex physical system established in labo- ratories. We are able to clarify that the phenomenon of double frequency is more delicate than originally suspected from pure physical considerations. It is shown that except for special cases, genuine double frequency does not arise. In particular, simulation results using the lab data is consistent with the experiment. iv I dedicate this work to my family. Even if they don’t understand it, they understand so much more. v ACKNOWLEDGMENTS I would like to express my sincerest gratitude to my advisor Dr. Chou. He has truly inspired me and made my graduate experience worthwhile. His guidance, both intellectually and spiritually, helped me through all the time spent researching and writing this thesis. I could not have asked for a better advisor, or a better instructor and I am truly appreciative of all the support he gave. In addition, I would like to thank the remaining faculty on my thesis committee: Dr. Tong Sun and Dr. Kit Chan, for supporting me through their instruction and mentorship. -
Electromagnetic Induction, Ac Circuits, and Electrical Technologies 813
CHAPTER 23 | ELECTROMAGNETIC INDUCTION, AC CIRCUITS, AND ELECTRICAL TECHNOLOGIES 813 23 ELECTROMAGNETIC INDUCTION, AC CIRCUITS, AND ELECTRICAL TECHNOLOGIES Figure 23.1 This wind turbine in the Thames Estuary in the UK is an example of induction at work. Wind pushes the blades of the turbine, spinning a shaft attached to magnets. The magnets spin around a conductive coil, inducing an electric current in the coil, and eventually feeding the electrical grid. (credit: phault, Flickr) 814 CHAPTER 23 | ELECTROMAGNETIC INDUCTION, AC CIRCUITS, AND ELECTRICAL TECHNOLOGIES Learning Objectives 23.1. Induced Emf and Magnetic Flux • Calculate the flux of a uniform magnetic field through a loop of arbitrary orientation. • Describe methods to produce an electromotive force (emf) with a magnetic field or magnet and a loop of wire. 23.2. Faraday’s Law of Induction: Lenz’s Law • Calculate emf, current, and magnetic fields using Faraday’s Law. • Explain the physical results of Lenz’s Law 23.3. Motional Emf • Calculate emf, force, magnetic field, and work due to the motion of an object in a magnetic field. 23.4. Eddy Currents and Magnetic Damping • Explain the magnitude and direction of an induced eddy current, and the effect this will have on the object it is induced in. • Describe several applications of magnetic damping. 23.5. Electric Generators • Calculate the emf induced in a generator. • Calculate the peak emf which can be induced in a particular generator system. 23.6. Back Emf • Explain what back emf is and how it is induced. 23.7. Transformers • Explain how a transformer works. • Calculate voltage, current, and/or number of turns given the other quantities. -
Effective Eddy Current Braking at Low and High Vehicular Speeds – a Simulation Study
Archives of Current Research International 8(4): 1-11, 2017; Article no.ACRI.34042 ISSN: 2454-7077 Effective Eddy Current Braking at Low and High Vehicular Speeds – A Simulation Study Alumona Louis Olisaeloka 1* , Azaka Onyemazuwa Andrew 2 and Nwadike Emmauel Chinagorom 2 1Department of Electrical Engineering, Nnamdi Azikiwe University, Awka, Nigeria. 2Department of Mechanical Engineering, Nnamdi Azikiwe University, Awka, Nigeria. Author’s contributions This work was carried out in collaboration between all authors. Author ALO designed the study, performed the statistical analysis, wrote the protocol, and wrote the first draft of the manuscript. Authors AOA and NEC managed the analyses of the study. Author NEC managed the literature searches. All authors read and approved the final manuscript. Article Information DOI: 10.9734/ACRI/2017/34042 Editor(s): (1) Preecha Yupapin, Department of Physics, King Mongkut’s Institute of Technology Ladkrabang, Thailand. (2) M. A. Elbagermi, Chemistry Department, Misurata University, Libya. (3) Alexandre Gonçalves Pinheiro, Physics, Ceara State University, Brazil. Reviewers: (1) Meshack Hawi, Jomo Kenyatta University of Agriculture and Technology, Kenya. (2) Mohamed Zaher, University of Illinois at Chicago, USA. Complete Peer review History: http://www.sciencedomain.org/review-history/20351 Received 10 th May 2017 Accepted 16 th July 2017 Original Research Article th Published 4 August 2017 ABSTRACT Conventional eddy current braking is limited in effectiveness to only the high vehicular speed region. As the vehicle slows, the conventional eddy current brake loses effectiveness. This inherent drawback is due to the use of static/stationary magnetic field in the brake system. This study presents a solution - the use of rotating magnetic field in the brake system. -
Lecture 30 Motional Emf
LECTURE 30 MOTIONAL EMF Instructor: Kazumi Tolich Lecture 30 2 ¨ Reading chapter 23-3 & 23-4. ¤ Motional emf ¤ Mechanical work and electrical energy Clicker question: 1 3 Motional emf 4 ¨ As the rod moves to the right at a constant velocity v, the motional emf is given by ΔΦ BΔA lvΔt E = N = = B = Bvl Δt Δt Δt Example: 1 5 ¨ A Boeing KC-135A airplane has a wingspan of L = 39.9 m and flies at constant altitude in a northerly direction with a speed of v = 240 m/s. If the vertical component of the Earth’s magnetic -6 field is Bv = 5.0 × 10 T, and its -6 horizontal component is Bh = 1.4 × 10 T, what is the induced emf between the wing tips? Clicker question: 2 & 3 6 Mechanical and electric powers 7 ¨ Suppose the rod is moving with a constant velocity �. ¨ The mechanical power delivered by the external force is: ¨ Compare this to the electrical power in the light bulb: ¨ Therefore, mechanical power has been converted directly into electrical power. Example: 2 8 ¨ In the figure, let the magnetic field strength be B = 0.80 T, the rod speed be v = 10 m/s, the rod length be l = 0.20 m, and the resistance of the resistor be R = 2.0 Ω. (The resistance of the rod and rails are negligible.) a) Find the induced emf in the circuit. b) Find the induced current in the circuit (including direction). c) Find the force needed to move the rod with constant speed (assuming negligible friction). -
Learn Why Eddy-Current Sensors Are Now Replacing Inductive Sensors and Switches
AP Corp | (508) 351-6200 | www.a-pcorp.com Learn Why Eddy-Current Sensors Are Now Replacing Inductive Sensors and Switches Both eddy-current sensors as well as inductive switches and displacement sensors have been used for many years, each having their respective advantages when it comes to measuring position and displacement of objects in harsh environments. However, recent advances in eddy-current sensor design, integration and packaging, as well as overall cost reduction, have made these sensors a much more attractive option. This is especially true where high linearity, high-speed measurements and high resolution are critical requirements. Common Inductive Sensors & Switches To appreciate the inherent advantages of eddy-current sensors, relative to inductive switches and displacement sensors, it’s important to first understand the principle of operation of both types. The classic inductive displacement sensor comprises a coil that is wound around a ferromagnetic core. When excited by an alternating current from an oscillator-based driver circuit, the coil generates a magnetic field that is concentrated around the core. The lines of flux interact with the target conductor as it approaches, creating eddy currents that are the reverse of the initial excitation current and have the effect of reducing the voltage across the oscillator. These variations in voltage due to the change in air gap distance are detected and converted to an analog output signal, such as a 4-20mA loop, and then processed upstream to determine displacement. 1 AP Corp | (508) 351-6200 | www.a-pcorp.com In an inductive displacement sensor, a coil is wrapped around a ferromagnetic core and when an alternating current is passed through the coil it generates a magnetic field. -
Conceptualization of a New Product Development Framework for Eddy Current Braking Systems for Heavy Vehicles in Zimbabwe
Proceedings of the 2017 International Conference on Industrial Engineering and Operations Management (IEOM) Bristol, UK, July 24-25, 2017 Conceptualization of a New Product Development Framework for Eddy Current Braking Systems for Heavy Vehicles in Zimbabwe Wilson R. Nyemba Department of Mechanical Engineering Science, Faculty of Engineering and the Built Environment, University of Johannesburg, Auckland Park 2006, Johannesburg, South Africa [email protected] Chris Pote, Tauyanashe Chikuku Department of Mechanical Engineering, University of Zimbabwe, P O Box MP 167, Mount Pleasant, Harare, Zimbabwe [email protected], [email protected] Charles Mbohwa Professor of Sustainability Engineering, Department of Quality and Operations Management & Vice Dean for Research and Innovation, Faculty of Engineering and the Built Environment, University of Johannesburg, Auckland Park 2006, Johannesburg, South Africa [email protected] Abstract One of the most critical requirements for safety in vehicles is the availability of reliable braking systems. Most heavy vehicles in Zimbabwe employ the conventional hydraulic braking system. However changes and improvements in technology have seen the introduction of retarders that make use of magnets and eddy currents. The new technology is friction free but still deemed expensive and thus not yet readily acceptable to vehicle manufacturers for fears of reliability and cost. Hydraulic brakes are equally expensive in the long run owing to maintenance and frequent replacement of brake pads and rotors, particularly in Zimbabwe where the road infrastructure has deteriorated significantly over the years. A case study was carried out at a Zimbabwean company which specializes in the sales, service and backup of Scania heavy vehicles, with a special focus on the braking systems. -
Eddy Current Brake Eddy Current Brake (Order Code DTS-ECB) (Order Code DTS-ECB)
Eddy Current Brake Eddy Current Brake (Order Code DTS-ECB) (Order Code DTS-ECB) The Eddy Current Brake is a braking mechanism for use with our Dynamics Cart The Eddy Current Brake is a braking mechanism for use with our Dynamics Cart and Track System (order code DTS) carts and and Track System (order code DTS) carts and Go Direct® Sensor Cart (order code GDX-CART). Go Direct® Sensor Cart (order code GDX-CART). As the cart moves over the track, the magnets in the Eddy Current Brake create an As the cart moves over the track, the magnets in the Eddy Current Brake create an electromagnetic drag on the cart that is proportional to the cart’s speed. electromagnetic drag on the cart that is proportional to the cart’s speed. The Eddy Current Brake is not compatible with older metal carts that were part of The Eddy Current Brake is not compatible with older metal carts that were part of the discontinued Vernier Dynamics Systems (order code VDS) sold from 2005 to the discontinued Vernier Dynamics Systems (order code VDS) sold from 2005 to 2012. 2012. Assembly Assembly Insert the desired number of magnets into the Eddy Current Brake. Insert the desired number of magnets into the Eddy Current Brake. The Eddy Current Brake connectors swivel to allow 4 mm of height adjustment The Eddy Current Brake connectors swivel to allow 4 mm of height adjustment when installed in a cart. when installed in a cart. When the DTS stamp on the connector is upright, it is set at the correct height for When the DTS stamp on the connector is upright, it is set at the correct height for our DTS carts. -
Lecture 3: Static Magnetic Solvers
Lecture 3: Static Magnetic Solvers ANSYS Maxwell V16 Training Manual © 2013 ANSYS, Inc. May 21, 2013 1 Release 14.5 Content A. Magnetostatic Solver a. Selecting the Magnetostatic Solver b. Material Definition c. Boundary Conditions d. Excitations e. Parameters f. Analysis Setup g. Solution Process B. Eddy Current Solver a. Selecting the Eddy Current Solver b. Material Definition c. Boundary Conditions d. Excitations e. Parameters f. Analysis Setup g. Solution Process © 2013 ANSYS, Inc. May 21, 2013 2 Release 14.5 A. Magnetostatic Solver Magnetostatic Solver – In the Magnetostatic Solver, a static magnetic field is solved resulting from a DC current flowing through a coil or due to a permanent magnet – The Electric field inside the current carrying coil is completely decoupled from magnetic field – Losses are only due to Ohmic losses in current carrying conductors – The Magnetostatic solver utilizes an automatic adaptive mesh refinement technique to achieve an accurate and efficient mesh required to meet defined accuracy level (energy error). Magnetostatic Equations – Following two Maxwell’s equations are solved with Magnetostatic solver H J 1 Jz (x, y) ( Az (x, y)) B 0 0r B μ0( H M ) 0 r H 0 M p Maxwell 2D Maxwell 3D © 2013 ANSYS, Inc. May 21, 2013 3 Release 14.5 a. Selecting the Magnetostatic Problem Selecting the Magnetostatic Solver – By default, any newly created design will be set as a Magnetostatic problem – Specify the Magnetostatic Solver by selecting the menu item Maxwell 2D/3D Solution Type – In Solution type window, select Magnetic> Magnetostatic and press OK Maxwell 3D Maxwell 2D © 2013 ANSYS, Inc. -
3-D Eddy Current Torque Modeling
CMP-843 3-D Eddy Current Torque Modeling Subhra Paul, Walter Bomela and Jonathan Z. Bird Laboratory for Electromechanical Energy Conversion and Control University of North Carolina at Charlotte, NC 28223, USA This paper presents an analytic based eddy current torque analysis procedure. The equations are derived using the second order vector potential and the magnetic rotor is modeled using the magnetic charge sheet concept. The formulation enables the damping and stiffness equations to be derived. The equations are numerically computed and the accuracy is compared against experimental torque and power measurements. Index Terms— eddy currents, torque, Halbach rotor, maglev, second order vector potential. I. INTRODUCTION HEN a magnetic source moves in the vicinity of a Wconductive plate, time varying magnetic fields induce eddy currents in the plate which in turn interacts with the source magnetic field to create velocity dependent drag and lift force. The generated drag force can be utilized in applications such as eddy current braking [1] and rotor vibration damping [2]. While the lift force can be utilized to (a) (b) provide suspension for high-speed maglev trains [3]. Fig. 2 The (a) x-y and (b) z-y view of the problem region. Electrodynamic maglev suspension systems typically rely on a II. GOVERNING EQUATIONS null-flux coil guideway topology in order to maximize the lift- A schematic showing the relevant problem regions is to-drag ratio [4]. Another way to avoid this drag and achieve shown in Fig. 2. The rotor velocity in the x, y and z directions integrated suspension and propulsion for the vehicle at low as well as rotational speed, ω , is shown. -
The Electromagnetic Analysis and Design of a New Permanent Magnetic Eddy Current Damper
Proceedings of the International MultiConference of Engineers and Computer Scientists 2014 Vol II, IMECS 2014, March 12 - 14, 2014, Hong Kong The Electromagnetic Analysis and Design of a New Permanent Magnetic Eddy Current Damper XIE Hu, MA Shuyuan, LI Wenbin Abstract—The thesis suggests the design of a passive Depending on different primary excitation sources, the permanent magnetic eddy current damper. The damping force electromagnetic damper has three sub-types: electrical from the eddy currents which are generated by a conductor excitation magnetic damper, hybrid excitation plate cutting through magnetic lines of forces can help make a electromagnetic damper and permanent magnetic damper[2]. maglev positioning platform more stable. The formulas for Electrical excitation magnetic damper can regulate the calculating damping force are proposed by applying molecular braking force by adjusting the air gap magnetic flux density current methods. The feasibility of the design is proved by the amplitude. However, its braking force is lower in density finite element simulation of the proposed damper. and has more excitation magnetic loss. Hybrid excitation air gap magnetic field is under the effects of excitation winding Keywords—Maglev Positioning Platform, Permanent and permanent magnets, with the advantages of large air gap Magnetic Eddy Current Damper, Molecular Current, Finite magnetic amplitude, flexibility and high efficiency and the Element Analysis, Damping Coefficient disadvantages of complicated structure and large size. Permanent magnetic damper does not require extra I. INTRODUCTION power supply or excitation winding, so it is energy-saving, [3] hen a conductor moves in a magnetic field, it will be highly efficient and greater in braking density .