Design of a Wireless Power Transfer System Using Inductive Coupling and MATLAB Programming Apoorva.P1 Deeksha.K.S2 Pavithra.N3 Student, Dept

Total Page:16

File Type:pdf, Size:1020Kb

Design of a Wireless Power Transfer System Using Inductive Coupling and MATLAB Programming Apoorva.P1 Deeksha.K.S2 Pavithra.N3 Student, Dept International Journal on Recent and Innovation Trends in Computing and Communication ISSN: 2321-8169 Volume: 3 Issue: 6 3817 - 3825 _______________________________________________________________________________________________ Design of a Wireless Power Transfer System using Inductive Coupling and MATLAB programming Apoorva.P1 Deeksha.K.S2 Pavithra.N3 Student, Dept. Of EEE, Student, Dept. Of EEE Student, Dept. Of EEE, Dr. T. Thimmaiah Institute of Dr. T. Thimmaiah Institute of Dr. T. Thimmaiah Institute of Technology Technology Technology K.G.F,India K.G.F, India K.G.F, India [email protected] [email protected] [email protected] Vijayalakshmi.M.N4 Somashekar.B5 David Livingston.D6 Student, Dept. Of EEE Asst Professor Dept. Of EEE, Asst Professor Dept. Of EEE, Dr. T. Thimmaiah Institute of Dr. T. Thimmaiah Institute of Dr. T. Thimmaiah Institute of Technology Technology Technology K.G.F, India K.G.F, India K.G.F, India [email protected] [email protected] [email protected] Abstract—Wireless power transfer (WPT) is the propagation of electrical energy from a power source to an electrical load without the use of interconnecting wires. It is becoming very popular in recent applications. Wireless transmission is useful in cases where interconnecting wires are difficult, hazardous, or non-existent. Wireless power transfer is becoming popular for induction heating, charging of consumer electronics (electric toothbrush, charger), biomedical implants, radio frequency identification (RFID), contact-less smart cards, and even for transmission of electrical energy from space to earth. In the design of the coils, the parameters of coils are obtained by using the basic calculations and measurements. The experimental results are presented and verified by using the MATLAB programming for the input and output wave forms. Keywords—Wireless power transfer, Electromagnetic Induction, MATLAB. __________________________________________________*****_________________________________________________ I. INTRODUCTION The goal of the present research is to develop a method of a) Size: The size of the transmitter or the receiver sometimes wireless power transmission. The idea of wireless power becomes too large to implement in a smaller system devices. transfer originated from the inconvenience of having too Thus by creating a wireless power transfer system, it would many wires sharing a limited amount of power sockets. We help clean up the clutter of wires around power sockets believe that many people have the same experience of making the space more tidy and lacking enough sockets for their electronic organized. b) Range: The range of wireless energy transfer is just a few Wireless power transfer can be divided into two major types meters, which represents a major hurdle towards its practical – electromagnetic induction and electromagnetic radiation. implementation. Electromagnetic induction can be of three type’s electrodynamics, electrostatic and evanescent wave c) Efficiency: Typical efficiency of wireless energy transfer coupling. Electromagnetic radiation can be divided into two ranges between 45% and 80% and is less efficient than categories – microwave power transfer (MPT) and laser. conventional wire based energy transfer methods. In our experiment we have considered electrodynamic or Electromagnetic Induction: It is the production of an inductive coupling. An inductive link is formed by a loosely induced voltage in a circuit which is excited by means of the coupled transformer consisting of a pair of coils that are magnetic flux. The condition for an induced current to flow usually placed in a coaxial arrangement .The external or the in a closed circuit is that the conductors and the magnetic primary coil is excited by an alternating current, and thus an field must rotate relative to each other electromagnetic field is produced with its magnitude Electromagnetic Radiation: Electromagnetic radiation dependent on the dimensions of the coil, the drive current travels through vacuum at the speed of light and propagates and the frequency of operation. A portion of the alternating by the interaction of time varying electric and magnetic flux lines generated this way link to the internal or the fields. It has a wavelength and a frequency. secondary coil, and the change in flux linkage produces a There are a number of limitations to the full implementation voltage in the secondary coil, which is proportional to the of wireless energy transfer: rate of change of the flux and the number of turns in the 3817 IJRITCC | June 2015, Available @ http://www.ijritcc.org _______________________________________________________________________________________ International Journal on Recent and Innovation Trends in Computing and Communication ISSN: 2321-8169 Volume: 3 Issue: 6 3817 - 3825 _______________________________________________________________________________________________ secondary coil (Faraday’s law of electromagnetic induction). converter or step-up converter) is a DC-DC power converter If the number of turns is n and the magnetic flux linking with an output voltage greater than its input voltage. It is a each turn is ψm, then the induced voltage for the circuit can switched-mode power supply (SMPS) containing one be written as, v=n (d ψm/dt). semiconductor (a transistor) and at least one energy storage element, a capacitor, inductor, or the two in combination. Hardware design for different turns in the receiver Booster circuit also power devices at small scale and transmitter coil is shown and the MATLAB applications, such as portable lighting systems. A LED programming is written for the input and output, finally the typically requires 3.3V to emit light. The transmitter coil comparative graph is plotted and checked for input and made up of copper turns of American Wire Gauge (AWG) output of hardware and programming. of 18 is used to transmit power wirelessly to the receiver coil. The receiver coil is also made up of same wire gauge as transmitter coil. The magnetic field generated by the II. BLOCK DIAGRAM transmitter coil couples with the receiver coil, exciting the coil and causing energy to build up in it. This energy is coupled out of the receiver coil to do useful work, for example, directly powering a load. The LED is used as a load. Filters made of capacitor (sometimes in combination with inductors) is used to the output to reduce output voltage ripple. The transmitter coil and receiver coil is constructed Fig.i Block Diagram of a Wireless power transfer system with 4.5cm radius and we have constructed both coils with 8 A. Source: The supply given here is 5V(DC). turns. B. Booster circuit: A booster circuit is a DC-DC power SPECIFICATIONS converter with an output voltage greater than its input TRANSMITTERCOIL SIDE voltage. It is of switched-mode power supply (SMPS) containing one semiconductor (a transistor), at least one Inputvoltage=5Volts energy storage element, a capacitor, an inductor, or the BD139Transistor two in combination. R = 1.5KΩ C =470pF C. Transmitter coil: The transmitter coil is the one which 1 C =4.7nF transmits power wirelessly to the receiver coil. 2 C3=100nF D. Receiver coil: The receiver coil is the one which receives Turns = 8 power from the transmitter coil. The receiver coil consists of filter circuit. RECEIVER COILSIDE E. Load: The load is an LED. D1 (IN4148) III. EXPERIMENT C4 = 4.7nF Turns = 5,8,10,15 Model picture for 8 turns (single load) Fig.ii Circuit Diagram of a Wireless Power Transfer System The fig. ii shows the circuit diagram of a wireless power Fig.iii Model picture of a Wireless Power Transfer transfer system. The input power to the system is DC supply System for single load of 5V is given. The booster circuit is also known as (boost 3818 IJRITCC | June 2015, Available @ http://www.ijritcc.org _______________________________________________________________________________________ International Journal on Recent and Innovation Trends in Computing and Communication ISSN: 2321-8169 Volume: 3 Issue: 6 3817 - 3825 _______________________________________________________________________________________________ IV Experimental Results Table 1.2: Receiver Coil of (5,8, 10, 15 turns) Table 1.1: Receiver Coil with 8 turns Experimental graph Experimental graph IV MATLAB PROGRAMMING MATLAB is a high-performance language for Model picture for multiple load technical computing. It integrates computation, visualization, and programming in an easy-to-use environment where problems and solutions are expressed in familiar mathematical notation. Typical uses include Math and computation Algorithm development Data acquisition Modeling, simulation, and prototyping Data analysis, exploration, and visualization Scientific and engineering graphics Application development, including graphical user interface building. MATLAB is an interactive system whose basic data element is an array that does not require dimensioning. This allows you to solve many technical computing problems, especially those with matrix and vector formulations, in a fraction of the time it would take to write a program in a scalar no interactive language such as C or Fig FORTRAN. The name MATLAB stands for matrix .iv Model picture of a Wireless Power Transfer System laboratory. MATLAB was originally written to provide easy for multiple load access to matrix software developed by the LINPAC and eispack projects. 3819 IJRITCC | June 2015, Available @ http://www.ijritcc.org _______________________________________________________________________________________
Recommended publications
  • Optimal Design of High-Frequency Induction Heating Apparatus for Wafer Cleaning Equipment Using Superheated Steam
    energies Article Optimal Design of High-Frequency Induction Heating Apparatus for Wafer Cleaning Equipment Using Superheated Steam Sang Min Park 1 , Eunsu Jang 2, Joon Sung Park 1 , Jin-Hong Kim 1, Jun-Hyuk Choi 1 and Byoung Kuk Lee 2,* 1 Intelligent Mechatronics Research Center, Korea Electronics Technology Institute (KETI), Bucheon 14502, Korea; [email protected] (S.M.P.); [email protected] (J.S.P.); [email protected] (J.-H.K.); [email protected] (J.-H.C.) 2 Department of Electrical and Computer Engineering, Sungkyunkwan University (SKKU), Suwon 16419, Korea; [email protected] * Correspondence: [email protected]; Tel.: +82-31-299-4581 Received: 19 October 2020; Accepted: 22 November 2020; Published: 25 November 2020 Abstract: In this study, wafer cleaning equipment was designed and fabricated using the induction heating (IH) method and a short-time superheated steam (SHS) generation process. To prevent problems arising from the presence of particulate matter in the fluid flow region, pure grade 2 titanium (Ti) R50400 was used in the wafer cleaning equipment for heating objects via induction. The Ti load was designed and manufactured with a specific shape, along with the resonant network, to efficiently generate high-temperature steam by increasing the residence time of the fluid in the heating object. The IH performance of various shapes of heating objects made of Ti was analyzed and the results were compared. In addition, the heat capacity required to generate SHS was mathematically calculated and analyzed. The SHS heating performance was verified by conducting experiments using the designed 2.2 kW wafer cleaning equipment.
    [Show full text]
  • Induction Heating Principles PRESENTATION
    Induction Heating Principles PRESENTATION www.ceia-power.com This document is property of CEIA which reserves all rights. Total or partial copying, modification and translation is forbidden FC040K0068V1000UK Main Applications of Induction Heating ¾ Hard (Silver) Brazing ¾ Tin Soldering ¾ Heat Treatment (Hardening, Annealing, Tempering, …) ¾ Melting Applications (ferrous and non ferrous metal) ¾ Forging This document is property of CEIA which reserves all rights. Total or partial copying, modification and translation is forbidden FC040K0068V1000UK Examples of induction heating applications This document is property of CEIA which reserves all rights. Total or partial copying, modification and translation is forbidden FC040K0068V1000UK Advantages of Induction Reduced Heating Time Localized Heating Efficient Energy Consumption Heating Process Controllable and Repeatable Improved Product Quality Safety for User Improving of the working condition This document is property of CEIA which reserves all rights. Total or partial copying, modification and translation is forbidden FC040K0068V1000UK Basics of Induction INDUCTIVE HEATING is based on the supply of energy by means of electromagnetic induction. A coil, suitably dimensioned, placed close to the metal parts to be heated, conducting high or medium frequency alternated current, induces on the work piece currents (eddy currents) whose intensity can be controlled and modulated. This document is property of CEIA which reserves all rights. Total or partial copying, modification and translation is forbidden FC040K0068V1000UK Basics of induction The heating occurs without physical contact, it involves only the metal parts to be treated and it is characterized by a high efficiency transfer without loss of heat. The depth of penetration of the generated currents is directly correlated to the working frequency of the generator used; higher it is, much more the induced currents concentrate on the surface.
    [Show full text]
  • Magnetic Flux Controllers in Induction Heating and Melting
    ASM Handbook, Volume 4C, Induction Heating and Heat Treatment Copyright # 2014 ASM InternationalW V. Rudnev and G.E. Totten, editors All rights reserved www.asminternational.org Magnetic Flux Controllers in Induction Heating and Melting Robert Goldstein, Fluxtrol, Inc. MAGNETIC FLUX CONTROLLERS are workpiece. For both cases, there are three closed is applied, it strongly reduces the reluctance of materials other than the copper coil that are used loops: flow of current in the coil, flow of mag- the back path for the magnetic flux (Ref 3). All in induction systems to alter the flow of the mag- netic flux, and flow of current in the workpiece. induction heating systems can be described in netic field. Magnetic flux controllers used in In most cases, the difference between induc- this way. power supplying components are not considered tion heating applications and transformers is that The benefits of a magnetic flux concentrator in this article. the magnetic circuit is open. The magnetic field on the electrical parameters for a given applica- Magnetic flux controllers have been in exis- path includes not only the area with the control- tion depends on the ratio of the reluctance of tence since the development of the induction ler, but also the workpiece surface layer and the the back path for magnetic flux to the overall technique. Michael Faraday used two coils of air between the surface and controller, which reluctance in the system. It is also possible to wire wrapped around an iron core in his experi- cannot be changed. Therefore, the reluctance of break down basic system components into sub- ments that led to Faraday’s law of electromagnetic the magnetic path only partially depends on the components to determine the most economical induction, which states that the electromotive magnetic permeability of the controller (Ref 3).
    [Show full text]
  • Handbook of Induction Heating Theoretical Background
    This article was downloaded by: 10.3.98.104 On: 28 Sep 2021 Access details: subscription number Publisher: CRC Press Informa Ltd Registered in England and Wales Registered Number: 1072954 Registered office: 5 Howick Place, London SW1P 1WG, UK Handbook of Induction Heating Valery Rudnev, Don Loveless, Raymond L. Cook Theoretical Background Publication details https://www.routledgehandbooks.com/doi/10.1201/9781315117485-3 Valery Rudnev, Don Loveless, Raymond L. Cook Published online on: 11 Jul 2017 How to cite :- Valery Rudnev, Don Loveless, Raymond L. Cook. 11 Jul 2017, Theoretical Background from: Handbook of Induction Heating CRC Press Accessed on: 28 Sep 2021 https://www.routledgehandbooks.com/doi/10.1201/9781315117485-3 PLEASE SCROLL DOWN FOR DOCUMENT Full terms and conditions of use: https://www.routledgehandbooks.com/legal-notices/terms This Document PDF may be used for research, teaching and private study purposes. Any substantial or systematic reproductions, re-distribution, re-selling, loan or sub-licensing, systematic supply or distribution in any form to anyone is expressly forbidden. The publisher does not give any warranty express or implied or make any representation that the contents will be complete or accurate or up to date. The publisher shall not be liable for an loss, actions, claims, proceedings, demand or costs or damages whatsoever or howsoever caused arising directly or indirectly in connection with or arising out of the use of this material. 3 Theoretical Background Induction heating (IH) is a multiphysical phenomenon comprising a complex interac- tion of electromagnetic, heat transfer, metallurgical phenomena, and circuit analysis that are tightly interrelated and highly nonlinear because the physical properties of materi- als depend on magnetic field intensity, temperature, and microstructure.
    [Show full text]
  • Induction Heating: Fundamentals
    30/10/17 LEP ELECTROMAGNETIC PROCESSING OF MATERIALS TECNOLGIE DEI PROCESSI ELETTROTERMICI Induction Heating: fundamentals Fabrizio Dughiero 2017-2018 Induction heating fundamentals May 28-30, 2014 1 30/10/17 Summary 1. Induction heating physical principles 2. Characteristics of the induction heating process • Physical parameters that affect induction heating 3. The skin effect: • What parameters modify the skin effect? • Change of skin effect during the heating 4. Examples: • Heating of a magnetic billet • Choosing the frequency appropriate to the workpiece • Coil thickness as a function of frequency 5. Proximity effect, ring effect, flux concentrators effect 1. Induction heating physical principles May 28-30, 2014 2 30/10/17 Induction heating physical principles Characteristics of induction heating • High temperature in the workpiece (in most cases). • High power density for a short heating time (in many applications). • High frequency (in many applications). • Thermal sources are inside the workpiece. Induction heating physical principles Induction heating: fundamental laws ? They state: A. Maxwell’s equations • how the electromagnetic (e.m.) field is generated rd 3 Maxwell’s equation or • how the e.m. field propagates and is Faraday-Neumann-Lenz’s law distributed in the space 4th Maxwell’s equation or • how the e.m. field interacts with the Ampere’s law charged particles. • they state what is the (approximate) B. Constitutive relations response of a specific material to an for materials external field or force. ? Ohm’s law Magnetic
    [Show full text]
  • Induction Heat Treatment
    a ...... ...... ....... ..... ...... .... ... ..... ...... .... ... ..... ...... ....... ..... ...... ....,...... ..... ...... .... ... ..... ...... ....... ..... ...... ....... ..... ...... .... ... ....I ...... ....... ..... ...... ....... ..... ...... ....... ..... ...... ....... ..... ...... .... ... ..... ...... .... ... ...... .... ... ...... .... ... ...... ....... ...... .... ... ...... ,....... ... ...... .... ... .....I .... .... ..... ... ... .....(... ....... ... ..... ... ........ ... ... ..... ...... i iG -i Publishedby the EPRl Center for MaterialsFabrication Vol. 2, No. 2, 1985Reprinted March, 1990 Using Induction Heat speed and selective heating capabil- Vol. 2, No. 1. Advantages specific to Treatment to Obtain ity, to produce quality parts cost induction heat treating are: Special Properties effectively. It will answer such ques- Speed - In heat treatment, the Cost Effectively tions as: What are the advantages higher heating rates play a central of induction heat treatment? What role in designing rapid, high- Heat treatment is often one of the heat treatments can I conduct with temperature heat treating most important stages of metal induction? What are some typical processes. Induction heat treating of processing because it determines parts and materials that are induc- steel may take as little as the final properties that enable tion heat treated? What properties 10 percent or less of the time cqmponents to perform under such can I obtain with induction heat required for furnace treatment. demanding service conditions
    [Show full text]
  • Induction Heating Work Coils
    Induction Heating Work Coils The work coil, also known as the inductor, is the component in the induction heating system that defines how effective and how efficiently the work piece is heated. Work coils range in complexity from a simple helical (or solenoid) wound coil consisting of a number of turns of copper tube wound around a mandrel to a coil precision machined from solid copper and brazed together. The work coil is used to transfer the energy from the induction heating power supply and workhead to the work piece by generating an alternating electromagnetic field. The electromagnetic field generates a current that flows in the work piece as a mirror image to the current flowing in the work coil. As the current flows through the resistivity of the work piece it generates the heat within the work piece from I²R losses. A second heating principle, hysteretic heating is also in effect when the work piece is a magnetic material such as carbon steel. Energy is generated within the work piece by the alternating magnetic field changing the magnetic polarity within the work piece. Hysteretic heating occurs in the work piece only up to the Curie temperature (750° C for steel) when the material’s magnetic permeability decreases to 1. Work Coil Basics A current flowing in a conductor creates a magnetic field. An alternating current creates an alternating field which produces an alternating current in a second conductor (the work piece). The current in the work piece is proportional to the field strength. The transformer effect where the amount of current induced in the work piece is proportional to the number of turns on the coil and is generated as a mirror image of the work coil.
    [Show full text]
  • Introduction
    Elements of Induction Heating Copyright © 1988 ASM International® Stanley Zinn, Lee Semiatin, p 1-8 All rights reserved. DOI: 10.1361/eoih1988p001 www.asminternational.org Chapter 1 Introduction Electromagnetic induction, or simply "induction," is a method of heating electrically conductive materials such as metals. It is commonly used in process heating prior to metalworking, and in heat treating, welding, and melting (Table 1.1). This technique also lends itself to various other applications involving packaging and curing. The number of industrial and consumer items which undergo induction heating during some stage of their production is very large and rapidly expanding. As its name implies, induction heating relies on electrical currents that are induced internally in the material to be heated-i.e., the workpiece. These Table 1,1. Induction heating applications and typical products Preheating prior to metalworking Heat treating Welding Melting Forging Surface Hardening, Seam Welding Air Melting of Steels Gears Tempering Oil-country Ingots Shafts Gears tubular Billets Hand tools Shafts products Castings Ordnance Valves Refrigeration Vacuum Induction Machine tools tubing Melting Extrusion Hand tools Line pipe Structural Ingots members Through Hardening, Billets Shafts Tempering Castings Structural "Clean" steels Heading members Nickel-base Bolts Spring steel superalloys Other fasteners Chain links Titanium alloys Rolling Slab Annealing Aluminum strip Sheet (can, ap- pliance, and Steel strip automotive industries) 2 Elements of Induction Heating: Design, Control, and Applications so-called eddy currents dissipate energy and bring about heating. The basic components of an induction heating system are an induction coil, an alter- nating-current (ac) power supply, and the workpiece itself.
    [Show full text]
  • Specifics of Induction Hardening of Powder Metallurgy (P/M) Components
    INDUCTION THOUGHTS INDUCTIONINDUCTION THOUGHTSTHOUGHTS Dr. Valery Rudnev, known as “Professor Induction”, discusses in the heat processing diffe- rent aspects of induction heating, novel theoretical and practical knowledge related to dif- ferent heat treating technologies accumulated in the North America and around the globe. Specifics of induction hardening of powder metallurgy (P/M) components uring the last decade, the use of advanced powder metallurgy type of heat treatment. However, differences in electromagnetic D(P/M) materials in several industries has been expanded at properties are specific for processing those materials applying an impressive pace further penetrating markets of demanding electromagnetic induction. Table 1 summarizes the effect of applications; however, the biggest market for ferrous P/M com- density reduction and porosity increase on IH. ponents remains to be the transportation industry, particularly The relative magnetic permeability μr of P/M materials is consid- the automotive and agricultural sectors. An ability to manufacture erably lower than the μr of the corresponding wrought steels, while net-shape complex geometries offering competitive performance their electrical resistivities ρ are greater to some extent. Both factors at an economical cost is an attractive feature of P/M parts (e. g. gears, lead to noticeably larger current penetration depth (δ) during the timing sprockets, cams, splined hubs, shafts, shock absorbers etc.) heating cycle, affecting not only heat generation and temperature [1]. Density and porosity in the sintered compact are major factors profiles but also the magnitude and distribution of transient and affecting strength and hardenability of ferrous P/M materials; both residual stresses as well as coil electrical parameters.
    [Show full text]
  • Induction Melt Thermoforming of Advanced Multi-Axial Thermoplastic Composite Laminates
    Journal of Manufacturing Processes 60 (2020) 673–683 Contents lists available at ScienceDirect Journal of Manufacturing Processes journal homepage: www.elsevier.com/locate/manpro Induction melt thermoforming of advanced multi-axial thermoplastic composite laminates P. Harrison a, I. Campbell a,*, E. Guliyev a, B. McLelland a, R. Gomes b, N. Curado-Correia b, E. McGookin a, D.M. Mulvihill a a James Watt School of Engineering, University of Glasgow, University Avenue, G12 8QQ, United Kingdom b INEGI, Composite Materials and Structures Research, Institute of Mechanical Engineering and Industrial Management, Porto 4200-465, Portugal ARTICLE INFO ABSTRACT Keywords: The viability of using induction heating to facilitate the wrinkle-free forming of multi-axial pre-consolidated Forming advanced thermoplastic composites over complex geometries is explored. The research focuses on the use of tin Thermoplastic resin as a medium to both heat and lubricate the forming laminate. Initial tests demonstrate the viability of the Carbon fibres fundamental ideas of the process; induction heating is used to melt the tin sheet, which is then shown to melt the Defects matrix phase of carbon-nylon composite laminates when stacked in a hybrid composite/tin layup. A novel low- cost reconfigurablemulti-step forming tool is used to demonstrate how most of the tin can be squeezed out of the layup prior to consolidation. The multi-step tool can be augmented with segmented tooling to rapidly manu­ facture composite parts of high geometric complexity. In this investigation, a ’ripple’ geometry containing three ’cavities’ is used to demonstrate the technique. Tests demonstrated that at least three sheets of inter-laminar tin can be simultaneously melted using the induction heating system.
    [Show full text]
  • Rigorous Electromagnetic Analysis of Domestic Induction Heating Appliances
    PIERS ONLINE, VOL. 5, NO. 5, 2009 491 Rigorous Electromagnetic Analysis of Domestic Induction Heating Appliances G. Cerri, S. A. Kovyryalov, V. Mariani Primiani, and P. Russo Universit`aPolitecnica Delle Marche | DIBET, Via Brecce Bianche, Ancona 60100, Italy Abstract| In this paper the developed analytical electromagnetic model of induction heating system is presented. The model was built up assuming equivalent electric and magnetic currents flowing in each planar element of the typical structure used for an induction heating system: the load disk represents the pan steel bottom, the copper inductor, and ferrite flux conveyor. A system of integral equations system was then obtained enforcing the boundary conditions on each element of the structure for the electric and magnetic ¯elds, produced by the equivalent currents. The numerical solution of the system is a matrix equation with a known voltage vector in the left-hand side, and product of impedance coe±cients matrix and unknown electric and magnetic currents vector in the right-hand side. Since the feeding voltage is known, and impedance coe±cients are calculated using of geometry and material parameters, currents vector can be also calculated. Thus, the whole model is solved and it gives a detailed picture of currents distribution in the system, which in its turn allows to analyze heating process in the load. Each step of developing of the model was veri¯ed by appropriate experimental measurements. Achieved results give a possibility to analyze and develop improvements to increase e±ciency, safety and to reduce the cost. 1. INTRODUCTION Domestic induction cookers become more and more popular because of their high e±ciency, safety and ease in use.
    [Show full text]
  • Losalamos NATIONAL LABORATORY
    LA-UR- 94-2627 T/h% (’)\● ZONE REFINING OF PLUTONIUM METAL Author(s); Michael S. Blau Submitted to: University of Idaho for the Partial Fulfillment of the Requirements for the Degree of Master of Science with a Major in Metallurgical Engineering in the College of Mines I and Earth Resources. ~- -— .—— .. .. --— LosAlamos NATIONAL LABORATORY LOSAlarnoaNationalLaboratory,an affirmativeadkxVequaloppornmifyarnpk%ar,ia operatedby the Uniwrsify of Caliiomia for tha U.S. Depanmenf of Energy undercommuW-740S-ENG-3S.Sy accuptsncaoffhiaartida. tha pubkher racqnizes thal the U.S. Oovammemrafains ● norKIxduo&o,royalfy-frea Iicenw to J .——_ L/ publishof faproducathe publishedformd thiscontribution,or to allowothersto do 00, for U.S. (iovemmanf w-. The LOOk ~~ ~ -~ti-ti~hk-MWPdwM Utitiwdti U.S. -roof E~y. FOm Noaa3R5 ST26201G91 ZONE REFINING OF PLUTONIUM METAL A THESIS Presented in Partial Fulfillment of the Requirements for the Degree of Master of Science with a Major in MetaUurgical Engineering in the College of Mines and Earth Resources University of Idaho by Michael S. Blau August 1994 Major Professors: Gene E. Bobeck and J. David Olivas AUTHORIZATION TO SUBMIT THESIS This thesis of Michael Steven Blau, submitted for the degree of Master of Science with a major in Metallurgical Engineering and titled “Zone Refining of Plutonium Metal,” has been reviewed in final form and approved, as indicated by the signatures and dates given below. Permission is now granted to submit final copies to the college of Graduate Studies for approval. First Major Professor Date Gene E. Bobeck Second Major Professor Date J. David Olivas Committee Members Date Sarit Bhaduri Date Dennis R.
    [Show full text]