A Capacitor Modeling Method for Integrated Magnetic Components in DC/DC Converters Liang Yan, Member, IEEE, and Brad Lehman, Member, IEEE
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Chapter 1 Magnetic Circuits and Magnetic Materials
Chapter 1 Magnetic Circuits and Magnetic Materials The objective of this course is to study the devices used in the interconversion of electric and mechanical energy, with emphasis placed on electromagnetic rotating machinery. The transformer, although not an electromechanical-energy-conversion device, is an important component of the overall energy-conversion process. Practically all transformers and electric machinery use ferro-magnetic material for shaping and directing the magnetic fields that acts as the medium for transferring and converting energy. Permanent-magnet materials are also widely used. The ability to analyze and describe systems containing magnetic materials is essential for designing and understanding electromechanical-energy-conversion devices. The techniques of magnetic-circuit analysis, which represent algebraic approximations to exact field-theory solutions, are widely used in the study of electromechanical-energy-conversion devices. §1.1 Introduction to Magnetic Circuits Assume the frequencies and sizes involved are such that the displacement-current term in Maxwell’s equations, which accounts for magnetic fields being produced in space by time-varying electric fields and is associated with electromagnetic radiations, can be neglected. Z H : magnetic field intensity, amperes/m, A/m, A-turn/m, A-t/m Z B : magnetic flux density, webers/m2, Wb/m2, tesla (T) Z 1 Wb =108 lines (maxwells); 1 T =104 gauss Z From (1.1), we see that the source of H is the current density J . The line integral of the tangential component of the magnetic field intensity H around a closed contour C is equal to the total current passing through any surface S linking that contour. -
Design of Magnetic Circuits
Design of Magnetic Circuits Fundamental Equations Circuit laws similar to those of electric circuits apply in magnetic circuits as well. That is, a magnetic circuit can be replaced by an equivalent electric circuit for Ohm’s Law to be applied. If the magnetomotive force of a magnet is F and the total magnetic flux is Φt, and assuming the magnetic resistance (reluctance) of the circuit is R, then the following equation is valid. (1) Assuming the vacant length of the circuit as ℓg and the vacant cross-sectional area as ag, the magnetic resistance is then given by the following equation. (2) μ is the magnetic permeability of the magnetic path and is equivalent to the magnetic permeability μ0 of a vacuum in the case of air. (μ0=4π×10-7 [H/m]) Yoke 〈Figure 7〉 Although the current in an electric circuit rarely leaks outside the circuit, as the difference in the magnetic permeability between the conductor yoke and insulated area in a magnetic circuit is not very large, leakage of the magnetic flux also becomes large in reality. The amount of the magnetic flux leakage is expressed by the leakage factor σ, which is the ratio of the total magnetic flux Φt generated in the magnetic circuit to the effective magnetic flux Φg of the vacant space. (3) In addition, the loss in the magnetic flux due to the joints in the magnetic circuit must also be taken into consideration. This is represented by the reluctance factor f. Since the leakage factor σ is equivalent to the increase in the vacant space area, and the reluctance factor f refers to the correction coefficient of the vacant space length, the corrected magnetic resistance becomes as follows. -
The Stripline Circulator Theory and Practice
The Stripline Circulator Theory and Practice By J. HELSZAJN The Stripline Circulator The Stripline Circulator Theory and Practice By J. HELSZAJN Copyright # 2008 by John Wiley & Sons, Inc. All rights reserved Published by John Wiley & Sons, Inc. Published simultaneously in Canada No part of this publication may be reproduced, stored in a retrieval system, or transmitted in any form or by any means, electronic, mechanical, photocopying, recording, scanning, or otherwise, except as permitted under Section 107 or 108 of the 1976 United States Copyright Act, without either the prior written permission of the Publisher, or authorization through payment of the appropriate per-copy fee to the Copyright Clearance Center, Inc., 222 Rosewood Drive, Danvers, MA 01923, (978) 750-8400, fax (978) 750-4470, or on the web at www.copyright.com. Requests to the Publisher for permission should be addressed to the Permissions Department, John Wiley & Sons, Inc., 111 River Street, Hoboken, NJ 07030, (201) 748-6011, fax (201) 748-6008, or online at http:// www.wiley.com/go/permission. Limit of Liability/Disclaimer of Warranty: While the publisher and author have used their best efforts in preparing this book, they make no representations or warranties with respect to the accuracy or completeness of the contents of this book and specifically disclaim any implied warranties of merchantability or fitness for a particular purpose. No warranty may be created or extended by sales representatives or written sales materials. The advice and strategies contained herein may not be suitable for your situation. You should consult with a professional where appropriate. Neither the publisher nor author shall be liable for any loss of profit or any other commercial damages, including but not limited to special, incidental, consequential, or other damages. -
Transient Simulation of Magnetic Circuits Using the Permeance-Capacitance Analogy
Transient Simulation of Magnetic Circuits Using the Permeance-Capacitance Analogy Jost Allmeling Wolfgang Hammer John Schonberger¨ Plexim GmbH Plexim GmbH TridonicAtco Schweiz AG Technoparkstrasse 1 Technoparkstrasse 1 Obere Allmeind 2 8005 Zurich, Switzerland 8005 Zurich, Switzerland 8755 Ennenda, Switzerland Email: [email protected] Email: [email protected] Email: [email protected] Abstract—When modeling magnetic components, the R1 Lσ1 Lσ2 R2 permeance-capacitance analogy avoids the drawbacks of traditional equivalent circuits models. The magnetic circuit structure is easily derived from the core geometry, and the Ideal Transformer Lm Rfe energy relationship between electrical and magnetic domain N1:N2 is preserved. Non-linear core materials can be modeled with variable permeances, enabling the implementation of arbitrary saturation and hysteresis functions. Frequency-dependent losses can be realized with resistors in the magnetic circuit. Fig. 1. Transformer implementation with coupled inductors The magnetic domain has been implemented in the simulation software PLECS. To avoid numerical integration errors, Kirch- hoff’s current law must be applied to both the magnetic flux and circuit, in which inductances represent magnetic flux paths the flux-rate when solving the circuit equations. and losses incur at resistors. Magnetic coupling between I. INTRODUCTION windings is realized either with mutual inductances or with ideal transformers. Inductors and transformers are key components in modern power electronic circuits. Compared to other passive com- Using coupled inductors, magnetic components can be ponents they are difficult to model due to the non-linear implemented in any circuit simulator since only electrical behavior of magnetic core materials and the complex structure components are required. -
Magnetism and Magnetic Circuits
UNIVERSITY OF BABYLON BASIC OF ELECTRICAL ENGINEERING LECTURE NOTES Magnetism and Magnetic Circuits The Nature of a Magnetic Field: Magnetism refers to the force that acts between magnets and magnetic materials. We know, for example, that magnets attract pieces of iron, deflect compass needles, attract or repel other magnets, and so on. The region where the force is felt is called the “field of the magnet” or simply, its magnetic field. Thus, a magnetic field is a force field. Using Faraday’s representation, magnetic fields are shown as lines in space. These lines, called flux lines or lines of force, show the direction and intensity of the field at all points. The field is strongest at the poles of the magnet (where flux lines are most dense), its direction is from north (N) to south (S) external to the magnet, and flux lines never cross. The symbol for magnetic flux as shown is the Greek letter (phi). What happens when two magnets are brought close together? If unlike poles attract, and flux lines pass from one magnet to the other. الصفحة 321 Saad Alwash UNIVERSITY OF BABYLON BASIC OF ELECTRICAL ENGINEERING LECTURE NOTES If like poles repel, and the flux lines are pushed back as indicated by the flattening of the field between the two magnets. Ferromagnetic Materials (magnetic materials that are attracted by magnets such as iron, nickel, cobalt, and their alloys) are called ferromagnetic materials. Ferromagnetic materials provide an easy path for magnetic flux. The flux lines take the longer (but easier) path through the soft iron, rather than the shorter path that they would normally take. -
MAGNETISM and Its Practical Applications
Mechanical Engineering Laboratory A short introduction to… MAGNETISM and its practical applications Michele Togno – Technical University of Munich, 28 th March 2014 – 4th April 2014 Mechanical Engineering laboratory - Magnetism - 1 - Magnetism A property of matter A magnet is a material or object that produces a magnetic field. This magnetic field is invisible but it is responsible for the most notable property of a magnet: a force that pulls on ferromagnetic materials, such as iron, and attracts or repels other magnets. History of magnetism Magnetite Fe 3O4 Sushruta, VI cen. BCE (lodestone) (Indian surgeon) J.B. Biot, 1774-1862 A.M. Ampere, 1775-1836 Archimedes (287-212 BCE) William Gilbert, 1544-1603 H.C. Oersted, 1777-1851 (English physician) C.F. Gauss, 1777-1855 F. Savart, 1791-1841 M. Faraday, 1791-1867 J.C. Maxwell, 1831-1879 Shen Kuo, 1031-1095 (Chinese scientist) H. Lorentz, 1853-1928 Mechanical Engineering laboratory - Magnetism - 2 - The Earth magnetic field A sort of cosmic shield Mechanical Engineering laboratory - Magnetism - 3 - Magnetic domains and types of magnetic materials Ferromagnetic : a material that could exhibit spontaneous magnetization, that is a net magnetic moment in the absence of an external magnetic field (iron, nickel, cobalt…). Paramagnetic : material slightly attracted by a magnetic field and which doesn’t retain the magnetic properties when the external field is removed (magnesium, molybdenum, lithium…). Diamagnetic : a material that creates a magnetic field in opposition to an externally applied magnetic field (superconductors…). Mechanical Engineering laboratory - Magnetism - 4 - Magnetic field and Magnetic flux Every magnet is a magnetic dipole (magnetic monopole is an hypothetic particle whose existence is not experimentally proven right now). -
Doppler-Based Acoustic Gyrator
applied sciences Article Doppler-Based Acoustic Gyrator Farzad Zangeneh-Nejad and Romain Fleury * ID Laboratory of Wave Engineering, École Polytechnique Fédérale de Lausanne (EPFL), 1015 Lausanne, Switzerland; farzad.zangenehnejad@epfl.ch * Correspondence: romain.fleury@epfl.ch; Tel.: +41-412-1693-5688 Received: 30 May 2018; Accepted: 2 July 2018; Published: 3 July 2018 Abstract: Non-reciprocal phase shifters have been attracting a great deal of attention due to their important applications in filtering, isolation, modulation, and mode locking. Here, we demonstrate a non-reciprocal acoustic phase shifter using a simple acoustic waveguide. We show, both analytically and numerically, that when the fluid within the waveguide is biased by a time-independent velocity, the sound waves travelling in forward and backward directions experience different amounts of phase shifts. We further show that the differential phase shift between the forward and backward waves can be conveniently adjusted by changing the imparted bias velocity. Setting the corresponding differential phase shift to 180 degrees, we then realize an acoustic gyrator, which is of paramount importance not only for the network realization of two port components, but also as the building block for the construction of different non-reciprocal devices like isolators and circulators. Keywords: non-reciprocal acoustics; gyrators; phase shifters; Doppler effect 1. Introduction Microwave phase shifters are two-port components that provide an arbitrary and variable transmission phase angle with low insertion loss [1–3]. Since their discovery in the 19th century, such phase shifters have found important applications in devices such as phased array antennas and receivers [4,5], beam forming and steering networks [6,7], measurement and testing systems [8,9], filters [10,11], modulators [12,13], frequency up-convertors [14], power flow controllers [15], interferometers [16], and mode lockers [17]. -
Magnetic Theory and Applications.Cdr
Magnetic Theory & Applications All materials are defined as being magnetic in that they respond to the application of an applied magnetic field differently to that of air or vacuum. Only selected elements or alloys have useful magnetic properties in engineering applications. B Magnetic materials which are easily magnetized and the magnetized are often termed soft. Conversely, those magnetic materials where any induced magnetism Normal is difficult to remove are termed hard or permanent. Intrinsic When a practical or highly permeable material is influenced by an external Initial magnetisation curve magnetic field it may acquire a large magnetization or magnetic induction. The level J of the magnetization will be related to the individual intrinsic permeability of the B HcJ HcB material in question. The relationship between the external field in the induction is: H B = µH where B is the magnetic induction and where µ is the permeability and where H is the external magnetic field. Br Remanence HcB Normal coercivity HcJ Intrinsic coercivity In the S. I. system of units, B is defined in terms of the tesla (T) and the magnetic field H in ampere per meter (A/m). When the external field, H and induction, B are identical (i.e. in a vacuum) the permeability µ is exactly 4π x 10-7 in units of henry per meter for the equation to balance. It is termed µo. Hence: B B = µo H Initial magnetisation curve Bmax In strongly magnetic materials the relationship is: B r A ΔB H B = µ µ H where µ is the relative c o r r H ΔH permeability of the Hysteresis loop material. -
Magnetic Circuits Magnetic Circuit Definitions
ELG2336: Magnetic Circuits Magnetic Circuit Definitions • Magnetomotive Force – The “driving force” that causes a magnetic field – Symbol, F – Definition, F = NI – Units, Ampere-turns, (A-t) 2 Magnetic Circuit Definitions • Magnetic Field Intensity – mmf gradient, or mmf per unit length – Symbol, H – Definition, H = F/l = NI/l – Units, (A-t/m) 3 Magnetic Circuit Definitions • Flux Density – he concentration of the lines of force in a magnetic circuit – Symbol, B – Definition, B = Φ/A – Units, (Wb/m2), or T (Tesla) 4 Magnetic Circuit Definitions • Reluctance – The measure of “opposition” the magnetic circuit offers to the flux – The analog of Resistance in an electrical circuit – Symbol, R – Definition, R = F/Φ – Units, (A-t/Wb) 5 Magnetic Circuit Definitions • Permeability – Relates flux density and field intensity – Symbol, μ – Definition, μ = B/H – Units, (Wb/A-t-m) ECE 441 6 Magnetic Circuit Definitions • Permeability of free space (air) – Symbol, μ0 -7 – μ0 = 4πx10 Wb/A-t-m 7 Definitions Combined (Unit is Weber (Wb)) = Magnetic Flux Crossing a Surface of Area ‘A’ in m2. B (Unit is Tesla (T)) = Magnetic Flux Density = /A B H (Unit is Amp/m) = Magnetic Field Intensity = = permeability = o r -7 o = 4*10 H/m (H Henry) = Permeability of free space (air) r = Relative Permeability r >> 1 for Magnetic Material 8 Magnetic Circuit 9 Air Gaps, Fringing, and Laminated Cores • Circuits with air gaps may cause fringing • Correction – Increase each cross-sectional dimension of gap by the size of the gap • Many applications use laminated cores -
Magnetic Circuit and Reluctance (How Do We Calculate Magnetic Field Or
Magnetic circuit and reluctance (How do we calculate magnetic field or flux in situations where we have an air gap or two materials with diferrent magnetic properties?) 1. A magnetic flux path is interrupted by an air gap are of practical importance. 2. The problems encountered here are more complicated than in calculating the flux in a single material. 3. The magnet engineer is often of calculating the magnetic flux in magnetic circuits with a combination of an iron and air core 1 (i) In closed circuit case ( a ring of iron is wound with N turns of a solenoid which carries a current i) Ni N : Turns Magnetic field H L L : The average length of the ring Flux density passing → Ampere’s law → Ni H dl B μo(H M) circuit in the ring path Ni B μ ( M) Ni HL (B μH) o L B Ni L B B L μ Ni M L μo μ We can define here the magnetomotive N: the number of turns i: the current flowing in the force η which for a solenoid is Ni solenoid A magnetic analogue of flow Ohm’s law We can formulate a general : magnetic flux equation relating the Rm magnetic flux Rm : magnetic relutcance V i i R V Rm R 2 If the iron ring has cross-section area A(m²) permeability μ Turns of solenoid N length L Starting from the B A H A - The term L/μA is the relationship between Ni magnetic reluctance of A path. flux, magnetic induction L and magnetic field Ni - Magnetic reluctance is L series in a magnetic A circuit may be added is analogous to L R R m A A 1 3 Magnetic circuit Electrical circuit magnetomotive force electromotive force Flux () Current (i) reluctance resistance l l Reluctance Resistance R A A 1 Reluctivity Resistivity 1 conductivity permeability (ii) In open circuit case • If the air gap is small, there will be little leakage of the flux at the gap, but B = μH can no longer apply since the μ of air and the iron ring are different. -
Modeling & Simulation 2019 Lecture 8. Bond Graphs
Modeling & Simulation 2019 Lecture 8. Bond graphs Claudio Altafini Automatic Control, ISY Linköping University, Sweden 1 / 45 Summary of lecture 7 • General modeling principles • Physical modeling: dimension, dimensionless quantities, scaling • Models from physical laws across different domains • Analogies among physical domains 2 / 45 Lecture 8. Bond graphs Summary of today • Analogies among physical domains • Bond graphs • Causality In the book: Chapter 5 & 6 3 / 45 Basic physics laws: a survey Electrical circuits Hydraulics Mechanics – translational Thermal systems Mechanics – rotational 4 / 45 Electrical circuits Basic quantities: • Current i(t) (ampere) • Voltage u(t) (volt) • Power P (t) = u(t) · i(t) 5 / 45 Electrical circuits Basic laws relating i(t) and u(t) • inductance d 1 Z t L i(t) = u(t) () i(t) = u(s)ds dt L 0 • capacitance d 1 Z t C u(t) = i(t) () u(t) = i(s)ds dt C 0 • resistance (linear case) u(t) = Ri(t) 6 / 45 Electrical circuits Energy storage laws for i(t) and u(t) • electromagnetic energy 1 T (t) = Li2(t) 2 • electric field energy 1 T (t) = Cu2(t) 2 • energy loss in a resistance Z t Z t Z t 1 Z t T (t) = P (s)ds = u(s)i(s)ds = R i2(s)ds = u2(s)ds 0 0 0 R 0 7 / 45 Electrical circuits Interconnection laws for i(t) and u(t) • Kirchhoff law for voltages On a loop: ( X +1; σk aligned with loop direction σkuk(t) = 0; σk = −1; σ against loop direction k k • Kirchhoff law for currents On a node: ( X +1; σk inward σkik(t) = 0; σk = −1; σ outward k k 8 / 45 Electrical circuits Transformations laws for u(t) and i(t) • transformer u1 = ru2 1 i = i 1 r 2 u1i1 = u2i2 ) no power loss • gyrator u1 = ri2 1 i = u 1 r 2 u1i1 = u2i2 ) no power loss 9 / 45 Electrical circuits Example State space model: d 1 i = (u − Ri − u ) dt L s C d 1 u = i dt C C 10 / 45 Mechanical – translational Basic quantities: • Velocity v(t) (meters per second) • Force F (t) (newton) • Power P (t) = F (t) · v(t) 11 / 45 Mechanical – translational Basic laws relating F (t) and v(t) • Newton second law d 1 Z t m v(t) = F (t) () v(t) = F (s)ds dt m 0 • Hook’s law (elastic bodies, e.g. -
Bond Graph Methodology
Bond Graph Methodology • An abstract representation of a system where a collection of components interact with each other through energy ports and are placed in a system where energy is exchanged. • A domain-independent graphical description of dynamic behavior o physical systems • System models will be constructed using a uniform notations for al types of physical system based on energy flow • Powerful tool for modeling engineering systems, especially when different physical domains are involved • A form of object-oriented physical system modeling Bond Graphs Use analogous power and energy variables in all domains, but allow the special features of the separate fields to be represented. The only physical variables required to represent all energetic systems are power variables [effort (e) & flow (f)] and energy variables [momentum p (t) and displacement q (t)]. Dynamics of physical systems are derived by the application of instant-by-instant energy conservation. Actual inputs are exposed. Linear and non-linear elements are represented with the same symbols; non-linear kinematics equations can also be shown. Provision for active bonds . Physical information involving information transfer, accompanied by negligible amounts of energy transfer are modeled as active bonds . A Bond Graph’s Reach Mechanical Rotation Mechanical Hydraulic/Pneumatic Translation Thermal Chemical/Process Electrical Engineering Magnetic Figure 2. Multi-Energy Systems Modeling using Bond Graphs • Introductory Examples • Electrical Domain Power Variables : Electrical Voltage (u) & Electrical Current (i) Power in the system: P = u * i Fig 3. A series RLC circuit Constitutive Laws: uR = i * R uC = 1/C * ( ∫i dt) uL = L * (d i/dt); or i = 1/L * ( ∫uL dt) Represent different elements with visible ports (figure 4 ) To these ports, connect power bonds denoting energy exchange The voltage over the elements are different The current through the elements is the same Fig.