Basic Design and Engineering of Normal-Conducting, Iron-Dominated Electromagnets
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Selecting the Optimal Inductor for Power Converter Applications
Selecting the Optimal Inductor for Power Converter Applications BACKGROUND SDR Series Power Inductors Today’s electronic devices have become increasingly power hungry and are operating at SMD Non-shielded higher switching frequencies, starving for speed and shrinking in size as never before. Inductors are a fundamental element in the voltage regulator topology, and virtually every circuit that regulates power in automobiles, industrial and consumer electronics, SRN Series Power Inductors and DC-DC converters requires an inductor. Conventional inductor technology has SMD Semi-shielded been falling behind in meeting the high performance demand of these advanced electronic devices. As a result, Bourns has developed several inductor models with rated DC current up to 60 A to meet the challenges of the market. SRP Series Power Inductors SMD High Current, Shielded Especially given the myriad of choices for inductors currently available, properly selecting an inductor for a power converter is not always a simple task for designers of next-generation applications. Beginning with the basic physics behind inductor SRR Series Power Inductors operations, a designer must determine the ideal inductor based on radiation, current SMD Shielded rating, core material, core loss, temperature, and saturation current. This white paper will outline these considerations and provide examples that illustrate the role SRU Series Power Inductors each of these factors plays in choosing the best inductor for a circuit. The paper also SMD Shielded will describe the options available for various applications with special emphasis on new cutting edge inductor product trends from Bourns that offer advantages in performance, size, and ease of design modification. -
Magnetic Materials: Hysteresis
Magnetic Materials: Hysteresis Ferromagnetic and ferrimagnetic materials have non-linear initial magnetisation curves (i.e. the dotted lines in figure 7), as the changing magnetisation with applied field is due to a change in the magnetic domain structure. These materials also show hysteresis and the magnetisation does not return to zero after the application of a magnetic field. Figure 7 shows a typical hysteresis loop; the two loops represent the same data, however, the blue loop is the polarisation (J = µoM = B-µoH) and the red loop is the induction, both plotted against the applied field. Figure 7: A typical hysteresis loop for a ferro- or ferri- magnetic material. Illustrated in the first quadrant of the loop is the initial magnetisation curve (dotted line), which shows the increase in polarisation (and induction) on the application of a field to an unmagnetised sample. In the first quadrant the polarisation and applied field are both positive, i.e. they are in the same direction. The polarisation increases initially by the growth of favourably oriented domains, which will be magnetised in the easy direction of the crystal. When the polarisation can increase no further by the growth of domains, the direction of magnetisation of the domains then rotates away from the easy axis to align with the field. When all of the domains have fully aligned with the applied field saturation is reached and the polarisation can increase no further. If the field is removed the polarisation returns along the solid red line to the y-axis (i.e. H=0), and the domains will return to their easy direction of magnetisation, resulting in a decrease in polarisation. -
Assignment 3
PHYSICS 2800 – 2nd TERM Introduction to Materials Science Assignment 3 Date of distribution: Tuesday, March 9, 2010 Date for solutions to be handed in: Tuesday, March 16, 2010 -7 2 You may assume the standard values µ0 = 4 π × 10 kg-m/C for the permeability of vacuum -24 2 and µB = 9.27 × 10 A-m for the Bohr magneton. 3 1. Nickel is a ferromagnetic metal with density 8.90 g/cm . Given that Avogadro’s number NA = 6.02 × 10 23 atoms/mol and the atomic weight of Ni is 58.7, calculate the number of atoms of Ni per cubic metre. If one atom of Ni has a magnetic moment of 0.6 Bohr magnetons, deduce the saturation magnetization Ms and the saturation magnetic induction Bs for Ni. Answer: 3 The saturation magnetization is given by Ms = 0.6 µBN , where N is the number of atoms/m . ρN A But N = , where ρ is the density and ANi is the atomic weight of Ni. ANi 90.8( ×10 6 g/m 3 )( 02.6 ×10 23 atoms/mol ) So N = = 9.13 × 10 28 atoms/m 3. 58 7. g/mol -24 28 5 Then Ms = 0.6 (9.27 × 10 )( 9.13 × 10 ) = 5.1 × 10 A/m. Finally (from the lecture notes), -7 5 BS = µ0MS = (4 π × 10 )(5.1 × 10 ) = 0.64 Tesla. 2. The magnetization within a bar of some metal alloy is 1.2 × 10 6 A/m when the H field is 200 A/m. Calculate (a) the magnetic susceptibility χm of this alloy, (b) the permeability µ, and (c) the magnetic induction B within the alloy. -
Magnetic Materials: Soft Magnets
Magnetic Materials: Soft Magnets Soft magnetic materials are those materials that are easily magnetised and demagnetised. They typically have intrinsic coercivity less than 1000 Am-1. They are used primarily to enhance and/or channel the flux produced by an electric current. The main parameter, often used as a figure of merit for soft magnetic materials, is the relative permeability (µr, where µr = B/ µoH), which is a measure of how readily the material responds to the applied magnetic field. The other main parameters of interest are the coercivity, the saturation magnetisation and the electrical conductivity. The types of applications for soft magnetic materials fall into two main categories: AC and DC. In DC applications the material is magnetised in order to perform an operation and then demagnetised at the conclusion of the operation, e.g. an electromagnet on a crane at a scrap yard will be switched on to attract the scrap steel and then switched off to drop the steel. In AC applications the material will be continuously cycled from being magnetised in one direction to the other, throughout the period of operation, e.g. a power supply transformer. A high permeability will be desirable for each type of application but the significance of the other properties varies. For DC applications the main consideration for material selection is most likely to be the permeability. This would be the case, for example, in shielding applications where the flux must be channelled through the material. Where the material is used to generate a magnetic field or to create a force then the saturation magnetisation may also be significant. -
Vocabulary of Magnetism
TECHNotes The Vocabulary of Magnetism Symbols for key magnetic parameters continue to maximum energy point and the value of B•H at represent a challenge: they are changing and vary this point is the maximum energy product. (You by author, country and company. Here are a few may have noticed that typing the parentheses equivalent symbols for selected parameters. for (BH)MAX conveniently avoids autocorrecting Subscripts in symbols are often ignored so as to the two sequential capital letters). Units of simplify writing and typing. The subscripted letters maximum energy product are kilojoules per are sometimes capital letters to be more legible. In cubic meter, kJ/m3 (SI) and megagauss•oersted, ASTM documents, symbols are italicized. According MGOe (cgs). to NIST’s guide for the use of SI, symbols are not italicized. IEC uses italics for the main part of the • µr = µrec = µ(rec) = recoil permeability is symbol, but not for the subscripts. I have not used measured on the normal curve. It has also been italics in the following definitions. For additional called relative recoil permeability. When information the reader is directed to ASTM A340[11] referring to the corresponding slope on the and the NIST Guide to the use of SI[12]. Be sure to intrinsic curve it is called the intrinsic recoil read the latest edition of ASTM A340 as it is permeability. In the cgs-Gaussian system where undergoing continual updating to be made 1 gauss equals 1 oersted, the intrinsic recoil consistent with industry, NIST and IEC usage. equals the normal recoil minus 1. -
Glossary of MRI Terms A
Glossary of MRI Terms A Absorption mode. Component of the MR signal that yields a symmetric, positive-valued line shape. Acceleration factor. The multiplicative term by which faster imaging pulse sequences such as multiple echo imaging reduce total imaging time compared to conventional imaging sequences such as spin echo imaging. Acoustic noise. Vibrations of the gradient coil support structures create sound waves. These vibrations are caused by interactions of the magnetic field created by pulses of the current through the gradient coil with the main magnetic field in a manner similar to a loudspeaker coil. Sound pressure is reported on a logarithmic scale called sound-pressure level expressed in decibels (dB) referenced to the weakest audible 1,000 Hz sound pressure of 2x10–5 pascal. Sound level meters contain filters that simulate the ear’s frequency response. The most commonly used filter provides what is called A weighting, with the letter A appended to the dB units, i.e., dBA. Acquisition matrix. Number of independent data samples in each direction, e.g., in 2DFT imaging it is the number of samples in the phase-encoding and frequency-encoding directions, and in reconstruction from projections imaging it is the number of samples in time and angle. The acquisition matrix may be asymmetric and of different size than the reconstructed image or display matrix, e.g., with zero filling or interpolation, or (for asymmetric sampling) by exploiting the symmetry of the data matrix. For symmetric sampling, the acquisition matrix will roughly equal the ratio of image field of view to spatial resolution along the corresponding direction (depending on filtering and other processing). -
Tuning Structural and Magnetic Properties of Fe Oxide Nanoparticles by Specifc Hydrogenation Treatments S
www.nature.com/scientificreports OPEN Tuning structural and magnetic properties of Fe oxide nanoparticles by specifc hydrogenation treatments S. G. Greculeasa1, P. Palade1, G. Schinteie1, A. Leca1, F. Dumitrache2, I. Lungu2, G. Prodan3, A. Kuncser1 & V. Kuncser1* Structural and magnetic properties of Fe oxide nanoparticles prepared by laser pyrolysis and annealed in high pressure hydrogen atmosphere were investigated. The annealing treatments were performed at 200 °C (sample A200C) and 300 °C (sample A300C). The as prepared sample, A, consists of nanoparticles with ~ 4 nm mean particle size and contains C (~ 11 at.%), Fe and O. The Fe/O ratio is between γ-Fe2O3 and Fe3O4 stoichiometric ratios. A change in the oxidation state, crystallinity and particle size is evidenced for the nanoparticles in sample A200C. The Fe oxide nanoparticles are completely reduced in sample A300C to α-Fe single phase. The blocking temperature increases from 106 K in A to 110 K in A200C and above room temperature in A300C, where strong inter-particle interactions are evidenced. Magnetic parameters, of interest for applications, have been considerably varied by the specifc hydrogenation treatments, in direct connection to the induced specifc changes of particle size, crystallinity and phase composition. For the A and A200C samples, a feld cooling dependent unidirectional anisotropy was observed especially at low temperatures, supporting the presence of nanoparticles with core–shell-like structures. Surprisingly high MS values, almost 50% higher than for bulk metallic Fe, were evidenced in sample A300C. Fe-based nanoparticles (NPs) show remarkable interest in the scientifc community for various applications such as biomedicine (hyperthermia1, targeted drug delivery2, computed tomography and magnetic resonance imaging contrast agents3,4), catalysis5,6, magnetic fuids7, gas sensors8, high-density magnetic storages 9, water treatment and environment protection 10,11. -
Characterization and Quantification of Magnetic Remanence in Unexploded Ordnance
CHARACTERIZATION AND QUANTIFICATION OF MAGNETIC REMANENCE IN UNEXPLODED ORDNANCE by Whitney Elizabeth Goodrich A thesis submitted to the Faculty and Board of Trustees of the Colorado School of Mines in partial fulfillment of the requirements for the degree of Master of Science (Geophysics). Golden, Colorado Date _______________ Signed: ____________________ Whitney Elizabeth Goodrich Approved: __________________ Dr. Gary Olhoeft Thesis Advisor Golden, Colorado Date ______________ ___________________________ Dr. Terence K. Young Professor and Head Department of Geophysics ii ABSTRACT Under the Range Rule (1997), the Department of Defense defines unexploded ordnance (UXO) as a piece of ordnance that has been deployed, but has not exploded. This study investigated a subset of UXO including artillery shells and mortars (projectiles), but excluding landmines. UXO contaminates approximately 15 million acres of land in the United States alone. The geophysical tools most frequently used for detection are electromagnetic and magnetic methods. These methods, however, produce a “hit” for any metallic object in the ground, not just UXO. In a given survey, this results in a large number of anomalies, only a small subset of which are actually UXO. Current practice dictates that most anomalies are dug up and identified, and the UXO is exploded in place. The estimated cost to remediate existing UXO, in the United States, with current methods, is tens to hundreds of billions of dollars. Discrimination is the process in which UXO (hazardous) is differentiated from non-UXO (non-hazardous), prior to anomaly excavation. Methods to discriminate the UXO greatly reduce the cost of remediation. Remanent magnetization in UXO is one quantity that must be understood to improve discrimination methodologies in the future. -
Electromagnetic Spacecraft Used for Magnetic Navigation Within Asteroid Belt, Mining Concepts and Asteroid Magnetic Classification G
Lunar and Planetary Science XXXVIII (2007) 1093.pdf ELECTROMAGNETIC SPACECRAFT USED FOR MAGNETIC NAVIGATION WITHIN ASTEROID BELT, MINING CONCEPTS AND ASTEROID MAGNETIC CLASSIFICATION G. Kletetschka 1,2,3, T. Adachi1,2, and V. Mikula1,2, 1Department of Physics, Catholic University of America, Washington DC, USA, 2NASA Goddard Space Flight Center, Greenbelt, MD, USA, 3Institute of Geology, Academy of Sciences of the Czech Republic, Prague, Czech Republic. Introduction: The objective of asteroid investiga- ments from asteroidal bodies, using them to adjust the tion is an establishment of the remote data acquisition speed and direction of the spacecraft and finally use system allowing sufficient characterization and classi- magnetic attraction for magnetic classification of as- fication of asteroids. It is generally accepted that aster- teroids. We modeled magnetic field generated by elec- oids are the parent bodies for most meteorites reaching tromagnets containing high permeability cores and the Earth [1]. Magnetic classification of meteorites connected with high permeability tubes. We use Finite indicates that the amount of iron in asteroids within Element Method Magnetics software written by David asteroid belt is efficiently detected by measurement of Meeker, 2004. magnetic susceptibility of asteroidal material [2, 3]. Magnetic navigation: Let us assume that a space- Presence of nearby magnetic source is enhanced by craft is located within the asteroid belt. Asteroids have any soft magnetic component, which in asteroidal ma- gravitational interactions orders of magnitude smaller terial is mostly iron and nickel compounds. Such mate- than planet Earth. Any orbiting spacecraft has very rial reaches magnetic susceptibility of 1 e-3 m^3/kg. low speed on its orbit allowing precise navigation and Even if diluted within the asteroid, the presence of maneuvering. -
Hot on the Trail of Residual Magnetism
4 Products and technology A new way of testing current transformers Hot on the trail of residual magnetism Current transformers play an important role in Testing of protection current transformers (CTs) the protection of electrical power systems. They Conventional testing methods apply a signal to one side of the CT and read the resulting output signal on the other side. However, provide the protection relay with a current pro- these methods can be time-consuming and use a lot of equip- portional to the line current so that it can iden- ment. Sometimes they are not even feasible as very high currents tify abnormal conditions and operate according are required, e.g. for on-site testing of current transformers to its settings. The transformation of the current designed for transient behavior (TP, TPX, TPY, TPZ types). As these conventional methods have limitations, OMICRON has developed values from primary to secondary must be ac- a new way of testing CTs. curate during normal operation and especially during system fault conditions (when overcur- Modeling concept rents up to 30-times the nominal current are not This led to the development of the CT Analyzer – a test device using a revolutionary testing concept. The new concept of model- an exception). ing a current transformer allows for a detailed view of its design and physical behavior to be created using parameters measured during the test. It then compares the model with the relevant OMICRON Magazine | Volume 1 Issue 2 2010 Products and technology 5 specification to confirm the accuracy of the CT. The CT Analyzer Different test devices and methods are used to verify the per- is small, lightweight and provides fully automated test plans, formance of current transformers during their development, keeping testing times as short as possible. -
Electromagnetic Fields and Energy
MIT OpenCourseWare http://ocw.mit.edu Haus, Hermann A., and James R. Melcher. Electromagnetic Fields and Energy. Englewood Cliffs, NJ: Prentice-Hall, 1989. ISBN: 9780132490207. Please use the following citation format: Haus, Hermann A., and James R. Melcher, Electromagnetic Fields and Energy. (Massachusetts Institute of Technology: MIT OpenCourseWare). http://ocw.mit.edu (accessed [Date]). License: Creative Commons Attribution-NonCommercial-Share Alike. Also available from Prentice-Hall: Englewood Cliffs, NJ, 1989. ISBN: 9780132490207. Note: Please use the actual date you accessed this material in your citation. For more information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms 9 MAGNETIZATION 9.0 INTRODUCTION The sources of the magnetic fields considered in Chap. 8 were conduction currents associated with the motion of unpaired charge carriers through materials. Typically, the current was in a metal and the carriers were conduction electrons. In this chapter, we recognize that materials provide still other magnetic field sources. These account for the fields of permanent magnets and for the increase in inductance produced in a coil by insertion of a magnetizable material. Magnetization effects are due to the propensity of the atomic constituents of matter to behave as magnetic dipoles. It is natural to think of electrons circulating around a nucleus as comprising a circulating current, and hence giving rise to a magnetic moment similar to that for a current loop, as discussed in Example 8.3.2. More surprising is the magnetic dipole moment found for individual electrons. This moment, associated with the electronic property of spin, is defined as the Bohr magneton e 1 m = ± ¯h (1) e m 2 11 where e/m is the electronic chargetomass ratio, 1.76 × 10 coulomb/kg, and 2π¯h −34 2 is Planck’s constant, ¯h = 1.05 × 10 joulesec so that me has the units A − m . -
Physics and Measurements of Magnetic Materials
Physics and measurements of magnetic materials S. Sgobba CERN, Geneva, Switzerland Abstract Magnetic materials, both hard and soft, are used extensively in several components of particle accelerators. Magnetically soft iron–nickel alloys are used as shields for the vacuum chambers of accelerator injection and extraction septa; Fe-based material is widely employed for cores of accelerator and experiment magnets; soft spinel ferrites are used in collimators to damp trapped modes; innovative materials such as amorphous or nanocrystalline core materials are envisaged in transformers for high- frequency polyphase resonant convertors for application to the International Linear Collider (ILC). In the field of fusion, for induction cores of the linac of heavy-ion inertial fusion energy accelerators, based on induction accelerators requiring some 107 kg of magnetic materials, nanocrystalline materials would show the best performance in terms of core losses for magnetization rates as high as 105 T/s to 107 T/s. After a review of the magnetic properties of materials and the different types of magnetic behaviour, this paper deals with metallurgical aspects of magnetism. The influence of the metallurgy and metalworking processes of materials on their microstructure and magnetic properties is studied for different categories of soft magnetic materials relevant for accelerator technology. Their metallurgy is extensively treated. Innovative materials such as iron powder core materials, amorphous and nanocrystalline materials are also studied. A section considers the measurement, both destructive and non-destructive, of magnetic properties. Finally, a section discusses magnetic lag effects. 1 Magnetic properties of materials: types of magnetic behaviour The sense of the word ‘lodestone’ (waystone) as magnetic oxide of iron (magnetite, Fe3O4) is from 1515, while the old name ‘lodestar’ for the pole star, as the star leading the way in navigation, is from 1374.