Magnet Handbook About This Handbook ®
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
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. -
Permanent Magnet DC Motors Catalog
Catalog DC05EN Permanent Magnet DC Motors Drives DirectPower Series DA-Series DirectPower Plus Series SC-Series PRO Series www.electrocraft.com www.electrocraft.com For over 60 years, ElectroCraft has been helping engineers translate innovative ideas into reality – one reliable motor at a time. As a global specialist in custom motor and motion technology, we provide the engineering capabilities and worldwide resources you need to succeed. This guide has been developed as a quick reference tool for ElectroCraft products. It is not intended to replace technical documentation or proper use of standards and codes in installation of product. Because of the variety of uses for the products described in this publication, those responsible for the application and use of this product must satisfy themselves that all necessary steps have been taken to ensure that each application and use meets all performance and safety requirements, including all applicable laws, regulations, codes and standards. Reproduction of the contents of this copyrighted publication, in whole or in part without written permission of ElectroCraft is prohibited. Designed by stilbruch · www.stilbruch.me ElectroCraft DirectPower™, DirectPower™ Plus, DA-Series, SC-Series & PRO Series Drives 2 Table of Contents Typical Applications . 3 Which PMDC Motor . 5 PMDC Drive Product Matrix . .6 DirectPower Series . 7 DP20 . 7 DP25 . 9 DP DP30 . 11 DirectPower Plus Series . 13 DPP240 . 13 DPP640 . 15 DPP DPP680 . 17 DPP700 . 19 DPP720 . 21 DA-Series. 23 DA43 . 23 DA DA47 . 25 SC-Series . .27 SCA-L . .27 SCA-S . .29 SC SCA-SS . 31 PRO Series . 33 PRO-A04V36 . 35 PRO-A08V48 . 37 PRO PRO-A10V80 . -
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. -
Equivalence of Current–Carrying Coils and Magnets; Magnetic Dipoles; - Law of Attraction and Repulsion, Definition of the Ampere
GEOPHYSICS (08/430/0012) THE EARTH'S MAGNETIC FIELD OUTLINE Magnetism Magnetic forces: - equivalence of current–carrying coils and magnets; magnetic dipoles; - law of attraction and repulsion, definition of the ampere. Magnetic fields: - magnetic fields from electrical currents and magnets; magnetic induction B and lines of magnetic induction. The geomagnetic field The magnetic elements: (N, E, V) vector components; declination (azimuth) and inclination (dip). The external field: diurnal variations, ionospheric currents, magnetic storms, sunspot activity. The internal field: the dipole and non–dipole fields, secular variations, the geocentric axial dipole hypothesis, geomagnetic reversals, seabed magnetic anomalies, The dynamo model Reasons against an origin in the crust or mantle and reasons suggesting an origin in the fluid outer core. Magnetohydrodynamic dynamo models: motion and eddy currents in the fluid core, mechanical analogues. Background reading: Fowler §3.1 & 7.9.2, Lowrie §5.2 & 5.4 GEOPHYSICS (08/430/0012) MAGNETIC FORCES Magnetic forces are forces associated with the motion of electric charges, either as electric currents in conductors or, in the case of magnetic materials, as the orbital and spin motions of electrons in atoms. Although the concept of a magnetic pole is sometimes useful, it is diácult to relate precisely to observation; for example, all attempts to find a magnetic monopole have failed, and the model of permanent magnets as magnetic dipoles with north and south poles is not particularly accurate. Consequently moving charges are normally regarded as fundamental in magnetism. Basic observations 1. Permanent magnets A magnet attracts iron and steel, the attraction being most marked close to its ends. -
Permanent Magnet Design Guidelines
NOTE(2019): THIS ORGANIZATION (MMPA) IS OBSOLETE! MAGNET GUIDELINES Basic physics of magnet materials II. Design relationships, figures merit and optimizing techniques Ill. Measuring IV. Magnetizing Stabilizing and handling VI. Specifications, standards and communications VII. Bibliography INTRODUCTION This guide is a supplement to our MMPA Standard No. 0100. It relates the information in the Standard to permanent magnet circuit problems. The guide is a bridge between unit property data and a permanent magnet component having a specific size and geometry in order to establish a magnetic field in a given magnetic circuit environment. The MMPA 0100 defines magnetic, thermal, physical and mechanical properties. The properties given are descriptive in nature and not intended as a basis of acceptance or rejection. Magnetic measure- ments are difficult to make and less accurate than corresponding electrical mea- surements. A considerable amount of detailed information must be exchanged between producer and user if magnetic quantities are to be compared at two locations. MMPA member companies feel that this publication will be helpful in allowing both user and producer to arrive at a realistic and meaningful specifica- tion framework. Acknowledgment The Magnetic Materials Producers Association acknowledges the out- standing contribution of Parker to this and designers and manufacturers of products usingpermanent magnet materials. Parker the Technical Consultant to MMPA compiled and wrote this document. We also wish to thank the Standards and Engineering Com- mittee of MMPA which reviewed and edited this document. December 1987 3M July 1988 5M August 1996 December 1998 1 M CONTENTS The guide is divided into the following sections: Glossary of terms and conversion A very important starting point since the whole basis of communication in the magnetic material industry involves measurement of defined unit properties. -
An Inexpensive Hands-On Introduction to Permanent Magnet Direct Current Motors
AC 2011-1082: AN INEXPENSIVE HANDS-ON INTRODUCTION TO PER- MANENT MAGNET DIRECT CURRENT MOTORS Garrett M. Clayton, Villanova University Dr. Garrett M. Clayton received his BSME from Seattle University and his MSME and PhD in Mechanical Engineering from the University of Washington (Seattle). He is an Assistant Professor in Mechanical Engineering at Villanova University. His research interests focus on mechatronics, specifically modeling and control of scanning probe microscopes and unmanned vehicles. Rebecca A Stein, University of Pennsylvania Rebecca Stein is the Associate Director of Research and Educational Outreach in the School of Engi- neering and Applied Science at the University of Pennsylvania. She received her B.S. in Mechanical Engineering and Masters in Technology Management from Villanova University. Her background and work experience is in K-12 engineering education initiatives. Rebecca has spent the past 5 years involved in STEM high school programs at Villanova University and The School District of Philadelphia. Ad- ditionally, she has helped coordinate numerous robotics competitions such as BEST Robotics, FIRST LEGO League and MATE. Page 22.177.1 Page c American Society for Engineering Education, 2011 An Inexpensive Hands-on Introduction to Permanent Magnet Direct Current Motors Abstract Motors are an important curricular component in freshman and sophomore introduction to mechanical engineering (ME) courses as well as in curricula developed for high school science and robotics clubs. In order to facilitate a hands-on introduction to motors, an inexpensive permanent magnet direct current (PMDC) motor experiment has been developed that gives students an opportunity to build a PMDC motor from common office supplies along with a few inexpensive laboratory components. -
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. -
Exploring the Earth's Magnetic Field
([SORULQJWKH(DUWK·V0DJQHWLF)LHOG $Q,0$*(6DWHOOLWH*XLGHWRWKH0DJQHWRVSKHUH An IMAGE Satellite Guide to Exploring the Earth’s Magnetic Field 1 $FNQRZOHGJPHQWV Dr. James Burch IMAGE Principal Investigator Dr. William Taylor IMAGE Education and Public Outreach Raytheon ITS and NASA Goddard SFC Dr. Sten Odenwald IMAGE Education and Public Outreach Raytheon ITS and NASA Goddard SFC Ms. Annie DiMarco This resource was developed by Greenwood Elementary School the NASA Imager for Brookville, Maryland Magnetopause-to-Auroral Global Exploration (IMAGE) Ms. Susan Higley Cherry Hill Middle School Information about the IMAGE Elkton, Maryland Mission is available at: http://image.gsfc.nasa.gov Mr. Bill Pine http://pluto.space.swri.edu/IMAGE Chaffey High School Resources for teachers and Ontario, California students are available at: Mr. Tom Smith http://image.gsfc.nasa.gov/poetry Briggs-Chaney Middle School Silver Spring, Maryland Cover Artwork: Image of the Earth’s ring current observed by the IMAGE, HENA instrument. Some representative magnetic field lines are shown in white. An IMAGE Satellite Guide to Exploring the Earth’s Magnetic Field 2 &RQWHQWV Chapter 1: What is a Magnet? , *UDGH 3OD\LQJ:LWK0DJQHWLVP ,, *UDGH ([SORULQJ0DJQHWLF)LHOGV ,,, *UDGH ([SORULQJWKH(DUWKDVD0DJQHW ,9 *UDGH (OHFWULFLW\DQG0DJQHWLVP Chapter 2: Investigating Earth’s Magnetism 9 *UDGH *UDGH7KH:DQGHULQJ0DJQHWLF3ROH 9, *UDGH 3ORWWLQJ3RLQWVLQ3RODU&RRUGLQDWHV 9,, *UDGH 0HDVXULQJ'LVWDQFHVRQWKH3RODU0DS 9,,, *UDGH :DQGHULQJ3ROHVLQWKH/DVW<HDUV ,; *UDGH 7KH0DJQHWRVSKHUHDQG8V -
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). -
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. -
Design of a Rail Gun System for Mitigating Disruptions in Fusion Reactors
© Copyright 2017 Wei-Siang Lay Design of a Rail Gun System for Mitigating Disruptions in Fusion Reactors Wei-Siang Lay A thesis submitted in partial fulfillment of the requirements for the degree of Masters of Science University of Washington 2017 Reading Committee: Thomas R. Jarboe, Chair Roger Raman, Thesis Advisor Program Authorized to Offer Degree: Aeronautics & Astronautics University of Washington Abstract Design of a Rail Gun System for Mitigating Disruptions in Fusion Reactors Wei-Siang Lay Chair of the Supervisory Committee: Thomas R. Jarboe Aeronautics & Astronautics Magnetic fusion devices, such as the tokamak, that carry a large amount of current to generate the plasma confining magnetic fields have the potential to lose magnetic stability control. This can lead to a major plasma disruption, which can cause most of the stored plasma energy to be lost to localized regions on the walls, causing severe damage. This is the most important issue for the $20B ITER device (International Thermonuclear Experimental Reactor) that is under construction in France. By injecting radiative materials deep into the plasma, the plasma energy could be dispersed more evenly on the vessel surface thus mitigating the harmful consequences of a disruption. Methods currently planned for ITER rely on the slow expansion of gases to propel the radiative payloads, and they also need to be located far away from the reactor vessel, which further slows down the response time of the system. Rail guns are being developed for aerospace applications, such as for mass transfer from the surface of the moon and asteroids to low earth orbit. A miniatured version of this aerospace technology seems to be particularly well suited to meet the fast time response needs of an ITER disruption mitigation system.