Measuring Permanent Magnet Characteristics with a Fluxmeter and Helmholtz Coil



Similar documents
A METHOD OF CALIBRATING HELMHOLTZ COILS FOR THE MEASUREMENT OF PERMANENT MAGNETS

Permanent Magnet Materials

Physics 221 Experiment 5: Magnetic Fields

CHAPTER 4 DESIGN OF INTEGRAL SLOT AND FRACTIONAL SLOT BRUSHLESS DC MOTOR

Modern Physics Laboratory e/m with Teltron Deflection Tube

Iron Powder Cores for Switchmode Power Supply Inductors. by: Jim Cox

Digital Energy ITI. Instrument Transformer Basic Technical Information and Application

A Comparison of the Measured Magnetic Field Strength Using Ampere-Turns (AT) and millitesla (mt)

Magnetic Field of a Circular Coil Lab 12

ELECTRIC FIELD LINES AND EQUIPOTENTIAL SURFACES

Force on a square loop of current in a uniform B-field.

Application Note. So You Need to Measure Some Inductors?

Chapter 27 Magnetic Field and Magnetic Forces

Physical Specifications (Custom design available.)

Voltage Loss Formula s

Experiment 7: Forces and Torques on Magnetic Dipoles

E/M Experiment: Electrons in a Magnetic Field.

Eðlisfræði 2, vor 2007

Chapter 7. Magnetism and Electromagnetism ISU EE. C.Y. Lee

PERMAGRAPH L. for the computer controlled measurement of hysteresis curves of hard magnetic materials. Introduction.

ABSTRACT 1. INTRODUCTION

An equivalent circuit of a loop antenna.

Demagnetization Studies on Permanent Magnets - Comparing FEM Simulations with Experiments

Massachusetts Institute of Technology Department of Electrical Engineering and Computer Science

Experiment 3: Magnetic Fields of a Bar Magnet and Helmholtz Coil

Review Questions PHYS 2426 Exam 2

Linear DC Motors Magnetic Flux Permanent Bar Magnets

Magnetic Field and Magnetic Forces

How strong are magnets?

Ampere's Law. Introduction. times the current enclosed in that loop: Ampere's Law states that the line integral of B and dl over a closed path is 0

Chapter 16. Current Transformer Design. Copyright 2004 by Marcel Dekker, Inc. All Rights Reserved.

Measurement of Charge-to-Mass (e/m) Ratio for the Electron

Vrieswijk, T & Srinivasan,A Amerongen,NL, 25 januari 2012

Chapter 21. Magnetic Forces and Magnetic Fields

Theory of Heating by Induction

Edmund Li. Where is defined as the mutual inductance between and and has the SI units of Henries (H).

5. Measurement of a magnetic field

Phys222 Winter 2012 Quiz 4 Chapters Name

Coupled Inductors. Introducing Coupled Inductors

E. K. A. ADVANCED PHYSICS LABORATORY PHYSICS 3081, 4051 NUCLEAR MAGNETIC RESONANCE

How to Optimize Performance and Minimize Size in High Speed Applications High Performance Brushless DC Motors

Motor Fundamentals. DC Motor

Insertion Devices Lecture 4 Permanent Magnet Undulators. Jim Clarke ASTeC Daresbury Laboratory

Magnetic electro-mechanical machines

Selecting IHLP Composite Inductors for Non-Isolated Converters Utilizing Vishay s Application Sheet

INDUCTOR DESIGN IN SWITCHING REGULATORS

Homework # Physics 2 for Students of Mechanical Engineering

Circumference of a Circle

Magnetism. d. gives the direction of the force on a charge moving in a magnetic field. b. results in negative charges moving. clockwise.

INSTRUMENTATION AND CONTROL TUTORIAL 2 ELECTRIC ACTUATORS

DIRECT CURRENT GENERATORS

Introduction to Linear Actuators: Precision Linear Motion Accomplished Easily and Economically

Nondestructive Examination (NDE) and Technology Codes Student Manual. Volume 2. Chapter 7.0. Introduction to Magnetic Particle Examination

13 ELECTRIC MOTORS Basic Relations

ELECTRON SPIN RESONANCE Last Revised: July 2007

DC GENERATOR THEORY. LIST the three conditions necessary to induce a voltage into a conductor.

MAG Magnetic Fields revised July 24, 2012

UNDERSTANDING PERMANENT MAGNET MATERIALS; AN ATTEMPT AT UNIVERSAL MAGNETIC LITERACY. S. R. Trout Molycorp Magnequench

Charlesworth School Year Group Maths Targets

Current Probes. User Manual

Toroids. Toroids. Design Considerations

Mutual Inductance and Transformers F3 3. r L = ω o

6/14/02 Chapter 14: Use of Electrical Test Equipment 1/20

Magnet FAQs. Steve Constantinides, Director of Technology Arnold Magnetic Technologies Corporation February 7, Arnold Magnetic Technologies

Physics 41, Winter 1998 Lab 1 - The Current Balance. Theory

AAT001-10E TMR Angle Sensor

Chapter 10. AC Inductor Design. Copyright 2004 by Marcel Dekker, Inc. All Rights Reserved.

CHAPTER 2 HYDRAULICS OF SEWERS

Magnetic Fields. I. Magnetic Field and Magnetic Field Lines

RICHARD T ELL ASSOCIATES,INC.

Magnetic Media Measurements with a VSM

Introduction to Beam. Area Moments of Inertia, Deflection, and Volumes of Beams

HPS Universal. Single and Three Phase Potted. Buck-Boost Transformers. Buck-Boost Applications & Standard Specification... 80

Chapter 15: Transformer design

Chapter 14: Inductor design

Fatigue Analysis of an Inline Skate Axel

Direction of Induced Current

2. Permanent Magnet (De-) Magnetization 2.1 Methodology

Force on Moving Charges in a Magnetic Field

Application Notes. Magnetics. Determining L min for Buck/Boost Converters

Objectives. Capacitors 262 CHAPTER 5 ENERGY

Chapter 22 Magnetism

1. The diagram below represents magnetic lines of force within a region of space.

Pre-lab Quiz/PHYS 224 Magnetic Force and Current Balance. Your name Lab section

Optimum proportions for the design of suspension bridge

Drive circuit basics + V. τ e. Industrial Circuits Application Note. Winding resistance and inductance

Perimeter. 14ft. 5ft. 11ft.

HOW ACCURATE ARE THOSE THERMOCOUPLES?

All I Ever Wanted to Know About Circles

Coupling Magnetic Signals to a SQUID Amplifier

Pennsylvania System of School Assessment

Application Information

Magnetic Circuits. Outline. Ampere s Law Revisited Review of Last Time: Magnetic Materials Magnetic Circuits Examples

Preview of Period 16: Motors and Generators

Electric Motors and Drives

Simple Analysis for Brushless DC Motors Case Study: Razor Scooter Wheel Motor

Guide to Magnet Design

Eðlisfræði 2, vor 2007

Chapter 19: Magnetic Forces and Fields

Physics 25 Exam 3 November 3, 2009

Transcription:

Measuring Permanent Magnet Characteristics with a Fluxmeter and Helmholtz Coil Lake Shore Cryotronics, Inc., 10/00

Measuring Permanent Magnet Characteristics with a Fluxmeter and Helmholtz Coil General Measurement of magnetic moment with a fluxmeter and a Helmholtz coil is a convenient way to test permanent magnet materials. Other values such as operating flux density ( d ), operating field strength ( ), coercive force (H c ), residual flux density ( ), and maximum energy product (H max ) can be derived from the measured moment value. Although this method is not as accurate as hysteresisgraph measurement, the measurement process is easy, values are useful and reliable, and equipment cost is substantially less. Making the Moment Measurement Features of Lake Shore's Model 480 Fluxmeter and Helmholtz coil simplify the measurement process. The Model 480 Fluxmeter automatically retrieves coil resistance and Helmholtz constant from a PROM in the coil connector at power-up. Only two fluxmeter settings are needed: RANGE and selection of units in MOMENT weber centimeters. When used with a Helmholtz coil, a fluxmeter provides a value for the magnetic moment of a test sample when the magnet is placed between the coils in alignment with the coil axis and rotated 180 degrees or withdrawn. The Model 480 easily accommodates magnetic moment measurement with single sample extraction, double extraction with sample rotation, or rotation of the sample within the coil. Reliable measurement is more a function of consistent adherence to a documented test procedure and operator comfort with the measurement method than selecting a superior test method. Record this value for use in subsequent calculations. The fluxmeter and Helmholtz coil can also be used with a non-magnetic sample fixture to ensure consistent testing of samples in series. Model 480 Fluxmeter FH-6 Helmholtz Coil

Recoil Permeability and Permeance Coefficient Values In adtion to the measured magnetic moment value, recoil permeability (µ rec ) and permeance coefficient ( d / ) values for the tested magnet are required for subsequent calculations. Recoil permeability is available from the magnet vendor specification sheet. Permeance coefficient is a function of magnet geometry such as length and ameter. The specific permeance coefficient for a particular magnet can be obtained from published equations or charts; for example, see Rollin J. Parker's Advances in Permanent Magnetism (John Wiley and Sons, 1990). The magnetic length used in these formulas is not always the physical length of the magnet. For constant cross-section, high coercivity magnets, magnetic and physical lengths can be assumed to be equal. For alnico magnets, magnetic length is about 70% of the magnet's physical length. Figure 1 is a graphical representation of the formulas that follow: Slope: Recoil Permeability d -H ci -H c Slope d Figure 1: The second quadrant

Deriving Intrinsic Flux Density The magnetic moment of interest in permanent magnet testing is generally defined as the intrinsic flux density per unit volume of magnet. ased on the magnetic moment measurement and measured magnet volume, intrinsic flux density,, can be calculated. Moment weber cm Volume cm 3 weber 2 cm For convenience in calculations, convert webers per cm 2 to gauss: Moment Volume weber cm 10 8 3 cm gauss Calculate Normal Operating Point (Field Strength) H d (PermeanceCoeff + 1) (oersteds) Calculate Normal Operating Point (Flux Density) d H d (gauss) Calculate Residual Flux Density (RecoilPerm + PermeanceCoeff) (PermeanceCoeff + 1) (gauss)

Calculate coercive force (straight line approximation) This value will be inaccurate if the magnet material exhibits a substantial knee in the second quadrant. µ rec Recoil Permeability H c µ rec (oersteds) Calculate Magnet Maximum Energy Product (H) max 2 4µ rec (gauss oersted) Example Actual measured and calculated values for a grade 27 neodymium-ironboron magnet are shown below. The magnet is 0.375 inches in ameter by 0.125 inches long for a magnet volume of 0.226 cm 3. The vendor values are: H c 9650 oersteds 10850 gauss H max 27 x 10 6 gauss oersteds Recoil Permeability 1.1 ased on a length to ameter ratio of 0.333, the permeance coefficient is 0.861. Using a Model 480 Fluxmeter and FH-6 Helmholtz coil, the sample's magnetic moment is measured: m 23.26 µ weber cm [23.26 x 10-6 wb cm / 0.226 cm 3 ] x 10 8 10,292 gauss 10,292 / (0.861 + 1) 5530 oersteds d 10,292 5530 4762 gauss

d 26.33 x 10 6 gauss oersteds (operating energy product) [10,292 (1.1 + 0.861)] / (0.861 + 1) 10,845 gauss H c 10845 / 1.1 9859 oersteds Designing and Fabricating a Helmholtz Coil Lake Shore's Helmholtz coils are easy to use and include factory calibration. For applications where local fabrication of a coil set is preferred, design parameters to construct, wind, and calibrate a Helmholtz coil are included here. Final coil ameter is often determined by available materials. Engineering plastics are very expensive for coil ameters exceeng 4 inches. Some heavy schedule PVC drainpipe can be adapted to construct a double coil form. Figure 2 illustrates design rules relative to coil and test sample size. W NO DIMENSION OF THE COIL CROSS-SECTION SHOULD EXCEED 1/10 OF THE COIL DIAMETER. M R W AVERAGE COIL RADIUS NO MAGNET DIMENSION SHOULD EXCEED 1/3 OF THE COIL DIAMETER. INDIVIDUAL, CIRCULAR COILS OF "N" TURNS EACH. Figure 2: Helmholtz coil design rules The Helmholtz coil constant, K, for a locally fabricated coil can either be calculated using the following formulas or measured. The calculated value offers accuracy of 5 to 10% when the coils are wound with normal care. Helmholtz constants are expressed in weber centimeters per volt second, which can be reduced to centimeters; the Model 480 Fluxmeter is designed for input of the Helmholtz coil constant in centimeters.

N Number of Turns in Each Coil R Average Coil Raus If R is in centimeters, R K 1.397 (cm) N If R is in inches, R K 3.548 (cm) N For greater accuracy, the Helmholtz constant can be derived from a gaussmeter reang of the magnetic field generated when a DC current is applied to the coil. CAUTION: Ensure that the applied current does not exceed the rating for the size of the coil wire. Accuracy depends on the instruments used and the care taken in orienting the gaussmeter probe in the center of the coil set. Accuracy to better than 1% is possible. Accurate measurement of the field generated per current supplied results in a value sometimes referred to as coil sensitivity. If coil sensitivity is expressed as gauss per ampere, 1.256 K (cm) coil sens. If the coil sensitivity is in millitesla per ampere, 0.1256 K (cm) coil sens. Lake Shore Cryotronics, Inc., 10/00