Magnetic Particles Testing (MT) Technique

Size: px
Start display at page:

Download "Magnetic Particles Testing (MT) Technique"

Transcription

1 Research Group Magnetic Particles Testing (MT) Technique Professor Pedro Vilaça * * Contacts: Address: Puumiehenkuja 3 (room 202), Espoo, Finland pedro.vilaca@aalto.fi October 2017 Contents Historical scope of magnetic particles testing (MT) technique Fundaments of the MT technique Sequence of phases in the application of the MT technique Fundaments of electromagnetism supporting the MT technique Detailed characterization of each of the application phases Classification of the magnetization methods Classification of the electric current in induced magnetic fields Classification of the magnetization equipment Classification of the application of the magnetic particles Method of demagnetization 2 1

2 Learning Outcomes At the end of the seminar the student should be able to: To establish the fundaments To characterize each of the application phases To classify and select the magnetization methods To select the electric current in induced magnetic fields To classify and select the magnetization equipment To classify and select the application method and condition of the magnetic particles To characterize the method of demagnetization 3 Introduction What is the historical scope of the Magnetic Particles Testing (MT) technique? The method appeared in the USA around It was only after World War II ( ) that it expanded as a method of NDT What are the main target application focus and materials of the Magnetic Particles Testing (MT) technique? Detection of superficial and subsuperficial defects Ferromagnetic materials (e.g. steels, alloys of nickel and cobalt) 4 2

3 Fundaments of the Technique What are the fundaments of the Magnetic Particles Testing (MT) technique? The detection of defects is based on the fact that the magnetic particles are attracted to the areas with magnetic flux leakage resulting from defects in the component being subjected to a magnetic field Magnetic particles cumulated due to magnetic flux leakage 5 Fundaments of the Technique What are the main phases in the application of the Magnetic Particles Testing (MT) technique? 1. Surface preparation (cleaning) 2. Magnetization of the component 3. Application of the magnetic particles 4. Inspection 5. Demagnetization 6. Cleaning of residues from the MT 6 3

4 Fundaments from the Electromagnetism The magnetic Flux Density (B) [Tesla] is defined as: The magnetic Flux Density (B) is the number of flux lines per unit of area produced by the material upon the application of a magnetic Field Strength (H) [A/m], i.e. external applied magnetic field that does not depend on the medium. B B H H Absolute magnetic Permeability (µ), measures the resistance of the material to be magnetized, and is defined as: µ = µ 0 x µ r Permeability of iron Where: Constant magnetic permeability: µ 0 = 4π 10 7 H m H m 1 or N A 2 ) corresponds to the permeability of free space (i.e. is a measure of the amount of resistance encountered when forming a magnetic field in a classical vacuum) Relative magnetic permeability: µ r - Unlike µ 0, µ r is not constant and changes with magnetic flux density B. Also, if the temperature is increased then typical there is a drop in permeability 7 Fundaments from the Electromagnetism Ferromagnetic Materials: Permeability (μ) > 1 Materials such as iron, nickel or cobalt, which are strongly attracted to magnets and can be magnetized. Some of the atoms or ions in material have a net magnetic moment due to unpaired electrons in partially filled orbitals. However, the individual magnetic moments do not interact magnetically, and magnetization is zero when the field is removed. In the presence of a field, there is now a partial alignment of the atomic magnetic moments in the direction of the field, resulting in a net positive magnetization and positive susceptibility Paramagnetic Materials : Permeability (μ) = 1 Materials such as austenitic steel, aluminum, tin, which are little attracted by magnetic forces, and can not be magnetized Diamagnetic Materials: Permeability (μ) < 1 Materials such as silver, zinc, lead, which are slightly repelled by magnetic forces, and can not be magnetized. It is due to the non-cooperative behavior of orbiting electrons when exposed to an applied magnetic field. These substances are composed of atoms which have no net magnetic moments (all the orbital shells are filled and there are no unpaired electrons). However, when exposed to a field, a negative magnetization is produced and thus susceptibility is negative 8 4

5 Fundaments from the Electromagnetism Magnetic Retentivity - the ability of a substance to retain or resist magnetization, frequently measured as the strength of the magnetic field that remains in a sample after removal of an inducing field "iron is easily magnetized but has low retentivity Lorentz Force, (F) [N] The magnetic Flux Density B, is related to the Lorentz force F, on a moving charge q (in Coulombs, C), with speed v (in meters per second, m/s): m V. s C.( J / C) F q( E v B) q( v B) C.. 2 s m m J m N 9 Fundaments from the Electromagnetism Magnetic Flux leakage - magnetic lines of force that flow out of the intended path in a magnetic circuit, due to a imperfection Biot-Savart law - relates the magnetic field generated due to the magnitude, direction, length, and proximity of the electric current. The law is valid in magnetostatic conditions db P I 4 r 2 ds grad P r 10 5

6 Phase 1: Surface Preparation The components to be inspected shall be cleaned in order not to jeopardize the efficiency of the PM inspection The same cleaning procedures applied to die Penetrant testing (PT) are normally used in MT although the result of MT are less sensitive to this phase, than the results of PT. WHY? Cleaning methods: - Alkaline: to remove organic materials. Typically by emersion - Acid: to remove oxides, calamines, and corrosion products. Careful to avoid the attack of the base materials. - With detergents: adhere to the dirty particles facilitating their removal - With solvents: to remove oils, masses, waxes and paints. A post-cleaning operation with detergent should be made - With vapor: typically in degassing tanks with solvent vapor - Ultrasonic: combining mechanical stirring with solvents or detergent. Suitable for removing contaminants inside defects - With bath salts: e.g. caustic soda (sodium hydroxide (NaOH)) to remove oxides and calamines. The exothermic reaction facilitates the oxide removal - Mechanical: sand blasting, blasting, wire brushes, etc. This method is not so critical to be applied in MT as in Die Penetrant Testing (PT). WHY? 11 Classification It consists of subjecting the component to a magnetic field of known intensity and direction, according to the following different methods: 12 6

7 Portability: typically applied when there is no power source available Field inspection or when there is a fire hazard Impossibility to magnetize large surfaces Impossibility to adjust the intensity of the magnetic field Permanent magnets 13 Electromagnets Made of a nucleus of plain steel in U shape with one coil of current carrying wire With YOKES It is possible to vary the intensity of the magnetic field Can be switched on and off, which facilitates aplication and removal 14 7

8 Electromagnets Application of YOKES with adjustable legs Portable Power Supplies for YOKES 15 By direct contact Only imperfections aligned with the current are possible to detect Circular magnetization induced by electric current In this case the current flows through the components 16 8

9 Only imperfections aligned with the current are possible to detect Circular magnetization induced by electric current In this case the current flows a copper shaft Good to inspect hollow components 17 Magnetization by single prod contacts: Circular magnetization induced by electric current 18 9

10 Only imperfections aligned with the current are possible to detect Longitudinal magnetization induced by electric current 19 Only imperfections aligned with the current are possible to detect Multidirectional magnetization induced by electric current 20 10

11 What kind of electric current is used? Direct Current (DC) Generates magnetic fields with higher penetration Better for subsuperficial defects Demands the magnetic particles to be applied via wet suspension The application of magnetic particles via dry do not have enough mobility to be sensitive to eventual magnetic leak flux induced by DC Magnetization induced by electric current typical value of electric currents : A 21 What kind of electric current is used? Alternating Current (AC) Range of frequencies: Hz Magnetization induced by electric current Generates magnetic fields with less penetration, due to the skin effect of AC. This effect is more relevant as the frequency increases Generates alternating magnetic fields that promote the agitation of the magnetic particles and consequently their mobility Better for superficial defects Enables the application of dry magnetic particles typical value of electric currents : A 22 11

12 Half wave rectified AC High penetration compared with AC, enabling to detect subsuperficial defects Promote similar mobility of magnetic particles as in AC Couples advantages of DC + AC Magnetization induced by electric current Full wave rectified AC Even higher penetration Less mobility of the magnetic particles 23 Selection of equipment depends on: Type of Component (namely: material, dimension, shape) Local of Inspection Portable equipment: Magnetization equipments 24 12

13 Fixed equipment: Tank with magnetic particles Coil for longitudinal magnetization Copper shat for longitudinal magnetization Control panel and power source with variable current (e.g A) Adjustable for components of different dimension Magnetization equipments 25 Phase 3: Application of the magnetic particles Classification 26 13

14 Phase 3: Application of the magnetic particles The magnetic particles are made of ferromagnetic materials: Iron and /or iron oxide Characteristics of the magnetic particles The main properties of the magnetic particles (MPs) are: Dimension (from 10 to 30 m) Strong influence on their behavior (mobility) A weak magnetic field attracts and retains better smaller MPs But small MPs can adhere to rough surfaces, reducing the mobility For this reason the MPs consist of a set of several granulometries: o The smaller ones increase the sensitivity and mobility of the set o The larger ones overcome the trend of the set to adhere to the surface 27 Phase 3: Application of the magnetic particles Characteristics of the magnetic particles The main properties of the magnetic particles (MPs) are: (cont.) Shape (Spherical or Elongated, e.g. needle) Elongated MPs are more likely to line up along force lines The spherical shape have better mobility Permeability Should be high as possible Retentivity Should be low as possible 28 14

15 Phase 3: Application of the magnetic particles The main properties of the magnetic particles (MPs) are: (cont.) Mobility When applying the MPs in Dry conditions the mobility should be increased by: o Vibrating the component o Using AC or Rectified AC o When applying the MPs via Wet suspension the viscosity of the suspension should be carefully considered Visibility (e.g. contrast) Colors for best contrast to the piece: red, yellow, black or white. Fluorescent pigments (demand the application of black light) Characteristics of the magnetic particles 29 Phase 3: Application of the magnetic particles In this case the MPs are supplied in powder form and have different colors The application can be done by sprayers or gun projectors On vertical surfaces or overhead position the leak flux must overcome gravity Advantages: Easy to apply on large parts; Portable equipment; Cleaner Disadvantages: More difficult to apply to complex geometries Difficult to automatize Magnetic particles Dry type of application 30 15

16 Phase 3: Application of the magnetic particles In this case the MPs are in suspension in water or Magnetic particles petroleum products The suspension needs to be stirred to keep the particles Wet Suspension uniformly distributed, but the stirring may also remove the particles attracted by small intensity magnetic fields type of application (e.g. subsuperficial defects and small defects) The suspension includes additives (e.g. corrosion inhibitors, wetting agents) The concentration of the MPs suspension ranges from 0.1 to 2 ml / 100 ml The application can be made: By pouring the suspension into the part By immersing the part in tanks with automated circulation systems Through pressurized packaging Advantages: Good mobility of the MPs in suspension Easy automatization and application to complex shapes Disadvantages: May demand more complex equipment 31 Phase 3: Application of the magnetic particles Continuous method The MPs are applied during the flow of magnetization current: The magnetic field is of high intensity More sensitive in the detection of subsuperficial and small superficial defects 32 16

17 Phase 3: Application of the magnetic particles Residual method The MPs are applied after ending the flow of magnetization current: It is only possible to apply to materials with some retention In these conditions the magnetic field is of small intensity It is not used to detect subsuperficial defects When using a central conductor for induction of the circular magnetic field, the accessibility for inspection increases significantly 33 Phase 4: Inspection, Analysis and Registration Inspector should have knowledge on the production engineering: Inspector should: Distinguish from relevant and non-relevant indications e.g. the ones produced by distortions of the magnetic field Proceed with the registration of the relevant indications, using: o transparent vernish or adhesive tape, photographs 34 17

18 Phase 5: Demagnetization It becomes necessary to demagnetize the component if: It interferes with in-service behavior in general May affect instrumentation or interfere with welding operations It may not be necessary to demagnetize if: The material has low retentivity The parts are subsequently subjected to temperatures above the Curie point 35 Phase 5: Demagnetization Most common method: Subjecting the magnetized part to a magnetic flux that continually reverses direction and decreases in intensity Typical Hysteresis cycles produced during the demagnetization operation: To verify the residual magnetic fields, it is typically applied: Hall effect probe 36 18

19 Phase 5: Demagnetization F m rv db B dx 0 37 Phase 5: Demagnetization 38 19

MAGNETIC PARTICLE INSPECTION (MPI)

MAGNETIC PARTICLE INSPECTION (MPI) MAGNETIC PARTICLE INSPECTION (MPI) Magnetic particle inspection (MPI) is a method that can be used to detect surface and near surface defects or flaws in ferromagnetic materials such as steel and iron.

More information

MAGNETISM. Magnetism. Magnetism is a result of electrons spinning on their own axis around the nucleus (Figure 18). Basic Electrical Theory

MAGNETISM. Magnetism. Magnetism is a result of electrons spinning on their own axis around the nucleus (Figure 18). Basic Electrical Theory Basic Electrical Theory Certain metals and metallic oxides have the ability to attract other metals. This property is called magnetism, and the materials which have this property are called magnets. Some

More information

Electromagnetic fields Learning outcome

Electromagnetic fields Learning outcome Electromagnetic fields Learning outcome At the end of this lecture you will be able to: List the most important electromagnetic field quantities Explain what these quantities describe Calculate some of

More information

Non-destructive testing of steel forgings- Part 1: Magnetic particle inspection (BS EN :1999)

Non-destructive testing of steel forgings- Part 1: Magnetic particle inspection (BS EN :1999) Non-destructive testing of steel forgings- Part 1: Magnetic particle inspection (BS EN 10228-1:1999) 1 Scope This part of EN 10228 describes the method and acceptance criteria to be used for the magnetic

More information

Chapter 13 Principles of Electromechanics

Chapter 13 Principles of Electromechanics Chapter 13 Principles of Electromechanics Jaesung Jang Electrostatics B-H Magnetization Curves & Magnetic Hysteresis 1 Electrostatics & Magnetic Flux The force on a stationary charge q in an electric field

More information

CHAPTER 2 MAGNETISM. 2.1 Magnetic materials

CHAPTER 2 MAGNETISM. 2.1 Magnetic materials CHAPTER 2 MAGNETISM Magnetism plays a crucial role in the development of memories for mass storage, and in sensors to name a few. Spintronics is an integration of the magnetic material with semiconductor

More information

Electric vs Magnetic Comparison

Electric vs Magnetic Comparison 5. MAGNETOSTATICS Electric vs Magnetic Comparison J=σE Most dielectrics µ = µo excluding ferromagnetic materials Gauss s Law E field is conservative Gauss s law (integral) Conservative E field Electric

More information

Chapter 14. Optical and Magnetic Materials. 경상대학교 Ceramic Design Lab.

Chapter 14. Optical and Magnetic Materials. 경상대학교 Ceramic Design Lab. Chapter 14 Optical and Magnetic Materials Magnetic field strength = H H = Ni/l (amp-turns/m) N = # turns i = current, amps l = conductor length B = Magnetic Induction or Magnetic flux density (Wb/m 2 )

More information

Physics 12. Unit 8 Magnetic Field and Electromagnetism Part I

Physics 12. Unit 8 Magnetic Field and Electromagnetism Part I Physics 12 Unit 8 Magnetic Field and Electromagnetism Part I 1. Basics about magnets Magnets have been known by ancient people since long time ago, referring to the iron-rich rocks, called magnetite or

More information

EDDY CURRENT TESTING

EDDY CURRENT TESTING EDDY CURRENT TESTING Introduction Eddy current inspection is a method that use the principal of electromagnetism as the basis for conducting examinations. Eddy Current NDT is a technique that can test

More information

B for a Long, Straight Conductor, Special Case. If the conductor is an infinitely long, straight wire, θ 1 = 0 and θ 2 = π The field becomes

B for a Long, Straight Conductor, Special Case. If the conductor is an infinitely long, straight wire, θ 1 = 0 and θ 2 = π The field becomes B for a Long, Straight Conductor, Special Case If the conductor is an infinitely long, straight wire, θ 1 = 0 and θ 2 = π The field becomes μ I B = o 2πa B for a Curved Wire Segment Find the field at point

More information

Displacement Current. Ampere s law in the original form is valid only if any electric fields present are constant in time

Displacement Current. Ampere s law in the original form is valid only if any electric fields present are constant in time Displacement Current Ampere s law in the original form is valid only if any electric fields present are constant in time Maxwell modified the law to include timesaving electric fields Maxwell added an

More information

Magnetostatics III. P.Ravindran, PHY041: Electricity & Magnetism 1 January 2013: Magntostatics

Magnetostatics III. P.Ravindran, PHY041: Electricity & Magnetism 1 January 2013: Magntostatics Magnetostatics III Magnetization All magnetic phenomena are due to motion of the electric charges present in that material. A piece of magnetic material on an atomic scale have tiny currents due to electrons

More information

Types of Magnetism and Magnetic Domains

Types of Magnetism and Magnetic Domains Types of Magnetism and Magnetic Domains Magnets or objects with a Magnetic Moment A magnet is an object or material that attracts certain metals, such as iron, nickel and cobalt. It can also attract or

More information

MAGNETIC FIELDS & UNIFORM PLANE WAVES

MAGNETIC FIELDS & UNIFORM PLANE WAVES MAGNETIC FIELDS & UNIFORM PLANE WAVES Name Section Multiple Choice 1. (8 Pts) 2. (8 Pts) 3. (8 Pts) 4. (8 Pts) 5. (8 Pts) Notes: 1. In the multiple choice questions, each question may have more than one

More information

~~r ~o~/, ' , I. l: z: n.-b -z 01. ?;Cl. 60) Pro CD'fCJ7 '; ftu-0j~

~~r ~o~/, ' , I. l: z: n.-b -z 01. ?;Cl. 60) Pro CD'fCJ7 '; ftu-0j~ i -1- ~~r ~o~/, ------', I l: z: n.-b -z 01?;Cl 60) 1---.-- Pro CD'fCJ7 '; ftu-0j~ APPLICATIONS 1/ What features of atomic structure determine whether an element is diamagnetic or paramagnetic? Explain.

More information

Chapter 5. Magnetism and Matter

Chapter 5. Magnetism and Matter Chapter 5 Magnetism and Matter TABLE 5.1 THE DIPOLE ANALO Diamagnetic materials, when placed in a magnetic field, are magnetized in the direction opposite to the magnetic field; whereas paramagnetic and

More information

The initial magnetization curve shows the magnetic flux density that would result when an increasing magnetic field is applied to an initially

The initial magnetization curve shows the magnetic flux density that would result when an increasing magnetic field is applied to an initially MAGNETIC CIRCUITS The study of magnetic circuits is important in the study of energy systems since the operation of key components such as transformers and rotating machines (DC machines, induction machines,

More information

Sources of Magnetic Field

Sources of Magnetic Field Chapter 28 Sources of Magnetic Field PowerPoint Lectures for University Physics, 14th Edition Hugh D. Young and Roger A. Freedman Lectures by Jason Harlow Learning Goals for Chapter 28 Looking forward

More information

Magnetic materials, & inductance & Torque. P.Ravindran, PHY041: Electricity & Magnetism 8 February 2013: Magnetic materials, inductance, and torque

Magnetic materials, & inductance & Torque. P.Ravindran, PHY041: Electricity & Magnetism 8 February 2013: Magnetic materials, inductance, and torque Magnetic materials, & inductance & Torque Magnetic Properties of Materials Magnetic behavior of a material is due to the interaction of magnetic dipole moments of its atoms with an external magnetic field.

More information

Detection of Wear in Oilwell Service Tubings using Magnetic Flux Leakage

Detection of Wear in Oilwell Service Tubings using Magnetic Flux Leakage Detection of Wear in Oilwell Service Tubings using Magnetic Flux Leakage Many methods have been developed and used for the inspection of oilwell service tubings to find wear, corrosion and fractures. One

More information

Electromagnetic Testing (ET)

Electromagnetic Testing (ET) Electromagnetic Testing Electromagnetic testing is a general test category that includes Eddy Current testing (ECT), Alternating Current Field Measurement (ACFM) and Remote Field testing. All of these

More information

Magnetic Fields INTRODUCTION. The Hall Effect

Magnetic Fields INTRODUCTION. The Hall Effect Magnetic Fields INTRODUCTION This experiment concerns magnetic forces and fields. You will examine magnetic field lines and forces qualitatively, and measure field strengths using a Hall probe. A magnaprobe

More information

Chapter 1 Updated: 1/22/12

Chapter 1 Updated: 1/22/12 ES 430 Electromagnetic Chapter 1 Updated: 1/22/12 General Notes A2 SI Units SI Prefixes Vectors Appendix A, pp. 473 Applications of EM Evolution of Electromagnetic Electromagnetic: Static or Dynamic (time

More information

Magnetic Force on a Moving Charge

Magnetic Force on a Moving Charge Magnetic Force on a Moving Charge Electric charges moving in a magnetic field experience a force due to the magnetic field. Given a charge Q moving with velocity u in a magnetic flux density B, the vector

More information

12:40-2:40 3:00-4:00 PM

12:40-2:40 3:00-4:00 PM PHY294H l Professor: Joey Huston l email:huston@msu.edu l office: BPS3230 l Homework will be with Mastering Physics (and an average of 1 handwritten problem per week) Help-room hours: 12:40-2:40 Monday

More information

Electromagnetism. Kevin Gaughan for. Bristol Myers Squibb

Electromagnetism. Kevin Gaughan for. Bristol Myers Squibb Electromagnetism Kevin Gaughan for Bristol Myers Squibb Contents Magnets and Ferromagnetism Domains Theory H, B and µ The links between electricity and Magnetism Electromagnets Induction Applications of

More information

Winmeen Tnpsc Group 1 & 2 Self Preparation Course Physics UNIT 10. Magnetism

Winmeen Tnpsc Group 1 & 2 Self Preparation Course Physics UNIT 10. Magnetism Physics UNIT 10 Magnetism The word magnetism is derived from iron ore magnetite (Fe3O4), which was found in the island of magnesia in Greece. It was Gilbert who laid the foundation for magnetism and had

More information

Physics 202, Lecture 14

Physics 202, Lecture 14 Physics 202, Lecture 14 Today s Topics Sources of the Magnetic Field (Ch. 30) Review: iot-savart Law, Ampere s Law Displacement Current: Ampere-Maxwell Law Magnetism in Matter Maxwell s Equations (prelude)

More information

FLUXA-CONTROL: AN AUTOMATED MONITORING OF FLUORESCENT PARTICLES IN MAGNETIC PARTICLE TESTING

FLUXA-CONTROL: AN AUTOMATED MONITORING OF FLUORESCENT PARTICLES IN MAGNETIC PARTICLE TESTING We 2.6.1 FLUXA-CONTROL: AN AUTOMATED MONITORING OF FLUORESCENT PARTICLES IN MAGNETIC PARTICLE TESTING V. Schuster, V. Deutsch, W. A. K. Deutsch, F. Bartholomai, P. Müller info@karldeutsch.de, www.karldeutsch.de

More information

However, in matter, magnetic induction depends on magnetization M in the following way:

However, in matter, magnetic induction depends on magnetization M in the following way: G1. Magnetic Hysteresis Cycle I. OBJECTIVE OF THE EXPERIMENT Magnetic materials are very important in technological fields, and have many different uses. The objective of the experiment is to study a few

More information

Ch. 28: Sources of Magnetic Fields

Ch. 28: Sources of Magnetic Fields Ch. 28: Sources of Magnetic Fields Electric Currents Create Magnetic Fields A long, straight wire A current loop A solenoid Slide 24-14 Biot-Savart Law Current produces a magnetic field The Biot-Savart

More information

Magnetic Field Lines for a Loop

Magnetic Field Lines for a Loop Magnetic Field Lines for a Loop Figure (a) shows the magnetic field lines surrounding a current loop Figure (b) shows the field lines in the iron filings Figure (c) compares the field lines to that of

More information

Magnetism & Electromagnetism

Magnetism & Electromagnetism Magnetism & Electromagnetism By: Dr Rosemizi Abd Rahim Click here to watch the magnetism and electromagnetism animation video http://rmz4567.blogspot.my/2013/02/electrical-engineering.html 1 Learning Outcomes

More information

Current Loop as a Magnetic Dipole & Dipole Moment:

Current Loop as a Magnetic Dipole & Dipole Moment: MAGNETISM 1. Bar Magnet and its properties 2. Current Loop as a Magnetic Dipole and Dipole Moment 3. Current Solenoid equivalent to Bar Magnet 4. Bar Magnet and it Dipole Moment 5. Coulomb s Law in Magnetism

More information

Key Contents. Magnetic fields and the Lorentz force. Magnetic force on current. Ampere s law. The Hall effect

Key Contents. Magnetic fields and the Lorentz force. Magnetic force on current. Ampere s law. The Hall effect Magnetic Fields Key Contents Magnetic fields and the Lorentz force The Hall effect Magnetic force on current The magnetic dipole moment Biot-Savart law Ampere s law The magnetic dipole field What is a

More information

MAGNETIC PROBLEMS. (d) Sketch B as a function of d clearly showing the value for maximum value of B.

MAGNETIC PROBLEMS. (d) Sketch B as a function of d clearly showing the value for maximum value of B. PHYS2012/2912 MAGNETC PROBLEMS M014 You can investigate the behaviour of a toroidal (dough nut shape) electromagnet by changing the core material (magnetic susceptibility m ) and the length d of the air

More information

MAGNETIC DIPOLES, HYSTERESIS AND CORE LOSES

MAGNETIC DIPOLES, HYSTERESIS AND CORE LOSES Power Quality For The Digital Age MAGNETIC DIPOLES, HYSTERESIS AND CORE LOSES A N E N V I R O N M E N T A L P O T E N T I A L S W H I T E P A P E R By Professor Edward Price Director of Research and Development

More information

Faraday s Law of Induction I

Faraday s Law of Induction I Faraday s Law of Induction I Physics 2415 Lecture 19 Michael Fowler, UVa Today s Topics Magnetic Permeability Faraday s Law of Induction Lenz s Law Paramagnets and Diamagnets Electromagnets Electromagnets

More information

2. When the current flowing through a wire loop is halved, its magnetic moment will become a. half. b. one-fourth. c. double. d. quadruple.

2. When the current flowing through a wire loop is halved, its magnetic moment will become a. half. b. one-fourth. c. double. d. quadruple. 13 1. When a magnetic needle is kept in a uniform magnetic field, it experiences a. neither a force nor a torque. b. a force and not a torque. c. a torque and a force. d. only a torque.. Magnetic lines

More information

Ferromagnetism. In free space, the flux density and magnetizing field strength are related by the expression

Ferromagnetism. In free space, the flux density and magnetizing field strength are related by the expression 1 Ferromagnetism B In free space, the flux density and magnetizing field strength are related by the expression H B =µ 0 H µ 0 =4π x 10-7 H.m -1, the permeability of free space. 2 Ferromagnetism B H For

More information

MAGNETIC FIELDS AND UNIFORM PLANE WAVES

MAGNETIC FIELDS AND UNIFORM PLANE WAVES MAGNETIC FIELDS AND UNIFORM PLANE WAVES Name Section 1. (8 Pts) 2. (8 Pts) 3. (8 Pts) 4. (6 Pts) 5. (6 Pts) 6. (4 Pts) 7. (20 Pts) 8. (20 Pts) 9. (20 Pts) Total Notes: 1. Please read over all questions

More information

MODULE 4.2 MAGNETISM ELECTRIC CURRENTS AND MAGNETISIM VISUAL PHYSICS ONLINE

MODULE 4.2 MAGNETISM ELECTRIC CURRENTS AND MAGNETISIM VISUAL PHYSICS ONLINE VISUAL PHYSICS ONLINE MODULE 4.2 MAGNETISM ELECTRIC CURRENTS AND MAGNETISIM When electric charges are in motion they exert forces on each other that can t be explained by Coulomb s law. If two parallel

More information

Physics 1402: Lecture 17 Today s Agenda

Physics 1402: Lecture 17 Today s Agenda Physics 1402: Lecture 17 Today s Agenda Announcements: Midterm 1 distributed today Homework 05 due Friday Magnetism Trajectory in Constant B Field Suppose charge q enters B field with velocity v as shown

More information

Magnetism. a) Ferromagnetic materials are strongly attracted to magnets. b) Paramagnetic materials are weakly attracted to magnets

Magnetism. a) Ferromagnetic materials are strongly attracted to magnets. b) Paramagnetic materials are weakly attracted to magnets Magnetism Types of Magnetic Materials Magnetic substances can be classified into three basic groups, according to their response to a magnet. Note the strength and direction of the interaction. a) Ferromagnetic

More information

Physics 202, Lecture 14

Physics 202, Lecture 14 Physics 202, Lecture 14 Today s Topics Sources of the Magnetic Field (Ch. 27) Review of Biot-Savart Law Ampere s Law Magnetism in Matter Magnetic Fields (Biot-Savart): Summary Current loop, distance on

More information

Magnetic Quantities. Magnetic fields are described by drawing flux lines that represent the magnetic field.

Magnetic Quantities. Magnetic fields are described by drawing flux lines that represent the magnetic field. Chapter 7 Magnetic fields are described by drawing flux lines that represent the magnetic field. Where lines are close together, the flux density is higher. Where lines are further apart, the flux density

More information

CHAPTER 20 Magnetism

CHAPTER 20 Magnetism CHAPTER 20 Magnetism Units Magnets and Magnetic Fields Electric Currents Produce Magnetic Fields Force on an Electric Current in a Magnetic Field; Definition of B Force on Electric Charge Moving in a Magnetic

More information

Torque on a Current Loop

Torque on a Current Loop Today Chapter 19 Magnetism Torque on a current loop, electrical motor Magnetic field around a current carrying wire. Ampere s law Solenoid Material magnetism Clicker 1 Which of the following is wrong?

More information

Chapter 21. Magnetism

Chapter 21. Magnetism Chapter 21 Magnetism Magnets Poles of a magnet are the ends where objects are most strongly attracted Two poles, called north and south Like poles repel each other and unlike poles attract each other Similar

More information

CHETTINAD COLLEGE OF ENGINEERING & TECHNOLOGY NH-67, TRICHY MAIN ROAD, PULIYUR, C.F , KARUR DT.

CHETTINAD COLLEGE OF ENGINEERING & TECHNOLOGY NH-67, TRICHY MAIN ROAD, PULIYUR, C.F , KARUR DT. CHETTINAD COLLEGE OF ENGINEERING & TECHNOLOGY NH-67, TRICHY MAIN ROAD, PULIYUR, C.F. 639 114, KARUR DT. DEPARTMENT OF ELECTRONICS AND COMMUNICATION ENGINEERING COURSE MATERIAL Subject Name: Electromagnetic

More information

Lecture PowerPoints. Chapter 20 Physics: Principles with Applications, 6 th edition Giancoli

Lecture PowerPoints. Chapter 20 Physics: Principles with Applications, 6 th edition Giancoli Lecture PowerPoints Chapter 20 Physics: Principles with Applications, 6 th edition Giancoli 2005 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for

More information

Electricity & Optics

Electricity & Optics Physics 24100 Electricity & Optics Lecture 15 Chapter 27 sec. 3-5 Fall 2016 Semester Professor Koltick Magnetic Fields B = μ 0 4π I dl r r 2 = μ 0 4π I dl r r 3 B = μ 0 2I 4π R B = μ 0 2 IR 2 R 2 + z 2

More information

Section 24.8 Magnets and Magnetic Materials Pearson Education, Inc.

Section 24.8 Magnets and Magnetic Materials Pearson Education, Inc. Section 24.8 Magnets and Magnetic Materials A Current Loop in a Uniform Field Slide 24-2 A Current Loop in a Uniform Field A magnetic dipole will rotate to line up with a magnetic field just as an electric

More information

ELECTROMAGNETISM The study of the relationship between electricity and magnetism is called

ELECTROMAGNETISM The study of the relationship between electricity and magnetism is called ELECTROMAGNETISM The study of the relationship between electricity and magnetism is called Electromagnetism Before, 1819 it was believed that there was no connection between electricity and magnetism.

More information

Chapter 19. Magnetism

Chapter 19. Magnetism Chapter 19 Magnetism The figure shows the path of a negatively charged particle in a region of a uniform magnetic field. Answer the following questions about this situation (in each case, we revert back

More information

Magnetic Forces and Fields (Chapters 29-30)

Magnetic Forces and Fields (Chapters 29-30) Magnetic Forces and Fields (Chapters 29-30) Magnetism Magnetic Materials and Sources Magnetic Field, Magnetic Force Force on Moving Electric Charges Lorentz Force Force on Current Carrying Wires Applications

More information

INTRODUCTION TO TRANSMISSION LINES DR. FARID FARAHMAND FALL 2012

INTRODUCTION TO TRANSMISSION LINES DR. FARID FARAHMAND FALL 2012 INTRODUCTION TO TRANSMISSION LINES DR. FARID FARAHMAND FALL 2012 http://www.empowermentresources.com/stop_cointelpro/electromagnetic_warfare.htm RF Design In RF circuits RF energy has to be transported

More information

Chapter 5: Static Magnetic Fields

Chapter 5: Static Magnetic Fields Chapter 5: Static Magnetic Fields 5-8. Behavior of Magnetic Materials 5-9. Boundary Conditions for Magnetostatic Fields 5-10. Inductances and Inductors 5-8 Behavior of Magnetic Materials Magnetic materials

More information

Problems in Magnetic Properties of Materials

Problems in Magnetic Properties of Materials Problems in Magnetic Properties of Materials Notations used: H: Magnetic field stregth B: Magnetic flux density I: Intensity of Magentization (Please note that, in text book, notation, M, is used for Intensity

More information

UNIT - IV SEMICONDUCTORS AND MAGNETIC MATERIALS

UNIT - IV SEMICONDUCTORS AND MAGNETIC MATERIALS 1. What is intrinsic If a semiconductor is sufficiently pure, then it is known as intrinsic semiconductor. ex:: pure Ge, pure Si 2. Mention the expression for intrinsic carrier concentration of intrinsic

More information

MODULE 6 ELECTROMAGNETISM MAGNETIC FIELDS MAGNETIC FLUX VISUAL PHYSICS ONLINE

MODULE 6 ELECTROMAGNETISM MAGNETIC FIELDS MAGNETIC FLUX VISUAL PHYSICS ONLINE VISUAL PHYSICS ONLINE MODULE 6 ELECTROMAGNETISM MAGNETIC FIELDS MAGNETIC FLUX Magnetic field (-field ): a region of influence where magnetic materials and electric currents are subjected to a magnetic

More information

Kirchhoff s rules, example

Kirchhoff s rules, example Kirchhoff s rules, example Magnets and Magnetism Poles of a magnet are the ends where objects are most strongly attracted. Two poles, called north and south Like poles repel each other and unlike poles

More information

Magnetic work and adiabatic cooling

Magnetic work and adiabatic cooling Discipline Course-I Semester-II Paper No: Thermal Physics : Physics-IIA Lesson: Lesson Developer: Dr. Ajay Kumar College/ Department: Deshbandhu College, Physics Department, University of Delhi Institute

More information

Electromagnetism. Topics Covered in Chapter 14:

Electromagnetism. Topics Covered in Chapter 14: Chapter 14 Electromagnetism Topics Covered in Chapter 14: 14-1: Ampere-turns of Magnetomotive Force (mmf) 14-2: Field Intensity (H) 14-3: B-H Magnetization Curve 14-4: Magnetic Hysteresis 14-5: Magnetic

More information

MAGNETIC EFFECTS OF CURRENT AND MAGNETISM

MAGNETIC EFFECTS OF CURRENT AND MAGNETISM UNIT III MAGNETIC EFFECTS OF CURRENT AND MAGNETISM Weightage 8 Marks Concept of magnetic field and Oersted s experiment Biot-savart law and its application to current carrying circular loop. Ampere s law

More information

Chapter 28 Magnetic Fields Sources

Chapter 28 Magnetic Fields Sources Chapter 28 Magnetic Fields Sources All known magnetic sources are due to magnetic dipoles and inherently macroscopic current sources or microscopic spins and magnetic moments Goals for Chapter 28 Study

More information

Class XII- Physics - Assignment Topic: - Magnetic Effect of Current

Class XII- Physics - Assignment Topic: - Magnetic Effect of Current LJPS Gurgaon 1. An electron beam projected along +X axis, experiences a force due to a magnetic field along +Y axis. What is the direction of the magnetic field? Class XII- Physics - Assignment Topic:

More information

NPTEL NPTEL ONLINE COURSE. NPTEL Online Certification Course (NOC) NPTEL. Theory and Practice of Non Destructive Testing

NPTEL NPTEL ONLINE COURSE. NPTEL Online Certification Course (NOC) NPTEL. Theory and Practice of Non Destructive Testing NPTEL NPTEL ONLINE COURSE NPTEL Online Certification Course (NOC) NPTEL Theory and Practice of Non Destructive Testing Dr. Ranjit Bauri Dept. of Metallurgical & Materials Engineering IIT Madras, Chennai

More information

NEW SOUTH WALES DEPARTMENT OF EDUCATION AND TRAINING Manufacturing and Engineering ESD. Sample Examination EA605

NEW SOUTH WALES DEPARTMENT OF EDUCATION AND TRAINING Manufacturing and Engineering ESD. Sample Examination EA605 Name: NEW SOUTH WALES DEPARTMENT OF EDUCATION AND TRAINING Manufacturing and Engineering ESD Sample Examination EA605 EDDY CURRENT TESTING AS3998 LEVEL 2 GENERAL EXAMINATION 6161C * * * * * * * Time allowed

More information

Unit 12: Magnetism. Background Reading

Unit 12: Magnetism. Background Reading Unit 12: Magnetism Background Reading What causes magnetism? Have you ever wondered why certain materials can be easily magnetized while others seem to be unaffected by magnets? The properties of certain

More information

ASNT. Level I. Study. Magn. cle. Testin. second e. by Charles W. Eick. The American Society for ssq~s

ASNT. Level I. Study. Magn. cle. Testin. second e. by Charles W. Eick. The American Society for ssq~s ASNT Level I Study Magn Testin cle second e by Charles W. Eick The American Society for ssq~s Acknowledgments A special thank you to everyone who helped with the publication of this book, especially the

More information

Magnetic field creation (example of a problem)

Magnetic field creation (example of a problem) 1 Magnetic field creation (example of a problem) Three long, straight wires are parallel to each other and perpendicular to the plane of the paper. Their mutual location is shown in Figure below. The currents

More information

Lecture PowerPoints. Chapter 20 Physics: Principles with Applications, 6 th edition Giancoli

Lecture PowerPoints. Chapter 20 Physics: Principles with Applications, 6 th edition Giancoli Lecture PowerPoints Chapter 20 Physics: Principles with Applications, 6 th edition Giancoli 2005 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for

More information

1 CHAPTER 12 PROPERTIES OF MAGNETIC MATERIALS

1 CHAPTER 12 PROPERTIES OF MAGNETIC MATERIALS 1 CHAPTER 12 PROPERTIES OF MAGNETIC MATERIALS 12.1 Introduction This chapter is likely to be a short one, not least because it is a subject in which my own knowledge is, to put it charitably, a little

More information

STATION 11 THE 11 ELEMENT ID CHALLENGE.

STATION 11 THE 11 ELEMENT ID CHALLENGE. STATION 11 THE 11 ELEMENT ID CHALLENGE. IN THE PERIODIC TABLE ON THE WALL, YOU WILL NOTICE THAT 11 OF THE ELEMENTS ARE HIGHLIGHTED WITH THE APPROXIMATE COLOR OF THE ELEMENT. YOUR GOAL FOR THIS STATION

More information

Chapter 2: Fundamentals of Magnetism. 8/28/2003 Electromechanical Dynamics 1

Chapter 2: Fundamentals of Magnetism. 8/28/2003 Electromechanical Dynamics 1 Chapter 2: Fundamentals of Magnetism 8/28/2003 Electromechanical Dynamics 1 Magnetic Field Intensity Whenever a magnetic flux, φ, exist in a conductor or component, it is due to the presence of a magnetic

More information

FB-DC6 Electric Circuits: Magnetism and Electromagnetism

FB-DC6 Electric Circuits: Magnetism and Electromagnetism CREST Foundation Electrical Engineering: DC Electric Circuits Kuphaldt FB-DC6 Electric Circuits: Magnetism and Electromagnetism Contents 1. Electromagnetism 2. Magnetic units of measurement 3. Permeability

More information

Magnetic Forces and Fields (Chapters 32)

Magnetic Forces and Fields (Chapters 32) Magnetic Forces and Fields (Chapters 32) Magnetism Magnetic Materials and Sources Magnetic Field, B Magnetic Force Force on Moving Electric Charges Lorentz Force Force on Current Carrying Wires Applications

More information

Haus, Hermann A., and James R. Melcher. Electromagnetic Fields and Energy. Englewood Cliffs, NJ: Prentice-Hall, ISBN:

Haus, Hermann A., and James R. Melcher. Electromagnetic Fields and Energy. Englewood Cliffs, NJ: Prentice-Hall, ISBN: 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

More information

Magnetism.

Magnetism. Magnetism Magnetism https://twistedsifter.files.wordpress.com/2012/05/visualizing-magnetic-fields-with-iron-filings-2.jpg?w=800&h=600 Magnets Are dipoles as opposed to monopoles + - + Referred to as North

More information

Module-16. Magnetic properties

Module-16. Magnetic properties Module-16 Magnetic properties Contents 1) Dia-, Para-, and Ferro-magnetism (Antiferro-magnetism and ferri-magnetism) 2) Influence of temperature on magnetic behavior 3) Domains and Hysteresis Introduction

More information

Electromagnetism II. Instructor: Andrei Sirenko Spring 2013 Thursdays 1 pm 4 pm. Spring 2013, NJIT 1

Electromagnetism II. Instructor: Andrei Sirenko Spring 2013 Thursdays 1 pm 4 pm. Spring 2013, NJIT 1 Electromagnetism II Instructor: Andrei Sirenko sirenko@njit.edu Spring 013 Thursdays 1 pm 4 pm Spring 013, NJIT 1 PROBLEMS for CH. 6 http://web.njit.edu/~sirenko/phys433/phys433eandm013.htm Can obtain

More information

Applications of Non-Contact Magnetising on Ring Shaped Components

Applications of Non-Contact Magnetising on Ring Shaped Components A Paper By George Downes Telephone +44 (0)1981 541122 Fax +44 (0)1981 541133 Email Sales@InsightNDT.com Web Site www.insightndt.com Insight NDT Equipment Ltd The Old Cider Mill Kings Thorn Herefordshire

More information

INTRODUCTION TO MATTER: CLASSI F ICATION OF MATTER, PHYSICAL AND C He MICAL PROPERTIES, AND PHYSICAL AND CHEMICAL CHANGES

INTRODUCTION TO MATTER: CLASSI F ICATION OF MATTER, PHYSICAL AND C He MICAL PROPERTIES, AND PHYSICAL AND CHEMICAL CHANGES Experiment 3 Name: INTRODUCTION TO MATTER: 9 4 CLASSI F ICATION OF MATTER, PHYSICAL AND C He MICAL e PROPERTIES, AND PHYSICAL AND CHEMICAL CHANGES In this experiment, you will encounter various classification

More information

Chapter 17: Magnetism

Chapter 17: Magnetism Chapter 17: Magnetism Section 17.1: The Magnetic Interaction Things You Already Know Magnets can attract or repel Magnets stick to some things, but not all things Magnets are dipoles: north and south Labels

More information

DO PHYSICS ONLINE MOTORS AND GENERATORS MAGNETIC FIELDS

DO PHYSICS ONLINE MOTORS AND GENERATORS MAGNETIC FIELDS DO PHYSICS ONLINE MOTORS AND GENERATORS MAGNETIC FIELDS Powerful magnets are essential components in motors and generators. Some electric motors and generators rely upon a combination of a permanent and

More information

Gravity Electromagnetism Weak Strong

Gravity Electromagnetism Weak Strong 19. Magnetism 19.1. Magnets 19.1.1. Considering the typical bar magnet we can investigate the notion of poles and how they apply to magnets. 19.1.1.1. Every magnet has two distinct poles. 19.1.1.1.1. N

More information

To measure ph s in a variety of solutions and mixtures and to account for the results obtained.

To measure ph s in a variety of solutions and mixtures and to account for the results obtained. Acid-Base Studies PURPOSE To measure ph s in a variety of solutions and mixtures and to account for the results obtained. GOALS 1 To learn to use ph paper and a ph meter to measure the ph of a given solution.

More information

Chapter 7. Chapter 7. Electric Circuits Fundamentals - Floyd. Copyright 2007 Prentice-Hall

Chapter 7. Chapter 7. Electric Circuits Fundamentals - Floyd. Copyright 2007 Prentice-Hall Chapter 7 Magnetic Quantities Magnetic fields are described by drawing flux lines that represent the magnetic field. Where lines are close together, the flux density is higher. Where lines are further

More information

Course no. 4. The Theory of Electromagnetic Field

Course no. 4. The Theory of Electromagnetic Field Cose no. 4 The Theory of Electromagnetic Field Technical University of Cluj-Napoca http://www.et.utcluj.ro/cs_electromagnetics2006_ac.htm http://www.et.utcluj.ro/~lcret March 19-2009 Chapter 3 Magnetostatics

More information

Modeling of Magnetic Flux Leakage. Carbon Steel Plates

Modeling of Magnetic Flux Leakage. Carbon Steel Plates Presented at the COMSOL Conference 2010 India Three-Dimensional Finite Element Modeling of Magnetic Flux Leakage Technique e for Detection of Defects in Carbon Steel Plates W. Sharatchandra Singh, S. Thirunavukkarasu,

More information

Chapter 22, Magnetism. Magnets

Chapter 22, Magnetism. Magnets Chapter 22, Magnetism Magnets Poles of a magnet (north and south ) are the ends where objects are most strongly attracted. Like poles repel each other and unlike poles attract each other Magnetic poles

More information

PHY331 Magnetism. Lecture 1

PHY331 Magnetism. Lecture 1 PHY331 Magnetism Lecture 1 Overview Course syllabus / general information Quick revision of basic concepts Magnetization and susceptibility Using susceptibility to define magnetic materials Diamagnetic

More information

Physical Properties: Mass, Volume, Density, Conductivity, Magnetism, State of Matter, Solubility Mixtures, Heterogeneous mixtures, suspension,

Physical Properties: Mass, Volume, Density, Conductivity, Magnetism, State of Matter, Solubility Mixtures, Heterogeneous mixtures, suspension, Physical Properties: Mass, Volume, Density, Conductivity, Magnetism, State of Matter, Solubility Mixtures, Heterogeneous mixtures, suspension, Homogeneous mixtures, colloid, solution Unit: Physical Properties

More information

Magnetic Fields Part 2: Sources of Magnetic Fields

Magnetic Fields Part 2: Sources of Magnetic Fields Magnetic Fields Part 2: Sources of Magnetic Fields Last modified: 08/01/2018 Contents Links What Causes a Magnetic Field? Moving Charges Right Hand Grip Rule Permanent Magnets Biot-Savart Law Magnetic

More information

Induction Heating: fundamentals

Induction Heating: fundamentals LEP ELECTROMAGNETIC PROCESSING OF MATERIALS TECNOLGIE DEI PROCESSI ELETTROTERMICI Induction Heating: fundamentals Fabrizio Dughiero 2017-2018 Induction heating fundamentals May 28-30, 2014 1 Summary 1.

More information

EWING S MOLECULAR THEORY OF MAGNETISM AND ITS FAILURES

EWING S MOLECULAR THEORY OF MAGNETISM AND ITS FAILURES 8. MAGNETISM Salient features Ewing s molecular theory and its failures Domain theory Inverse square law of magnetism Magnetic induction Magnetic field due to a bar magnet Magnetic lines of force Magnetic

More information

Atomic Electron Configurations and Periodicity

Atomic Electron Configurations and Periodicity Atomic Electron Configurations and Periodicity Electron Spin The 4 th quantum number is known as the spin quantum number and is designated by m s. It can have the value of either + ½ or ½ It roughly translates

More information

Magnetic field and magnetic poles

Magnetic field and magnetic poles Magnetic field and magnetic poles Magnetic Field B is analogically similar to Electric Field E Electric charges (+ and -)are in analogy to magnetic poles(north:n and South:S). Paramagnetism, Diamagnetism,

More information