This document provides a syllabus for a course on Non-Destructive Testing and Evaluation. It outlines 5 units that will be covered: Overview of NDT, Surface NDE Methods, Thermography and Eddy Current Testing, Ultrasonic Testing and Acoustic Emission, and Radiography. Unit 2 focuses on Liquid Penetrant Testing and Magnetic Particle Testing, covering their principles, materials, procedures, advantages, and limitations. The course aims to teach students various NDE methods, theories, and their industrial applications.

1. Karpagam Institute of Technology
Coimbatore-105
Department of Mechanical Engineering
Course Code with Name: ME8097 –Non Destructive Testing and
Evaluation
Staff Name/Designation: VIJAYAN S N/AP
Department: Mechanical Engineering
Year/Semester: IV/VII
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2. Course Syllabus
UNIT I OVERVIEW OF NDT 9
NDT Versus Mechanical testing, Overview of the Non Destructive Testing Methods for the detection of
manufacturing defects as well as material characterisation. Relative merits and limitations, Various
physical characteristics of materials and their applications in NDT., Visual inspection – Unaided and
aided.
UNIT II SURFACE NDE METHODS 9
Liquid Penetrant Testing - Principles, types and properties of liquid penetrants, developers, advantages
and limitations of various methods, Testing Procedure, Interpretation of results. Magnetic Particle
Testing- Theory of magnetism, inspection materials Magnetisation methods, Interpretation and
evaluation of test indications, Principles and methods of demagnetization, Residual magnetism.
UNIT III THERMOGRAPHY AND EDDY CURRENT TESTING (ET) 9
Thermography- Principles, Contact and non contact inspection methods, Techniques for applying
liquid crystals, Advantages and limitation - infrared radiation and infrared detectors, Instrumentations
and methods, applications. Eddy Current Testing-Generation of eddy currents, Properties of eddy
currents, Eddy current sensing elements, Probes, Instrumentation, Types of arrangement,
Applications, advantages, Limitations, Interpretation/Evaluation.
UNIT IV ULTRASONIC TESTING (UT) AND ACOUSTIC EMISSION (AE) 9
Ultrasonic Testing-Principle, Transducers, transmission and pulse-echo method, straight beam and
angle beam, instrumentation, data representation, A/Scan, B-scan, C-scan. Phased Array Ultrasound,
Time of Flight Diffraction. Acoustic Emission Technique –Principle, AE parameters, Applications
UNIT V RADIOGRAPHY (RT) 9
Principle, interaction of X-Ray with matter, imaging, film and film less techniques, types and use of
filters and screens, geometric factors, Inverse square, law, characteristics of films - graininess, density,
speed, contrast, characteristic curves, Penetrameters, Exposure charts, Radiographic equivalence.
Fluoroscopy- Xero-Radiography, Computed Radiography, Computed Tomography
2

3. Course Objective
To study and understand the various Non Destructive
Evaluation and Testing methods, theory and their
industrial applications.
3

4. Course Outcome
• Explain the fundamental concepts of NDT
• Discuss the different methods of NDE
• Explain the concept of Thermography and
Eddy current testing
• Explain the concept of Ultrasonic Testing and
Acoustic Emission
• Explain the concept of Radiography
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5. Program Outcomes
1. An ability to apply knowledge of mathematics and engineering sciences to
develop mathematical models for industrial problems.
2. An ability to identify, formulates, and solve complex engineering problems.
with high degree of competence.
3. An ability to design and conduct experiments, as well as to analyze and
interpret data obtained through those experiments.
4. An ability to design mechanical systems, component, or a process to meet
desired needs within the realistic constraints such as environmental, social,
political and economic sustainability.
5. An ability to use modern tools, software and equipment to analyze
multidisciplinary problems.
6. An ability to demonstrate on professional and ethical responsibilities.
7. An ability to communicate, write reports and express research findings in a
scientific community.
8. An ability to adapt quickly to the global changes and contemporary practices.
9. An ability to engage in life-long learning.
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6. Program Specific Outcomes
• An ability to identify, analyze and solve engineering
problems relating to mechanical systems together
with allied engineering streams.
• An ability to build the nation, by imparting
technological inputs and managerial skills to become
Technocrats and Entrepreneurs, build the attitude of
developing new concepts on emerging fields and
pursuing advanced education.
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7. CO vs PO and PSO Mapping
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8. UNIT II
SURFACE NDE METHODS
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9. UNIT II: Topics
• Liquid Penetrant Testing - Principles, types and properties of
liquid penetrants
• developers
• advantages and limitations of various methods, Testing Procedure,
• Interpretation of results.
• Magnetic Particle Testing - Theory of magnetism
• inspection materials Magnetisation methods
• Interpretation and evaluation of test indications
• Principles and methods of demagnetization
• Residual magnetism.
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10. Video and Animation
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Dye Penetrant Inspection:
https://www.youtube.com/watch?v=xEK-c1pkTUI
Magnetic Particle Inspection:
https://www.youtube.com/watch?v=qpgcD5k1494

11. Assignment Questions
• Illustrate with neat sketching about the principle of liquid
penetrant testing
• Explain the testing procedure for liquid penetrant testing
• Explain with suitable sketch of various stages of liquid penetrant
testing
• Explain with suitable sketch about the working principle of
Magnetic particle inspection
• Discuss in detail about the general procedure of magnetic particle
test
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12. QUIZ Questions
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IMPORTANT CHARACTERISTICS OF PENETRANTS

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TYPE OF PENETRANT
Type 1 – Fluorescent Penetrants
Type 2 – Visible Penetrants

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PHYSICAL PROPERTIES OF PENETRANT
MATERIALS
• Viscosity
• Surface Tension
• Wetting ability
• Specific gravity
• Volatility
• Flash Point
• Solubility
• Ability to spread or creep
• Tolerance to contaminants
• Toxicity
• Odour / Freedom from skin irritation tendencies
• Inertness or non-corrosiveness
• Washability

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Theoretically, good penetrant shoud have :
Good wetting ability
• very small contact angle
• High surface tension
Surface tension in a liquid is an example of cohesive force,
when the molecules are attracted to like
molecules. The cohesive force tends to bind them together.
Wetting action in a liquid is an example of the adhesive force,
where the molecules are attracted to
foreign matter and the adhesive force tends to spread the liquid

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Liquid penetrant inspection (LPI) is one of the most
widely used nondestructive evaluation (NDE) methods. Its
popularity can be attributed to two main factors: its relative ease
of use and its flexibility.
LPI can be used to inspect almost any material provided
that its surface is not extremely rough or porous. Materials that
are commonly inspected using LPI include the following:
• Metals (aluminum, copper, steel, titanium, etc.)
• Glass
• Many ceramic materials
• Rubber
• Plastics

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PROPERTIES OF DEVELOPER MATERIALS
• The material must be absorptive
• It must have a fine texture but not be too fine, as this may block
imperfections
• It must be easily and evenly applicable
• It must form a light and even coat
• There must be no fluorescing of the developer when used with fluorescent
penetrant
• The penetrant bleeding from a discontinuity must easily wet the material
• When used with a colour contrast penetrant it must be of a highly
contrasting colour. It seems agreed that the best colour is white
• It must be readily removable after the test is completed
• It must be non-toxic and non-irritant

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TYPES OF DEVELOPER

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Dry Powder Developer Water Soluble Developer
Nonaqueous Developer

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MAGNETIC PARTICLE TESTING

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In theory, magnetic particle testing has a relatively simple concept.
It can be considered as a combination of two nondestructive testing
methods: magnetic flux leakage testing and visual testing. For the
case of a bar magnet, the magnetic field is in and around the magnet.
Any place that a magnetic line of force exits or enters the magnet is
called a “pole” (magnetic lines of force exit the magnet from north
pole and enter from the south pole).
BASIC PRINCIPLE

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When a bar magnet is broken in the center of its length, two
complete bar magnets with magnetic poles on each end of each
piece will result. If the magnet is just cracked but not broken
completely in two, a north and south pole will form at each edge of
the crack. The magnetic field exits the north pole and reenters at the
south pole.
The magnetic field spreads out when it encounters the small air gap
created by the crack because the air cannot support as much
magnetic field per unit volume as the magnet can. When the field
spreads out, it appears to leak out of the material and, thus is called
a flux leakage field.

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If iron particles are sprinkled on a cracked magnet, the particles
will be attracted to and cluster not only at the poles at the ends of
the magnet, but also at the poles at the edges of the crack. This
luster of particles is much easier to see than the actual crack and
this is the basis for magnetic particle inspection.

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The first step in a magnetic particle testing is to
magnetize the component that is to be inspected. If any defects
on or near the surface are present, the defects will create a
leakage field. After the component has been magnetized, iron
particles, either in a dry or wet suspended form, are applied to
the surface of the magnetized part. The particles will be attracted
and cluster at the flux leakage fields, thus forming a visible
indication that the inspector can detect.

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Advantages
• High sensitivity (small discontinuities can be detected).
• Indications are produced directly on the surface of the part and
constitute a visual representation of the flaw.
• Minimal surface preparation (no need for paint removal)
• Portable (small portable equipment & materials available in
spray cans)
• Low cost (materials and associated equipment are relatively
inexpensive)

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Disadvantages
• Only surface and near surface defects can be detected.
• Only applicable to ferromagnetic materials.
• Relatively small area can be inspected at a time.
• Only materials with a relatively nonporous surface can be
inspected.
• The inspector must have direct access to the surface being
inspected.

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Magnetism
The concept of magnetism centers around the magnetic field
and what is known as a dipole. The term "magnetic field"
simply describes a volume of space where there is a change in
energy within that volume. The location where a magnetic field
exits or enters a material is called a magnetic pole. Magnetic
poles have never been detected in isolation but always occur in
pairs, hence the name dipole. Therefore, a dipole is an object
that has a magnetic pole on one end and a second, equal but
opposite, magnetic pole on the other. A bar magnet is a dipole
with a north pole at one end and south pole at the other.

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The source of magnetism lies in the basic building block of all
matter, the atom. Atoms are composed of protons, neutrons and
electrons. The protons and neutrons are located in the atom‘s
nucleus and the electrons are in constant motion around the
nucleus. Electrons carry a negative electrical charge and
produce a magnetic field as they move through space. A
magnetic field is produced whenever an electrical charge is in
motion. The strength of this field is called the magnetic
moment.

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When an electric current flows
through a conductor, the movement of
electrons through the conductor causes
a magnetic field to form around the
conductor. The magnetic field can be
detected using a compass. Since all
matter is comprised of atoms, all
materials are affected in some way by
a magnetic field; however, materials
do not react the same way to the
magnetic field.

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When a material is placed within a
magnetic field, the magnetic forces of the
material‘s electrons will be affected. This
effect is known as Faraday's Law of
Magnetic Induction.
However, materials can react quite
differently to the presence of an external
magnetic field. The magnetic moments
associated with atoms have three origins: the
electron motion, the change in motion caused
by an external magnetic field, and the spin of
the electrons.

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In most atoms, electrons occur in pairs where these pairs
spin in opposite directions. The opposite spin directions of
electron pairs cause their magnetic fields to cancel each other.
Therefore, no net magnetic field exists. Alternately, materials
with some unpaired electrons will have a net magnetic field and
will react more to an external field.
According to their interaction with a magnetic field, materials can
be classified as:
• Diamagnetic materials
• Paramagnetic materials
• Ferromagnetic materials

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Diamagnetic materials
which have a weak, negative susceptibility to magnetic fields.
Diamagnetic materials are slightly repelled by a magnetic field
and the material does not retain the magnetic properties when the
external field is removed. In diamagnetic materials all the
electrons are paired so there is no permanent net magnetic
moment per atom. Most elements in the periodic table, including
copper, silver, and gold, are diamagnetic.

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Paramagnetic materials
which have a small, positive susceptibility to magnetic fields.
These materials are slightly attracted by a magnetic field and the
material does not retain the magnetic properties when the
external field is removed. Paramagnetic materials have some
unpaired electrons. Examples of paramagnetic materials include
magnesium, molybdenum, and lithium.

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Ferromagnetic materials
have a large, positive susceptibility to an external magnetic field.
They exhibit a strong attraction to magnetic fields and are able to
retain their magnetic properties after the external field has been
removed. Ferromagnetic materials have some unpaired electrons
so their atoms have a net magnetic moment. They get their strong
magnetic properties due to the presence of magnetic domains.
In these domains, large numbers of atom's moments are
aligned parallel so that the magnetic force within the domain is
strong (this happens during the solidification of the material where
the atom moments are aligned within each crystal ”i.e., grain”
causing a strong magnetic force in one direction).

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When a ferromagnetic material is in the unmagnetized state, the
domains are nearly randomly organized and the net magnetic field for the part
as a whole is zero.
When a magnetizing force is applied, the domains become aligned to
produce a strong magnetic field within the part. Iron, nickel, and cobalt are
examples of ferromagnetic materials. Components made of these materials
are commonly inspected using the magnetic particle method.

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General Properties of Magnetic Lines of Force
Magnetic lines of force have a number of important properties, which
include:
• They seek the path of least resistance between opposite magnetic
poles (in a single bar magnet shown, they attempt to form closed loops
from pole to pole).
• They never cross one another.
• They all have the same strength.
• Their density decreases with increasing distance from the poles.
• Their density decreases (they spread out) when they move from an
area of higher permeability to an area of lower permeability.

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•They are considered to have direction as if flowing, though no
actual movement occurs.
•They flow from the south pole to the north pole within a
material and north pole to south pole in air.

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Electromagnetic Fields
Magnets are not the only source of magnetic fields. The flow of
electric current through a conductor generates a magnetic field. When
electric current flows in a long straight wire, a circular magnetic field
is generated around the wire and the intensity of this magnetic field is
directly proportional to the amount of current carried by the wire.
The strength of the field is strongest next to the wire and
diminishes with distance. In most conductors, the magnetic field exists
only as long as the current is flowing. However, in ferromagnetic
materials the electric current will cause some or all of the magnetic
domains to align and a residual magnetic field will remain.

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Also, the direction of the magnetic
field is dependent on the direction of
the electrical current in the wire. The
direction of the magnetic field around a
conductor can be determined using a
simple rule called the “right-hand
clasp rule”. If a person grasps a
conductor in one's right hand with the
thumb pointing in the direction of the
current, the fingers will circle the
conductor in the direction of the
magnetic field.

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Magnetic Field Produced by a Coil
When a current carrying wire is formed into several loops to form a
coil, the magnetic field circling each loop combines with the fields
from the other loops to produce a concentrated field through the
center of the coil.

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When the coil loops are tightly wound, a uniform
magnetic field is developed throughout the length of the coil.
The strength of the magnetic field increases not only
with increasing current but also with each loop that is added to
the coil.
A long, straight coil of wire is called a solenoid and it
can be used to generate a nearly uniform magnetic field similar
to that of a bar magnet. The concentrated magnetic field inside a
coil is very useful in magnetizing ferromagnetic materials for
inspection using the magnetic particle testing method.

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Magnetic Field Orientation and Flaw Detectability
To properly inspect a component for cracks or other defects, it
is important to understand that the orientation of the crack relative to
the magnetic lines of force determinies if the crack can or cannot be
detected.
There are two general types of magnetic fields that can be
established within a component
•A longitudinal magnetic field
•A circular magnetic field

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A longitudinal magnetic field has magnetic lines of force that run
parallel to the long axis of the part. Longitudinal magnetization of
a component can be accomplished using the longitudinal field set
up by a coil or solenoid. It can also be accomplished using
permanent magnets or electromagnets.
A longitudinal magnetic field A circular magnetic field

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A circular magnetic field has magnetic lines of force that run
circumferentially around the perimeter of a part. A circular magnetic
field is induced in an article by either passing current through the
component or by passing current through a conductor surrounded by
the component.
Being able to magnetize the part in two directions is important
because the best detection of defects occurs when the lines of
magnetic force are established at right angles to the longest dimension
of the defect. This orientation creates the largest disruption of the
magnetic field within the part and the greatest flux leakage at the
surface of the part. If the magnetic field is parallel to the defect, the
field will see little disruption and no flux leakage field will be
produced.

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An orientation of 45 to 90 degrees between the magnetic
field and the defect is necessary to form an indication. Since defects
may occur in various and unknown directions, each part is normally
magnetized in two directions at right angles to each other.
If the component shown is considered, it is known that
passing current through the part from end to end will establish a
circular magnetic field that will be 90 degreesto the direction of the
current. Therefore, defects that have a significant dimension in the
direction of the current (longitudinal defects) should be detectable,
while transverse-type defects will not be detectable with circular
magnetization.

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Magnetization of Ferromagnetic Materials
There are a variety of methods that can be used to establish a
magnetic field in a component for evaluation using magnetic
particle inspection.
It is common to classify the magnetizing methods as either direct
or indirect.

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Magnetization Using Direct Induction (Direct Magnetization)
With direct magnetization, current is passed directly
through the component. The flow of current causes a circular
magnetic field to form in and around the conductor.
When using the direct magnetization method, care must be
taken to ensure that good electrical contact is established and
maintained between the test equipment and the test component to
avoid damage of the the component (due to arcing or overheating
at high resistance ponts).

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There are several ways that direct magnetization is commonly
accomplished.
One way involves clamping the component between two
electrical contacts in a special piece of equipment. Current is
passed through the component and a circular magnetic field is
established in and around the component.
When the magnetizing current is stopped, a residual magnetic field
will remain within the component. The strength of the induced
magnetic field is proportional to the amount of current passed
through the component.

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A second technique involves using clamps or prods, which are
attached or placed in contact with the component. Electrical
current flows through the component from contact to contact. The
current sets up a circular magnetic field around the path of the
current.

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Magnetization Using Indirect Induction (Indirect
Magnetization)
As with direct magnetization, there are several ways that indirect
magnetization can be accomplished.
The use of permanent magnets is a
low cost method of establishing a
magnetic field. However, their use is
limited due to lack of control of the
field strength and the difficulty of
placing and removing strong
permanent magnets from the
component.

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Electromagnets in the form of an
adjustable horseshoe magnet (called
a yoke) eliminate the problems
associated with permanent magnets
and are used extensively in industry.
Electromagnets only exhibit a
magnetic flux when electric current
is flowing around the soft iron core.
When the magnet is placed on the
component, a magnetic field is
established between the north and
south poles of the magnet.

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Another way of indirectly inducting a
magnetic field in a material is by using
the magnetic field of a current carrying
conductor. A circular magnetic field can
be established in cylindrical components
by using a central conductor. Typically,
one or more cylindrical components are
hung from a solid copper bar running
through the inside diameter. Current is
passed through the copper bar and the
resulting circular magnetic field
establishes a magnetic field within the
test components.

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The use of coils and solenoids is a
third method of indirect
magnetization. When the length of a
component is several times larger than
its diameter, a longitudinal magnetic
field can be established in the
component. The component is placed
longitudinally in the concentrated
magnetic field that fills the center of a
coil or solenoid. This magnetization
technique is often referred to as a "coil
shot".

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Demagnetization
After conducting a magnetic particle inspection, it is usually
necessary to demagnetize the component. magnetic fields can:
- affect machining by causing cuttings to cling to a component.
- interfere with electronic equipment such as a compass.
- create a condition known as "arc blow" in the welding process.
Arc blow may cause the weld arc to wonder or filler metal to be
repelled from the weld.
- cause abrasive particles to cling to bearing or faying surfaces and
increase wear.

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Removal of a field may be accomplished in several ways.
The most effective way to demagnetize a material is by heating the
material above its curie temperature (for instance, the curie
temperature for a low carbon steel is 770°C).
When steel is heated above its curie temperature then it is
cooled back down, the orientation of the magnetic domains of the
individual grains will become randomized again and thus the
component will contain no residual magnetic field.
The material should also be placed with its long axis in an
east-west orientation to avoid any influence of the Earth‘s magnetic
field.

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However, it is often inconvenient to heat a material above
its curie temperature to demagnetize it, so another method that
returns the material to a nearly unmagnetized state is commonly
used.
Subjecting the component to a reversing and decreasing
magnetic field will return the dipoles to a nearly random
orientation throughout the material. This can be accomplished
by pulling a component out and away from a coil with AC
passing through it. With AC Yokes, demagnetization of local
areas may be accomplished by placing the yoke contacts on the
surface, moving them in circular patterns around the area, and
slowly withdrawing the yoke while the current is applied.

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Magnetic Particles
As mentioned previously, the particles that are used for magnetic
particle inspection are a key ingredient as they form the indications that
alert the inspector to the presence of defects. Particles start out as tiny
milled pieces of iron or iron oxide. A pigment (somewhat like paint) is
bonded to their surfaces to give the particles color.
The metal used for the particles has high magnetic permeability
and low retentivity. High magnetic permeability is important because it
makes the particles attract easily to small magnetic leakage fields from
discontinuities, such as flaws. Low retentivity is important because the
particles themselves never become strongly magnetized so they do not
stick to each other or the surface of the part. Particles are available in a
dry mix or a wet solution.

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Dry Magnetic Particles
Dry magnetic particles can typically be purchased in red,
black, gray, yellow and several other colors so that a high level
of contrast between the particles and the part being inspected can
be achieved. The size of the magnetic particles is also very
important.
Dry magnetic particle products are produced to include a
range of particle sizes. The fine particles have a diameter of
about 50 μm while the course particles have a diameter of 150
μm (fine particles are more than 20 times lighter than the coarse
particles). This makes fine particles more sensitive to the leakage
fields from very small discontinuities.

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small particles easily adhere to
surface contamination, such as remnant dirt
or moisture, and get trapped in surface
roughness features. It should also be
recognized that finer particles will be more
easily blown away by the wind; therefore,
windy conditions can reduce the sensitivity of
an inspection. Also, reclaiming the dry
particles is not recommended because the
small particles are less likely to be recaptured
and the "once used" mix will result in less
sensitive inspections.

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The particle shape is also important.
Long, slender particles tend to align
themselves along the lines of magnetic force.
However, if dry powder consists only of
elongated particles, the application process
would be less than desirable since long
particles lack the ability to flow freely.
Therefore, a mix of rounded and
elongated particles is used since it results in a
dry powder that flows well and maintains good
sensitivity. Most dry particle mixes have
particles with L/D ratios between one and two.

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Wet Magnetic Particles
Magnetic particles are also supplied in a wet suspension such
as water or oil. The wet magnetic particle testing method is generally
more sensitive than the dry because the suspension provides the
particles with more mobility and makes it possible for smaller
particles to be used (the particles are typically 10 μm and smaller)
since dust and adherence to surface contamination is reduced or
eliminated.
The wet method also makes it easy to apply the particles
uniformly to a relatively large area.

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Wet method magnetic particles products differ from dry
powder products in a number of ways. One way is that both visible
and fluorescent particles are available. Most non-fluorescent
particles are ferromagnetic iron oxides, which are either black or
brown in color.
Fluorescent particles are coated with pigments that
fluoresce when exposed to ultraviolet light. Particles that fluoresce
green-yellow are most common to take advantage of the peak
color sensitivity of the eye but other fluorescent colors are also
available. Also, both visible and fluorescent wet suspended
particles are available in aerosol spray cans for increased
portability and ease of application.

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95. Thank You
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