graphically designates the coercive force, H
c
, in the material. Ferromagnetic materials retain a certain amount of residual
magnetism after being subjected to a magnetizing force. When the magnetic domains of a ferromagnetic material have
been oriented by a magnetizing force, some domains remain so oriented until an additional force in the opposite direction
causes them to return to their original random orientation. This force is commonly referred to as coercive force.
As the reversed field is increased beyond c, point d is reached (Fig. 16d). At this point, the specimen is again magnetically
saturated. The magnetizing force is now decreased to zero, and the de line is formed and retains reversed-polarity residual
magnetism, B
r
, in the specimen. Further increasing the magnetizing force in the original direction completes the curve efa.
The cycle is now complete, and the area within the loop abcdefa is called the hysteresis curve.
The definite lag throughout the cycle between the magnetization force and the flux is called hysteresis. If the hysteresis
loop is slender (Fig. 16e), the indication usually means that the material has low retentivity (low residual field) and is easy
to magnetize (has low reluctance). A wide loop (Fig. 16f) indicates that the material has high reluctance and is difficult to
magnetize.
Magnetic Particle Inspection
Revised by Art Lindgren, Magnaflux Corporation
Magnetic Particles and Suspending Liquids
Magnetic particles are classified according to the medium used to carry the particles to the part. The medium can be air
(dry-particle method) or a liquid (wet-particle method). Magnetic particles can be made of any low-retentivity
ferromagnetic material that is finely subdivided. The characteristics of this material, including magnetic properties, size,
shape, density, mobility, and degree of visibility and contrast, vary over wide ranges for different applications.
Magnetic Properties. The particles used for magnetic particle inspection should have high magnetic permeability so
that they can be readily magnetized by the low-level leakage fields that occur around discontinuities and can be drawn by
these fields to the discontinuities themselves to form readable indications. The fields at very fine discontinuities are
sometimes extremely weak.
Low coercive force and low retentivity are desirable for magnetic particles. If high in coercive force, wet particles
become strongly magnetized and form an objectionable background. In addition, the particles will adhere to any steel in
the tank or piping of the unit and cause heavy settling-out losses. Highly retentive wet particles tend to clump together
quickly in large aggregates on the test surface. Excessively large clumps of particles have low mobility, and indications
are distorted or obscured by the heavy, coarse-grain backgrounds.
Dry particles having coercive force and high retentivity would become magnetized during manufacture or in first use and
would therefore become small, strong permanent magnets. Once magnetized, their control by the weak fields at
discontinuities would be subdued by their tendency to stick magnetically to the test surface wherever they first touch. This
would reduce the mobility of the powder and would form a high level of background, which would reduce contrast and
make indications difficult to see.
Effect of Particle Size. Large, heavy particles are not likely to be arrested and held by weak fields when such particles
are moving over a part surface, but fine particles will be held by very weak fields. However, extremely fine particles may
also adhere to surface areas where there are no discontinuities (especially if the surface is rough) and form confusing
backgrounds. Coarse dry particles fall too fast and are likely to bounce off the part surface without being attracted by the
weak leakage fields at imperfections. Finer particles can adhere to fingerprints, rough surfaces, and soiled or damp areas,
thus obscuring indications.
Magnetic particles for the wet method are applied as a suspension in some liquid medium, and particles much smaller
than those for the dry method can be used. When such a suspension is applied over a surface, the liquid drains away, and
the film remaining on the surface becomes thinner. Coarse particles would quickly become stranded and immobilized.
The stranding of finer particles as a result of the draining away of the liquid occurs much later, giving these particles
mobility for a sufficient period of time to be attracted by leakage fields and to accumulate and thus form true indications.