Introduction to Magnetic Particle Testing | Welding and NDT Tips

 Introduction to Magnetic Particle Testing

With magnetic particle inspection (MPI), surface defects such as cracks of ferromagnetic components are made visible.

Like the dye penetrant inspection, magnetic particle inspection is also a method for examining surface defects such as cracks. In contrast to the dye penetrant inspection, flaws near the surface that do not reach directly to the surface can also be localized. Magnetic particle testing can only be applied to ferromagnetic materials and is based on the principle of deflecting magnetic field lines at defects. A distinction is made between two inspection methods, which are explained in more detail below:

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• magnetic field flow method
• current flow method

Magnetic field flow method:

First, the component to be examined is thoroughly cleaned and the test site magnetized with a yoke. Magnetic field lines are formed in the component between the ends of the yoke. In the crack-free state, the field lines run in a straight line and parallel to each other near the surface.

However, at imperfections such as cracks, a stray magnetic field is created, which causes the magnetic field lines to be increasingly forced out of the interior of the workpiece. In this area, there is a particularly large magnetic effect on the surface. Iron particles applied to the surface therefore adhere well to these imperfections.

After magnetization, a ferromagnetic iron oxide powder is applied as test medium, which is mixed with an oil-based fluorescent carrier liquid (test suspension). By adding the fluorescent agent, the flaws can be made particularly visible under ultraviolet light.

Current flow method:

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Instead of “flooding” the workpiece directly with a magnetic field, a current flow is first generated in the workpiece. For this purpose, an electric field is introduced via the yoke instead of a magnetic field. Due to the electrical conductivity of the metallic workpiece, an electrical current is generated. This current flow in turn causes a magnetic field whose field lines form concentrically to the current flow (“magnetic field of a current-carrying wire”).

Compared to the magnetic flow method, the magnetic field is now perpendicular aligned to it, so that even the previously unfavourably oriented flaws can now be optimally resolved.