This NDT method consists in generating induced currents
in electricity conducting materials via an alternative magnetic
field (generated by a solenoid) and variable in time (low
or high frequency).
The currents locally induced and generated are called Eddy
currents. Their distribution and repartition depend on the
magnetic excitation field , as well as on the geometry the
electrical conductivity and the magnetic permeability of the
controlled structure.
The presence of a defect in the testpiece generates disturbances
in the circulation of Eddy currents, entailing a variation
in the solenoid impedance.
The method is applicable to all electricity conducting materials.
Extract from COFREND
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