Characterisation of ferritic stainless steel by Barkhausen techniques

Magneto-acoustic emission (MAE) and magnetic Barkhausen noise (MBN) sensing techniques were developed and employed to characterise plastically deformed and heat-treated AISI 430 ferritic stainless steel samples. These results have been compared to the mechanical hardness, coercivity and residual stress of the samples. MAE and MBN were shown to decrease with increasing permanent material deformation. It was found that the inverse of MAE (absolute energy) and MBN (RMS) are linearly proportional to hardness. With increased deformation, the resultant change in dislocation density was found to effect material coercivity. It has been shown that the inverse of MAE absolute energy and MBN have an exponential relationship to the change in material coercivity. The results are explained in terms of the different mechanisms that effect dislocation-domain wall interactions. A new measurement parameter has been developed for microstructural characterisation called MAE absolute energy and has proved to be a useful quantitative method in MAE waveform measurement.

[1]  R. A. Taylor,et al.  Direct observation of the interaction between magnetic domain walls and dislocations in iron , 1983 .

[2]  R. Vergne,et al.  Predictions of the random potential energy models of domain wall motion: An experimental investigation on high-purity iron , 1982 .

[3]  David L. Atherton,et al.  Plastic versus elastic deformation effects on magnetic Barkhausen noise in steel , 2000 .

[4]  G. Briggs,et al.  Magneto-acoustic and Barkhausen emission: Their dependence on dislocations in iron , 1987 .

[5]  C. Kittel,et al.  Ferromagnetic Domain Theory , 1956 .

[6]  D. Hwang,et al.  The influence of plastic deformation on Barkhausen effects and magnetic properties in mild steel , 1988 .

[7]  G. Voort Metallography and microstructures , 2004 .

[8]  Michael E. Fitzpatrick,et al.  Determination of residual stresses by X-ray diffraction , 2005 .

[9]  H. Richter,et al.  On the magnetic properties of fine-milled barium and strontium ferrite , 1968 .

[10]  H. Kojima,et al.  Effect of Milling on the Intrinsic Coercivity of Barium Ferrite Powders , 1974 .

[11]  H. Kusanagi,et al.  Stress effect on the magnitude of acoustic emission during magnetization of ferromagnetic materials , 1979 .

[12]  B. Tanner,et al.  The magnetic properties of plastically deformed steels. , 1990 .

[13]  R. Nolan,et al.  Anisotropy-field distributions in barium ferrite micropowders , 1969 .

[14]  B. Augustyniak,et al.  The effect of mechanical stress on a Barkhausen noise signal integrated across a cycle of ramped magnetic field , 1996 .

[15]  A. E. Lord,et al.  Acoustic barkhausen emission in amorphous metallic alloys Fe40Ni40P14B6 and Fe78Mo2B20 , 1981 .

[16]  G. Briggs,et al.  Magnetoacoustic and Barkhausen emission in ferromagnetic materials , 1986, Philosophical Transactions of the Royal Society of London. Series A, Mathematical and Physical Sciences.

[17]  R. Honeycombe,et al.  Plastic Deformation of Metals , 1932, Nature.

[18]  David L. Atherton,et al.  CORRIGENDUM: Theory of the magnetisation process in ferromagnets and its application to the magnetomechanical effect , 1984 .

[19]  Song Xu,et al.  Microcoercivity, bulk coercivity and saturation remanence in multidomain materials , 1990 .