Thin-skin electromagnetic fields in the neighbourhood of surface-breaking cracks in metals
journal contribution
posted on 2013-02-25, 15:02authored byD.H. Michael, A.M. Lewis, Maureen McIver, R. Collins
Electromagnetic non-destructive evaluation techniques are widely used to detect
and size surface-breaking cracks in metal structures and components. The precise
distribution of the electromagnetic field around such a crack depends on the
frequency of the applied field, the material properties of the metal and the crack
geometry. In many situations, the skin depth of the electromagnetic field in the
metal is small compared with the crack dimensions. If this is the case, the crucial
parameter that determines the way the electromagnetic field in air couples to the
field in the metal is m = o l//S, where a and /,0 are the metal and free space
permeabilities respectively and 1/6 is the ratio of the crack length scale 1 to the skin
depth 8. If the metal is ferromagnetic, m can take a wide range of values and the
distribution of the electromagnetic field around the crack is very different in the two
limiting cases m = 0 and m > 1. In the first case, the magnetic flux emerging from the
crack is directed into the metal surface whereas in the second case, the flux is directed
into free space. In this work, the distribution of the electromagnetic field around a
surface-breaking crack is determined for arbitrary values of m. The theory is
developed for cracks of general shape and numerical calculations of the free-space
components of the magnetic field are made for rectangular and semi-elliptical shaped
cracks. The numerical predictions are found to be in good agreement with
experimental measurements of the magnetic field above a rectangular slot, cut in a
flat plate of mild steel.
History
School
Science
Department
Mathematical Sciences
Citation
MICHAEL, D.H. ... et al, 1991. Thin-skin electromagnetic fields in the neighbourhood of surface-breaking cracks in metals. Proceedings of the Royal Society of London: Series A, Mathematical and Physical Sciences [Proc. R. Soc. Lond. A], 434 (no. 1892), pp.587-603.