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EMATs for Science and Industry: Noncontacting Ultrasonic by Masahiko Hirao PDF

By Masahiko Hirao

ISBN-10: 1441953663

ISBN-13: 9781441953667

ISBN-10: 1475737432

ISBN-13: 9781475737431

EMATs for technological know-how and Industry includes the actual rules of electromagnetic acoustic transducers (EMATs) and the functions to clinical and business ultrasonic measurements on fabrics. The textual content is prepared in 4 components:
-PART I is meant to be a self-contained description of the fundamental parts of coupling mechanism in addition to functional designing of EMATs for numerous reasons. There are numerous implementations to make amends for the low move potency of the EMATs. worthwhile how one can make an EMAT also are offered.
-PART II describes the primary of electromagnetic acoustic resonance (EMAR), which makes the main of contactless nature of EMATs and is the main profitable amplification mechanism for distinctive pace and attenuation measurements.
-PART III applies EMAR to learning the actual acoustics. New measurements emerged on 3 significant matters; in situ tracking of dislocation habit, selection of anisotropic elastic constants, and acoustic nonlinearity evolution.
-PART IV bargains with various person subject matters encountered in business purposes, for which the EMATs are believed to the simplest solutions.

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Extra info for EMATs for Science and Industry: Noncontacting Ultrasonic Measurements

Sample text

6 Axial-Shear-Wave EMAT An axially polarized shear wave, called axial shear wave, travels in the circumferential direction along a cylindrical surface of a circular rod or pipe specimen. , 1996b). lt consists of a solenoid coil to supply the biasing magnetic field along the axial direction, and a meander-line coil surrounding the cylindrical surface to induce the dynamic field in the circumferential direction. The total field oscillates about the axial direction at the same frequency as the driving currents and produces a shearing vibration through the magnetostriction effect, resulting in the axial-shear-wave excitation.

Focalline Fig. 22 Foeusing of the SV waves on a foeal line in solid by the line-foeusing EMAT. (After Ogi et al.. 1999a. ) Fig. 23 Meander-line eoil with nonunifonn spacing fabrieated by a printed cireuit teehnique. to the surface and a meander-line coil to induce eddy currents and the dynamic fields in the surface region. The meander-line spacing is not uniform (Fig. 23).

The magnitude of magnetostriction is of the order of 10-6 for steels and 10-5 for nickel. Coupling between the elastic and magnetic fields for such a ferromag- 25 Coupling Mechanism netic (or piezomagnetic) material can be assumed to take a similar form as that for a piezoelectric material: S1-- d(MS)H lj } H +SUaJ. (J,J=1,2, .. 43) sZ a component of the Here, SI is a component of the engineering strain, compliance matrix at a constant field, and aJ the stress component in contracted notation (Auld, 1973).

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EMATs for Science and Industry: Noncontacting Ultrasonic Measurements by Masahiko Hirao


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