Quasi-shear

Notch tip With perpendicular grain orientation no notch tips are detected. The snapshots (see Fig. 7 second and third snapshot from top on the right) show that in the direction to the receiver there is a gap in the reflected / diffracted quasi shear wavefront. In contrast, the notch tips can be detected within the herringbone structure. 

Figure 9 Slowness diagram At the interface between isotropic steel and a V-bntt weld with 10° inclination and perpendicular grain orientation the incident 45° (with regard to the sample top surface) shea.r wave will split into two quasi shear waves qSV and qSV( 2.)...

Splitting into two quasi shear waves If the transducer is coupling to the isotropic steel the incident shear wave may split into two independent quasi shear vertical wave-... 

The isotropic part has not changed. The quasi pressure (qP) curve splits up into a real and an imaginary branch . During this real part the transversal share of the polarization increases until the wave becomes a quasi shear vertical wave. Furthermore, the wave is not anymore a propagating but an evanescent wave in this part. The branch is again only real, it is part of the quasi shear vertical (qSV) curve of the homogeneous case (dotted line), its polarization is dominated by the transversal share and the wave is a propagating one. For the branches (real) and... 

Using now the phase matching condition, it can be seen that besides the quasi shear wave (qSV) which is obtained as usual, a second quasi shear wave (qSV(2)) results from the upper quasi shear wave part. Since the direction of the group velocity vector points downwards this wave is able to propagate and can be seen in the snapshot (see Fig. 10) if a is properly adjusted, i.e. is pointing upwards as in Fig. 2. 

Like the isotropic wave equation the Christoffel equation has three solutions, although in general there is no degeneracy except along symmetry directions. The motions of the particles are orthogonal for the three solutions, but not necessarily exactly parallel or perpendicular to the propagation direction, and so the waves are described as quasi-longitudinal or quasi-shear. 

For each section, the quantity p(w/k)2 is given for the pure shear wave, which is polarized perpendicular to the plane of the section, and for the quasi-shear and quasi-longitudinal waves, which each have particle motion in the plane of the section. The angle between the wavevector k and the lowest symmetry direction in the plane is denoted by 0. 

In the surface of an anisotropic solid the situation is more complicated. Pure Rayleigh waves can exist only along certain symmetry directions in which pure SV waves exist. Away from these directions, however, the two quasi-shear polarizations are not pure SV and SH therefore, although the particle motions are orthogonal, at the surface they can be weakly coupled. If the SH mode has a higher velocity than the SV, then there can be no real solution to Snell s law... 

The quasi-tensiie and quasi-shear tape tests showed that the films were strongly adhered to the surface of the polymers. This is believed to result from the establishment of covalent bonding in a four-stage process and is not due to the initial effect of the formation of the expected hydrogen bonding between the ceramic and polymer phases. The stages in the formation of the bonding include ... 

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