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Increasing σg, Z, Cs reduces the width of the layer.
The speed and the width of the layer are rigorously defined via dimensionless quantities.
The micro-statistical model is formulated in terms of hypersingular integral equations and used to investigate in detail the influences of the material constants of the piezoelectric layer and the half-space and the width of the layer on the effective properties of the interface.
Width of the layer in glass micromodel (ft).
In Figure 5d, it is clear that the width of the layer structure is about 3 μm.
According to our estimation, width of the layer on the small angle cross section more than 60 times exceeds its width on the vertical cross section.
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The magnitude of the effects depends on the surface and interface scattering parameters and the width of the layers.
We show that the quality of the image is affected not only by absorption but also the finite width of the layers.
The profound effect of parameters like material gradients (piezoelectric, dielectric and elastic) and width of the layers, on the phase velocity of Love type wave are presented graphically.
We found that previous SZP descriptions of these layers underestimate the width of the layers by almost 15%.
This has to be taken into account especially when the width of the layers and the probe size are in the same range.
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