## reflection and transmission of waves pdf

15-7 Reflection and Transmission. A large number of possibilities exist, depending on the combinations of solid, fluid and vacuum of the two media and, if the incident media is a solid, whether the incident wave is pressure or shear wave. Considering that there is no S-wave in the upper layer, we assume that three possible incident waves are Fig. 3.2 Reflection/transmission - oblique incidence A more general situation of reflection and transmission of waves at an interface occurs when the incident wave strikes at an oblique angle. Figure 15-18. Lecture 08 - Reflection and transmission of waves.ppt - Free download as Powerpoint Presentation (.ppt), PDF File (.pdf), Text File (.txt) or view presentation slides online. first solutions for the problem of reflection and transmission of plane waves by a dielectric half-space in vacuum moving parallel and perpendicular to the interface was solved , . (a) The end of the cord is fixed to a peg. Nikolova 2012 LECTURE 05: PLANE WAVE REFLECTION AND TRANSMISSION 8 Reflection and Transmission (Fresnel) Coefficients (Review) • by definition the reflection coefficient Γgives the ratio of the reflected to incident tangential E-field component at the interface • the ratio of the reflected to incident tangential H-field component at the interface is −Γ reflection and transmission phenomena in fluid saturated elastic solids. The work by Huang  discussed the problem of reflection and transmission of electromagnetic waves when the dielectric is moving in any arbitrary direction. (1992). 1 Incidence, reﬂection and transmission waves at the ﬂuid–solid interface. Reflection of a wave pulse on a cord lying on a table. Param eters of bubbly liquid are the same as on figure 2, curves 1 – α 20 =0.0025, curves 2 – α 20 =0.005, curves 3 – α 20 =0.01. 6.2 Plane wave reflection from media interface at normal incidence where ηis the wave impedance of lossy medium 2 and τis z Et xˆ Eoe 2 = τ −γ r o z t e E H y 2 2 ˆ γ η = τ − r 19 Electromagnetic Field Theory by R. S. Kshetrimayum 3/25/2014 2 the transmission coefficient intrinsic wave impedance and propagation constant are The reflection loss during acoustic wave scattering from solid boundaries at the ocean bottom was calculated by Kuo (1992). (b) The end 漀昀 琀栀攀 挀漀爀搀 椀猀 昀爀攀攀 琀漀 洀漀瘀攀⸀ഀ The mode conversions during the reflection and transmission of seismic waves at the boundaries of porous media were studied by de la Cruz et al. density, P-wave velocity and S-wave velocity in a solid medium. wave transmission and reflection is illustrated.