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Wave reflections

This study detects the defect of the void and the exfoliation in the solid phase diffusion bonding interface of ductile cast iron and stainless steel with a nickel insert metal using ultrrasonic testing method, and examine the influence of mutual interference of the reflectional wave both the defect and the interface. [Pg.833]

As a result, the interference of the reflectional wave is shown the change for the position both the defects and the interfaces, and the size of the defect. And, the defect detection quantitatively clarified the change for the wave lengths, the reflection coefficient of sound pressure between materials and the reverse of phase. [Pg.833]

Therefore, the ultrasonic testing method in the diffusion joint of the dissimiler materials shall considered the influence of the interference with the reflective wave. [Pg.839]

For the reflected wave associated with equation (A3.11.13a). the total outgoing flux is ss /i -[ [,so the reflection probability is... [Pg.962]

Reflected wave a wave that is repelled at the joint. Sec Figure 18.9... [Pg.597]

E = voltage of the incident wave (incoming wave) /T = voltage of the reflected wave. [Pg.597]

E = IncidenI wave = Reflected wave E" = Refracted wave... [Pg.597]

Figure 18.10 Magnitudes of refracted and reflected waves under different junction conditions. Figure 18.10 Magnitudes of refracted and reflected waves under different junction conditions.
The reflected wave will dampen the incidence surge by... [Pg.603]

When an electron scatters from an atom, its phase is changed so that the reflected wave is not in phase with the incoming wave. This changes the interference pattern and hence the apparent distance between the two atoms. Knowledge of this phase shift is the key to getting precise bond lengths from SEXAFS. Phase shifts depend mainly on which atoms are involved, not on their detailed chemical environment, and should therefore be transferable from a known system to unknown systems. The phase shifts may be obtained ftom theoretical calculations, and there are published tabulations, but practically it is desirable to check the phase shifts using... [Pg.229]

A powerful characteristic of RAIR spectroscopy is that the technique can be used to determine the orientation of surface species. The reason for this is as follows. When parallel polarized infrared radiation is specularly reflected off of a substrate at a large angle of incidence, the incident and reflected waves combine to form a standing wave that has its electric field vector (E) perpendicular to the substrate surface. Since the intensity of an infrared absorption band is proportional to / ( M), where M is the transition moment , it can be seen that the intensity of a band is maximum when E and M are parallel (i.e., both perpendicular to the surface). / is a minimum when M is parallel to the surface (as stated above, E is always perpendicular to the surface in RAIR spectroscopy). [Pg.251]

Deflagrations and detonations produce pressures associated with the resulting shock/pressure waves. These pressures can be sufficiently large to damage and/or demolish enclosed vessels, equipment, and buildings. A deflagration can produce pressure rises in excess of 8 1 and rises of 40 1 when a reflected wave develops from a detonation, referenced to the initial pressure of the sys-... [Pg.496]

The term exp[iax] in equations (2.47) indicates travel in the positive x-direction, while exp[—iax] refers to travel in the opposite direction. The coefficient A is, then, the amplitude of the incident wave, B is the amplitude of the reflected wave, and F is the amplitude of the transmitted wave. In region III, the particle moves in the positive x-direction, so that G is zero. The relative probability of tunneling is given by the transmission coefficient T... [Pg.54]

In a bath-type sonochemical reactor, a damped standing wave is formed as shown in Fig. 1.13 [1]. Without absorption of ultrasound, a pure standing wave is formed because the intensity of the reflected wave from the liquid surface is equivalent to that of the incident wave at any distance from the transducer. Thus the minimum acoustic-pressure amplitude is completely zero at each pressure node where the incident and reflected waves are exactly cancelled each other. In actual experiments, however, there is absorption of ultrasound especially due to cavitation bubbles. As a result, there appears a traveling wave component because the intensity of the incident wave is higher than that of the reflected wave. Thus, the local minimum value of acoustic pressure amplitude is non-zero as seen in Fig. 1.13. It should be noted that the acoustic-pressure amplitude at the liquid surface (gas-liquid interface) is always zero. In Fig. 1.13, there is the liquid surface... [Pg.21]

When microwaves travel along a waveguide terminated by the microwave heating application (for example a resonant cavity loaded by the object to be heated) a reflected wave travels back towards the source. The wave traveling towards the termination is called the incident wave and the wave traveling back to the magnetron is... [Pg.20]


See other pages where Wave reflections is mentioned: [Pg.164]    [Pg.838]    [Pg.2866]    [Pg.127]    [Pg.670]    [Pg.134]    [Pg.164]    [Pg.568]    [Pg.570]    [Pg.597]    [Pg.597]    [Pg.598]    [Pg.598]    [Pg.599]    [Pg.624]    [Pg.647]    [Pg.87]    [Pg.88]    [Pg.249]    [Pg.57]    [Pg.195]    [Pg.418]    [Pg.132]    [Pg.133]    [Pg.203]    [Pg.167]    [Pg.346]    [Pg.310]    [Pg.97]    [Pg.129]    [Pg.21]   
See also in sourсe #XX -- [ Pg.20 ]

See also in sourсe #XX -- [ Pg.20 ]

See also in sourсe #XX -- [ Pg.91 , Pg.94 ]




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Attenuated total reflection surface plasmon waves

Electromagnetic wave reflected

Evanescent light wave reflection

Internal reflection evanescent wave

Laser wave, evanescent, electron reflection

Light wave reflection

Normal reflection, blast waves

Plane waves vacuum interface, reflection

Plane-wave reflection

Plasma Absorption and Reflection of Electromagnetic Waves Bouguer Law Critical Electron Density

Protein internal reflection evanescent wave

Reflected Detonation Wave Parameters

Reflected stress waves

Reflected vector plane wave

Reflected vector spherical wave functions

Reflected wave

Reflection Rayleigh wave

Reflection and Refraction of Plane Waves

Reflection and Transmission of Electromagnetic Waves

Reflection of Shock Wave

Reflection of a plane wave

Reflection of electromagnetic waves

Reflection of plane wave

Reflection of the Blast Wave at a Surface

Reflection of waves from interfaces

Reflection, blast waves

Reflection, shock wave

Regular and Mach Reflection of Detonation Waves

Retonation Caused by the Reflection of Divergent Waves

Shear wave reflectance method

Shock Wave Propagation and Reflection in Solid Materials

Total internal reflectance fluorescence evanescent wave

Traveling wave multiple reflection

Traveling wave reflection coefficients

Travelling wave reflection

Ultrasonic wave reflection coefficient

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