Source wave

All these circumstances have lead the industry to begin searching for a new source of energy an alternative and completely petroleum-independent power source. Several technologies are being researched, such as biomass (bio-diesel, ethanol), renewable ocean sources (wave, tidal, and thermal), hydrogen, and many more. 

Subtractive synthesis uses a complex source wave—such as an impulse, a periodic train of impulses, or white noise—to excite a spectral-shaping filter. Linear prediction, or linear predictive coding (LPC), gives us a mathematical technique for automatically decomposing a sound into a source and a filter. For low order LPC (6-20 poles or so), the filter is fit to the coarse spectral... 

Another meaningful observation is that the Green function convolution (integration) with (source) wave-function is done upon the coordinate only in the basic definition, while the entirely time evolution is contained within the Green function. In relation with this aspect one may establish... 

The adaptation of a Bragg X-ray goniometer to measure optical diffraction was described previoxisly (3) as was the procedure utilized to obtain lattice parameters from diffraction data. For studies of variation of diffraction with temperature, the source wave length was varied at fixed Bragg angle (9). 

As a renewable energy source, wave power is an untapped source which could help alleviate the rising cost of energy and its continued development must be encouraged. 

In ecCCSD methods this improvement is achieved by extracting a subset of important three- and four-body cluster amplitudes from the external source wave function and by using them for a physically more meaningful decoupling of the CC chain of equations at the pair cluster level. In practice this means that the external source wave function is first cluster analyzed, and the resulting approximate three- and four-body clusters and respectively, are then used to evaluate the corresponding terms A 3), A 4), and A l,3) in... 

Under ideal conditions (e.g., point sources producing spherical waves and no multiple reflections) a rectified backscattered signal represents line integrals of the ultrasonic reflectivity over concentric arcs centered at the transducer position. To reconstruct the reflection tomo-... 

Using Equ. (3.1), we can now compute the optimum frequency for cracks in various depths (see Fig. 3.2). For comparison, the optimum excitation frequency for a planar wave or a sheet inducer (300 x 160 mm) is also displayed. One finds that for a planar excitation source, a much lower excitation frequency is required, which causes a reducfion in the response signal of the crack of up to an order of magnitude in case of a small circular coil. 

The transmission coefficient Cl (Qj,t), considering transient (broadband) sources, is time-dependent and therefore accounts for the possible pulse deformation in the refraction process. It also takes account of the quantity actually computed in the solid (displacement, velocity potential,...) and the possible mode-conversion into shear waves and is given by... 

Echo directivity was experimentally studied for surface SH Wave probes and SH Wave angle probes. Frequencies used in the experiment were 5MHz and 2MHz, the angles of refraction 90°and 70°, the crystal size 10X 10mm and 5X5mm. The echo directivity was evaluated, using side drilled holes of various depths. The experimental results showed consistency with the calculation based on a point sound source assumption on the test surface in different phases. 

This is an approximation to the complete dispersion equation [131]. The amplitude of a train of waves originating from an infinitely long linear source decays exponentially with the distance x from the source... 

Continuous wave (CW) lasers such as Ar and He-Ne are employed in conmionplace Raman spectrometers. However laser sources for Raman spectroscopy now extend from the edge of the vacuum UV to the near infrared. Lasers serve as an energetic source which at the same hme can be highly monochromatic, thus effectively supplying the single excitation frequency, v. The beams have a small diameter which may be... 

This is not the case for stimulated anti-Stokes radiation. There are two sources of polarization for anti-Stokes radiation [17]. The first is analogous to that in figure B1.3.3(b) where the action of the blackbody (- 2) is replaced by the action of a previously produced anti-Stokes wave, with frequency 03. This radiation actually experiences an attenuation since the value of Im x o3 ) is positive (leading to a negative gam coefficient). This is known as the stimulated Raman loss (SRL) spectroscopy [76]. Flowever the second source of anti-Stokes polarization relies on the presence of Stokes radiation [F7]. This anti-Stokes radiation will emerge from the sample in a direction given by the wavevector algebra = 2k - kg. Since the Stokes radiation is... 

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