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Electric wave

The velocity of current or voltage waves in any medium is called the velocity of propagation of electricity in that medium. The velocity of electromagnetic waves (electricity) through a conductor is a measure of line or conductor parameters through which it propagates and is represented by... [Pg.564]

When infrared beam incidents upon thin organic films extended over a plain metal surface (Figure 1), there usually occurs a standing wave electric field on the metal surface as a consequence of the interference between the incident and reflected beams. Since the standing wave may interact with, i. e. be absorbed by, molecules in the organic film, the reflectance of the beam from the metal surface is reduced. [Pg.157]

Wave energy is a capital-intensive technology, with most of the costs for construction. But, after 3 decades major breakthroughs are in sight and wave electricity should be part of the renewable mix in many countries before long. [Pg.277]

Determinants and Matrices STATl ST 1CA L M A T11E MATICS Waves Electricity Projective Geometry Integration... [Pg.166]

Let us now consider an infinite right circular cylinder of radius a, which is illuminated by a plane homogeneous wave E, = E0e ke, x propagating in the direction e, = - sin ex — cos fez, where is the angle between the incident wave and the cylinder axis (Fig. 8.3). There are two possible orthogonal polarization states of the incident wave electric field polarized parallel to the xz plane and electric field polarized perpendicular to the xz plane. We shall consider each of these polarizations in turn. [Pg.195]

This equation allows for the fact that the density of light flux is equal to the squared modulus of the wave electric field in a semiconductor < (2) is found by solving Eq. (51). [Pg.297]

The perturbation, H" = -p E, represents the interaction of the light wave electric field with the molecule. The solutions to the wave equation 6 are given by... [Pg.15]

The electric dipole interaction of the standing wave electric field in a Fabry-Perot cavity with a two-level system has been treated theoretically by Campbell, Buxton,... [Pg.709]

Figure 10 shows the amplitude-weighted phase difference (AWPD) and phase structure (AWPS) functions 1.37 measured using PALS for the aqueous CdS particles (144] discussed in Fig. 9. The conditions are identical (24 C and u = 24 ) with the experiment employing a moving real fringe setup [1.37] and a. 30 Hz, 1.37 V/mm sine wave electric field. The autotrack results utilize a feature of the experimental analysis software [140] that corrects for other convective effects such as sedimentation. The mobility of the particles can be determined by analyzing the data in Fig. 10 with appropriate models for AWPD and AWPS functions (137], Analysis of the data in Fig. 10 yielded AWPD and AWPS... Figure 10 shows the amplitude-weighted phase difference (AWPD) and phase structure (AWPS) functions 1.37 measured using PALS for the aqueous CdS particles (144] discussed in Fig. 9. The conditions are identical (24 C and u = 24 ) with the experiment employing a moving real fringe setup [1.37] and a. 30 Hz, 1.37 V/mm sine wave electric field. The autotrack results utilize a feature of the experimental analysis software [140] that corrects for other convective effects such as sedimentation. The mobility of the particles can be determined by analyzing the data in Fig. 10 with appropriate models for AWPD and AWPS functions (137], Analysis of the data in Fig. 10 yielded AWPD and AWPS...
FIG. 10 Amplitude-weighted phase difference (AWPD) and phase structure (AWPS) functions measured using PALS with autotrack on and off for aqueous CdS particles 1144] at 24 C and 0 = 24 subject to 30 Hz, 1.37 V/mm sine wave electric field. [Pg.241]

The coupling between strain and electrical polarization that occurs in many crystals provides a means for generating acoustic waves electrically. When die structure of a crystal lacks a center of inversion symmetry , the application of strain changes the distribution of charge on the atoms and bonds comprising the crystal in such a manner that a net, macroscopic, electrical polarization of the crys-... [Pg.22]

I applied a brief train of 60-cyclc sine wave electrical current w hencvcr the animal entered one corner of the enclosure. The animal did not stav away from the corner, but rather came back quickly after a brief sortie which followed the first stimulation and came back even more quickly after a briefer sortie which followed the second stimulation. By the time the third electrical stimulus had been applied the animal seemed indubitably to be coming back for more. (Carlson, 2001, p. 457)... [Pg.73]

In order to rigorously describe the nonlinear interaction between the weak pulsed fields, we now turn to the fully quantum treatment of the system. The traveling-wave electric fields can be expressed through single mode operators as j(z, t) = dj(t) Cqz (j = 1, 2), where uj is the annihilation operator for the field mode with the wavevector kp + q. The singlemode operators a and aq possess the standard bosonic commutation relations... [Pg.85]

The layered medium approach is particularly well suited for analysis of standing-wave electric fields in multilayered structures. The recursion relation employed generally has the following form ... [Pg.306]

Figure 7d shows a schematic depiction of the active mixer chip design, consisting of a main flow channel and six pairs of orthogonal side channels [76]. Operation of the mixer chip relies on the perturbation of the main x-directional channel flow by y-directional cross-stream side-channel flows. The side-channel flows are per-turbated by pressure changes through thin membranes affected by a GERF microvalve (Fig. 7e). Square-wave electrical voltage signals (0-800 V) are applied between the electrodes to control the microvalve and, in turn, the perturbation, leading to pulsating sinusoidal cross-stream flows in the six pairs of side channels, as shown in Fig. 8f. Figure 7d shows a schematic depiction of the active mixer chip design, consisting of a main flow channel and six pairs of orthogonal side channels [76]. Operation of the mixer chip relies on the perturbation of the main x-directional channel flow by y-directional cross-stream side-channel flows. The side-channel flows are per-turbated by pressure changes through thin membranes affected by a GERF microvalve (Fig. 7e). Square-wave electrical voltage signals (0-800 V) are applied between the electrodes to control the microvalve and, in turn, the perturbation, leading to pulsating sinusoidal cross-stream flows in the six pairs of side channels, as shown in Fig. 8f.
For a monolayer of dye molecules, Aq may be much smaller than unity. Then, we have an approximated expression of p/s=AAp/AAs [34]. The absorption by the chromophore in the thin film is determined by the square of the scalar product of the two vectors the electric dipole moment of the chromophore and the standing wave electric field of the light at the position of the chromophore. Therefore, AA is proportional to the square of the scalar product of reduced forms (remember that the oxidized form is presumed to be colorless). [Pg.70]

Robertson-Dunn, B. and Linkens, D.A. 1974. A mathematical model of the slow wave electrical activity of the human small intestine. Med. Biol Eng., 12 750 758. [Pg.104]


See other pages where Electric wave is mentioned: [Pg.790]    [Pg.19]    [Pg.448]    [Pg.260]    [Pg.223]    [Pg.306]    [Pg.309]    [Pg.119]    [Pg.190]    [Pg.239]    [Pg.6104]    [Pg.119]    [Pg.749]    [Pg.128]    [Pg.478]    [Pg.34]    [Pg.154]    [Pg.304]    [Pg.51]    [Pg.117]    [Pg.163]    [Pg.84]    [Pg.86]    [Pg.87]    [Pg.91]    [Pg.6103]    [Pg.116]    [Pg.441]    [Pg.53]    [Pg.105]   
See also in sourсe #XX -- [ Pg.42 ]




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Electric Potential Wave Method

Electric Waves in Living Matter

Electric degenerate four-wave mixing

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Electric polarization waves

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Electromagnetic wave electric field

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Harmonic electric-field wave

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Transverse electric wave

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Waves, electric velocity

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