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Amplitude, sound waves

Figure 4.8, the difference being in the measurement of electrical potential rather than sound wave amplitude). The sound wave moves along a delay rod to a transducer, which is induced to vibrate. By measuring the amplitude of that sound wave over a range of frequencies, one can calculate the mobihty, hence the zeta potential. [Pg.154]

The previous subsection described single-experiment perturbations by J-jumps or P-jumps. By contrast, sound and ultrasound may be used to induce small periodic perturbations of an equilibrium system that are equivalent to periodic pressure and temperature changes. A temperature amplitude 0.002 K and a pressure amplitude 5 P ss 30 mbar are typical in experiments with high-frequency ultrasound. Fignre B2.5.4 illustrates the situation for different rates of chemical relaxation with the angular frequency of the sound wave... [Pg.2121]

For sufficiently long times (index n ), the exponential can be neglected, leaving an oscillation of the turnover variable phase shifted with respect to the sound wave and with its amplitude reduced by the finite relaxation... [Pg.2122]

When the elastic shock-front speed U departs significantly from longitudinal elastic sound speed c, immediately behind the elastic shock front, the decaying elastic wave amplitude is governed by (Appendix)... [Pg.225]

One of the most important characteristics necessary to completely identify a wave is its intensity, where the intensity is a measure of the sound energy the wave produces. For a sound wave in air, the mass (m) of air moving with an average velocity (v) will have associated with it a kinetic energy of (mv )/2 (joules). In the strictest sense the intensity is the amount of energy carried per second per unit area by the wave. Since the units of energy are joules (J) and a joule per second is a watt (W), then the usual unit of sound intensity (especially in sonochemistry) will be W cm. As we will see later (Eq. 2.13), the maximum intensity (I) of the sound wave is proportional to the square of the amplitude of vibration of the wave (P ). This will have important repercussions in our study of chemical systems. [Pg.30]

As in the case of sound waves, pressure, p, and particle velocity,u, must match at the boundary. The amplitudes... [Pg.518]

This relation is valid only when the compressions and expansions of the sound wave are truly reversible and adiabatic. This is the case if the frequency is fairly low and the amplitude small. [Pg.429]

Lighthill, M. J. 1956 Viscosity effects in sound waves of finite amplitude. Surveys in mechanics. Cambridge University Press. [Pg.146]

Equality occurs in the limit of very small shock wave amplitude as the amplitude increases, D increases indefinitely. The structure of the wave front substantially depends on the relation between the wave velocity D and the speed of sound in the frozen equilibrium, cx. [Pg.156]

The lowest frequency is called the fundamental, all of the other frequencies are multiples of the fundamental and are called harmonics. Doubling the frequency corresponds to raising a note by one octave. When a piano and a flute play middle-A, they both produce a distribution of sound waves with a fundamental frequency of 440 Hertz, but they sound different because the amplitudes of the different harmonics depend on the instrument. [Pg.42]

Consider a stationary sound wave. It is composed of a progressive wave traveling from right to left, and a reflected wave traveling in the reverse direction. Let the amplitude of the wave be A, n its frequency, a any point along the horizontal axis connecting two nodes, X the wave length, and t any instant of time for which a displacement x is to be measured. Then for the first wave,... [Pg.38]

Thus we see that the ratio amplitudes for the particle and the sound wave (or gas element), for constant values of p and p, depend upon the term nd2, so that for a particle having a diameter d the ratio corresponds to one and only one frequency n. Therefore, we conclude that nd2 is a critical function determining the behavior of a particle in a vibrating field. [Pg.39]

These nebulizers rely on a transducer made from a piezo-electric crystal which produces high frequency sound waves in the liquid in the nebulizing unit. The waves give rise to vertical capillaries of liquid ( fountains ) which, when the amplitude of the energy applied is sufficient, break up to provide an aerosol. [Pg.264]

Figure 40. Dependence of ota/v2 (where aa is the amplitude absorption coefficient and v the frequency of the sound wave) on mole fraction of t-butyl alcohol in aqueous mixtures at 70 MHz and 298 K. Figure 40. Dependence of ota/v2 (where aa is the amplitude absorption coefficient and v the frequency of the sound wave) on mole fraction of t-butyl alcohol in aqueous mixtures at 70 MHz and 298 K.
The Helmholtz equation resembles the spatial part of the classical wave equation for matter waves (waves in ocean, sound waves, vibrations of a string, electromagnetic waves in vacuum, etc.) of amplitude F = F(r, f) ... [Pg.56]

As all waves, sound waves are characterised by speed, frequency and amplitude. [Pg.506]

Electroacoustics — Ultrasound passing through a colloidal dispersion forces the colloidal particles to move back and forth, which leads to a displacement of the double layer around the particles with respect to their centers, and thus induces small electric dipoles. The sum of these dipoles creates a macroscopic AC voltage with the frequency of the sound waves. The latter is called the Colloid Vibration Potential (CVP) [i]. The reverse effect is called Electrokinetic Sonic Amplitude (ESA) effect [ii]. See also Debye effect. [Pg.184]


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