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Sound absorption method

AiST Methods. After a rapid alteration of K by changing an external condition, the solution composition readjusts at a finite rate in an attempt to reattain equilibrium this process of adjustment is called relaxation. Several experimental techniques for achieving the necessarily rapid alterations of K have been developed. These include a pressure-jump (sound-absorption) method, an electric-field (dissociation) method, and a temperature-jump method. A temperature jump is brought about by passing an electrical current through the solution in a special cuvette, producing an abrupt, nearly instantaneous, rise in the temperature of the solution. A reaction then takes place as the concentrations adjust to the new temperature. Regardless of the type of perturbation used, the treatment of the data is essentially the same. [Pg.530]

The dissociation field effect, pressure jump, and sound absorption methods have all made important contributions to our present understanding of fast reactions in aqneous solutions. We will discuss the first technique in some detail and do little more than refer the interested reader to recent sources of information on the two other relaxation methods. [Pg.79]

Test Methods. Two basic types of test methods are commonly used to measure sound-absorption in test laboratories the reverberation room method and the impedance tube method. [Pg.311]

Because the reverberation room test method approximates many real-world conditions, it is used to derive sound-absorption coefficients for evaluating the effect of most actual appHcations of sound-absorbing treatments. Sound-absorption coefficients pubflshed in acoustical textbooks and by manufacturers of acoustical materials are almost exclusively from reverberation room tests, and this may be assumed unless specified otherwise. [Pg.311]

One advantage of the impedance tube test methods is the small (usually <10 cm (4 ia.) dia) size of the test samples. For these tests sound impinges on the test sample only at normal iacidence to the surface, and the sound-absorption coefficients derived ia this manner are vaUd only at this angle. [Pg.312]

Test Methodfor Sound Absorption and Sound Absorption Coefficients by the Reverberation Room Method, ASTM C423-90a, ASTM, Philadelphia, Pa., 1990. Standard Practices for Mounting Test Specimens During Sound Absorption Tests, ASTM E795-92, ASTM, Philadelphia, Pa., 1992. [Pg.321]

Method. When rapid techniques are involved the following abbreviations apply F, flow TJ, temperature jump PJ, pressure jump E, electrochemical NMR, nuclear magnetic resonance ESR, electron spin resonance SA, sound absorption EF, electric field. Classical methods for investigating kinetics are not specified unless low temperatures (LT) have been used. [Pg.59]

To answer the above question new results have been obtained by the study of very fast protolytic reactions in aqueous solution. These were carried out during the last few years by means of relaxation methods (sound absorption, dispersion of the dissociation field effect, temperature jump method) (for a survey cf. [3]). The neutralization reaction HgO+ -j- OH- - (Ha0)8 is the most characteristic example. It was possible to determine the rate constant of this reaction by measuring the time dependence of the dissociation field effect of very pure water of specific conductivity of 6 7 10-8 (at 25°C). [Pg.430]

The volume difference can be found without the use of high-pressure techniques in favorable cases from the amplitude of the sound absorption observed in ultrasonic relaxation of the spin equilibrium. This method will be described below in Section III,C. [Pg.10]

Perturbation of a chemical equilibrium by ultrasound results in absorption of the sound. Ultrasonic methods determine the absorption coefficient, a (neper cm-1), as a function of frequency. In the absence of chemical relaxation the background absorption, B, increases with the square of the frequency f (hertz) that is, a/f2 is constant. For a single relaxation process the absorption increases with decreasing frequency, passing through an inflection point at the frequency at (radians sec-1 = 2nf) which is the inverse of the relaxation time, t (seconds), of the chemical equilibrium [Eq. (6) and Fig. 3]. [Pg.18]

The imaginary part of the transfer function Sim has a frequency dependence shown in Fig. 10(b). It represents the amount of energy transferred to the system per period of oscillation owing to the relaxation, and the relaxation time corresponds to the frequency at which the greatest interaction occurs. Again, the effect on sound waves has been widely used. Methods making use ofS, , all involve the measurement of energy absorption they are called absorption methods. [Pg.138]

ASTM C 522 covers the measurement of airflow resistance and the related measurements of specific airflow resistance and airflow resistivity of porous materials that can be used for the absorption and attenuation of sound. The method describes how to measure a steady flow of air through a test specimen, how to measure the air-pressure difference across the specimen, and how to measure the volume velocity of airflow through the specimen. The airflow resistance, R, the specific airflow resistance, r, and the airflow resistivity, rQ, may be calculated from the measurements. The apparatus includes a suction generator or positive air supply arranged to draw or force air at a uniform rate through the specimen. A flowmeter is used to measure the volume velocity of airflow through the specimen, and a differential-pressure-measuring device measures the static-pressure difference between the two faces of the specimen with respect to atmosphere. [Pg.372]

Measured by NMR. sound absorption, or miJtidentate tigand method. [Pg.545]

The main industrial control approaches include use of sound absorption, enclosures, barriers, and vibration isolation and damping. These methods are briefly described below. [Pg.865]

The rates of complex formation of valinomycin with Na+ and K+ were obtained by a combination of measurements carried out with the help of the sound absorption and T-jump method. Both techniques were required in order to resolve the relaxation spectrum, which includes the rate processes for complex formation as well as for structural changes of the valinomycin molecule 37). [Pg.20]

Two-component IPN foams consisting of polyurethane and epoxy were prepared by the one-shot, free-rise method. The effects of PU/E ratio on the sound absorption and mechanical energy attenuation characteristics were determined with varying levels of different fillers and plasticizers. The formulations (Table IX) were based on the best elastomer results. An average of over 90X absorption was obtained at high frequencies by the Impedance tube method. However, this average drops dramatically at low frequencies. This reduction may be seen in Figs. 3 and 4 for 90/10 and 70/30 IPN foams vlth 20X... [Pg.289]

Stationary relaxation methods include sound absorption und dlNpcrRlon and dielectric dispersion. A sound wave is used to perturb thc system (hat causes temperature and pressure alterations on an oscillating electric field. Then, chemical relaxation is measured by determining adsorbed energy (acoustical absorption or dielectric loss), or a phase lag that is dependent on the frequency of a forcing function (Bernasconi, 1986 Sparks, 1989). In this chapter, only transient relaxation methods will be discussed. [Pg.63]

During a second step we carried out measurements of the Brillouin position and Brillouin line width which are related to the sound velocity and sound absorption. We use the method of Zamir, et al. ° With our current setup, the Rayleigh line provides us with the apparatus window function from where the FSR and the finesse for each spectrum are measured. During a second step we carried out measurements of the Brillouin position and Brillouin line width which are related to the sound velocity and sound absorption. We use the method of Zamir, etal. °... [Pg.158]

The normal incidence sound absorption coefficient of a material can be determined using the method described in BS EN ISO 9614 [69] (BS 4196. Part 5 [70]). In this type of determination, a plane sound wave is made to be reflected by the sample mounted in a standing wave tube. The single-frequency wave hits the sample at normal incidence, and the amplitudes of the incident and reflected waves are measured over a series of chosen frequencies. Usually the frequencies of interest lie between 50 and. 00 Hz, although some automotive specifications will cover much wider ranges (sec Ford Engineering Specification WSK-M2D406-A). [Pg.403]

Acoustic standing wave method (Markiewicz et al., 2009) is the most popular way to determine the sound absorptive power of the material sample subjected to the plane acoustic wave. In this method, plane acoustic waves are generated by a loudspeaker placed at one end of a tube while the other end is terminated by the material sample. Due to the reflections from the sample, standing wave is produced in the tube as the superposition of the incident wave with the amplitude A and the reflected one with the amplitude B. The reflected wave is characterized by lower amplitude and shifted phase in comparison to the incident one. The probe microphone, moved inside the tube, receives the alternating acoustic pressure of minimum amplitude pmin=A-B at the distance of, i/4 X - wavelength) from the sample followed by the pressure of maximum value pmax=A+B at XI2. As the acoustic wave energy is proportional to the square of the sound pressure, the equation (3) can be written ... [Pg.197]


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