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Surface waves variation with frequency

With the laser pulse energy W = 10 5 J, the laser spot diameter d = 10X on the dielectric surface, and the light frequency v = 5x 1014 s 1, the electron velocity variation is Au = 2x 108exp(-z/zo) centimeters per second. This means that an electron beam with an energy E - 100 eV (v = 5.9 x 108 cm/s) reflects at a substantial angle of

evanescent wave produced by a femtosecond laser pulse. [Pg.190]

Acoustical properties of soybeans can be used to help distinguish between healthy and diseased soybeans. Misra et al. (1990) measured acoustic properties of soybeans by transmitting sound waves through soybeans using acoustic transmission and by an impact force method. In the impact force method, a seed is dropped on an acoustic transducer creating an impulse wave. The acoustic transmission method was slow but was able to predict the mass of individual soybeans. The impact force method showed that diseased soybeans had a narrower bandwidth than healthy soybeans. Soybeans with wrinkled surfaces and diseased and damaged soybeans were detected from healthy soybeans based on wide variations at low frequencies. [Pg.174]

Figure 6.22. The output of a white light source is modulated with a variable-frequency beam chopper so that a square wave is produced which illuminates one surface of the sample. The fluctuating alternating temperature is measured on the other surface using a thermocouple. Figure 6.23 shows the variation in Fac as a function of time for materials of large and small heat capacity. Owing to recent improvements... Figure 6.22. The output of a white light source is modulated with a variable-frequency beam chopper so that a square wave is produced which illuminates one surface of the sample. The fluctuating alternating temperature is measured on the other surface using a thermocouple. Figure 6.23 shows the variation in Fac as a function of time for materials of large and small heat capacity. Owing to recent improvements...
Fig. 6, which shows that the amplitude of the pressure wave in a liquid following a collapsing cavitation bubble rises steeply as the bubble radius diminishes. The pressure can attain enormously high values, but their dpr ioa is only a small fraction of the total collapse time and their effects are concentrated Oder a very small voitime of the liquid near the bubble surface only. The variation of this maximum liquid pressure with ultrasonic frequency is shown in Fig. 7. From this it follows that, if intense cavitation is desired, the ultrasonic frequency should be as low as possible. Fig. 6, which shows that the amplitude of the pressure wave in a liquid following a collapsing cavitation bubble rises steeply as the bubble radius diminishes. The pressure can attain enormously high values, but their dpr ioa is only a small fraction of the total collapse time and their effects are concentrated Oder a very small voitime of the liquid near the bubble surface only. The variation of this maximum liquid pressure with ultrasonic frequency is shown in Fig. 7. From this it follows that, if intense cavitation is desired, the ultrasonic frequency should be as low as possible.

See other pages where Surface waves variation with frequency is mentioned: [Pg.46]    [Pg.253]    [Pg.352]    [Pg.336]    [Pg.8817]    [Pg.1671]    [Pg.22]    [Pg.280]    [Pg.89]    [Pg.154]    [Pg.938]    [Pg.478]    [Pg.221]    [Pg.246]    [Pg.313]    [Pg.177]    [Pg.154]    [Pg.98]    [Pg.303]    [Pg.173]    [Pg.514]    [Pg.52]    [Pg.329]    [Pg.509]    [Pg.35]    [Pg.32]    [Pg.55]    [Pg.222]    [Pg.188]    [Pg.782]    [Pg.20]    [Pg.53]    [Pg.265]    [Pg.4674]    [Pg.627]    [Pg.27]    [Pg.710]    [Pg.1012]    [Pg.177]    [Pg.429]    [Pg.108]    [Pg.205]    [Pg.240]    [Pg.258]    [Pg.104]    [Pg.499]    [Pg.10]   
See also in sourсe #XX -- [ Pg.102 , Pg.103 , Pg.104 , Pg.105 , Pg.106 , Pg.110 , Pg.163 , Pg.164 , Pg.176 ]




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Frequency variations

Surface waves

Variation with

Waves wave frequency

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