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Bursting process

Fig. 31. Maximum pressures produced throughout the bursting process plotted against bubble radius [118]... Fig. 31. Maximum pressures produced throughout the bursting process plotted against bubble radius [118]...
Fig. 32. Maximum energy dissipation rates produced throughout the bursting process, plotted against bubble radius. The logarithmic scale indicates an exponential dependence of maximum stress on bubble radius for large bubbles. The slight drop in the data point for the smallest bubble as compared to the next smallest may be because of the difficulty in locating the exact place and time of the peak, due to large spatial and temporal gradients beneath the forming jet [113]... Fig. 32. Maximum energy dissipation rates produced throughout the bursting process, plotted against bubble radius. The logarithmic scale indicates an exponential dependence of maximum stress on bubble radius for large bubbles. The slight drop in the data point for the smallest bubble as compared to the next smallest may be because of the difficulty in locating the exact place and time of the peak, due to large spatial and temporal gradients beneath the forming jet [113]...
A. The bursting process as frozen by high-speed photography... [Pg.43]

Surface or internal bursts Processing Ferrous or nonferrous wrought sample Ultrasonic method Magnetic particle method used on wrought ferrous sample... [Pg.140]

Nitrate anions are one of the major ionic species present in the Po Valley fog water drops (Decesari et al, 2001). Recently, the Black Sea was shown to release NOs rich aerosols into the troposphere due to the bubble bursting process (Karakas et al., 2001). In general, aerosol nitrate is estimated to double in the next half century (Thiemens et al., 2003). [Pg.254]

Because by their very nature instabilities are random, the burst process will be random and localised. This means that at any moment of time a proportion of the surface is experiencing burst activity while the remainder will be subject to the more normal laminar sub-layer conditions as discussed in Section 5.2. Over a period of time however, the whole of the surface will have experienced burst activity in addition to the more stable sub-layer conditions. [Pg.42]

The bubble growth and bursting process eventually transforms the flow from a liquid flow with separate bubbles to a vapor flow with separate droplets. Assuming closed pack array of vapor bubbles, the volumes occupied by vapor and liquid per unit volume are n/6 and 1 n/6, respectively. Based on this assumption and log normal... [Pg.249]

Heterostructure and bipolar devices as lasers, diodes, solar cells (Chobola 2001) and transistors (Koncza-kowska 1987) are similar from the point of view of the physical processes, taking place during the device operation. This infers that the basis of the methods of their quahty testing can be similar for all of them. The main source of noise is the excess current which has 1/f spectral density. Occasionally the g-r noise, created by burst processes, is observed. Qualitative characterization of the 1/f excess noise is possible with the use of generalized Hooge s formula (6). The measurable quantity of sample quality and reliability is the indicator Mg given by... [Pg.1830]

Extensional fields are present when turbulent kinetic energy is produced by means of the burst-process. Donohue et al. [133 have shown that the number and intensities of bursts in a turbulent flow are reduced by the addition of polymers. A turbulent time scale, which was derived from measurements of Donohue et al. [133 and which is identical with equation (2), has been presented in C143, [153. The relaxation time derived by Bird... [Pg.85]

Another important parameter of the droplet breakup process is the time necessary for the interfacial-driven instabilities to cause breakup, tb, when the actual capillary number exceeds the critical capillary number. Grace (1982) provided this information in Figure 6.21 for Newtonian fluids. Note that the dimensionless burst time is denoted as which is equal to tb/r, where r is the time scale of the bursting process and it is equal to Rp-Jy- For example, for a polymer blend with p = 0.1,)/ = 10 mN/m, / = 10 qm, Pc = 1.000 Pa s, and Ca/Cac — 10, the dimensionless burst time is 11, and the time scale is equal to 1 s. Thus, the burst time, tb, is equal to 11 s. [Pg.184]

Solution. The time scale of the bursting process is t = RoIJ c/y = s. = 0.07 at p = 1 from Figure 6.24b. The amplitude of the distortion that leads to burst is usually considered to be 0.3% of the initial radius of the midsection. Then Eq. 6.196 gives the dimensionless burst time as... [Pg.187]


See other pages where Bursting process is mentioned: [Pg.133]    [Pg.265]    [Pg.2]    [Pg.47]    [Pg.114]    [Pg.115]    [Pg.446]    [Pg.444]    [Pg.133]    [Pg.115]    [Pg.573]    [Pg.212]    [Pg.300]    [Pg.303]    [Pg.257]    [Pg.522]    [Pg.151]    [Pg.812]    [Pg.182]    [Pg.27]    [Pg.426]    [Pg.371]   
See also in sourсe #XX -- [ Pg.184 , Pg.187 ]




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