By A. E. Dukler, Y. Taitel (auth.), G. F. Hewitt, J. M. Delhaye, N. Zuber (eds.)
ISBN-10: 3662016575
ISBN-13: 9783662016572
ISBN-10: 3662016591
ISBN-13: 9783662016596
This is the second one quantity of Multiphase technology and TechnoJogy, a brand new foreign sequence of books meant to supply authoritative overviews of im portant components in multiphase structures. The alm is to have systematic and instructional displays of the country of data in quite a few parts. the target of the chapters is to permit the nonspecialist reader to realize an updated inspiration of the current nation of improvement in a given topic. The reaction to quantity 1 of the se ries has been very confident, and we think that the current quantity may be both weil acquired. quantity 1 used to be involved solely with gas-liquid platforms, and the 1st 4 chapters of the current quantity additionally relate to such structures. despite the fact that, the inten tion of the se ries is to hide a variety of multiphase platforms, and we're, as a result, happy to incorporate within the current quantity chapters that seek advice from liquid liquid and gas-solid multiphase flows, respectively. the 1st bankruptcy within the current quantity is through Professor A. E. Dukler of the collage of Houston, Texas, and Professor Y. Taitel of Tel-Aviv collage, Israel.
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Additional resources for Multiphase Science and Technology: Volume 2
Example text
47 ) and (48) is to predict the smooth liquid level with time and position in the absence of local waves. Then, at each point of space and time this level is used to determine if a wave will grow in accordance with the mechanism leading to Eq. (26). Once the Bernoulli term is neglected, Eqs. the form au L ah L 3X + g dX + E at ah 3t aU L + U + Ur 1J ah + ax H aU L 3x (47) and (48) take (50 ) 0 0 (5I) where H H(h) = AL/A'L' and E = E(h, UL) is minus the right-hand side of Eq. (47). Using standard methods (Stoker, 1957) we can convert Eqs.
The comparison for intermittent flow is not as definitive. 61-m-long test sections are in paor agreement with prediction, as would be expected since these pipes are not long enough to establish slug flow. 4-mm-diameter tube 1. 27-m-long, are in agreement ,>lith theory, as shown in Fig. 29. For the data displaying slug flow, the value of Q was less than 5, and the theoretical transition curves have been calculated accordingly. The theoretical region for slug flow is above A and to the right of B, precisely where the da ta are seen to fall.
6 The Flow Pattern Map: Summary Figures 12 and 13 display the resulting gener2~i2ed flow pattern maps. The transitions shown in Fig. 12 are independent of inclination angle. Given the gas and liquid rates, the tube size, and inclination angle, the values of X and Y are calculated and Fig. 10 is used to find hiD. The parameters F, T, and Kare then determined, and the location of the coordinate pairs (F versus kiD, T versus kiD, 11. versus hlD) is used to determine the pattern. For any fixed angle a map such as that shown in Fig.
Multiphase Science and Technology: Volume 2 by A. E. Dukler, Y. Taitel (auth.), G. F. Hewitt, J. M. Delhaye, N. Zuber (eds.)
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