By Boris Pasternak
First released in Italy in 1957 amid foreign controversy, Doctor Zhivago is the tale of the existence and loves of a poet/physician in the course of the turmoil of the Russian Revolution. Taking his kinfolk from Moscow to what he hopes may be preserve within the Ural Mountains, Zhivago reveals himself as an alternative embroiled within the conflict among the Whites and the Reds. Set by contrast backdrop of cruelty and strife is Zhivago's love for the gentle and gorgeous Lara, the very embodiment of the ache and chaos of these cataclysmic instances. Pevear and Volokhonsky masterfully repair the spirit of Pasternak's original—his kind, rhythms, voicings, and tone—in this pretty translation of a vintage of worldwide literature.
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Extra resources for Doctor Zhivago
The RFD correction factor falls between two extreme values: (i) for open bundles where the subchannel flow and enthalpy imbalance is small, and the maximum heat flux controls the initial occurrence of CHF. 8) depends also on the subchannel and flow imbalance. For this case a technique for obtaining a K6 value based on RFD was proposed by Yin et al. (1991), but this still requires knowledge of the RFD corresponding to simultaneous CHF occurrence across the bundle (this could possibly be obtained from subchannel codes).
Design 124 229–245. , 1974, “Study of CHF in rod bundles for WWER type reactors”, Proc. Thermophysical Mtg TF-74, Moscow (57–66). , 1976, Experimental study and statistical analysis of CHF data for WWER type reactors, Teploenergetika 2 80–82. , 1995, A method of evaluating the critical heat flux in channels and cells of arbitrary geometries, Thermal Engineering 42 3 (221–231). , 1997, Considerations in describing burnout in rod bundles, Thermal Engineering 44 3 (2–7). , 1967, HAMBO, A Computer Programme for the Subchannel Analysis and Burnout Characteristics of Rod Clusters, Part I.
1996) have presented a complete description of the new table including its derivation, and accuracy with respect to the world database, and a comparison with other widely used CHF prediction methods. 2. Rod bundles The tube CHF look up [Groeneveld et al. (1996), see also Appendix II] needs to be converted into a prediction method for bundle geometries. 4 item 3. Ideally a subchannel code should be used to predict the CHF for bundle geometry. Several subchannel codes are currently in existence [see review article by Weisman (1975) for more details] but their validation tends to be limited to a narrow range of bundle geometries and flow conditions for which their constitutive relations have been tuned to agree with the experimental database.