1964
DOI: 10.1007/bf01116388
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Experimental study of a heat transfer crisis

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“…The Reynolds number is formed herein with the mean velocity of the two-phase flow. If one postulates that in the post-dryout region the phase slip can be neglected, one obtains as Reynolds number of the two-phase flow: The Reynolds number determined with equation 3-14is identical with the Reynolds number given in Chapter 6, equation (3)(4)(5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17)(18), for the determination of the pressure loss with unwetted wall. For the determination of the pressure loss and also for the determination of the heat transfer in the post-dryout region it is assumed, that the properties of the steam determine the momentum and heat exchange with the heating surface.…”
Section: Nr= 2 + a -R B 'Pcmentioning
confidence: 81%
“…The Reynolds number is formed herein with the mean velocity of the two-phase flow. If one postulates that in the post-dryout region the phase slip can be neglected, one obtains as Reynolds number of the two-phase flow: The Reynolds number determined with equation 3-14is identical with the Reynolds number given in Chapter 6, equation (3)(4)(5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15)(16)(17)(18), for the determination of the pressure loss with unwetted wall. For the determination of the pressure loss and also for the determination of the heat transfer in the post-dryout region it is assumed, that the properties of the steam determine the momentum and heat exchange with the heating surface.…”
Section: Nr= 2 + a -R B 'Pcmentioning
confidence: 81%