P20-T50-V15-H08
P20-T50-V20-H09
P20-T50-V25-H10
P20-T50-V30-H08
P20-T50-V35-H11
P20-T50-V20-H67
P20-T50-V25-H66
P20-T50-V30-H65
P20-T50-V35-H64
P25-T50-V20-H71
P25-T50-V25-H70
P25-T50-V30-H71
P25-T50-V35-H74
P25-T50-V15-H02
P25-T50-V20-H02
P25-T50-V25-H03
P25-T50-V30-H03
P25-T50-V35-H05
P05-T40-V06-H03
P05-T40-V06-H33
P05-T40-V06-H34
P05-T40-V06-H39
P05-T40-V06-H47
P05-T40-V06-H52
P05-T40-V06-H55
P05-T40-V06-H57
P05-T40-V06-H59
P05-T40-V06-H62
P05-T40-V06-H62
P05-T40-V06-H64
P05-T40-V06-H65
P05-T40-V06-H66
P05-T40-V06-H67
P05-T40-V06-H69
P05-T40-V06-H70
Temperature and relative humidity of the incoming mixture, bulk mixture temperature, accumulated condensate level, volumetric flow of mixture, condesing plate temperature, helium injected mass, helium molar concentration, and pressure
Condensation models: Uchida correlation, heat and mass transfer analogy, fog model with time relaxation and rain out, purely diffusive approach.
References: [1] M. Bucci, W. Ambrosini, & N. Forgione. Experimental and Computational Analysis of Steam Condensation in the Presence of Air and Helium. Nuclear Technology, 181(1), 115–132 (2013).
https://doi.org/10.13182/NT13-A15761
[2] W. Ambrosini, N. Forgione, F. Merli, F. Oriolo, S. Paci, I. Kljenak, P. Kostka, L. Vyskocil, J. R. Travis, J. Lehmkuhl, S. Kelm, Y.-S. Chin, & M. Bucci. Lesson learned from the SARNET wall condensation benchmarks. Annals of Nuclear Energy, 74, 153–164 (2014).
https://doi.org/10.1016/j.anucene.2014.07.014
[3] W. Ambrosini, M. Bucci, N. Forgione, A. Manfredini, & F. Oriolo. Experiments and Modelling Techniques for Heat and Mass Transfer in Light Water Reactors. Science and Technology of Nuclear Installations, 2009, 738480 (2009).
https://doi.org/10.1155/2009/738480