2015
DOI: 10.1016/j.fusengdes.2015.03.021
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Simulation of the ICE P1 test for a validation of COCOSYS and ASTEC codes

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Cited by 4 publications
(4 citation statements)
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“…The mathematical model of heat/mass transfer in the containment (Zaitsev 2005, Levchenko 2007) is a system of ordinary differential equations for conservation of momentum, energy and gas mixture components recorded for each selected control volume. This approach (i.e., modeling in lumped parameters) has become a frequent practice (Gauntt et al 2001, Murata 1997, Povilaitis et al 2015. In view of the significant effect of compressibility on the gas flow characteristics, instead of the momentum-conservation equation, dependences obtained for the adiabatic gas flow from pressure vessels are used.…”
Section: Calculation Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…The mathematical model of heat/mass transfer in the containment (Zaitsev 2005, Levchenko 2007) is a system of ordinary differential equations for conservation of momentum, energy and gas mixture components recorded for each selected control volume. This approach (i.e., modeling in lumped parameters) has become a frequent practice (Gauntt et al 2001, Murata 1997, Povilaitis et al 2015. In view of the significant effect of compressibility on the gas flow characteristics, instead of the momentum-conservation equation, dependences obtained for the adiabatic gas flow from pressure vessels are used.…”
Section: Calculation Methodsmentioning
confidence: 99%
“…The pressure in the left branch at the "0 m" elevation is equal to Р 0 + 40r 0 g. The pressure in the right branch at the "0 m" elevation will be greater, since the branch height-average gas density due to its compressibility in calculated Boxes 4, 3 and 2 is greater than r 0 , i.e., this nodalization scheme (if the Boltzmann density distribution throughout the box height is ignored) leads to the appearance of a non-zero pressure drop, causing the gas flow. Figures 3 and 4 show the results of numerical calculations of the considered closed loop with parameters close to the actual values of modern NPP containments (Table 2); the calculations were based on two mathematical models (one of height invariable dencity gas inside the box and the other of the SIMCO code, taking into account the gas compressibility (Povilaitis et al 2015)).…”
Section: Figure 1 Difference Between the Analytical And Numerical Somentioning
confidence: 99%
“…The program COCOSYS, a lumped-parameter code, is being developed by the Gesellschaft für Anlagen-und Reaktorsicherheit (GRS) gGmbH, Germany, for the simulation of all relevant processes and plant states during severe accidents in containment of light water reactors. And this code is widely used in nuclear engineering [8,9]. The characteristic feature of lumped-parameter approach is that mass and energy are transferred between control volumes by junctions, according to momentum equation solution for each junction.…”
Section: Introductionmentioning
confidence: 99%
“…Skaitiniame modelyje daroma prielaida, kad ITER struktūrinių ir funkcinių medžiagų bandiniai buvo apšvitinti dideliais 14 MeV neutronų srautais (O-I)LTIS lokalizacijose. Šioje pozicijoje neutronų srautas yra didžiausias (iki 1020 n/m 2 , palyginti su sumine 1,7 • 10 21 neutronų išeiga), kaip ir dislokacijų kiekis, tenkantis atomui (10 -5 dpa). Bandinių aktyvumas ir dozės galios skaičiavimai po neutronų apšvitos buvo atlikti naudojant FISPACT-2010 programų paketą su EAF-2010 duomenų biblio teka.…”
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