Thermal modes of heterogeneous exothermic reactions. Solid-phase interaction

2017 ◽  
Vol 185 ◽  
pp. 93-104 ◽  
Author(s):  
Valeriy Yu. Filimonov ◽  
Konstantin B. Koshelev ◽  
Alexander A. Sytnikov
2016 ◽  
Vol 26 (5) ◽  
pp. 405-406 ◽  
Author(s):  
Sergey S. Ostakhov ◽  
Gul'shat A. Masyagutova ◽  
Alexander V. Mamykin ◽  
Sergey L. Khursan

2019 ◽  
Vol 2 (2) ◽  
pp. 61-77
Author(s):  
Puskar R. Pokhrel ◽  
Bhadra Man Tuladhar

In this paper, we present simple and exact eigenvalues for both the solid- and fluid-phases of the real two-phase general model developed by Pudasaini (2012); we call these phase-eigenvalues, the solid- phase-eigenvalues and the fluid-phase-eigenvalues. Results are compared by applying the derived phase- eigenvalues that incorporate the phase-interactions in the two-phase debris movements against the simple and classical solid and fluid eigenvalues without any phase interaction. We have constructed several different set of eigenvalues including the coupled phase eigenvalues by using rational factorization method. At first, we consider for general debris height; factorizing the solid and fluid lateral pressure contributions by considering the negligible pressure gradient; negligible solid lateral pressure; negligible fluid lateral pressure; negligible solid and fluid lateral pressure. Secondly, for a thin debris ow height, we also construct the fourth set of eigenvalues in three different cases. These phase-eigenvalues incorporate strong interaction between the solid and fluid dynamics. The simulation results are produced by taking all these different sets of coupled phase-eigenvalues and are compared with the classical uncoupled set of solid and fluid eigenvalues. The results indicate the importance of phase-eigenvalues and supports for a complete description of the phase- eigenvalues for the enhanced description of real two-phase debris flows and landslide motions.


2017 ◽  
Vol 192 ◽  
pp. 801-807 ◽  
Author(s):  
Ramil G. Bulgakov ◽  
Gul'shat A. Masyagutova ◽  
Alexander V. Mamykin ◽  
Sergey S. Ostakhov ◽  
Dim I. Galimov ◽  
...  

2016 ◽  
Vol 50 (6) ◽  
pp. 438-441 ◽  
Author(s):  
A. V. Mamykin ◽  
G. A. Masyagutova ◽  
S. L. Khursan

Atomic Energy ◽  
2017 ◽  
Vol 122 (3) ◽  
pp. 200-206
Author(s):  
S. V. Chizhevskaya ◽  
A. V. Zhukov ◽  
G. D. Polenov ◽  
A. B. Arzmanova

2021 ◽  
Vol 91 (2) ◽  
pp. 232
Author(s):  
В.Б. Хабенский ◽  
В.И. Альмяшев ◽  
В.С. Грановский ◽  
Е.В. Крушинов ◽  
С.А. Витоль ◽  
...  

At a severe accident of nuclear power plants with light-water reactors, the most effective way to localize the forming melt (corium) is to keep it in the cooled reactor vessel, the integrity of which depends on the value of heat flux from the melt to the reactor vessel. In this case, one of the critical processes is the melt oxidation by a water steam or a steam-air mixture. It process can lead to a significant increase in the thermal load on the reactor vessel due to a heat of exothermic reactions of oxidation of reducing agents, which presents in the melt, a thickness decreasing of the metallic part of the molten pool, and a hydrogen release. All of these factors strictly depends on the rate of oxidation. When considering the conditions of melt oxidation, it taken into account that for the accepted scenarios of a severe accident, the most realistic situation is the presence of a solid-phase oxide layer (oxidic crust) on the melt surface. Under these conditions, a dependence for calculating the rate of core melt oxidation based on the diffusion model proposed and its validation by using the obtained experimental data performed.


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