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reactor core
A new supercritical water-cooled reactor (SCWR) core structure (the mixed reactor core) and a new fuel assembly design (two-rows FA) are proposed.
      
By simulating the whole reactor core, the detailed mass flow distribution in the core was obtained.
      
The possibility is discussed of using the obtained data in simulating emergency conditions in the reactor core.
      
The interaction of nuclear reactor core melt with oxide sacrificial material of localization device for a nuclear power plant wi
      
The neutron spectrum at the center of the reactor core was measured by the neutron activation method using the a priori spectrum as a superposition of partial fission and evaporation spectra.
      
Experimental Study of the Deformation of Instantaneous Neutron Spectra from the Fission of 235U Nuclei in Fast-Reactor Core Mate
      
The results from studies of the deformation of the instantaneous neutron spectra resulting from the fission of 235U nuclei in the material of structural elements of a fast reactor core are presented.
      
The neutron spectra at and near the center of the reactor core were measured using neutron activation and fission neutron detectors.
      
A mathematical model of the ГИР-2 reactor core and its experimental room is described.
      
In the dynamical system, lithium is pumped over in a closed cycle through a converter near the reactor core and further to a remote detector.
      
Inelastic scattering on electrons bound in the germanium (Z=32) and iodine (Z=53) atoms is studied for antineutrinos generated in a nuclear reactor core and in 90Sr-90Y and 147Pm artificial sources.
      
In the case of reactivity emergency, an absorbent is introduced into the reactor core automatically without human intervention and any external control.
      
In a typical liquid metal cooled fast breeder reactor (LMFBR), a cylindrical sodium filled main vessel, which carries the internals such as reactor core, pumps, intermediate heat exchangers etc.
      
The measurement of the activity concentration of the primary coolant was able to detect fuel failures in the reactor core.
      
The highly enriched targets (150 - 800 γg/cm2) were placed in a fission chamber at a distance of approximately 110 m from the reactor core.
      
In this paper we apply the homogenization method to the optimization of the position of fuel assemblies in a nuclear reactor core.
      
The aim of this paper is to propose a new approach for optimizing the position of fuel assemblies in a nuclear reactor core.
      
This procedure differs from gas injection since the gas is produced at the reactor core as it happens in the actual situation, thus the simulation is more realistic.
      
A search of neutrino magnetic moment was carried out at the Kuo-Sheng Nuclear Power Station at a distance of 28?m from the 2.9?GW reactor core.
      
Long time irradiation periods (about 48 hours) for specimens of the monazite ore sample were carried out at the (ET-RR-1) reactor core periphery.
      
 

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