Simulation and optimization of the deprotiation cascade of a heavy-water moderator

2017 ◽  
Vol 51 (2) ◽  
pp. 133-141 ◽  
Author(s):  
E. P. Magomedbekov ◽  
D. Yu. Belkin ◽  
I. L. Rastunova ◽  
A. B. Sazonov ◽  
I. L. Selivanenko ◽  
...  
Radiocarbon ◽  
1995 ◽  
Vol 37 (2) ◽  
pp. 485-496 ◽  
Author(s):  
G. M. Milton ◽  
S. J. Kramer ◽  
R. M. Brown ◽  
C. J. W. Repta ◽  
K. J. King ◽  
...  

Canadian deuterium uranium (CANDU) pressurized heavy-water reactors produce 14C by neutron activation of trace quantities of nitrogen in annular gas and reactor components (14N(n,p)14C), and from 17O in the heavy water moderator by (17O(n,α)14C). The radiocarbon produced in the moderator is removed on ion exchange resins incorporated in the water purification systems; however, a much smaller gaseous portion is vented from reactor stacks at activity levels considerably below 1% of permissible derived emission limits. Early measurements of the carbon speciation indicated that >90% of the 14C emitted was in the form of CO2. We conducted surveys of the atmospheric dispersion of 14CO2 at the Chalk River Laboratories and at the Pickering Nuclear Generating Station. We analyzed air, vegetation, soils and tree rings to add to the historical record of 14C emissions at these sites, and to gain an understanding of the relative importance of the various carbon pools that act as sources/sinks within the total 14C budget. Better model parameters than those currently available for calculating the dose to the critical group can be obtained in this manner. Global dose estimates may require the development of techniques for estimating emissions occurring outside the growing season.


1984 ◽  
Vol 62 (8) ◽  
pp. 1452-1454
Author(s):  
L. W. Green ◽  
E. C. Davey ◽  
J. Gulens ◽  
T. H. Longhurst ◽  
J. P. Mislan

Five analysis methods were compared for the determination of boron in heavy water moderator: isotope dilution mass spectrometry, spectrophotometry, neutron activation, inductively coupled plasma – atomic emission spectrometry, and ion selective electrode potentiometry. Ten samples were analysed by each method; the results showed close agreement between all of the methods. Only mass spectrometry achieved the required precision (<1% rsd) for samples taken during initial reactor operation, but all of the methods achieved sufficient precision (<10% rsd) for samples taken during normal operation. For samples for which the 10B concentration must be determined, only mass spectrometry and neutron activation are applicable.


2017 ◽  
Vol 51 (4) ◽  
pp. 384-391 ◽  
Author(s):  
E. P. Magomedbekov ◽  
D. Yu. Belkin ◽  
I. L. Rastunova ◽  
A. B. Sazonov ◽  
I. L. Selivanenko ◽  
...  

Author(s):  
B. Lekakh ◽  
K. Hau ◽  
S. Ford

The Advanced CANDU Reactor™ (ACR™) is a Generation III+ pressure tube type reactor using light water coolant and heavy water moderator. The ACR-1000 reactor design is an evolutionary extension of the proven CANDU reactor design. The ACR-1000 incorporates multiple and diverse passive systems for accident mitigation. Where necessary, one or more features that are passive in nature have been included for mitigation of any postulated accident event. This paper describes how the use of passive design elements complements active features enhances reliability and improves safety margins.


2005 ◽  
Vol 277-279 ◽  
pp. 747-752
Author(s):  
B.J. Min ◽  
W.Y. Kim

An investigation on the effect of the neutronic behavior on the lattice for a Deuterium Critical Assembly (DCA) in JNC (Japan Nuclear Cycle Development Institute) has been performed. The DCA, the heavy water moderated and light water cooled pressure-tube type research facility, was designed not only for the core physics research, but also for the development of the core-related technology for the Advanced Thermal Reactor (ATR). The core structure of the ATR is highly heterogeneous and it is separated from the heavy water moderator by a calandria tube. Therefore, the neutron behavior is quite complicated and sensitive to a change of the core structure. In this study, the assessment of the core physics characteristics such as the multiplication factor and the void coefficient for the DCA was conducted using the WIMS-D5 code and the results were compared with those of both the experimental data and WIMS-AECL.


Author(s):  
J. J. Baschuk ◽  
Alan West ◽  
B. W. Leitch

The Pressurized Heavy Water Reactor (PHWR) is based on natural uranium fuel and heavy water moderator. A unique feature of the PHWR is the horizontal fuel channel that allows for on-line re-fuelling and fuel management. A fuel channel consists of two concentric tubes, each approximately 6 meters long. The inner tube, known as the pressure tube, contains the uranium fuel bundles and the pressurized (∼10 MPa) primary coolant. The outer tube, known as the calandria tube, separates the heavy water moderator (∼70°C) from the pressure tube (∼300°C). A potential accident scenario is the bursting of a fuel channel. The escaping hot fluid generates a pressure wave in the moderator, which would interact with the adjacent pressure/calandria tube assemblies and the outer containment calandria vessel, potentially damaging components within the reactor core. To improve the understanding of channel bursts and associated fluid structure interaction, a 1:6 scale reactor vessel test facility (Small Scale Burst Facility) was constructed at the Atomic Energy of Canada Ltd, Chalk River Laboratories. The test facility allows for the measurement of transient pressures, the development and collapse of the steam bubble created by the burst tube, and resultant response of the neighboring tubes and scaled calandria vessel. A single bursting tube, or a single tube bursting within an array of neighboring tubes, can be tested. The results from recent tests are presented, which include a three-dimensional map of the pressure pulse from a single, bursting tube. Future work will include 3-D mapping of near wall bursts and modeling the experiments using Arbitary Lagrangian Eulerian methods in the finite element program, LS-DYNA. This work is part of the development of a next generation modeling tool for fuel channel phenomena.


1993 ◽  
Vol 144 (2) ◽  
pp. 293-303 ◽  
Author(s):  
Hiroyasu Mochizuki ◽  
Mitsutaka H. Koike ◽  
Takaaki Sakai

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