scholarly journals Neutron Intensity Measurements of BWR Spent Fuels

2000 ◽  
Vol 37 (sup1) ◽  
pp. 594-597
Author(s):  
Ryuichi Tayama ◽  
Ryo Iwasaki ◽  
Hiroshi Sakurai ◽  
Katsumi Hayashi ◽  
Masana Sasaki
2013 ◽  
Vol 17 (2) ◽  
pp. 453-460 ◽  
Author(s):  
T. E. Franz ◽  
M. Zreda ◽  
R. Rosolem ◽  
T. P. A. Ferre

Abstract. A cosmic-ray soil moisture probe is usually calibrated locally using soil samples collected within its support volume. But such calibration may be difficult or impractical, for example when soil contains stones, in presence of bedrock outcrops, in urban environments, or when the probe is used as a rover. Here we use the neutron transport code MCNPx with observed soil chemistries and pore water distribution to derive a universal calibration function that can be used in such environments. Reasonable estimates of pore water content can be made from neutron intensity measurements and by using measurements of the other hydrogen pools (water vapor, soil lattice water, soil organic carbon, and biomass). Comparisons with independent soil moisture measurements at one cosmic-ray probe site and, separately, at 35 sites, show that the universal calibration function explains more than 79% of the total variability within each dataset, permitting accurate isolation of the soil moisture signal from the measured neutron intensity signal. In addition the framework allows for any of the other hydrogen pools to be separated from the neutron intensity measurements, which may be useful for estimating changes in biomass, biomass water, or exchangeable water in complex environments.


2014 ◽  
Author(s):  
Mie Andreasen ◽  
Majken Caroline Looms* ◽  
Karsten Høgh Jensen ◽  
Torben O. Sonnenborg ◽  
Heye Bogena ◽  
...  

Author(s):  
M.D. Ball ◽  
H. Lagace ◽  
M.C. Thornton

The backscattered electron coefficient η for transmission electron microscope specimens depends on both the atomic number Z and the thickness t. Hence for specimens of known atomic number, the thickness can be determined from backscattered electron coefficient measurements. This work describes a simple and convenient method of estimating the thickness and the corrected composition of areas of uncertain atomic number by combining x-ray microanalysis and backscattered electron intensity measurements.The method is best described in terms of the flow chart shown In Figure 1. Having selected a feature of interest, x-ray microanalysis data is recorded and used to estimate the composition. At this stage thickness corrections for absorption and fluorescence are not performed.


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