A method of measuring the mean charge in a pulse and an estimate of the limit pulse sensitivity of a fission chamber

Atomic Energy ◽  
1999 ◽  
Vol 86 (6) ◽  
pp. 427-431
Author(s):  
E. K. Malyshev ◽  
A. I. Filatov ◽  
M. E. Malyshev ◽  
V. S. Shepel'
Keyword(s):  
The Mean ◽  
2016 ◽  
Vol 187 (1) ◽  
pp. 497-510 ◽  
Author(s):  
C. G. Beneventano ◽  
I. V. Fialkovsky ◽  
E. M. Santangelo

2019 ◽  
Vol 73 (10) ◽  
Author(s):  
Jennifer Schofield ◽  
Jay A. LaVerne ◽  
Daniel Robertson ◽  
Philippe Collon ◽  
Simon M. Pimblott

1990 ◽  
Vol 68 (4) ◽  
pp. 768-772 ◽  
Author(s):  
Conrad Richter ◽  
Jack Dainty

According to the Manning condensation theory, the structure of cation-binding uronates in the cell wall can influence ionic behaviour. Assuming the theory is valid, we measured, in cation-binding experiments, the dimensionless linear charge density parameter and the mean charge separation distance in the fully ionized delignified Sphagnum russowii cell wall. Our charge separation estimate, 1.00 ± 0.02 nm, indicates that approximately 1.3 neutral sugars are interpolated between the uronic acids in the polyuronate chains of the cation exchanger. This compares well with chemical data of isolated wall fractions from another Sphagnum species reported by other workers. The charge density parameter estimate, 0.71 ± 0.02, implies that univalent cations never condense, whereas cations with two or more positive charges condense when the degree of ionization of the fixed (wall) charges is high enough. Key words: ion exchange, cell wall, charge density.


2000 ◽  
Vol 18 (4) ◽  
pp. 647-653 ◽  
Author(s):  
M. OGAWA ◽  
U. NEUNER ◽  
H. KOBAYASHI ◽  
Y. NAKAJIMA ◽  
K. NISHIGORI ◽  
...  

An energy loss of 240 MeV argon ions in a Z-pinch helium plasma has been for the first time observed throughout the entire pinching process. Standard Stark broadening analysis gives an electron density ranging from 4 to 6 × 1017 cm−3 during the pinch. To deduce stopping power from the energy loss, the target thickness of the helium plasma has been evaluated assuming the mean charge of helium based on thermal equilibrium. The observed electron density and the mean charge of helium give a target thickness of 30 ± 3 μg cm−2 from 1 μs to 1.8 μs after the discharge ignition. The measured stopping power exceeds a tabulated value for cold helium gas by a factor of 2 to 3 around the time of the first pinch. The experimental stopping power is compared with theoretical values calculated using an equation of stopping power for a partially ionized plasma.


1983 ◽  
Vol 38 (6) ◽  
pp. 189-200
Author(s):  
Chien-er Lee ◽  
Yeou Wei Yang ◽  
Lai Kin Hung

2004 ◽  
Vol 231 (2-3) ◽  
pp. 131-137 ◽  
Author(s):  
Mélanie Hautreux ◽  
Nathalie Hue ◽  
Alexis Du Fou de Kerdaniel ◽  
Abdelattif Zahir ◽  
Valérie Malec ◽  
...  

Clay Minerals ◽  
1982 ◽  
Vol 17 (2) ◽  
pp. 209-216 ◽  
Author(s):  
M. S. Stul ◽  
L. Van Leemput

AbstractDifferent montmorillonites (Otay, Chambers, Marnia, Camp Berteau, Moosburg, Greek White, Wyoming bentonite were deferrated with a dithionite/citrate solution; iron sulphide by-products were eliminated with an HCl washing and citrates with an H2O2 oxidation. The smaller CEC after deferration could not be assigned to either (i) the occurrence of a positive correlation between CEC and particle sizes smaller than 0.2 µm or (ii) to the mean charge density of these sub-fractions. All sub-fractions had a heterogeneous interlayer cation density distribution.


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