The method for determining the charge collection time and the mean charge in the pulse of the ionization fission chamber

2019 ◽  
pp. 60-64
Author(s):  
V. A. Vorobev ◽  
◽  
S. Yu. Obudovskii ◽  
Yu. A. Kashchuk ◽  
◽  
...  
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.


1984 ◽  
Vol 31 (1) ◽  
pp. 900-906
Author(s):  
Alessandro Alberigi Quaranta ◽  
Alessandra Catellani ◽  
Giorgio Pizziolo ◽  
Gianni Zanarini

1983 ◽  
Vol 49 (3) ◽  
pp. 287-294 ◽  
Author(s):  
Gabor Huszar ◽  
George Golenwsky ◽  
John Maiocco ◽  
Edward Davis

1. The influence of dietary meat and meat stock intake on urinary excretion of 3-methylhistidine (3MH) was examined in human adults.2. In the absence of 3MH ingestion for 48 h, the study subjects adjusted to an intrinsic urinary 3MH: creatinine value. If the meat and meat stock-free diet was maintained on subsequent days, only minute diurnal variations occurred, and the values of random urine samples during the day were representative of the 24 h 3MH: creatinine value.3. The mean 3MH: creatinine value (SD) for a group of adults (n 7) was 0·105 ± 0·023 (μmol of 3MH/mg creatinine), which is approximately 35% lower than the corresponding value in healthy growing infants (0·148 ± 0·039) (Seashore et al. 1981).4. Ingestion of meat soup and meat causes different patterns of urinary excretion of 3MH which are consistent with the finding that meat extracts, such as soup and stock, contain considerable amounts of 3MH. The 3MH contents of beef, chicken and turkey were 3·8 ± 0·15, 3·0 ± 0·09 and 2·3 ± 0·29 μmol/g dry wt meat respectively. All three meats contained a water-soluble 3MH-fraction (% total 3MH: beef 8, chicken 21, turkey 23). Amino acid analysis of the soluble fraction with or without hydrochloric acid hydrolysis demonstrated free 3MH in chicken and turkey (5·2 and 2·8% of the total respectively) but not in beef.5. Patients undergoing urinary 3MH measurements should maintain a diet that is free not only of solid meats, but also of meat stock. The ingestion of commercial food products (e.g. frozen or canned meals, sauces, pizza, etc.) may impair the validity of such measurements because of their meat-stock content.6. A dietary regimen is presented which is based on a shorter 12 h urine collection. The shorter collection time is satisfactory in the light of the steady rate of 3MH-excretion after 2 d of a diet free of meat and meat stock.


1990 ◽  
Vol 192 ◽  
Author(s):  
Homer Antoniadis ◽  
E.A. Schiff

ABSTRACTThe drift of electrons generated by a 3 ns illumination impulse was studied in several undoped a-Si:H specimens by using transient photocharge measurements from 10 ns to 50 sec. The transients show four stages of evolution: band transport, deep-trapping and subsequent re-emission, and recombination. From the temperature dependence of the emission time we estimated the mean energy of the trap distribution and the attempt-to-escape frequency associated with this trap to be 0.6 eV below the conduction band and 5×1012 sec−1 respectively; this trap has been identified in previous work with the D-center found in electron spin resonance. In addition the data resolve the two orders of magnitute discrepancy between mobility-lifetime estimates from earlier charge-collection experiments and from steady-state photoconductivity.


Sign in / Sign up

Export Citation Format

Share Document