Under non-denaturing solvent conditions, the mean charge state of a multiply charged protein ion formed by electrospray is linearly correlated with the macromolecular surface

2004 ◽  
Vol 231 (2-3) ◽  
pp. 131-137 ◽  
Author(s):  
Mélanie Hautreux ◽  
Nathalie Hue ◽  
Alexis Du Fou de Kerdaniel ◽  
Abdelattif Zahir ◽  
Valérie Malec ◽  
...  
2019 ◽  
Vol 73 (10) ◽  
Author(s):  
Jennifer Schofield ◽  
Jay A. LaVerne ◽  
Daniel Robertson ◽  
Philippe Collon ◽  
Simon M. Pimblott

2002 ◽  
Vol 20 (3) ◽  
pp. 475-478 ◽  
Author(s):  
M. KOJIMA ◽  
M. MITOMO ◽  
T. SASAKI ◽  
J. HASEGAWA ◽  
M. OGAWA

The charge-state distribution and the energy loss of oxygen ions in a laser-produced hydrogen plasma have been investigated experimentally. The plasma target had a maximum electron density of 5 × 1018 cm−3 and a maximum electron temperature of 13 eV. The mean charge state of the oxygen ions in the hydrogen plasma was measured to be 5.1, which was considerably higher than that in hydrogen gas. The energy loss of oxygen ions in the plasma of a density less than 1 × 1018 cm−3 in the plasma showed a large enhancement compared with that in hydrogen gas. However, the energy loss in the plasma of a density above 1 × 1018 cm−3 showed no enhancement.


2016 ◽  
Vol 187 (1) ◽  
pp. 497-510 ◽  
Author(s):  
C. G. Beneventano ◽  
I. V. Fialkovsky ◽  
E. M. Santangelo

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 28 (6) ◽  
pp. 2194-2201 ◽  
Author(s):  
D.T.-K. Kwok ◽  
P.K. Chu ◽  
M.M.M. Bilek ◽  
I.G. Brown ◽  
A. Vizir

1973 ◽  
Vol 28 (10) ◽  
pp. 1687-1696 ◽  
Author(s):  
G. Hertenberger ◽  
K. Roch ◽  
H. Winter

Regarding both step by step and direct ionization by electron impact, and including losses from radiative recombination and charge exchange, a simple model for calculation of charge state densities in electron beam multiply charged ion sources has been developed. The diffusion of the created charged particles out of the ionization volume is included in the model. A monoenergetic electron beam of high current density interacts with a gas at a pressure range from 10-6 to 10-4 Torr. The calculations were performed for Argon, Krypton and Xenon with an impact energy from 2 keV to 10 keV. Influences of several elementary processes were discussed in regard to developments of new types of multiply charged ion sources.


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

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