Spatial Distribution and Kinetics of Negative Ions in Glow DC Discharge in Pure O2 and H2

1999 ◽  
pp. 495-496
Author(s):  
V. V. Ivanov ◽  
K. S. Klopovskiy ◽  
D. V. Lopaev ◽  
A. T. Rakhimov ◽  
T. V. Rakhimova
Keyword(s):  
Spatial Distribution ◽  
Negative Ions ◽  
Dc Discharge ◽  
Kinetics Of

The structure of the impulse corona in a rod/plane gap I. The positive corona

1970 ◽  
Vol 315 (1520) ◽  
pp. 1-25 ◽  
Keyword(s):  
Spatial Distribution ◽  
Electric Field ◽  
Space Charge ◽  
Negative Ions ◽  
Corona Discharges ◽  
Theoretical Derivation ◽  
Plane Electrode ◽  
Positive Space Charge ◽  
Positive Ion ◽  
Positive Space

The dissipation of space charge following the growth of impulse corona discharges in positive rod/earthed plane gaps has been measured with an electrostatic fluxmeter. A method is described to determine the spatial distribution and magnitude of the space charge together with the associated electric field. Initial positive ion densities of up to 100 μC m -3 have been found. The total positive space charge deposited in a 40 cm gap at 160 kV is 500 nC. Electrons emitted from the plane electrode as a result of corona channels crossing the gap are shown to be trapped in the discharge space as negative ions. The recovery of the gap over several seconds is largely due to ionic drift to the electrodes. A theoretical derivation of the rate of deionization agrees with observed values.

Kinetics of DC discharge-induced degradation of phenol in aqueous solutions

2014 ◽  
Vol 48 (5) ◽  
pp. 346-349 ◽  
Author(s):  
E. S. Bobkova ◽  
E. S. Ivanova ◽  
R. A. Nevedomyi ◽  
A. V. Sungurova
Keyword(s):  
Aqueous Solutions ◽  
Dc Discharge ◽  
Kinetics Of

scholarly journals Influence of Grain Refinement on Oxidation Behavior of Two-Phase Cu–Cr Alloys at 973–1,073 K in Air

2016 ◽  
Vol 35 (10) ◽  
pp. 1005-1011
Author(s):  
T. J. Pan ◽  
J. Chen ◽  
Y. X. He ◽  
W. Wei ◽  
J. Hu
Keyword(s):  
Grain Size ◽  
Spatial Distribution ◽  
Oxidation Behavior ◽  
Second Phase ◽  
Two Phase ◽  
Reactive Component ◽  
Parabolic Law ◽  
Second Phase Particles ◽  
Kinetics Of ◽  
Lower Oxidation

AbstractThe oxidation behavior of grain-refined Cu–7.0 Cr alloy (GR Cu–7.0 Cr) in air at 973–1,073 K was investigated in comparison with normal casting Cu–7.0 Cr alloy (CA Cu–7.0 Cr). The oxidation of CA Cu–7.0 Cr alloy nearly followed parabolic law, while the oxidation kinetics of GR Cu–7.0 Cr slightly deviated from parabolic law. Both alloys almost produced multi-layered scales consisting of the outer layer of CuO and the inner layer of mixed Cr2O3 and Cu2O oxides plus internal oxidation zones of chromium. The grain-refined Cu–7.0 Cr alloy produced a more amount of Cr2O3 in the inner layer of the scale, and thus was oxidized at much lower oxidation rate than that of CA Cu–7.0 Cr with normal grain size. The experimental results indicated that the differences in oxidation behavior between two alloys may be ascribed to the different size and spatial distribution of the second-phase particles and the reactive component contents in localized zone.

Electron kinetics of molecular nitrogen dc discharge

1989 ◽  
Vol 39 (4) ◽  
pp. 415-426 ◽  
Author(s):  
K. Rohlena ◽  
K. Mašek
Keyword(s):  
Molecular Nitrogen ◽  
Electron Kinetics ◽  
Dc Discharge ◽  
Kinetics Of

Spatial Distribution and Cell Kinetics of the Glands in the Human Esophageal Mucosa

2001 ◽  
Vol 39 (3) ◽  
pp. 163-168 ◽  
Author(s):  
G. Willems ◽  
H. Destordeur ◽  
Y. van Nieuwenhove
Keyword(s):  
Spatial Distribution ◽  
Cell Kinetics ◽  
Esophageal Mucosa ◽  
Kinetics Of

Kinetics of nonhomogeneous chemical processes in tracks of high-energy charged particles

1990 ◽  
Vol 68 (9) ◽  
pp. 858-871 ◽  
Author(s):  
A. Hummel
Keyword(s):  
Spatial Distribution ◽  
Large Fraction ◽  
Charged Particles ◽  
Coulomb Field ◽  
High Energy ◽  
Transient Species ◽  
Charged Species ◽  
Solvent Molecules ◽  
Kinetics Of ◽  
Initial Spatial Distribution

High-energy charged particles, when slowing down in a molecular medium, lose their energy by electronic excitations and ionizations of molecules along their paths. If the secondary electrons that are formed as a result of the ionizations have sufficient energy, they give rise to further excitations and ionizations. In this way tracks of excited states, positive ions, and electrons are formed. The spatial distribution of the species initially formed in the track will change in time owing to diffusion; the charged species will also drift in each other's Coulomb field. In nonpolar systems the range of the Coulomb forces is very large (30 nm) and neutralization of the oppositely charged species in the track is a dominant process, which in turn leads to formation of excited molecules that generally decompose into reactive fragments. In polar liquids, like water, neutralization is less prevalent and a relatively large fraction of the charged species escapes from the Coulombic attraction. The transient species formed may react with one another and with molecules of the medium, either solvent molecules or solute molecules. The probability of the occurrence of these reactions depends on the initial spatial distribution of the reactive species in the track. The present state of the theory of the kinetics of the nonhomogeneous processes in tracks of high-energy charged particles, which relates the initial spatial distribution of the transient species in the track to the various experimental observables, will be discussed.

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