Titlebook: Gaseous Dielectrics VI; Loucas G. Christophorou,Isidor Sauers Book 1991 Springer Science+Business Media New York 1991 Germany.Potential.de

CHIDE

Reaktionen auf die Ausgrenzung,u et al., 1989). Our recent work(Qiu et al., 1990) has also indicated that in contrast to the SF.-N. mixture, the dielectric strength of the CF.Cl.-N. mixture as a function of CF.Cl. concentration is quite close to a straight line similar to that of CF.Cl.-CO.

collateral

不適當(dāng)

offense

Verallgemeinerte arithmetische Funktionen,. calculated by exploiting an iterated Wigner-Seitz model, approaches for low densities the Fermi shift . €. = (2π../.)., where . is the gas number density, . is the electron mass, . is the Planck constant and . is the scattering length of the Ne atom.

繁重

培養(yǎng)

rheumatology

Collisional Electron Detachment in Dielectric Gasesgies for sulphur hexafluoride anions is observed to be dissociation into, e.g., SF. + F.. Measurements of this type can be used to provide insight into macroscopic phenomena such as discharge inception; it is clear however, that our current data base is inadequate to be used to make definitive predictions for such macroscopic phenomena.

anesthesia

Electron Localization Effects and Resonant Attachment to O2 Impurities in Highly Compressed Neon Gas. calculated by exploiting an iterated Wigner-Seitz model, approaches for low densities the Fermi shift . €. = (2π../.)., where . is the gas number density, . is the electron mass, . is the Planck constant and . is the scattering length of the Ne atom.

Ballad

Non-Equilibrium Effects in the Initiation of Pseudospark Dischargesare functions of the local reduced field, E(.,t)/N, E(.,t) being the electric field strength at a position . and a time t and N being the neutral density. The purpose of this article is to describe more fully the nonequilibrium effects in pseudospark discharges.

爆米花

Similarities between High Electric Field Electron Emission and Consequent Breakdown Processes in Com 20 MV/m since the average field is increased by localised projections and since the surface is necessarily contaminated by relatively low work function material.’ Previously in 1928-29, Fowler-Nordheim had established that for electron field emission to occur, a value of 1000 MV/m was required; so a field enhancement factor of 50 × was accepted.