CHIDE
发表于 2025-3-25 06:43:01
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
发表于 2025-3-25 08:06:17
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不适当
发表于 2025-3-25 15:22:08
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offense
发表于 2025-3-25 19:09:26
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
发表于 2025-3-25 21:21:06
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培养
发表于 2025-3-26 03:58:02
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rheumatology
发表于 2025-3-26 08:13:07
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
发表于 2025-3-26 12:28:04
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
发表于 2025-3-26 14:43:06
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
发表于 2025-3-26 19:37:21
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.