THE MATHEMATICAL THEORY OF ELECTRICAL DISCHARGES IN GASES B-VELOCITY-DISTRIBUTION OF POSITIVE IONS IN A STATIC FIELD
THE MATHEMATICAL THEORY OF ELECTRICAL DISCHARGES IN GASES B-VELOCITY-DISTRIBUTION OF POSITIVE IONS IN A STATIC FIELD
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DOI：
10.1103/revmodphys.25.844
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发表时间：
1953-01-01
影响因子：
44.1
通讯作者：
KIHARA, T
中科院分区：
文献类型：
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作者：
KIHARA, T
这里c（N，e，w）和f（c）是速度，当s轴沿离子的电速度分布函数的方向取时，c，（ui，oi，wi）场E。这里e和m表示电荷和质量，f（c）是气体分子的电荷和质量。的离子，分别; f ′ fi ′ ffi是f（c ′）fi（ci ′）-f（c）fi（ci）的缩写，c ′和ci ′是离子和气体分子遇到初始速度c和c ′时的最终速度，相对运动轨道的夹角为8; I（g，ti）sintidede表示相对速度g= I c-cnci 'I时散射到立体角sin 8dede中的微分截面（见图1）。
Here c (N, e, w) and f (c) are the velocity and the when the s axis is taken in the direction of the electric velocity-distribution function of the ions; c,(ui, oi, wi) field E. Here e and m denote the charge and the mass and f,(c,) are those of the gas molecules. of the ion, respectively; f'fi'ffi is the—abbreviation for f (c') fi (ci')—f (c) fi (ci), c'and ci'are the final velocities of the ion and the gas molecule encountering with initial velocities c and c1with diGraction angle 8 for the orbit of relative motion; I (g, ti) sintidede indi-cates the differential cross section for scattering into the solid angle sin8dede for the relative speed g= I c—cil ci'I (see Fig. 1).