理想玻色和费米气体分子在保守场中按势能的分布

On the Potential Energy Distribution Function of the Ideal B·E's and the F·D's Gases in a Conservative Field

应用量子统计力学方法,推证遵从玻色-爱因斯坦和费米-狄拉克统计法的理想气体分子,处在保守力场中按势能的分布规律。其结论为分子数密度是势能的幂级数函数。尽管玻尔兹曼分布律完全遵从于麦克斯韦-玻尔兹曼统计法,与保守力场中理想气体分子存在的空间维数以及遵从何种能谱无关。但由此可以证明玻尔兹曼分布律只是上述分布规律的零级近似和权重因子。因此,这里讨论的情况才是理想气体处于保守力场中按势能的更为具有一般性的分布律。

This text apply the way of statistical mechanics to the ideal gases, it disscussed the pottential energy distribution funcction of ideal gases in deference to the B·E's statistcal way and the F·D's statistcal way in a conservative field. This have shown the special case of that the Boltzman's distribution law is oney above two kind distribution functions.