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1)  microcanonical ensemble
微正则系综
1.
Thermodynamical funcions of the few-body hard-sphere system when it reaches ergodicity are discussed in detail by using microcanonical ensemble method.
利用微正则系综详细地讨论了少体硬球系统达到各态历经时的热力学函数。
2)  microcanomical ensemble
微正则系综(合)
3)  Canonical ensemble
正则系综
1.
Rigid multibody molecular dynamics algorithm in canonical ensemble;
刚性多原子分子的正则系综分子动力学算法
2.
Canonical ensemble(NVT) Monte Carlo simulations have been carried out to get the chemical potentials of the mixture of nitrogen and benzene by the Widom test particle method.
用正则系综测试粒子MonteCarlo(GCMC)方法模拟常温下空气(以氮气为代表)及其污染物微量有机物(以苯为例)的混合物中各组分的化学势。
3.
The compound adsorption process on the solid surface of two gases was analysed on the basis of principle of canonical ensemble.
应用正则系综原理,推导两种气体在固体表面复合吸附过程,进而推广到多元吸附系统。
4)  grand canonical ensemble
巨正则系综
1.
Adsorption behavior of monochlorodifluoromethane (R22) , represented by the Stockmayer (SM) fluid, in activated carbon pores with defectives has been simulated by the grand canonical ensemble Monte Carlo(GCMC)method.
应用巨正则系综Monte Carlo方法模拟Stockmayer流体[以一氯二氟甲烷(R22)为代表]在活性炭孔中的吸附。
2.
This paper models the carrier number in silicon semiconductor using the method of grand canonical ensemble and Fermi-Dirac statistical distributions.
将巨正则系综的Fermi-Dirac(F-D)统计法与计算机模拟相结合,从本征半导体硅出发,探讨温度和光照能量对载流子数的影响,试图从理论上定量分析太阳能电池工作状况,对本征硅半导体中载流子数进行计算机模拟,模拟结果与理论规律基本吻合,此方法可为进一步研究掺杂半导体及氧化物半导体空间电荷层载流子数提供参考。
3.
The effects due to the interaction and finite size are given simultaneously by using the sum method for the grand canonical ensemble and mean field theory.
利用巨正则系综的求和方法与平均场理论 ,给出了有限粒子数与原子间相互作用对系统热力学性质的共同修正 ;并将所得结果与三维时的情况进行了比较 。
5)  NVT canonical ensemble
NVT正则系综
1.
The phase equilibrium of linear molecule,ethane,has been simulated by using the NVT canonical ensemble Monte Carlo method,and the thermodynamic properties of the system including chemical potentials?temperature?density?pressure,etc.
用恒NVT正则系综MonteCarlo方法模拟线形分子—乙烷的相平衡 ,得出化学势、温度、密度、压力等热力学数据。
6)  microcanonical ensemble
微正则系统
1.
Starting from Gibbs microcanonical ensemble theory,the distribution function of the nearly independent particle system that consists of any number of particles is derived.
从微正则系统理论出发,导出了任意数目粒子构成的近独立子系系统的分布函数,在粒子数N趋于无限大的极限情况下,得到了麦克斯韦分布律。
补充资料:微正则系综
      见统计物理学。
  

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