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理想体系巨正则系综中粒子数密度的热力学涨落 被引量:1

Thermodynamical Fluctuation of Number Density of Particles in Grand Canonical Ensemble of Perfect Systems
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摘要 巨正则系综与大粒子源相接触,它的化学势是一个常数,而系统的粒子数可以涨落.对体积 一定的系统,密度与粒子数成正比,用巨正则系综求解热力学系统的粒子数和密度的涨落是可行 的.由巨正则系综的配分函数,结合热力学关系,首先将粒子数密度的涨落用易观测的量表示出 来,然后由低温和高温体系的状态方程,通过严格的理论推导,给出理想体系在低温和高温情况下 的粒子数密度的热力学涨落规律,并对其进行物理分析. The chemistry potential of grand canonical ensemble contacting big particle fountain is a con- stant. The particle numbers of system may fluctuate. For the system of definite volume, density be- ing directly proportional to particle number, solving the fluctuation of particle numbers and density of thermodynamical system is viable by using grand canonica1 ensemble. At first the fluctuation of num- ber density of particles is expressed into easy observation quantum by partition function of grand canonical ensemble and linking thermodynamical relation. Then through state equation of system un- der low temperature conditions,thermodynamical low for fluctuation in number density of particles of perfect system is given under low and high temperature conditions. lt is physically analyzed.
作者 门福殿
出处 《武汉理工大学学报(交通科学与工程版)》 北大核心 2001年第4期426-428,共3页 Journal of Wuhan University of Technology(Transportation Science & Engineering)
关键词 理想体系 巨正则系综 状态方程 能量密度 涨落 热力学 粒子数 perfect system grand canonical ensemble equation of state energy density fluctuation
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  • 1北京大学物理系编写组.量子统计物理学[M].北京:北京大学出版社,1987.350.
  • 2Moling F. Statistical mechanics: methods and applications. Creative Services Inc,1982. 186-188.
  • 3Isihara A. Statistical physics. Academic Press, NewYork, London, 1971.94- 96.
  • 4Zubarev D N. No equilibrium statistical thermodynamics. Consultants Bureau, New York, London,1974. 323-324.
  • 5Reif F. Fundamentals of statistical and thermal physics. MeGrawHill Book Co. , 1965. 285.
  • 6门福殿.正则系综高温条件下相对论量子理想气体的能量和压强的涨落[J].武汉水利电力大学学报,2000,33(4):107-109. 被引量:1

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