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Thermodynamic Properties of $^{4}$ He Gas in the Temperature Range 4.2-0?K
- 作者:S. M. Mosameh (1)
A. S. Sandouqa (2) H. B. Ghassib (3) B. R. Joudeh (4) (5)
- 关键词:Second virial coefficient ; Galitskii–Migdal–Feynman formalism ; $$^{4}$$ 4 He gas ; Phase ; transition point ; Equation of state
- 刊名:Journal of Low Temperature Physics
- 出版年:2014
- 出版时间:May 2014
- 年:2014
- 卷:175
- 期:3-4
- 页码:523-542
- 全文大小:1,743 KB
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- 作者单位:S. M. Mosameh (1)
A. S. Sandouqa (2) H. B. Ghassib (3) B. R. Joudeh (4) (5)
1. Department of Applied Sciences, Irbid University College, Al-Balqa-Applied University, Irbid, Jordan 2. Department of Applied Sciences, Faculty of Engineering Technology, Al-Balqa-Applied University, Amman, Jordan 3. Department of Physics, The University of Jordan, Amman, Jordan 4. Applied Physics Department, Tafila Technical University, Tafila, Jordan 5. Department of Computer Science, College of Shari’a and Islamic Studies in Al Ahsaa, Al Imam Muhammad Ibn Saud Islamic University (IMSIU), Riyadh, Saudi Arabia
- ISSN:1573-7357
文摘
The thermodynamic properties of $^{4}$ He gas are investigated in the temperature-range 4.2-0?K, with special emphasis on the second virial coefficient in both the classical and quantum regimes. The main input in computing the quantum coefficient is the ‘effective-phase shifts. These are calculated within the framework of the Galitskii–Migdal–Feynman (GMF) formalism, using the HFDHE2 and Sposito potentials. The virial equation of state is constructed. Extensive calculations are carried out for the pressure–volume–temperature (P–V–T) behavior, as well as chemical potential, and nonideality of the system. The following results are obtained. First, the validity of the GMF formalism for the present system is demonstrated beyond any doubt. Second, the boiling point (phase-transition point) of $^{4}$ He gas is determined from the P–V behavior using the virial equation of state, its value being closest than all previous results to the experimental value. Third, the chemical potential $\upmu $ is evaluated from the quantum second virial coefficient. It is found that $\upmu $ increases (becomes less negative) as the temperature decreases or the number density n increases. Further, $\upmu $ shows no sensitivity to the differences between the potentials used up to n = 10 $^{27}$ m $^{-3}$ . Finally, the compressibility Z is computed and discussed as a measure of the nonideality of the system.
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