Numerical evaluation of second and third virial coefficients of some inert gases via classical cluster expansion
Abstract In this project we evaluate second virial coefficient of some inert gases via classical cluster expansion, assuming each atomic pair interaction is of Lennard-Jones type. We also try to numerically evaluate the third virial coefficient of Argon gas based on bipolar-coordinate integration (M...
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| Autor*in: |
Hutem, Artit [verfasserIn] |
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| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2012 |
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| Schlagwörter: |
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| Anmerkung: |
© Springer Science+Business Media, LLC 2011 |
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| Übergeordnetes Werk: |
Enthalten in: Journal of mathematical chemistry - Springer Netherlands, 1987, 50(2012), 5 vom: 04. Jan., Seite 1262-1276 |
|---|---|
| Übergeordnetes Werk: |
volume:50 ; year:2012 ; number:5 ; day:04 ; month:01 ; pages:1262-1276 |
| Links: |
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| DOI / URN: |
10.1007/s10910-011-9966-5 |
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OLC2060415829 |
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| 520 | |a Abstract In this project we evaluate second virial coefficient of some inert gases via classical cluster expansion, assuming each atomic pair interaction is of Lennard-Jones type. We also try to numerically evaluate the third virial coefficient of Argon gas based on bipolar-coordinate integration (Mas et al. in J Chem Phys 10:6694, 1999), assuming the same Lennard-Jones potential as before. The second virial coefficient (Vega et al. in Phys Chem Chem Phys 4:3000–3007, 2002) calculated from our model are compatible to the experimental data [19] The temperature at which B2(T) → 0 is called the Boyle’s temperature TB (Vega et al. in Phys Chem Chem Phys 4:3000–3007, 2002) for the Lennard-Jines (12-6) potential. For the second virial coefficient of He, we obtain the Boyle’s temperature as follow: TB = 34.9312438964844 (K) B2(T) = 9.82958 × $ 10^{−6} $ ($ cm^{3} $/mol). | ||
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10.1007/s10910-011-9966-5 doi (DE-627)OLC2060415829 (DE-He213)s10910-011-9966-5-p DE-627 ger DE-627 rakwb eng 510 540 VZ Hutem, Artit verfasserin aut Numerical evaluation of second and third virial coefficients of some inert gases via classical cluster expansion 2012 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media, LLC 2011 Abstract In this project we evaluate second virial coefficient of some inert gases via classical cluster expansion, assuming each atomic pair interaction is of Lennard-Jones type. We also try to numerically evaluate the third virial coefficient of Argon gas based on bipolar-coordinate integration (Mas et al. in J Chem Phys 10:6694, 1999), assuming the same Lennard-Jones potential as before. The second virial coefficient (Vega et al. in Phys Chem Chem Phys 4:3000–3007, 2002) calculated from our model are compatible to the experimental data [19] The temperature at which B2(T) → 0 is called the Boyle’s temperature TB (Vega et al. in Phys Chem Chem Phys 4:3000–3007, 2002) for the Lennard-Jines (12-6) potential. For the second virial coefficient of He, we obtain the Boyle’s temperature as follow: TB = 34.9312438964844 (K) B2(T) = 9.82958 × $ 10^{−6} $ ($ cm^{3} $/mol). The second virial coefficient The third virial coefficient Cluster expansion Inert gases Boonchui, Sutee aut Enthalten in Journal of mathematical chemistry Springer Netherlands, 1987 50(2012), 5 vom: 04. Jan., Seite 1262-1276 (DE-627)129246441 (DE-600)59132-4 (DE-576)27906036X 0259-9791 nnns volume:50 year:2012 number:5 day:04 month:01 pages:1262-1276 https://doi.org/10.1007/s10910-011-9966-5 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-CHE SSG-OLC-MAT SSG-OLC-PHA SSG-OLC-DE-84 SSG-OPC-MAT GBV_ILN_70 GBV_ILN_2409 GBV_ILN_4012 AR 50 2012 5 04 01 1262-1276 |
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10.1007/s10910-011-9966-5 doi (DE-627)OLC2060415829 (DE-He213)s10910-011-9966-5-p DE-627 ger DE-627 rakwb eng 510 540 VZ Hutem, Artit verfasserin aut Numerical evaluation of second and third virial coefficients of some inert gases via classical cluster expansion 2012 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media, LLC 2011 Abstract In this project we evaluate second virial coefficient of some inert gases via classical cluster expansion, assuming each atomic pair interaction is of Lennard-Jones type. We also try to numerically evaluate the third virial coefficient of Argon gas based on bipolar-coordinate integration (Mas et al. in J Chem Phys 10:6694, 1999), assuming the same Lennard-Jones potential as before. The second virial coefficient (Vega et al. in Phys Chem Chem Phys 4:3000–3007, 2002) calculated from our model are compatible to the experimental data [19] The temperature at which B2(T) → 0 is called the Boyle’s temperature TB (Vega et al. in Phys Chem Chem Phys 4:3000–3007, 2002) for the Lennard-Jines (12-6) potential. For the second virial coefficient of He, we obtain the Boyle’s temperature as follow: TB = 34.9312438964844 (K) B2(T) = 9.82958 × $ 10^{−6} $ ($ cm^{3} $/mol). The second virial coefficient The third virial coefficient Cluster expansion Inert gases Boonchui, Sutee aut Enthalten in Journal of mathematical chemistry Springer Netherlands, 1987 50(2012), 5 vom: 04. Jan., Seite 1262-1276 (DE-627)129246441 (DE-600)59132-4 (DE-576)27906036X 0259-9791 nnns volume:50 year:2012 number:5 day:04 month:01 pages:1262-1276 https://doi.org/10.1007/s10910-011-9966-5 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-CHE SSG-OLC-MAT SSG-OLC-PHA SSG-OLC-DE-84 SSG-OPC-MAT GBV_ILN_70 GBV_ILN_2409 GBV_ILN_4012 AR 50 2012 5 04 01 1262-1276 |
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10.1007/s10910-011-9966-5 doi (DE-627)OLC2060415829 (DE-He213)s10910-011-9966-5-p DE-627 ger DE-627 rakwb eng 510 540 VZ Hutem, Artit verfasserin aut Numerical evaluation of second and third virial coefficients of some inert gases via classical cluster expansion 2012 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media, LLC 2011 Abstract In this project we evaluate second virial coefficient of some inert gases via classical cluster expansion, assuming each atomic pair interaction is of Lennard-Jones type. We also try to numerically evaluate the third virial coefficient of Argon gas based on bipolar-coordinate integration (Mas et al. in J Chem Phys 10:6694, 1999), assuming the same Lennard-Jones potential as before. The second virial coefficient (Vega et al. in Phys Chem Chem Phys 4:3000–3007, 2002) calculated from our model are compatible to the experimental data [19] The temperature at which B2(T) → 0 is called the Boyle’s temperature TB (Vega et al. in Phys Chem Chem Phys 4:3000–3007, 2002) for the Lennard-Jines (12-6) potential. For the second virial coefficient of He, we obtain the Boyle’s temperature as follow: TB = 34.9312438964844 (K) B2(T) = 9.82958 × $ 10^{−6} $ ($ cm^{3} $/mol). The second virial coefficient The third virial coefficient Cluster expansion Inert gases Boonchui, Sutee aut Enthalten in Journal of mathematical chemistry Springer Netherlands, 1987 50(2012), 5 vom: 04. Jan., Seite 1262-1276 (DE-627)129246441 (DE-600)59132-4 (DE-576)27906036X 0259-9791 nnns volume:50 year:2012 number:5 day:04 month:01 pages:1262-1276 https://doi.org/10.1007/s10910-011-9966-5 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-CHE SSG-OLC-MAT SSG-OLC-PHA SSG-OLC-DE-84 SSG-OPC-MAT GBV_ILN_70 GBV_ILN_2409 GBV_ILN_4012 AR 50 2012 5 04 01 1262-1276 |
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10.1007/s10910-011-9966-5 doi (DE-627)OLC2060415829 (DE-He213)s10910-011-9966-5-p DE-627 ger DE-627 rakwb eng 510 540 VZ Hutem, Artit verfasserin aut Numerical evaluation of second and third virial coefficients of some inert gases via classical cluster expansion 2012 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media, LLC 2011 Abstract In this project we evaluate second virial coefficient of some inert gases via classical cluster expansion, assuming each atomic pair interaction is of Lennard-Jones type. We also try to numerically evaluate the third virial coefficient of Argon gas based on bipolar-coordinate integration (Mas et al. in J Chem Phys 10:6694, 1999), assuming the same Lennard-Jones potential as before. The second virial coefficient (Vega et al. in Phys Chem Chem Phys 4:3000–3007, 2002) calculated from our model are compatible to the experimental data [19] The temperature at which B2(T) → 0 is called the Boyle’s temperature TB (Vega et al. in Phys Chem Chem Phys 4:3000–3007, 2002) for the Lennard-Jines (12-6) potential. For the second virial coefficient of He, we obtain the Boyle’s temperature as follow: TB = 34.9312438964844 (K) B2(T) = 9.82958 × $ 10^{−6} $ ($ cm^{3} $/mol). The second virial coefficient The third virial coefficient Cluster expansion Inert gases Boonchui, Sutee aut Enthalten in Journal of mathematical chemistry Springer Netherlands, 1987 50(2012), 5 vom: 04. Jan., Seite 1262-1276 (DE-627)129246441 (DE-600)59132-4 (DE-576)27906036X 0259-9791 nnns volume:50 year:2012 number:5 day:04 month:01 pages:1262-1276 https://doi.org/10.1007/s10910-011-9966-5 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-CHE SSG-OLC-MAT SSG-OLC-PHA SSG-OLC-DE-84 SSG-OPC-MAT GBV_ILN_70 GBV_ILN_2409 GBV_ILN_4012 AR 50 2012 5 04 01 1262-1276 |
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10.1007/s10910-011-9966-5 doi (DE-627)OLC2060415829 (DE-He213)s10910-011-9966-5-p DE-627 ger DE-627 rakwb eng 510 540 VZ Hutem, Artit verfasserin aut Numerical evaluation of second and third virial coefficients of some inert gases via classical cluster expansion 2012 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media, LLC 2011 Abstract In this project we evaluate second virial coefficient of some inert gases via classical cluster expansion, assuming each atomic pair interaction is of Lennard-Jones type. We also try to numerically evaluate the third virial coefficient of Argon gas based on bipolar-coordinate integration (Mas et al. in J Chem Phys 10:6694, 1999), assuming the same Lennard-Jones potential as before. The second virial coefficient (Vega et al. in Phys Chem Chem Phys 4:3000–3007, 2002) calculated from our model are compatible to the experimental data [19] The temperature at which B2(T) → 0 is called the Boyle’s temperature TB (Vega et al. in Phys Chem Chem Phys 4:3000–3007, 2002) for the Lennard-Jines (12-6) potential. For the second virial coefficient of He, we obtain the Boyle’s temperature as follow: TB = 34.9312438964844 (K) B2(T) = 9.82958 × $ 10^{−6} $ ($ cm^{3} $/mol). The second virial coefficient The third virial coefficient Cluster expansion Inert gases Boonchui, Sutee aut Enthalten in Journal of mathematical chemistry Springer Netherlands, 1987 50(2012), 5 vom: 04. Jan., Seite 1262-1276 (DE-627)129246441 (DE-600)59132-4 (DE-576)27906036X 0259-9791 nnns volume:50 year:2012 number:5 day:04 month:01 pages:1262-1276 https://doi.org/10.1007/s10910-011-9966-5 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-CHE SSG-OLC-MAT SSG-OLC-PHA SSG-OLC-DE-84 SSG-OPC-MAT GBV_ILN_70 GBV_ILN_2409 GBV_ILN_4012 AR 50 2012 5 04 01 1262-1276 |
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Numerical evaluation of second and third virial coefficients of some inert gases via classical cluster expansion |
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Abstract In this project we evaluate second virial coefficient of some inert gases via classical cluster expansion, assuming each atomic pair interaction is of Lennard-Jones type. We also try to numerically evaluate the third virial coefficient of Argon gas based on bipolar-coordinate integration (Mas et al. in J Chem Phys 10:6694, 1999), assuming the same Lennard-Jones potential as before. The second virial coefficient (Vega et al. in Phys Chem Chem Phys 4:3000–3007, 2002) calculated from our model are compatible to the experimental data [19] The temperature at which B2(T) → 0 is called the Boyle’s temperature TB (Vega et al. in Phys Chem Chem Phys 4:3000–3007, 2002) for the Lennard-Jines (12-6) potential. For the second virial coefficient of He, we obtain the Boyle’s temperature as follow: TB = 34.9312438964844 (K) B2(T) = 9.82958 × $ 10^{−6} $ ($ cm^{3} $/mol). © Springer Science+Business Media, LLC 2011 |
| abstractGer |
Abstract In this project we evaluate second virial coefficient of some inert gases via classical cluster expansion, assuming each atomic pair interaction is of Lennard-Jones type. We also try to numerically evaluate the third virial coefficient of Argon gas based on bipolar-coordinate integration (Mas et al. in J Chem Phys 10:6694, 1999), assuming the same Lennard-Jones potential as before. The second virial coefficient (Vega et al. in Phys Chem Chem Phys 4:3000–3007, 2002) calculated from our model are compatible to the experimental data [19] The temperature at which B2(T) → 0 is called the Boyle’s temperature TB (Vega et al. in Phys Chem Chem Phys 4:3000–3007, 2002) for the Lennard-Jines (12-6) potential. For the second virial coefficient of He, we obtain the Boyle’s temperature as follow: TB = 34.9312438964844 (K) B2(T) = 9.82958 × $ 10^{−6} $ ($ cm^{3} $/mol). © Springer Science+Business Media, LLC 2011 |
| abstract_unstemmed |
Abstract In this project we evaluate second virial coefficient of some inert gases via classical cluster expansion, assuming each atomic pair interaction is of Lennard-Jones type. We also try to numerically evaluate the third virial coefficient of Argon gas based on bipolar-coordinate integration (Mas et al. in J Chem Phys 10:6694, 1999), assuming the same Lennard-Jones potential as before. The second virial coefficient (Vega et al. in Phys Chem Chem Phys 4:3000–3007, 2002) calculated from our model are compatible to the experimental data [19] The temperature at which B2(T) → 0 is called the Boyle’s temperature TB (Vega et al. in Phys Chem Chem Phys 4:3000–3007, 2002) for the Lennard-Jines (12-6) potential. For the second virial coefficient of He, we obtain the Boyle’s temperature as follow: TB = 34.9312438964844 (K) B2(T) = 9.82958 × $ 10^{−6} $ ($ cm^{3} $/mol). © Springer Science+Business Media, LLC 2011 |
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Numerical evaluation of second and third virial coefficients of some inert gases via classical cluster expansion |
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