Thermal Diffusion Columns and Intermolecular Potential. III. The Noble Gases Ar and Xe

1971 ◽  
Vol 55 (1) ◽  
pp. 387-393 ◽  
Author(s):  
J. C. Yarza ◽  
M. A. Hidalgo ◽  
D. González Alvarez ◽  
J. M. Savirón
1971 ◽  
Vol 54 (7) ◽  
pp. 3105-3111 ◽  
Author(s):  
M. A. Hidalgo ◽  
J. C. Yarza ◽  
D. González Alvarez ◽  
J. M. Savirón

1969 ◽  
Vol 50 (9) ◽  
pp. 3936-3941 ◽  
Author(s):  
D. González Alvarez ◽  
J. M. Savirón ◽  
J. C. Yarza

1963 ◽  
Vol 18 (2) ◽  
pp. 242-245 ◽  
Author(s):  
W. W. Watson ◽  
A. J. Howard ◽  
N. E. Miller ◽  
R. M. Shiffrin

With an all-metal “swing separator” having unique features, thermal diffusion factors αT for He3/He4 and Ne20Ne22 have been measured with improved accuracy down to average gas temperatures T̅=136°K. For helium αT is 0.0696 ± 0.0010 at 136°K, dropping gradually to 0.0651 ±0.0010 at 313°K. These data, plus measurements by Van der Valk and de Vries at somewhat higher temperatures, agree best with values predicted by an exp-six intermolecular potential with ε/k=9.16 and α=12.7. We are extending these helium measurements down to T=4°K for the lower temperature, to detect if possible quantum corrections to the intermolecular potential. For neon αT increases from 0.0166 ± 0.0010 at 136°K to 0.0233 ± 0.0020 at 310°K, considerably higher than our previously reported values. These T. D. factors for neon are in good agreement with values calculated from an exp-six potential with ε/k = 46.0 ± 0.6 and α=13.


Author(s):  
Felix Sharipov ◽  
Victor Juan Benites

The transport coefficients such as viscosity, thermal conductivity, diffusion and thermal diffusion of neon, argon, krypton, and xenon taking into consideration their real isotopic compositions are computed for a wide...


1974 ◽  
Vol 60 (4) ◽  
pp. 1624-1627 ◽  
Author(s):  
J. Maya ◽  
P. Davidovits

1998 ◽  
Vol 39-40 ◽  
pp. 1015-1020
Author(s):  
Hiroshi Yamakawa ◽  
Akira Segi ◽  
Noboru Kobayashi ◽  
Takayuki Matsunaga ◽  
Youichi Enokida ◽  
...  

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