Some Further Observations on the Critical Region. II

1964 ◽  
Vol 40 (9) ◽  
pp. 2747-2748 ◽  
Author(s):  
George W. Brady
Keyword(s):  
1939 ◽  
Vol 17b (9) ◽  
pp. 241-250 ◽  
Author(s):  
R. L. McIntosh ◽  
J. R. Dacey ◽  
O. Maass

The data of a previous publication have been extended. Nine pressure isothermals of the one component system ethylene in the critical region are given. Further evidence of the existence of a two phase system above the temperature of meniscus disappearance as normally determined is presented. The existence of a latent heat of vaporization above this temperature is pointed out. An explanation of the hysteresis of liquid phase density with temperature at constant volume is offered, and a qualitative description of the changes occurring in the transition region of liquid to gas is developed from the experimental evidence.


1950 ◽  
Vol 18 (12) ◽  
pp. 1683-1683 ◽  
Author(s):  
E. B. Giller ◽  
R. B. Duffield ◽  
H. G. Drickamer

1950 ◽  
Vol 18 (5) ◽  
pp. 655-656 ◽  
Author(s):  
A. L. Babb ◽  
H. G. Drickamer

1953 ◽  
Vol 31 (6) ◽  
pp. 569-584 ◽  
Author(s):  
S. G. Whiteway ◽  
S. G. Mason

Liquid–vapor coexistence curves of ethane, ethylene, and xenon have been measured in the region of the critical point. Impurities present in the ethane and ethylene gave retrograde systems; reduction of the impurities yielded coexistence curves which were flat along the temperature axis to 0.001 °C. When the height of the ethylene system was decreased the range of densities over which the curve was flat was diminished. Stirring of the system caused the curve to be rounded. Similar results, confirming those of Weinberger and Schneider, were obtained with xenon. The observed behavior is in good agreement with the hypothesis that the major part of the flat top effect is due to gravitational compression.


1950 ◽  
Vol 18 (8) ◽  
pp. 1027-1030 ◽  
Author(s):  
E. B. Giller ◽  
R. B. Duffield ◽  
H. G. Drickamer

1998 ◽  
Vol 109 (12) ◽  
pp. 5119-5125 ◽  
Author(s):  
Valentina V. Vasilevskaya ◽  
Pavel G. Khalatur ◽  
Alexei R. Khokhlov

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