scholarly journals Temperature dependence of the vapor pressure and evaporation coefficient of supercooled water

2014 ◽  
Vol 119 (18) ◽  
pp. 10,931-10,940 ◽  
Author(s):  
James F. Davies ◽  
Rachael E. H. Miles ◽  
Allen E. Haddrell ◽  
Jonathan P. Reid
2008 ◽  
Vol 25 (9) ◽  
pp. 1724-1729 ◽  
Author(s):  
Will Cantrell ◽  
Eli Ochshorn ◽  
Alexander Kostinski ◽  
Keith Bozin

Abstract Measurements are presented of the vapor pressure of supercooled water utilizing infrared spectroscopy, which enables unambiguous verification that the authors’ data correspond to the vapor pressure of liquid water, not a mixture of liquid water and ice. Values of the vapor pressure are in agreement with previous work. Below −13°C, the water film that is monitored to determine coexistence of liquid water (at one temperature) and ice (at another, higher, temperature) de-wets from the hydrophilic silicon prism employed in the authors’ apparatus. The de-wetting transition indicates a quantitative change in the structure of the supercooled liquid.


1977 ◽  
Vol 22 (2) ◽  
pp. 131-134 ◽  
Author(s):  
Heiko K. Cammenga ◽  
Friedrich W. Schulze ◽  
Wilhelm Theuerl

1972 ◽  
Vol 50 (16) ◽  
pp. 1881-1886 ◽  
Author(s):  
J. A. Cowan ◽  
R. N. Ball

Attenuation measurements have been made on liquid argon for temperatures between 90 and 150 °K and pressures between saturated vapor and 1000 p.s.i. Values of bulk viscosity were calculated and compared with theoretical results. For densities above 1.15 gcm−3 the PNM theory is in excellent agreement. However, below these values the theoretical results continue to decrease with density where the experimental results increase sharply. The values of the ratio of bulk to shear viscosity for saturated vapor pressure are found to be a linear function of (Tc–T)−3/2 from 90 to 140 °K.


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