Kinetics of the establishment of steady homogeneous condensation of a supersaturated vapor

1982 ◽  
Vol 52 (1) ◽  
pp. 699-706
Author(s):  
A. P. Grinin ◽  
F. M. Kuni ◽  
A. K. Shchekin
2009 ◽  
Vol 54 (11) ◽  
pp. 483-487
Author(s):  
N. M. Kortsenshteyn ◽  
E. V. Samuĭlov ◽  
A. K. Yastrebov

1992 ◽  
Vol 25 (3) ◽  
pp. 487-491
Author(s):  
L M Biberman ◽  
I A Goodilin ◽  
I L Erukhimovich ◽  
A V Kirillin ◽  
A G Kobzunenko ◽  
...  

1986 ◽  
Vol 7 (6) ◽  
pp. 588-616 ◽  
Author(s):  
V. F. Gordiets ◽  
L. A. Shelepin ◽  
Yu. S. Shmotkin

1999 ◽  
Vol 111 (18) ◽  
pp. 8265-8266 ◽  
Author(s):  
S. H. Bauer ◽  
Yi‐Xue Zhang ◽  
C. F. Wilcox

2004 ◽  
Vol 121 (24) ◽  
pp. 12490 ◽  
Author(s):  
A. P. Grinin ◽  
I. A. Zhuvikina ◽  
F. M. Kuni ◽  
H. Reiss

Author(s):  
J. F. DeNatale ◽  
D. G. Howitt

The electron irradiation of silicate glasses containing metal cations produces various types of phase separation and decomposition which includes oxygen bubble formation at intermediate temperatures figure I. The kinetics of bubble formation are too rapid to be accounted for by oxygen diffusion but the behavior is consistent with a cation diffusion mechanism if the amount of oxygen in the bubble is not significantly different from that in the same volume of silicate glass. The formation of oxygen bubbles is often accompanied by precipitation of crystalline phases and/or amorphous phase decomposition in the regions between the bubbles and the detection of differences in oxygen concentration between the bubble and matrix by electron energy loss spectroscopy cannot be discerned (figure 2) even when the bubble occupies the majority of the foil depth.The oxygen bubbles are stable, even in the thin foils, months after irradiation and if van der Waals behavior of the interior gas is assumed an oxygen pressure of about 4000 atmospheres must be sustained for a 100 bubble if the surface tension with the glass matrix is to balance against it at intermediate temperatures.


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