scholarly journals Time-evolution of bubble formation in a viscous liquid

2008 ◽  
Vol 60 (6) ◽  
pp. 661-679 ◽  
Author(s):  
Kou Yamada ◽  
Hiroyuki Emori ◽  
Kiyoshi Nakazawa
2019 ◽  
Vol 14 (6) ◽  
Author(s):  
Md. Tariqul Islam ◽  
Poo Balan Ganesan ◽  
Md. Masum Billah ◽  
Md. Nasir Uddin

1997 ◽  
Vol 75 ◽  
pp. S105-S115 ◽  
Author(s):  
J.F. Davidson ◽  
B.O.G. Schüler

2019 ◽  
Vol 23 (5) ◽  
Author(s):  
Xiaohui Lin ◽  
Fubing Bao ◽  
Chengxu Tu ◽  
Zhaoqin Yin ◽  
Xiaoyan Gao ◽  
...  

2011 ◽  
Vol 37 (9) ◽  
pp. 1059-1071 ◽  
Author(s):  
Mitsuhiro Ohta ◽  
Daisuke Kikuchi ◽  
Yutaka Yoshida ◽  
Mark Sussman

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.


Author(s):  
A. C. Faberge

Benzylamine tartrate (m.p. 63°C) seems to be a better and more convenient substrate for making carbon films than any of those previously proposed. Using it in the manner described, it is easy consistently to make batches of specimen grids as open as 200 mesh with no broken squares, and without individual handling of the grids. Benzylamine tartrate (hereafter called B.T.) is a viscous liquid when molten, which sets to a glass. Unlike polymeric substrates it does not swell before dissolving; such swelling of the substrate seems to be a principal cause of breakage of carbon film. Mass spectroscopic examination indicates a vapor pressure less than 10−9 Torr at room temperature.


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