scholarly journals Bubble formation in liquid Sn under different plasma loading conditions leading to droplet ejection

2021 ◽  
Author(s):  
Wei Ou ◽  
Frédéric Brochard ◽  
T W Morgan
Author(s):  
O. E. Ruiz

Numerical simulations of the thermal inkjet (TIJ) droplet ejection process are performed. The computational approach is based on a volume of fluid (VOF) formulation. This method allows determining the coupled flow and thermal fields in the firing chamber in addition to the phase change processes that take place during the drive bubble formation, expansion, and collapse. The drive bubble pressure is a result of the phase change heat transfer during the heating pulse and is not imposed by a pressure heuristic approach. A commercially available TIJ architecture was chosen as a baseline to assess the computational model predictions of ejected droplet volume and droplet velocity during a firing cycle. These computational model predictions were compared to experimental results demonstrating an excellent agreement. The transient histories of pressure in the vapor bubble, temperature, and heat transfer rate to the fluid are analyzed to explain some of the relevant physical processes observed.


1999 ◽  
Author(s):  
Yi-Kuen Lee ◽  
Ui-Chong Yi ◽  
Fan-Gang Tseng ◽  
Chang-Jin “CJ” Kim ◽  
Chih-Ming Ho

Abstract This paper reports a new application of a thermal microinjector for fuel injection. The paper estimates the ejected velocity of the diesel fuel droplet, and the minimum temperature for bubble formation. The fuel spray penetration is calculated by solving nonlinear equations of motion. Analysis of the temperature profile evolution and activation curve between water and diesel fuel is helpful for optimization of the microinjector design. The microinjector is fabricated using combined surface and bulk micromaching. The preliminary testing of the microinjector with fuel demonstrates the possibility of droplet ejection. Also, discussion about design issues reveals some advantages of the microinjector over the conventional fuel injector.


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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