The effects of cavitation position on the velocity of a laser-induced microjet extracted using explainable artificial intelligence

The control of the velocity of a high-speed laser-induced microjet is crucial in applications such as needle-free injection. Previous studies have indicated that the jet velocity is heavily influenced by the volumes of secondary cavitation bubbles generated through laser absorption. However, there has been a lack of investigation of the relationship between the positions of cavitation bubbles and the jet velocity. In this study, we investigate the effects of cavitation bubbles on the jet velocity of laser-induced microjets extracted using explainable artificial intelligence (XAI). An XAI is used to classify the jet velocity from images of cavitation bubbles and to extract features from the images through visualization of the classification process. For this purpose, we run 1000 experiments and collect the corresponding images. The XAI model, which is a feedforward neural network (FNN), is trained to classify the jet velocity from the images of cavitation bubbles. After achieving a high classification accuracy, we analyze the classification process of the FNN. The predictions of the FNN, when considering the cavitation positions, show a higher correlation with the jet velocity than the results considering only cavitation volumes. Further investigation suggested that cavitation that occurs closer to the laser focus position has a higher acceleration effect. These results suggest that the velocity of a high-speed microjet is also affected by the cavitation position.Comment: 11 pages, 13 figures, 4 table

A phase diagram of the pinch-off-type behavior of impulsively-induced viscoelastic liquid jets

In this study, we systematically investigate the jet behaviors of viscoelastic liquids, focusing on the region of high velocity and high viscoelasticity, which has not been investigated in previous studies. We generate viscoelastic jets using an impulsive force and categorize the resulting jets into two types: pinch-off jets (jets that break up during elongation after ejection) and no-pinch-off jets (jets that pull back to the nozzle after maximum elongation or jets that return without elongation after ejection). We then propose criteria to characterize these regions using the Weissenberg number and the Reynolds number, which are dimensionless numbers composed of the rheological properties of the solution and the initial conditions of the jet injection. It is found that pinch-off jets occur at $Re \gtrsim 23.4Wi$ in regions of high elasticity $Wi \gtrsim 10$, and at $Re \gtrsim 250$ in regions of low elasticity $Wi \lesssim 10$. We also show that the phase diagram can be explained by modeling a focused jet using the finitely extensible non-linear elastic dumbbell model with the Chilcott-Rallison closure approximation (FENE-CR)

Wake-induced lateral migration of approaching bubbles

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