arXiv subjects

Hiroaki Kusuno

Publications and source records attributed to Hiroaki Kusuno.

7 recordsLinked to original sources

arXiv2026

Prediction of Spherical Bubble-Chain-Induced Liquid Flow through Far-Wake Superposition Based on Bubble-Chain Hydrodynamics

Recent experimental observations revealed that clean spherical bubble chains generate a nearly uniform upward liquid flow. The physical origin of this liquid flow, however, remains unclear. Hydrodynamic interactions in aligned bubble chains were therefore investigated using high-accuracy embedded-boundary simulations that resolve the interfacial boundary layer while capturing long-range interactions among multiple clean spherical bubbles. The simulations were used to quantify the evolution of hydrodynamic interactions within bubble chains and to identify the conditions under which bubble-induced liquid flow can be represented by the superposition of isolated-bubble far wakes. Based on these findings, a reduced-order model was developed and applied to experimentally measured bubble trajectories. The model successfully reproduced the nearly uniform upward liquid flow observed in the experiments. To clarify the role of bubble dispersion, the predictions were compared with those for a uniformly dispersed bubble arrangement having the same overall dispersion width. While the uniformly dispersed arrangement produced a center-peaked velocity distribution, only the experimentally observed bubble trajectories reproduced the nearly uniform upward liquid flow. These results demonstrate that the liquid flow is governed not simply by the dispersion width but by the bubble trajectories that establish the spatial distribution of far wakes. The present study provides a physical framework linking hydrodynamic interactions among bubbles, bubble dispersion, and bubble-induced liquid flow, together with a reduced-order model for predicting the liquid flow generated by bubble chains.

physics.flu-dyn↗

arXiv2026

Interfacial dynamics induced by impacts across rigid and soft substrates

We investigate impact-induced gas-liquid interfacial dynamics through experiments in which a liquid-filled container impacts substrates with elastic moduli from $O(10^{-1})$ MPa to $O(10^{5})$ MPa. Upon impact, the concave gas-liquid interface inside the container deforms and emits a focused jet. When the jet velocity is normalized by the container impact velocity, all data collapse onto a single curve when plotted against the Cauchy number, $Ca = ρ_{\rm e} V_{\rm i}^2 / E$, which represents the ratio of the inertial force of the container-liquid system to the elastic restoring force of the substrate. The dimensionless jet velocity remains nearly constant for $Ca< 10^{-4}$, but decreases significantly for $Ca > 10^{-4}$. Based on this observation, we define the boundary between the rigid-impact and soft-impact regimes using the Cauchy number, providing a quantitative criterion for what constitutes ``softness'' in impact-driven interfacial flows. To explain the reduction in jet velocity observed in the soft-impact regime, we introduce a framework in which only the impulse transferred within the effective time window for jet formation contributes to interface acceleration. This concept, referred to as the partial impulse, captures the situation where the impact interval (the duration of contact between the container and the substrate) exceeds the focusing interval (the time required for jet formation). By modelling the contact force using an elastic foundation model and solving the resulting momentum equation over the finite impulse window, we quantitatively reproduce the experimental results. This partial impulse framework unifies the dynamics of impact-driven jetting across both rigid and soft substrate regimes, extending the applicability of classical impulse-based models.

cond-mat.soft↗

arXiv2025

Effect of converging shape of container on the velocity of impact-induced focused liquid jet

We investigated the effect of container shape on the behavior of the impact-induced focused liquid jets by dropping a converging-shaped container (e.g., Kjeldahl flask) partially filled with liquid onto a floor to develop a method for increasing the jet velocity. Note that a similar well-known experiment, Pokrovski's experiment, in which a focused liquid jet is generated in a test tube, is free from the effect of the converging shape. The results showed that the jet was up to about 1.6 times faster in a converging-shaped container than in a test tube, despite the same impact velocity. To understand the mechanism of the increase in the jet velocity, the Laplace equation on the pressure impulse was solved numerically under the boundary condition that the pressure impulse is given at the bottom of the container. The normalized gas-liquid interfacial velocity obtained from the numerical solution of the pressure impulse field agrees well with the normalized jet velocity in experiments, showing that the jets we observed are driven by the pressure impulse generated at the bottom. In addition, numerical solutions of pressure impulse fields in a simpler-shaped container with different degrees of convergence were compared with analytical solutions obtained from a lower-order model of the pressure impulse field. We confirmed that the gas-liquid interfacial velocity of the impact-induced focused liquid jet is governed by changes in both the flow rate and pressure impulse gradient at the central axis of the container caused by changes in the cross-sectional area of the container. We showed that by changing the container shape, we can increase the velocity of the gas-liquid interface after the container impact. This finding is expected to be applied to the ejection and application of high-viscosity liquids as well as to needle-free injection technology using fast focused liquid jets.

physics.flu-dyn↗

arXiv2025

Stress field in the vicinity of a bubble/sphere moving in a dilute surfactant solution

In this study, we experimentally investigate the stress field around a bubble rising in a dilute surfactant solution (20 < Re < 220, high Peclet numbers) whose surface gradually becomes contaminated, and compare it with that around a sphere free from surface contamination. We employ a newly developed polarization measurement technique, highly sensitive to stress fields near interfaces. First, we validate this method by measuring the flow around a solid sphere settling at Re = 120 and comparing results with numerical predictions, confirming its accuracy. We then measure the stress field around a bubble whose drag force transitions from that of a clean interface to that of a rigid interface within the observation region. The stress near the bubble's front resembles that of a clean bubble, while the rear behaves like a solid sphere. Between these regions, a discontinuous phase retardation near the cap angle indicates a transition from slip to no-slip boundary conditions. Axisymmetric stress reconstruction reveals localized stress spike at the cap angle, which shifts as surfactant accumulates and increases the drag. Remarkably, the measured cap angle versus normalized drag coefficient agrees well with numerical simulations at Re = 100 (Cuenot et al. 1997) and shows only a slight deviation from the creeping-flow stagnant cap model (Sadhal and Johnson 1983). This work demonstrates that polarization-based stress field measurements effectively capture the interplay between surface contamination and hydrodynamics at intermediate Reynolds numbers.

physics.flu-dyn↗

arXiv2024

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

In this study, we systematically investigate the behaviors of viscoelastic liquid jets using an impulsive force, particularly in the high velocity and high elasticity regimes. The resulting jets are categorized into two types: (i) pinch-off jets, which break up during elongation after ejection, and (ii) no-pinch-off jets, which either retract to the nozzle after maximum elongation, known as `bungee-jumper jets' or return without elongation after ejection. We then propose criteria to delineate these regions using Reynolds number $Re$ and Weissenberg number $Wi$, reflecting the initial conditions at the jet ejection and the solution's rheological properties, respectively. We find that pinch-off jets occur at $Re \gtrsim 23.4Wi$ in high elasticity regimes ($Wi \gtrsim 10$), and at $Re \gtrsim 250$ in low elasticity regimes ($Wi \lesssim 10$). In addition, we demonstrate that the phase diagram of these behaviors can be rationalized through the focused jet modeling using the finitely extensible non-linear elastic dumbbell model with the Chilcott-Rallison closure approximation (FENE-CR).

physics.flu-dyn↗

arXiv2024

Optimal standoff distance for a highly focused microjet penetrating a soft material

A needle-free injector using a highly focused microjet has the potential to minimize the invasiveness of drug delivery. In this study, the jet penetration depth in a soft material-which is a critical parameter for practical needle-free injections-was investigated. We conducted jet penetration experiments by varying the inner diameter of the injection tube and the standoff distance between the meniscus surface and the soft material. Interestingly, the results showed that the penetration depths peaked at certain distances from the meniscus, and the positions shifted further away as the inner diameter was increased. By analyzing the velocity distribution of the microjet, the peak positions of the penetration depth and the maximum velocities were inconsistent due to the effects of the jet shape. To account for this, we introduce the concept of the 'jet pressure impulse', a physical quantity that unifies the velocity and jet shape. However, direct estimation of this parameter from experimental data is challenging due to limitations in spatiotemporal resolution. Therefore, we used numerical simulations to replicate the experimental conditions and calculate the jet pressure impulse. Remarkably, the results show that the jet pressure impulse has peak values, which is consistent with the penetration depth. In addition, there is a correlation between the magnitude of the jet pressure impulse and the penetration depth, highlighting its importance as a key parameter. This study underlines the importance of the jet pressure impulse in controlling the penetration depth of a focused microjet, providing valuable insights for the practical use of needle-free injection techniques.

physics.flu-dyn↗

arXiv2023

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.

physics.flu-dyn↗