Laser beam properties and microfluidic confinement control thermocavitation

TL;DR

This study investigates how the size of a laser beam affects bubble formation in thermocavitation, revealing that larger beams delay nucleation and increase bubble growth, with implications for microfluidic applications.

Contribution

The paper introduces a novel method to control laser beam size via fiber distance, and demonstrates its impact on bubble dynamics in continuous-wave thermocavitation.

Findings

Larger beam size delays nucleation time.

Maximum temperature at nucleation is approximately 237°C, independent of laser parameters.

Total bubble energy depends only on absorbed optical energy, not beam size or laser power.

Abstract

Thermocavitation, the creation of a vapor bubble by heating a liquid with a continuous-wave laser, has been studied for a wide range of applications. Examples include the development of an actuator for needle-free jet injectors, as the pumping mechanism in microfluidic channels and crystallization or nanoparticle synthesis. Optimal use in these applications require control over the dynamics of the laser-generated bubble through the laser power and beam radius. In contrast to pulsed lasers, for continuous-wave lasers the influence of the laser beam radius on the bubble characteristics is not fully understood. Here, we present a novel way to control the size of the beam from an optical fiber by changing the distance from the glass-liquid interface. We show that the increase in beam size results in a longer nucleation time. Numerical simulations of the experiment show that the maximum temperature at the moment of nucleation is 237$\pm$5{\deg}C and independent of laser parameters. Due to delayed nucleation for larger beam sizes, more energy is absorbed by the liquid at the nucleation instant. Consequently, a larger beam size results in a faster growing bubble, producing the same effect as reducing the laser power. We conclude that the total bubble energy only depends on the amount of absorbed optical energy and it is independent of the beam radius and laser power for any amount of absorbed energy. This effect contrasts with pulsed lasers, where an increase in beam radius results in a reduction of bubble energy. Our results are of relevance for the use of continuous-wave laser-actuated cavitation in needle-free jet injectors as well as other applications of thermocavitation in microfluidic confinement.