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激光辐照水浸等离子体纳米粒子周围的蒸汽和气泡生长动力学。

Vapor and Gas-Bubble Growth Dynamics around Laser-Irradiated, Water-Immersed Plasmonic Nanoparticles.

机构信息

Robotics Institute, School of Mechanical Engineering and Automation, Beihang University , Beijing 100191, P.R. China.

MESA+ Institute for Nanotechnology, MIRA Institute for Biomedical Technology and Technical Medicine, University of Twente , Drienerlolaan 5, 7522 NB Enschede, The Netherlands.

出版信息

ACS Nano. 2017 Feb 28;11(2):2045-2051. doi: 10.1021/acsnano.6b08229. Epub 2017 Jan 20.

Abstract

Microbubbles produced by exposing water-immersed metallic nanoparticles to resonant light play an important role in emerging and efficient plasmonic-enhanced processes for catalytic conversion, solar energy harvesting, biomedical imaging, and cancer therapy. How do these bubbles form, and what is their gas composition? In this paper, the growth dynamics of nucleating bubbles around laser-irradiated, water-immersed Au plasmonic nanoparticles are studied to determine the exact origin of the occurrence and growth of these bubbles. The microbubbles' contact angle, footprint diameter, and radius of curvature were measured in air-equilibrated water (AEW) and degassed water (DGW) with fast imaging. Our experimental data reveals that the growth dynamics can be divided into two regimes: an initial bubble nucleation phase (regime I, < 10 ms) and, subsequently a bubble growth phase (regime II). The explosive growth in regime I is identical for AEW and DGW due to the vaporization of water. However, the slower growth in regime II is distinctly different for AEW and DGW, which is attributed to the uptake of dissolved gas expelled from the water around the hot nanoparticle. Our scaling analysis reveals that the bubble radius scales with time as R(t) ∝ t for both AEW and DGW in the initial regime I, whereas in the later regime II it scales as R(t) ∝ t for AEW and is constant for perfectly degassed water. These scaling relations are consistent with the experiments.

摘要

将水浸金属纳米颗粒暴露在共振光下产生的微泡在新兴的、高效的等离子体增强催化转化、太阳能收集、生物医学成像和癌症治疗过程中发挥着重要作用。这些气泡是如何形成的,它们的气体成分是什么?在本文中,研究了激光辐照下水浸 Au 等离子体纳米颗粒周围成核气泡的生长动力学,以确定这些气泡发生和生长的确切起源。使用快速成像技术在空气平衡水(AEW)和除气水中测量了微泡的接触角、足迹直径和曲率半径。我们的实验数据表明,生长动力学可以分为两个阶段:初始气泡成核阶段(I 区,<10ms)和随后的气泡生长阶段(II 区)。由于水的蒸发,I 区的爆炸式增长在 AEW 和 DGW 中是相同的。然而,II 区的较慢增长在 AEW 和 DGW 中明显不同,这归因于从热纳米颗粒周围水中逸出的溶解气体的吸收。我们的标度分析表明,在初始的 I 区,气泡半径与时间的标度关系为 R(t)∝t,对于 AEW 和 DGW 都是如此,而在后期的 II 区,对于 AEW,它与时间的标度关系为 R(t)∝t,对于完美除气的水则是常数。这些标度关系与实验一致。

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