Numerical simulation of the optical radiation absorption by dielectric microcapsules of different spatial shapes

Y. Geints, E. K. Panina
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Abstract

The heating dynamics a micron-sized two-layer capsules simulating transport microcontainers with water-containing load and light-absorbing composite shell exposed to a near-IR laser pulse (wavelength 800 nm) is theoretically studied. Both single microcapsules and the microassemblies of particles with various spatial shapes and different packing densities are considered. Using FDTD and FEM calculations, the numerical simulations of the optical field distribution inside and near the microcapsules are carried out, and the temporal dynamics of the temperature profiles of microparticles shells is obtained. Based on the simulation results, one can conclude that the particle morphology introduces specificity in the spatial profile of the optical field and the distribution of light absorption regions. Variation in the geometric shape of a capsule leads to dramatic changes in the distribution of absorbed light energy and, accordingly, particle temperature field. In order to increase the efficiency of absorption of optical radiation in capsule volume and to obtain the maximum heating of absorbing shells, the capsules of cubic, cylindrical and partly rectangular shapes are preferable. Thus, having a 100-fs laser pulse with energy of only 20 μJ it becomes possible to heat a cylindrical microcapsule to the temperature of thermal destruction of its polymeric shell (~ 410 K). Worthwhile notice, the water-filling of a capsule core remains cold. At the same conditions, the ellipsoid-shaped capsule is heated to multiple lower temperatures (~ 340 K).
不同空间形状介质微胶囊对光辐射吸收的数值模拟
本文从理论上研究了近红外激光脉冲(波长800 nm)作用下微米级含水负载和吸光复合壳双层模拟输运微容器胶囊的加热动力学。考虑了不同空间形状和不同堆积密度的单个微胶囊和颗粒微组合体。采用时域有限差分法和有限元法对微胶囊内部和附近的光场分布进行了数值模拟,得到了微胶囊壳体温度分布的时间动态特征。根据模拟结果可以得出结论,粒子形态在光场的空间分布和光吸收区域的分布中引入了特异性。胶囊几何形状的变化会导致吸收光能分布的剧烈变化,从而导致粒子温度场的剧烈变化。为了提高胶囊体积对光辐射的吸收效率和获得最大的吸收壳的热量,可以采用立方、圆柱形和部分矩形形状的胶囊。因此,使用能量仅为20 μJ的100 fs激光脉冲,就可以将圆柱形微胶囊加热到其聚合物外壳的热破坏温度(~ 410 K),值得注意的是,胶囊芯的充水仍然是冷的。在相同条件下,将椭球形胶囊加热到多个较低温度(~ 340 K)。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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