局部激光加热生物组织时的热过程

N. Kokodii, A. Korobov, H. Shi, M. F. Posokhov, S. Shulga, V. Timaniuk, Г. Кокодій, А. М. Коробов, Хе Ші, М. Ф. Посохов, С. М. Шульга
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引用次数: 0

摘要

介绍。激光目前在医学上广泛用于诊断和治疗。对人暴露于激光辐射时所发生的热过程的研究,使开发治疗许多疾病的创新方法成为可能。目的:研究生物组织局部激光加热过程中的热过程(数学模型和实验)。材料和方法。利用建立的生物组织内某一区域局部加热过程的数学模型,研究了波长为0.98 μm的红外光、波长为0.65 μm的红光、波长为0.5微米的绿光和波长为0.435微米的蓝光对环境进行连续脉冲激光加热的过程。确定了加热区域的大小、建立时间和温度下降。计算结果与实测数据吻合较好。用激光辐射加热生物组织的方式取决于波长。当辐射脉冲持续时间远短于热时间常数时,辐射截面的最高加热温度与脉冲的形状和持续时间无关,仅由吸收辐射的能量决定。在脉冲持续时间内热量在介质中的分布是由脉冲持续时间和组织的热扩散率决定的。为了减少对周围组织的加热,有必要使用短辐射脉冲。一系列辐射脉冲对组织加热的过程取决于脉冲持续时间、脉冲重复周期和介质热时间常数之间的关系。平均(平滑)温度与连续加热功率等于脉冲调制辐射的平均功率时的温度相同。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Thermal processes during local laser heating of biological tissues
Introduction. Lasers in medicine are currently widely used for both diagnosis and treatment. Studies of the thermal processes that occur when a person is exposed to laser radiation have made it possible to developinnovative methods of treating many diseases. Purpose: to study thermal processes in biological tissues during their local laser heating (mathematical model and experiment). Materials and methods. Using the developed mathematical model of the process of local heating of a certain region inside biological tissue, we studied the process of heating the environment by continuous and pulsed laser radiation using infrared light with a wavelength of 0.98 μm, red light with a wavelength of 0.65 μm, green light with a wavelength 0.5 microns and blue light with a wavelength of 0.435 microns. Results. The sizes of the heated region, the time of establishment and decrease in temperature are determined. The calculation results are in good agreement with the obtained experimental data. Findings. The mode of heating biological tissue with laser radiation depends on the wavelength. The maximum heating temperature of the irradiated section with a radiation pulse duration much shorter than the thermal time constant is independent of the shape and duration of the pulse and is determined only by the energy of the absorbed radiation. The distribution of heat into the medium during the duration of the pulse is determined by its duration and thermal diffusivity of the tissue. To reduce the heating of the surrounding tissue, it is necessary to use short radiation pulses. The progress of tissue heating by a sequence of radiation pulses depends on the relationship between the duration of the pulses, the period of their repetition, and the thermal time constant of the medium. The average (smoothed) temperature is the same as when heated with continuous power equal to the average power of the pulse-modulated radiation.
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