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呼气过程中人体鼻腔热回收能力的数值研究。

Numerical study on the heat-recovery capacity of the human nasal cavity during expiration.

作者信息

Na Yang, Chung Seung-Kyu, Byun Seongsu

机构信息

Department of Mechanical Engineering, Konkuk University, Seoul 05029, Republic of Korea.

Department of Otorhinolaryngology: Head and Neck Surgery, Samsung Medical Center, Sungkyunkwan University, School of Medicine, Seoul, Republic of Korea.

出版信息

Comput Biol Med. 2020 Nov;126:103992. doi: 10.1016/j.compbiomed.2020.103992. Epub 2020 Sep 26.

Abstract

The characteristics of the thermal field in the human nasal cavity during the expiration period were investigated using computational fluid dynamics. Heat and water-vapor recovery features were quantitatively investigated under realistic distributions of the epithelial surface and air temperature. A constant expiratory flow rate of 250 mL/s was assumed. The epithelial surface temperature was approximately 34.3-34.4 °C in the nasopharynx and 33.5-33.6 °C in the vestibule region, and these values are in good agreement with the measurement data in the literature. We observed that heat-recovery from the exhaled air mostly occurred in the posterior turbinate region, and the amount of heat recovered is estimated to be approximately 1/3 of the heat supply during inspiration. Because of this heat transfer from the exhaled air to the epithelial surface, the temperature of the epithelial surface increased in this region, and the exhaled air temperature dropped through the turbinate airway. Water-vapor recovery primarily occurs in the posterior segments of the turbinates; however, the amount of water-vapor transfer was approximately 1/5 of that in inspiration. Accordingly, the relative humidity of the exhaled air remained constant throughout the airway.

摘要

利用计算流体动力学研究了呼气期人体鼻腔内的热场特性。在真实的上皮表面和空气温度分布条件下,对热量和水蒸气回收特性进行了定量研究。假设呼气流量恒定为250 mL/s。鼻咽部上皮表面温度约为34.3 - 34.4°C,前庭区域为33.5 - 33.6°C,这些值与文献中的测量数据高度吻合。我们观察到,呼出气体的热量回收主要发生在鼻后鼻甲区域,回收的热量估计约为吸气时供热量的1/3。由于呼出气体向上皮表面的这种热传递,该区域上皮表面温度升高,呼出气体温度通过鼻甲气道下降。水蒸气回收主要发生在鼻甲的后部;然而,水蒸气转移量约为吸气时的1/5。因此,呼出气体的相对湿度在整个气道中保持恒定。

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