Modelling of volatile organic compounds emission from dry building materials

扩散 分配系数 传质 材料科学 传质系数 挥发性有机化合物 机械 空气流速 室内空气 分析化学(期刊) 热力学 化学 环境科学 环境化学 环境工程 色谱法 有机化学 物理
作者
Hongyu Huang,Fariborz Haghighat
出处
期刊:Building and Environment [Elsevier BV]
卷期号:37 (11): 1127-1138 被引量:160
标识
DOI:10.1016/s0360-1323(01)00089-0
摘要

A numerical and an analytical model were developed to predict the volatile organic compound (VOC) emission rate from dry building materials. Both models consider the mass diffusion process within the material and the mass convection and diffusion processes in the boundary layer. All the parameters, the mass diffusion coefficient of the material, the material/air partition coefficient, and the mass transfer coefficient of the air can be either found in the literature or calculated using known principles. The predictions of the models were validated at two levels: with experimental results from the specially designed test and with predictions made by a CFD model. The results indicated that there was generally good agreement between the model predictions, the experimental results, and the CFD results. The analytical and numerical models then were used to investigate the impact of air velocity on emission rates from dry building materials. Results showed that the impact of air velocity on the VOC emission rate increased as the VOC diffusion coefficient of the material increased. For the material with a diffusion coefficient >10−10m2/s, the VOC emission rate increased as the velocity increased; air velocity had significant effect on the VOC emission. For the material with a VOC diffusion coefficient <10−10m2/s, the VOC emission rate increased as the velocity increased only in the short term; <24h. In the medium- to long-term time range, the VOC emission rate decreased slightly as the air velocity increased; velocity did not have much impact on these materials. Furthermore, the study also found that the VOC concentration distribution within the material; the VOC emission rate and the VOC concentration in the air were linearly proportional to the initial concentration. However, the normalized emitted mass was not a function of the initial concentration: it was a function of the properties of the VOC and the material.
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