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首页> 外文期刊>The Korean journal of chemical engineering >High Gas Permeability in Open-Structure Membranes
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High Gas Permeability in Open-Structure Membranes

机译:开放结构膜中的高透气性

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For most polymeric membranes, the gas permeability coefficient (P) is often interpreted as the product of diffusivity (D) and solubility (S) of a penetrant gas in the polymer (P=D S). The basic assumption is that molecular diffusion is primarily responsible for mass transport in the membrane permeation process. However, for some open structure membranes, such as poly(1-trimethylsilyl-1-propyne) [PTMSP] or poly(dimethylsiloxane) [PDMS], the high permeabilities of some gases yield much higher diffusivities when calculated from the above relationship (P=D S) than when calculated by using the direct kinetic measurement of diffusivity. It is hypothesized that this discrepancy is due to the convective transport of gas molecules through such open structured polymers. In most cases, the convective contribution to mass transport through membranes is negligible. However, for polymer membranes with high free volume, such as PTMSP, whose free volume fraction is 20 to 25%, the convective term may dominate the permeation flux. In this study, a non-equilibrium thermodynamic formalism is employed to properly treat the diffusion term and convective term that constitute the Nernst-Planck equation. The current analysis indicates that the total permeation flux, which consists of a diffusion term and a convective term, agrees well with the experimental data for several permeation systems: pure components propane and n-butane/PTMSP, pure gas hydrogen/PTMSP, and mixed gas hydrogen/PTMSP. Also, the permeation systems of a nonporous rubbery membrane, PDMS, and eight organophosphorus compounds were included in the study. It is recommended that the proposed model be validated by using other polymers with high free volumes and high permeabilities of gases and vapors, such as poly(1-trimethylgermyl-1-propyne) [PTMGeP] and poly(4-methyl-2-pentyne) [PMP].
机译:对于大多数聚合物膜,气体渗透系数(P)通常解释为渗透剂气体在聚合物中的扩散率(D)和溶解度(S)的乘积(P = D S)。基本假设是分子扩散是膜渗透过程中质量传输的主要负责人。但是,对于某些开放结构的膜,例如聚(1-三甲基甲硅烷基-1-丙炔)[PTMSP]或聚(二甲基硅氧烷)[PDMS],根据上述关系式计算,某些气体的高渗透率会产生更高的扩散率(P = DS)时,则使用直接动力学测量扩散率进行计算。据推测,这种差异是由于气体分子通过这种开放结构的聚合物的对流传输所致。在大多数情况下,对流通过膜的传质贡献可以忽略不计。但是,对于具有高自由体积的聚合物膜(例如PTMSP),其自由体积分数为20%到25%,对流项可能会主导渗透通量。在这项研究中,采用非平衡热力学形式主义来正确处理构成Nernst-Planck方程的扩散项和对流项。目前的分析表明,由扩散项和对流项组成的总渗透通量与几种渗透系统的实验数据非常吻合:纯组分丙烷和正丁烷/ PTMSP,纯净氢气/ PTMSP和混合气体。氢气/ PTMSP。此外,研究还包括无孔橡胶膜,PDMS和八种有机磷化合物的渗透系统。建议通过使用具有高自由体积和高透气性的其他聚合物来验证所提出的模型,例如聚(1-三甲基锗烷基-1-丙炔)[PTMGeP]和聚(4-甲基-2-戊炔) )[PMP]。

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