Ning Yang, Zundong Xiao, Hanyang Liu, Junan Jiang, Fei Liu, Xiaoxia Yang, Rijie Wang
{"title":"环比对微/毫微米级反应器中停留时间分布和佩克莱特数的影响","authors":"Ning Yang, Zundong Xiao, Hanyang Liu, Junan Jiang, Fei Liu, Xiaoxia Yang, Rijie Wang","doi":"10.1002/cjce.25428","DOIUrl":null,"url":null,"abstract":"Micro/milli‐scale annular reactor with straight and helical forms has excellent heat and mass transfer performance due to the short molecular diffusion distance and dual‐wall surface transport. The annular gap spacing is scalable by adjusting the inner and outer tube diameter. The influence of diffusion and convection effects on axial dispersion as expanding the flow scale requires further elucidation with the help of residence time distribution (RTD) curves and Péclet (Pe) numbers. The correlation of RTD characteristics with annulus ratio <jats:italic>γ = D</jats:italic><jats:sub>h</jats:sub>/<jats:italic>D</jats:italic> (ratio of annulus characteristic size to outer diameter) is investigated using computational fluid dynamics. Results show that with enlarging the straight annular gap from micro‐scale to milli‐scale, RTD characteristics exhibit opposing patterns. This can be attributed to the transition from diffusion‐dominated to convection‐dominated on momentum transfer, and the transition interval is 0.167 < <jats:italic>γ</jats:italic> < 0.250. Correlation equations of Pe number with Reynolds (Re) number and <jats:italic>γ</jats:italic> are established under diffusion‐dominated and convection‐dominated states. The symmetrically distributed secondary flow in the helical annular gap effectively elevates the Pe (Pe<jats:sub>max</jats:sub> > 100). Correlation equations of Pe with Re and <jats:italic>γ</jats:italic> are established in helical annular gaps with 0.083 < <jats:italic>γ</jats:italic> < 0.208 and 0.167 < <jats:italic>γ</jats:italic> < 0.500. The above results contribute to understanding the annular flow RTD characteristics for better applications of tube‐in‐tube reactors.","PeriodicalId":501204,"journal":{"name":"The Canadian Journal of Chemical Engineering","volume":"100 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-08-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Effect of annulus ratio on the residence time distribution and Péclet number in micro/milli‐scale reactors\",\"authors\":\"Ning Yang, Zundong Xiao, Hanyang Liu, Junan Jiang, Fei Liu, Xiaoxia Yang, Rijie Wang\",\"doi\":\"10.1002/cjce.25428\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Micro/milli‐scale annular reactor with straight and helical forms has excellent heat and mass transfer performance due to the short molecular diffusion distance and dual‐wall surface transport. The annular gap spacing is scalable by adjusting the inner and outer tube diameter. The influence of diffusion and convection effects on axial dispersion as expanding the flow scale requires further elucidation with the help of residence time distribution (RTD) curves and Péclet (Pe) numbers. The correlation of RTD characteristics with annulus ratio <jats:italic>γ = D</jats:italic><jats:sub>h</jats:sub>/<jats:italic>D</jats:italic> (ratio of annulus characteristic size to outer diameter) is investigated using computational fluid dynamics. Results show that with enlarging the straight annular gap from micro‐scale to milli‐scale, RTD characteristics exhibit opposing patterns. This can be attributed to the transition from diffusion‐dominated to convection‐dominated on momentum transfer, and the transition interval is 0.167 < <jats:italic>γ</jats:italic> < 0.250. Correlation equations of Pe number with Reynolds (Re) number and <jats:italic>γ</jats:italic> are established under diffusion‐dominated and convection‐dominated states. The symmetrically distributed secondary flow in the helical annular gap effectively elevates the Pe (Pe<jats:sub>max</jats:sub> > 100). Correlation equations of Pe with Re and <jats:italic>γ</jats:italic> are established in helical annular gaps with 0.083 < <jats:italic>γ</jats:italic> < 0.208 and 0.167 < <jats:italic>γ</jats:italic> < 0.500. 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引用次数: 0
摘要
采用直管和螺旋管形式的微米/毫微米级环形反应器由于分子扩散距离短和双壁表面传输,具有出色的传热和传质性能。环形间隙间距可通过调整内外管直径进行扩展。随着流动尺度的扩大,扩散和对流效应对轴向分散的影响需要借助停留时间分布(RTD)曲线和佩克莱特(Pe)数来进一步阐明。利用计算流体动力学研究了 RTD 特性与环形比 γ = Dh/D(环形特性尺寸与外径之比)的相关性。结果表明,随着直环间隙从微米级扩大到毫米级,热电阻特性呈现出相反的模式。这可归因于动量传递从扩散主导型过渡到对流主导型,过渡区间为 0.167 < γ < 0.250。在扩散主导和对流主导状态下,建立了 Pe 值与雷诺(Re)值和 γ 的相关方程。螺旋环形间隙中对称分布的二次流有效地提高了 Pe 值(Pemax > 100)。在 0.083 < γ < 0.208 和 0.167 < γ < 0.500 的螺旋环形间隙中,建立了 Pe 与 Re 和 γ 的相关方程。上述结果有助于了解环流热电阻特性,从而更好地应用管中管反应器。
Effect of annulus ratio on the residence time distribution and Péclet number in micro/milli‐scale reactors
Micro/milli‐scale annular reactor with straight and helical forms has excellent heat and mass transfer performance due to the short molecular diffusion distance and dual‐wall surface transport. The annular gap spacing is scalable by adjusting the inner and outer tube diameter. The influence of diffusion and convection effects on axial dispersion as expanding the flow scale requires further elucidation with the help of residence time distribution (RTD) curves and Péclet (Pe) numbers. The correlation of RTD characteristics with annulus ratio γ = Dh/D (ratio of annulus characteristic size to outer diameter) is investigated using computational fluid dynamics. Results show that with enlarging the straight annular gap from micro‐scale to milli‐scale, RTD characteristics exhibit opposing patterns. This can be attributed to the transition from diffusion‐dominated to convection‐dominated on momentum transfer, and the transition interval is 0.167 < γ < 0.250. Correlation equations of Pe number with Reynolds (Re) number and γ are established under diffusion‐dominated and convection‐dominated states. The symmetrically distributed secondary flow in the helical annular gap effectively elevates the Pe (Pemax > 100). Correlation equations of Pe with Re and γ are established in helical annular gaps with 0.083 < γ < 0.208 and 0.167 < γ < 0.500. The above results contribute to understanding the annular flow RTD characteristics for better applications of tube‐in‐tube reactors.