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Interfacial areas and gas hold-ups in gas-liquid contactors at elevated pressures from 0.1 to 8.0 MPa

机译:在0.1至8.0 MPa的高压下,气液接触器中的界面区域和气体滞留量

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摘要

Interfacial areas and gas hold-ups have been determined at pressures up to 8.0 MPa in a mechanically agitated gas—liquid reactor and a bubble column with a diameter of 81 mm for superficial gas velocites between 1 and 5 and 1 and 10 cm/s, respectively. The interfacial areas have been determined by the chemical method using the model reaction between CO2 and aqueous diethanolamine (DEA). Contrary to earlier reported results on interfacial areas in a mechanically agitated reactor at pressures up to 1.7 MPa, a positive influence of pressure on the interfacial areas has been observed for higher pressures and higher superficial gas velocities. The product of the gas density G and the superficial gas velocity at the orifice υG, or was found to be an important parameter for the manifestation of the pressure effect. For values of GυG, or larger than 200 kg/m2 s the interfacial areas increase with increasing reactor pressure. Below this value of 200 kg/m2 s no influence of pressure could be observed. The gas hold-ups in the bubble column in water as well as in an aqueous solution of DEA with antifoam increase with increasing pressure. This pressure effect on the gas hold-up in bubble columns originates from the formation of smaller bubbles at the gas distributor. The relative increase in the gas hold-ups is smaller in water and also if a porous plate instead of a perforated plate is used as gas distributor. The differences in the magnitude of the pressure effect are caused by differences in the coalescence behaviour of the gas bubbles in both liquids and by differences in the bubble formation process at the two types of gas distributors, respectively. The interfacial areas in the bubble column also increase with increasing pressure. The relative increase in the interfacial areas aP/aatm with increasing pressure may be as large as 200% for a pressure increase from P = 0.15 to 8.0 MPa, depending on the type of gas distribution and the superficial gas velocity used.
机译:在机械搅拌的气液反应器和直径为81 mm的鼓泡塔中,对于1至5至1至10 cm / s的表观气体速度,已经确定了在8.0 MPa压力下的界面面积和气体滞留量,分别。界面面积已通过化学方法使用CO2与二乙醇胺水溶液(DEA)之间的模型反应确定。与先前报道的在压力高达1.7 MPa的机械搅拌反应器中界面区域的结果相反,对于更高的压力和更高的表观气体速度,已经观察到压力对界面区域的积极影响。气体密度G和孔口υG处的表观气体速度的乘积或被发现是压力效应表现的重要参数。对于G?G值或大于200 kg / m2 s,界面面积随反应堆压力的增加而增加。低于此值200 kg / m2 s时,无法观察到压力的影响。随着压力的增加,气泡中的水以及含消泡剂的DEA水溶液中的气体滞留量会增加。这种对气泡塔中气体滞留的压力影响源自气体分配器处较小气泡的形成。在水中,以及如果使用多孔板而不是多孔板作为气体分配器,则气体滞留量的相对增加较小。压力作用大小的差异是由于两种液体中气泡的聚结行为不同以及两种气体分布器上的气泡形成过程不同而引起的。鼓泡塔中的界面面积也随着压力的增加而增加。对于从P = 0.15到8.0 MPa的压力增加,界面面积aP / aatm随压力增加的相对增加可能高达200%,这取决于气体分布的类型和所使用的表观气体速度。

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