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In-duct Removal of Mercury from Coal-Fired Power Plant Flue Gas by Activated Carbon: Assessment of Entrained Flow Versus Wall Surface Contributions

机译:活性炭从火电厂烟道气中去除汞的研究:夹带流量与壁面贡献的评估

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In-duct mercury capture efficiency by activated carbon from coal-combustion flue gas was investigated. To this end, elemental mercury capture experiments were conducted at 100°C in a purposely designed 65-mm ID lab-scale pyrex apparatus operated as an entrained flow reactor. Gas residence times were varied between 0.7 and 2.0 s. Commercial-powdered activated carbon was continuously injected in the reactor and both mercury concentration and carbon elutriation rate were followed at the outlet. Transient mercury concentration profiles at the outlet showed that steady-state conditions were reached in a time interval of 15–20 min, much longer than the gas residence time in the reactor. Results indicate that the influence of the walls is non-negligible in determining the residence time of fine carbon particles in the adsorption zone, because of surface deposition and/or the establishment of a fluid-dynamic boundary layer near the walls. Total mercury capture efficiencies of 20–50% were obtained with carbon injection rates in the range 0.07–0.25 g/min. However, only a fraction of this capture was attributable to free-flowing carbon particles, a significant contribution coming from activated carbon staying near the reactor walls. Entrained bed experiments at lab-scale conditions are probably not properly representative of full-scale conditions, where the influence of wall interactions is lower. Moreover, previously reported entrained flow lab-scale mercury capture data should be reconsidered by taking into account the influence of particle-wall interactions.
机译:研究了活性炭从燃煤烟气中捕获汞的效率。为此,在一个专门设计的65毫米内径实验室规模的耐热玻璃设备中作为夹带流动反应器在100°C下进行了元素汞捕获实验。气体停留时间在0.7至2.0 s之间变化。将工业粉状活性炭连续注入反应器中,并在出口处同时跟踪汞浓度和碳淘析速率。出口处的瞬态汞浓度曲线表明,在15–20分钟的时间间隔内达到了稳态条件,比气体在反应器中的停留时间长得多。结果表明,由于表面沉积和/或在壁附近建立了流体动力学边界层,壁的影响在确定细碳颗粒在吸附区中的停留时间方面不可忽略。在0.07–0.25 g / min范围内的碳注入速率下,汞的总捕集效率为20–50%。然而,这种捕获的一小部分归因于自由流动的碳颗粒,其中很大的贡献来自留在反应器壁附近的活性炭。实验室规模条件下的夹带床实验可能无法恰当地代表全尺寸条件,因为壁相互作用的影响较低。此外,应考虑颗粒物-壁间相互作用的影响,重新考虑先前报道的气流实验室规模的汞捕获数据。

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