首页> 外文会议>Proceedings of the 11th International Conference on Fluidized Bed Technology >BED-TO-WALL HEAT TRANSFER IN A LARGE-SCALE SUPERCRITICAL CFB COMBUSTOR UNDER FLUE GAS RECIRCULATION CONDITIONS
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BED-TO-WALL HEAT TRANSFER IN A LARGE-SCALE SUPERCRITICAL CFB COMBUSTOR UNDER FLUE GAS RECIRCULATION CONDITIONS

机译:烟气再循环条件下大型超临界CFB燃烧器的床间换热

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In the present work the effect of flue gas recirculation on bed-to-wall heat transfer in a large-scale CFB combustor is investigated.A mechanistic model based on a cluster renewal approach is used in this investigation.The heat transfer mechanism in a CFB combustor has been analysed for a dilute phase and a dense phase conditions above the secondary air injection, where membrane wall surfaces and radiant superheaters are located.Experimental heat transfer studies were conducted on a 1296 [t·h-1] supercritical CFB combustor at the high bed pressure (ca.7.7 [kPa]), the ratio of secondary air to primary air SA/PA=0.33 and also under flue gas recirculation rate 6.9% using the bed material of mean size in the range of 219 to 246 [μm] (group B).The fluidizing gas velocity and the solid circulation flux varied in the range of 3.89-4.27 [m·s-1] and 23.7-25.6 [kg·(m2·s-1)], respectively.Furthermore, the bed temperature and the suspension density were regarded as experimental variables along furnace height.The percentage contributions of convection and radiation heat transfer components were estimated.The variation in contributions was depended on the operating conditions i.e.both solid suspension density and bed temperature.During all tests, the average contribution of convection and radiation heat transfer components varied between 29%-45% and 55%-71%, respectively.The results confirmed an increasing trend of the heat transfer coefficient (110-241 [W· (m2·K-1)] with an increase in average suspension density (1.93-1200 [kg·m-3]).
机译:在本工作中,研究了烟气再循环对大型CFB燃烧室中床到壁传热的影响。本研究使用基于簇更新方法的机械模型.CFB的传热机理已经对燃烧器进行了二次空气注入上方稀相和致密相条件的分析,该条件位于膜壁表面和辐射过热器所在的位置。在1296 [t·h-1]超临界CFB燃烧器上进行了实验传热研究。高床压(约7.7 [kPa]),使用平均尺寸为219至246 [μm]的床层材料,二次空气与一次空气之比SA / PA = 0.33,并且在烟气再循环率6.9%的情况下](B组)。流化气体速度和固体循环通量分别在3.89-4.27 [m·s-1]和23.7-25.6 [kg·(m2·s-1)]范围内变化。床温和悬浮液密度被认为是沿着毛皮的实验变量鼻高;估计对流和辐射热传递成分的百分比贡献。贡献的变化取决于操作条件,即固体悬浮液密度和床层温度。在所有测试中,对流和辐射热传递成分的平均贡献均发生变化分别在29%-45%和55%-71%之间。结果证实了传热系数(110-241 [W·(m2·K-1)]随着平均悬浮密度(1.93)的增加而增加的趋势。 -1200 [kg·m-3]。

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