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GAS-PHASE COMBUSTION IN THE FREEBOARD OF A FLUIDIZED BED-FREEBOARD CHARACTERIZATION

机译:在流化床流动床间特征的干燥器中的气相燃烧

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The prediction of propane autoignition in the freeboard of a fluidized bed is complicated by the presence of solids, intermediate products and non-homogeneities (solids, temperature and species gradients) that should be accounted for in a reaction model. However, the simultaneous characterization of these parameters during combustion is very challenging. An experimental study of propane combustion inside the freeboard (I.D. = 0.2 m) of a fluidized bed of sand (d_p = 290 μm) was performed at a low superficial gas velocity (U_g = 0.24 m/s). Propane was injected inside the fluidized bed (T_(Bed) = 650°C) through a downward-facing sparger. Also, solids flux and species volume fractions were measured using a non-isokinetic sampling probe. The results showed an exponential decrease with height of the upward solids flux (G_(SU)) - G_(SU) was zero at 0.17 m above the bed surface, which was taken as the inflection point of the G_(SU) curve. G_(SUo) measurements were significantly higher than the values given by the correlation of Wen et al. (1982). The bed surface (boundary condition) and freeboard were characterized by measuring pressure, solids flux, species volume fractions and temperature at several radial and axial positions. During the experiments, the fluidized bed achieved a pseudo steady-state operation that ensured that the measured temperature profile corresponded to the solids flux and species fractions. Partial propane combustion in the fluidized bed (71%) produced CO and cracking species that were transported in the freeboard. Complete combustion occurred within 0.15 m of the bed surface and the propane induction time in the freeboard (< 0.25 s) was on the same order as the values given by three induction time correlations for homogeneous systems.
机译:通过固体,中间产物和非均匀性(固体,温度和物种梯度)的存在,在流化床的流量化床的干燥器中的预测复杂化,该反应模型应该被占用。然而,在燃烧过程中同时表征这些参数非常具有挑战性。在低浅表气体速度(U_G = 0.24m / s)中进行流化床(D_P =290μm)内的丙烷燃烧的实验研究。通过向下的侧面的喷射器在流化床(T_(床)= 650℃)内注入丙烷。此外,使用非等因内采样探针测量固体通量和物质体积级分。结果表明,随着向上固体通量的高度(G_(SU)) - G_(SU)在床表面上方0.17米处为0.17μm,其作为G_(SU)曲线的拐点为指数降低。 G_(SUO)测量显着高于Wen等人的相关性的值。 (1982)。通过测量压力,固体助焊剂,物种体积分数和在几个径向和轴向位置处的温度的特征表征床面(边界条件)和干床。在实验期间,流化床实现了伪稳态操作,确保测量的温度分布对应于固体通量和物种级分。流化床(71%)中的部分丙烷燃烧产生的CO和裂化物种在干燥器中运输。在床表面0.15米内发生完全燃烧,并且在干舷(<0.25秒)中的丙烷诱导时间与由均匀系统的三个诱导时间相关给出的值相同。

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