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RADIATIVE HEAT TRANSFER THROUGH THE FUEL-RICH CORE OF LABORATORY-SCALE POOL FIRES

机译:通过实验室级池火的富燃料核心进行辐射传热

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Radiative heat transfer calculations are conducted along the axis of six axisymmetric pool fires by using the "exact" line-by-line (LBL) method, the narrow band correlated k (NBCK) model, the full-spectrum correlated k (FSCK) model, the multi-scale full-spectrum k-distribution (MSFSK) model, and the wide-band model implemented in the fire dynamic simulator (FDS). The two baseline cases correspond to 34 kW and 176 kW methane pool fires generated on a burner of 0.38 m diameter. For each heat release rate, two other moderately and heavily sooting pool fires were generated by considering higher soot volume fractions while keeping temperature and gaseous species concentrations unaltered. For each radiative model, the corresponding absorption coefficients for carbon dioxide, water vapor, carbon monoxide, and methane were generated from the same high-resolution spectroscopic databases. Model results show that the contribution of carbon monoxide to the radiative intensity can be neglected, whereas that of methane increases with the heat release rale (HRR) and decreases as the soot loading increases. It is also found that the gray approximation for soot holds for the 34 kW pool fires and the weakly and moderately sooting 176 kW pool fires but ceases to be valid for the heavily sooting 176 kW pool fire. Concerning the accuracy of the different approximate radiative models, comparisons with the LBL solutions show that the NBCK model can be used as a reference if LBL solutions are not available. On the other hand, the FDS wide-band model fails in predicting accurately the radiative intensity through the fuel-rich core of pool fires. Finally, the FSCK provide predictions within 10% of LBL solutions with the exception of the heavily sooting 176 kW pool fire where the strong attenuation of radiation by methane invalidates the "correlated" assumption of the absorption coefficient. In this case, the MSFSK model must be considered, improving substantially the predictions of the FSCK.
机译:通过使用“精确”逐行(LBL)方法,窄带相关k(NBCK)模型,全光谱相关k(FSCK)模型,沿着六个轴对称池火的轴进行辐射传热计算。 ,多尺度全频谱k分布(MSFSK)模型以及在火灾动态模拟器(FDS)中实现的宽带模型。这两个基准案例对应于直径为0.38 m的燃烧器产生的34 kW和176 kW甲烷池火。对于每种放热速率,通过考虑更高的烟灰体积分数,同时保持温度和气态物质浓度不变,又产生了另外两次中度和重度烟灰池火。对于每个辐射模型,二氧化碳,水蒸气,一氧化碳和甲烷的相应吸收系数是从相同的高分辨率光谱数据库中生成的。模型结果表明,可以忽略一氧化碳对辐射强度的影响,而甲烷随放热规则(HRR)的增加而增加,而随着烟灰负荷的增加而减小。还发现,对于34 kW池火和轻度和中度烟尘176 kW池火,烟灰的灰色近似值对严重烟灰的176 kW池火不再有效。关于不同的近似辐射模型的准确性,与LBL解决方案的比较表明,如果没有LBL解决方案,则可以将NBCK模型用作参考。另一方面,FDS宽带模型无法准确预测通过富燃料的池火核心的辐射强度。最后,FSCK提供了在LBL解决方案的10%范围内的预测,除了重度积碳的176 kW池火,其中甲烷的强烈辐射衰减使吸收系数的“相关”假设无效。在这种情况下,必须考虑MSFSK模型,从而大大改善了FSCK的预测。

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