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    660 MW对冲燃烧和切圆燃烧塔式锅炉热偏差及壁面气氛对比研究

    Comparative study on the thermal deviation and near-wall environment of 660 MW opposed combustion and tangential combustion tower boilers

    • 摘要: 超临界锅炉的整体布置形式主要为Π型和塔式,由于Π型锅炉存在烟气转向、后烟道易于积灰、受热面蒸汽压力损失较高的问题,塔式炉逐渐得到发展。目前,塔式锅炉通常采用切圆燃烧方式,而对冲燃烧具有相对稳燃、结渣易于控制、上升气流更加均匀的特点。为详细研究对冲塔式锅炉与切圆塔式锅炉的炉内特性,采用数值计算方法对某660 MW超超临界一次再热对冲塔式锅炉和某660 MW超超临界二次再热切圆塔式锅炉进行研究,对比塔式锅炉不同燃烧方式下的炉内特性。结果表明:2种锅炉炉内CO与O2沿炉膛高度方向的整体分布趋势相同,主燃区生成大量的NO,燃尽区NO浓度下降;切圆锅炉受热面区域烟温偏差明显,过热器区域切圆锅炉烟温不均匀系数明显大于对冲锅炉,最大达到1.456,高温再热器区域切圆锅炉烟温不均匀系数小于对冲锅炉;过热器与高温再热器区域2种锅炉速度不均匀系数逐渐增加,并且切圆锅炉速度不均匀系数始终大于对冲锅炉;过热器与高温再热器区域切圆锅炉受热面热负荷不均匀系数始终大于对冲锅炉;对冲锅炉与切圆锅炉侧墙高温腐蚀比例分别为36.59%和85.04%;对冲锅炉与切圆锅炉水冷壁最大热负荷偏差系数分别为2.64及2.02。对冲塔式锅炉和切圆塔式锅炉在烟温分布均匀性、减小侧墙高温腐蚀和水冷壁热负荷均匀性等方面各有优势,对冲塔式锅炉在受热面区域烟温偏差较小,侧墙高温腐蚀比例较小,而切圆塔式锅炉水冷壁热负荷偏差较小。

       

      Abstract: The overall layout of supercritical boilers is primarily divided into Π-type and tower-type configurations. Due to issues such as flue gas turning, easy ash deposition in the rear flue, and higher steam pressure losses in the heating surface of Π-type boilers, tower-type boilers have gradually been developed. Currently, tower-type boilers typically adopt the tangential combustion method, while opposed combustion offers advantages such as relatively stable combustion, easier slagging control, and more uniform upward airflow. To thoroughly investigate the within characteristics of opposed firing and tangential firing tower boilers, numerical simulation methods were employed to study a 660 MW ultra-supercritical single-reheat opposed firing tower boiler and a 660 MW ultra-supercritical double-reheat tangential firing tower boiler. The results showed that the overall distribution trends of CO and O2 the furnaces of both boilers were similar. A large amount of NO was generated in the primary combustion zone, while the NO concentration decreased in the burnout zone. In the tangential firing boiler, the flue gas deviation in the heating surface area was significant. The temperature unevenness coefficient in the superheater region of the tangential firing boiler was notably higher than that of the opposed combustion boiler, with a maximum value of 1.456. However, the temperature unevenness coefficient in the high-temperature reheater region was lower than that of the opposed combustion boiler. In the superheater and high-temperature reheater regions, the velocity unevenness coefficient gradually increased for both types of boilers. Moreover, the unevenness index of the tangential firing boiler was always higher than that of the opposed firing boiler. Additionally, in the superheater and high-temperature reheater regions, the heat load unevenness coefficient of the tangential firing boiler was consistently higher than that of the opposed combustion boiler. The high-temperature corrosion ratios on the side walls of the opposed firing boiler and the tangential boiler were 36.59% and 85.04%, respectively. The maximum heat load deviation coefficients of the water wall were 2.64 for the opposed firing boiler and 2.02 for the tangential firing boiler. Opposed firing tower boiler and tangential firing tower boiler each have their own advantages in terms of uniform flue gas temperature distribution, reducing high-temperature corrosion on side walls, and uniform heat load on water walls. Opposed firing tower boiler exhibits smaller flue gas temperature deviations in the heating surface area and a lower proportion of high-temperature corrosion on side walls, while tangential firing tower boiler has smaller heat load deviations on the water walls.

       

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