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Experimental and Numerical Investigations of Soot Formation in Laminar Coflow Ethylene Flames Burning in O_2/N_2 and O_2/CO_2 Atmospheres at Different O_2 Mole Fractions

机译:O_2分子分数在O_2 / N_2和O_2 / CO_2气氛中层流共流乙烯火焰中烟尘形成的实验和数值研究

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摘要

This paper presents an experimental and numerical study of the distributions of the temperature and soot volume fraction in laminar coflow ethylene diffusion flames burning in O-2/N-2 and O-2/CO2 atmospheres with the O-2 mole fraction varying from 21 to SO% in both atmospheres. The fuel flow rate was maintained constant in all of the experiments and simulations. The two-color flame emission method based on the response spectrum of R and G bands of a three-color charge coupled device camera was applied to measure the temperature and soot volume fraction. Numerical calculations were conducted using the C-2 chemistry model [Appel-Bockhorn-Frenklach (ABF), Appel, J.; Bockhorn, H.; Frenklach, M. Kinetic modeling of soot formation with detailed chemistry and physics: Laminar premixed flames of C-2 hydrocarbons. Combust. Flame 2000, 121 (1-2), 122-136, DOI: 10.1016/S0010-2180(99)00135-2] with formation of polycyclic aromatic hydrocarbons (PAHs) up to pyrene and a soot model incorporating the dimerization of two pyrene molecules as the soot inception step and hydrogen abstraction acetylene addition mechanism and PAH condensation as the surface growth processes. Numerical results are in qualitative agreement with the experimental measurements when the oxidizer stream is air. The numerical model predicts the temperature well but overpredicts the soot volume fraction in oxygen-enriched flames in both O-2/N-2 and O-2/CO2 atmospheres. With the increase of the oxygen mole fraction in the oxidizer stream, the flame becomes brighter and shorter, the peak temperature zone shifts from the flame wing to the upper part, and the peak soot volume fraction moves from the flame wing to the flame center. The soot loading grows rapidly with increasing the oxygen mole fraction in the oxidizer stream. Under the same oxygen mole fraction, the temperature and soot volume fraction in the O-2/N-2 atmosphere are always higher than those in the O-2/CO2 atmosphere as a result of the higher heat capacity of CO, and soot formation suppression by CO,. The chemical effect of CO, may promote 0 and OH, which enhance the oxidation of the critical soot formation species, including H, C2H2, C6H6, and C16H10. The primary pathway for the chemical effect of CO, is its competition for the H radical to form CO and OH, i.e., CO2 + H reversible arrow CO + OH. Soot formation in these flames is affected by two primary reactions: CO2 + H reversible arrow CO + OH and H + O-2 reversible arrow O + OH.
机译:本文提供了在O-2 / N-2和O-2 / CO2气氛中燃烧的层状同流乙烯扩散火焰中温度和烟so体积分数分布的实验和数值研究,其中O-2摩尔分数从21在两个大气中达到SO%。在所有实验和模拟中,燃料流速均保持恒定。应用基于三色电荷耦合器件相机的R和G波段响应光谱的双色火焰发射方法来测量温度和烟灰体积分数。使用C-2化学模型[Appel-Bockhorn-Frenklach(ABF),Appel,J。 Bockhorn,H。 Frenklach,M.具有详细化学和物理原理的烟灰形成动力学模型:C-2碳氢化合物的层流预混火焰。燃烧Flame 2000,121(1-2),122-136,DOI:10.1016 / S0010-2180(99)00135-2],形成直至pyr的多环芳烃(PAHs)和结合了两个pyr的二聚化的烟灰模型分子作为烟灰的起始步骤,氢提取乙炔的加成机理和PAH缩合作为表面生长过程。当氧化剂流是空气时,数值结果与实验测量结果在质量上吻合。数值模型可以很好地预测温度,但是会过度预测O-2 / N-2和O-2 / CO2气氛中富氧火焰中的烟灰体积分数。随着氧化剂流中氧气摩尔分数的增加,火焰变得更亮或更短,峰值温度区从火焰翼移到上部,并且峰值烟灰体积分数从火焰翼移到火焰中心。随着氧化剂流中氧气摩尔分数的增加,烟灰负荷迅速增长。在相同的氧气摩尔分数下,由于CO的较高热容和烟灰的形成,O-2 / N-2气氛中的温度和烟灰体积分数始终高于O-2 / CO2气氛中的温度和烟灰体积分数被CO抑制。 CO的化学作用可能促进0和OH,这会增强关键烟灰形成物质(包括H,C2H2,C6H6和C16H10)的氧化。 CO产生化学作用的主要途径是它与H自由基竞争形成CO和OH,即CO2 + H可逆箭头CO + OH。这些火焰中的烟尘形成受两个主要反应的影响:CO2 + H可逆箭头CO + OH和H + O-2可逆箭头O + OH。

著录项

  • 来源
    《Energy & fuels》 |2018年第5期|6252-6263|共12页
  • 作者单位

    Yangtze Univ, Sch Petr Engn, Wuhan 430100, Hubei, Peoples R China;

    Natl Res Council Canada, Measurement Sci & Stand, 1200 Montreal Rd,Bldg M-9, Ottawa, ON K1A 0R6, Canada;

    Huazhong Univ Sci & Technol, State Key Lab Coal Combust, Wuhan 430074, Hubei, Peoples R China;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

  • 入库时间 2022-08-18 00:39:08

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