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基于混合物分数Z和反应进度变量(Y)的二维层流火焰面模型,数值研究了混合物分数标量耗散率、反应进度标量耗散率等对Z-(Y)区域边界以及部分预混火焰结构的影响.结果表明,混合物分数标量耗散率对火焰结构有较大的影响,在混合物分数标量耗散率较小时产生了双火焰的结构;而反应进度标量耗散率对当量混合附近的结果有明显的影响,尤其是当混合物分数标量耗散率较小时;在稳定燃烧情况下,稳态一维火焰面模型只是二维火焰面模型的一个边界,表明二维火焰面模型方程的解给出的化学热力学参数表包含更多的信息,可用于多机制共存的火焰数值模拟. 相似文献
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在非结构网格中,发展有限体积法和Monte Carlo法相结合的混合算法来模拟湍流燃烧,求解相互耦合并且相容的平均密度、动量、能量方程组和脉动速度-标量-频率的联合概率密度函数方程,采用稳态层流火焰面模型计算半详细的化学反应机理.对轴对称钝体火焰驻定器后的扩散燃烧进行模拟,比较了速度和标量的平均量和二阶矩的计算结果和实验数据,并研究了速度的扭率(三阶矩)、扁平因子(四阶矩)及边缘概率密度函数的分布.计算表明,高阶统计矩包含的统计误差比低阶统计矩的大,扭率和扁平系数的峰值则集中在剪切层处. 相似文献
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采用直接数值模拟(DNS)方法,研究了低速机缸内热力学状态下甲烷/正庚烷混合物的着火及燃烧过程,分析了湍流状态下双燃料混合层中的着火特性及火焰发展过程.结果表明:第一阶段着火后,湍流作用下混合气偏浓区域生成冷焰;第二阶段着火后,甲烷/空气预混气侧生成多个高温膨胀核心.混合分数梯度平缓区域更易生成高温核心,而混合分数梯度较大时会增大标量耗散率、加强热量和活性基团的耗散,不利于燃烧反应的稳定发展.湍流作用下火焰前沿形成褶皱向两侧传播,热膨胀核心位置的火焰前沿传播较快.甲烷/空气预混气侧含氧量增加导致火焰前沿传播加快,前沿褶皱程度逐渐降低;正庚烷侧火焰前沿在传播下游存在冷焰反应区域,形成“双火焰”结构,随着反应进行,火焰前沿传播进入更浓的混合物中,双火焰面之间的距离逐渐缩短. 相似文献
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室内火灾区域模拟烟气羽流模型的适用性 总被引:1,自引:0,他引:1
结合不同的烟气羽流模型与门口溢流模型,对室内火灾过程进行建模,利用区域模拟方法计算室内热烟气层厚度及温度随时间的变化情况.利用ISO 9705全尺寸标准火灾实验系统进行实验研究,通过计算结果与实验结果的比较,分析不同羽流模型的适用性.结果表明:Thomas模型与MeCaffrey模型预测的羽流流量值偏大,导致烟气温度计算值比实验值偏低,不适用于大功率火源的情况;Zukoski模型预测的羽流卷吸量偏低,其温度计算值比实验值偏高,适合于小功率火源的情况;Heskestad模型预测的羽流流量值较为稳定,区域模拟结果与实验符合得较好,可用于大功率火灾羽流的预测. 相似文献
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研究了几何对称性处理自由平面湍射流大涡模拟的影响,以Re数为113000的平面不可压缩湍射流流动为例,采用Chorin的分步投影法求解大尺度涡运动的Navier-Stokes方程,小尺度涡采用标准Smagorinsky亚格子模式模拟。初始条件采用平面射流无粘流动解,出流速度边界使用Sommerfeld辐射开边界条件处理,计算域的横向外边界使用自由裹入边界条件,对计算域的横向对称中心平面分别采用对称性条件和直接求解两种方法。模拟结果显示,采用对称性条件处理,会抑制自由平面湍射流中拟序结构的生长,阻碍大尺度涡从中心平面的穿透、长时间的统计平均不能给出合理的湍流低阶矩的时均结果。相反,对中心平面进行直接求解的做法能真实再现自由平面射流中涡的合并与破碎过程,得到合理的模拟结果。 相似文献
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本文在极坐标系下建立了一个模拟溢流反弧水流平均运动特性的数学模型.用Κ—ε紊流模式使基本方程封闭,用控制体积法对计算区域进行离散,最后编制大型计算机通用程序对四种不同反弧半径的紊流流场进行了求解.通过四个算例获得速度分布、边界层厚度、紊动动能变化、紊动能耗散率变化、反弧壁面切应力变化等资料.除紊动资料和反弧壁面切应力资料无实测资料验证外,其余计算均与实验结果吻合良好. 相似文献
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The conditional moment closure method (CMC) has been extended to improve reactive species predictions in flames with significant local extinction and reignition. Simple first-order closure of the conditionally averaged reaction rate term does not give satisfactory results due to large fluctuations around the conditional mean and an alternative closure is suggested here. The new closure is based on a precomputed parameterized reference field that maps reactive species mass fractions as functions of mixture fraction and sensible enthalpy. During the computations, the reference field is continuously adjusted to ensure consistency with the CMC solution and doubly conditioned chemical source terms that are functions of time, space, mixture fraction, and sensible enthalpy can thus be obtained. Integration over sensible enthalpy space yields the improved singly conditioned chemical source term that can be used for the solution of the CMC equations. Full closure can be achieved by assuming a β-PDF for the probability distribution in sensible enthalpy space and an additional conditional variance equation needs to be solved. The overall agreement between the measured and the computed variance is satisfactory and the extended CMC model is applied to Sandia Flames D, E, and F. Excellent predictions of temperature, major species, intermediates, and NO are obtained in Flames D and E while temperature predictions can be significantly improved in Sandia Flame F. 相似文献
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Thomas G. Almeida Farhad A. Jaberi 《International Journal of Heat and Mass Transfer》2008,51(3-4):683-695
The numerical results obtained by large-eddy simulation (LES) of a particle-laden axisymmetric turbulent jet are compared with the available experimental data. The results indicate that with a new stochastic subgrid-scale (SGS) closure, the effects of the particles on the carrier gas and those of the carrier gas on the particles are correctly captured by the LES. Additional numerical experiments are conducted and used to investigate the effects of particle size, mass-loading ratio, and other flow/particle parameters on the statistics of both the carrier gas phase and the particle dispersed phase. 相似文献
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In this study, reaction rate sub-models are investigated in the framework of conditional moment closure (CMC) using the direct numerical simulation (DNS) database of a lifted turbulent H2/N2 flame. The DNS code solves the fully compressible Navier–Stokes equation system. A 9 species and 19-step mechanism for hydrogen combustion is adopted. The comparison of the DNS results and the measurements shows that, in spite of the under predicted lift-off height, the predictions of the conditional means are satisfactory. Two improved models for the conditionally averaged reaction rate are investigated a-priori. The doubly conditioned reaction rate accounts for the fluctuations with two conditioning variables while the second-order closure is based on the Taylor expansion. It is shown that both of the models give promising results. 相似文献
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S. Sreedhara 《Combustion and Flame》2005,143(4):386-401
The performance of second-order conditional moment closure (CMC) depends on models to evaluate conditional variances and covariances of temperature and species mass fractions. In this paper the closure schemes based on the steady laminar flamelet model (SLFM) are validated against direct numerical simulation (DNS) involving extinction and ignition. Scaling is performed to reproduce proper absolute magnitudes, irrespective of the origin of mismatch between local flamelet structures and scalar dissipation rates. DNS based on the pseudospectral method is carried out to study hydrogen-air combustion with a detailed kinetic mechanism, in homogeneous, isotropic, and decaying turbulent media. Lewis numbers are set equal to unity to avoid complication of differential diffusion. The SLFM-based closures for correlations among fluctuations of reaction rate, scalar dissipation rate, and species mass fractions show good comparison with DNS. The variance parameter in lognormal PDF and the constants in the dissipation term have been estimated from DNS results. Comparison is made for the resulting conditional profiles from DNS, first-order CMC, and second-order CMC with correction to the most critical reaction step according to sensitivity analysis. Overall good agreement ensures validity of the SLFM-based closures for modeling conditional variances and covariances in second-order CMC. 相似文献
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The present study is focused on the analysis of non-premixed combustion in high-velocity (supersonic) flows. The computations make use of a large eddy simulation (LES) model, which has been recently introduced to address combustion in high Reynolds number turbulent flows featuring moderate Damköhler values. We expect that the corresponding closure is able to account for the specificities encountered in high Mach number turbulent reactive flows featuring chemical reaction time scales with the same order of magnitude as flow time scales. The model takes finite-rate chemistry and micro-mixing effects into account within the framework of the partially stirred reactor (PaSR) concept, it is hereafter denoted by U-PaSR (unsteady partially stirred reactor). (i) In a first step of the present investigation, the capabilities of the U-PaSR closure hence proposed are evaluated through a detailed comparison performed between numerical results and the data obtained from an experimental study devoted to non-premixed combustion in supersonic co-flowing jets of hydrogen and vitiated air. The simulated test case corresponds to a well-documented experimental database that includes Raman scattering and laser-induced pre-dissociative fluorescence measurements. The comparisons performed between computational results and experimental data establish that the physical processes are well-described by the performed simulation. (ii) In a second step of this study, the flame structure and associated stabilization zone are analysed in the light of numerical simulation results. The post-processing to the computational results indeed confirms the importance of self-ignition processes, as well as the relevance of diagnostic tools recently introduced by Boivin et al. [1,2]. Considering the stabilization zone, it also emphasizes the essential importance of the pressure dynamics associated with the discharge of compressible coflowing jets into the atmosphere – an importance that was not so clearly evidenced from previous numerical simulations conducted on the same experimental benchmark. 相似文献
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The LES–ODT model is implemented for the study of twin turbulent premixed flames in decaying isotropic turbulence. The approach is based on the coupling of large-eddy simulation (LES) for mass and momentum with a fixed 3D lattice of 1D fine-grained solutions based on the one-dimensional turbulence (ODT) model. The ODT solutions for momentum and reactive scalars are designed to capture subgrid scale physics that is not captured by LES. The LES–ODT formulation is capable of capturing important fine-scale processes, such as flame–flame interactions, which play an important role in flame shortening in turbulent premixed flames, and the role of preferential diffusion on curved flames’ structures. 相似文献