单只水平浓缩煤粉燃烧器在1MW燃烧试验台上的试验研究

单只水平浓缩煤粉燃烧器在１ＭＷ燃烧试验台上的试验研究孙绍增，吴少华，李争起，杨明新，王新雷，陈力哲，庞丽君，邢春礼，朱彤，孙恩召，秦裕琨（哈尔滨工业大学动力工程系哈尔滨１５０００１）关键词：水平浓淡燃烧，煤粉燃烧器，稳燃，低ＮＯ_ｘ一、引言电力工业对?..     

混煤氮的热解析出特性及燃料NO_x的形成规律

混煤氮的热解析出特性及燃料ＮＯ_ｘ的形成规律邱建荣，马毓义，曾汉才，吕焕尧，喻秋梅（华中理工大学煤燃烧国家重点实验室武汉４３００７４）关键词：混煤，ＮＯ_ｘ，混合比，燃烧。ＥＭＩＳＳＩＯＮＯＦＮＩＴＲＯＧＥＮＣＯＭＰＯＵＮＤＳＡＮＤＮＯ_ｘＦＯＲＭＡＴ?..     

水平浓淡与上下浓淡煤粉燃烧方式气固混合特性的实验研究

本文针对四角切向燃烧锅炉燃用劣质煤时的稳燃及水冷壁高温腐蚀等问题,采用ＰＤＡ测量设备,对水平浓淡及上下浓淡两种煤粉燃烧方式下的气固两相混合规律进行了实验研究。实验表明,与上下浓淡煤粉燃烧方式相比,水平浓淡煤粉燃烧方式的气固两相流动特性使燃烧器在稳燃、低ＮＯｘ排放、防结渣、防高温腐蚀等方面具有优良的性能。     

逆向复式射流预燃室燃烧器

预燃室是一种高效、低ＮＯｘ排放很有发展前途的洁净煤燃烧技术。但是，目前由于其体积过大，使它在实际应用中受到限制。本文叙述的逆向复式射流预燃室燃烧器结构简单、体积小、燃烧效率高、煤种适应性强，可望成为符合洁净煤技术要求的高效、低ＮＯｘ主燃烧器。     

径向浓浓淡旋流煤粉燃烧器直流二次风对气固流动的影响

本文综述了旋流燃烧器直流二次风对燃烧器区单相流动、烟气温度、煤粉燃尽及ＮＯｘ生成的影响,采用三维ＰＤＡ系统对不同直流二次风率下的气固速度分布、颗粒体积流量分布进行了测量,得出了其对气固流动的影响,分析了对燃烧器性能的影响。     

煤粉低尘燃烧器热态试验研究

以液排渣旋风燃烧技术为基础的煤粉低尘燃烧器可在燃烧过程实现捕渣,为工业加热提供含尘浓度低的高温火焰,是工业加热过程实现以煤代油的先进燃烧技术。本论文介绍了新型煤粉低尘燃烧器的热态燃烧试验研究结果,该燃烧器采用端面旋流进风,煤粉和一次风在旋转气流外层送入,分级燃烧等技术。热态试验研究表明,采用上述技术的煤粉低尘燃烧器具有燃烧完全,捕渣率高,NOx排放浓度低等特点。     

粉煤燃烧的新概念——粉气分离

一、前言 近年来,我国在煤粉燃烧技术发展方面取得了丰硕的成果,陆续开发成功了多项煤粉稳定燃烧装置如钝体煤粉燃烧器、大速差同向射流直流式煤粉预燃室和火焰稳定船式直流煤粉燃烧器以及夹心风浓缩燃烧器等。这些新型燃烧器的应用,大大改善了劣质煤的燃烧过程,煤粉燃烧着火提前,火焰稳定性加强,使劣质煤的燃烧利用达到了一个新的水平。     

花瓣燃烧器低负荷运行理论与应用的研究

本文应用贴体坐标结构化网格对复杂曲面的花瓣燃烧器进行了三维(360°)煤粉燃烧的数值模拟.给出了在75%BMCR和55%BMCR工况下花瓣燃烧器的流场和浓度场,重点分析了花瓣燃烧器的稳燃原理和特性.计算结果表明,在花瓣稳燃器的作用下,煤粉气流进入炉内能立即在瓣后的径向回流区内着火燃烧,并在此区域形成稳定的"值班火焰",为整个风粉气流的着火燃烧提供稳定的热量来源.有利于低挥发分煤在广泛负荷范围内的稳定着火和完全燃烧.     

煤粉旋风燃烧过程流场特性研究

煤粉旋风燃烧器可用于工业加热过程,实现以煤代油,本论文根据旋流燃烧流动特点,采用能考虑非均向湍流应力的雷诺应力模型,对煤粉旋风燃烧器内气流流动过程场进行数值模拟计算,流场计算结果表明,燃烧室几何参数对其内部的流动特性有很大的影响。计算结果与流场实验测试相吻合。     

掺杂分子晶体NH_（4－x）D_xNO_3相变中的分形行为──NO_3~－u_1、u_4振动模临界态拉曼峰强的研究

掺杂分子晶体ＮＨ＿（４－ｘ）Ｄ＿ｘＮＯ＿３相变中的分形行为──ＮＯ_３~－ｕ＿１、ｕ＿４振动模临界态拉曼峰强的研究马树国，吴国祯（清华大学物理系北京１０００８４）ＴｈｅＦｒａｃｔａｌＩｎｔｅｒｐｒｅｔａｔｉｏｎｏｆｔｈｅＰｈａｓｅＴｒａｓｉｔｉｏｎｏｆ...     

煤粉燃烧火焰辐射光谱实验研究

针对煤粉燃烧辐射光谱问题,利用光纤光谱仪对煤粉平面火焰炉实验装置煤粉燃烧火焰辐射光谱进行了测量,详细分析了煤粉辐射光谱特征,并基于普朗克辐射传热定律,通过对光谱仪波长响应特性的标定,得到火焰绝对辐射强度随波长的分布情况,进而利用最小二乘法获得火焰温度与辐射率参数,由此提出基于煤粉燃烧火焰辐射光谱测量的火焰参数测量方法。利用该方法对不同燃烧条件下煤粉燃烧参数进行测量,开展了不同燃烧参数下煤粉火焰辐射光谱实验研究,研究结果表明：煤粉燃烧火焰辐射在200～1 100 nm波段具有较强且连续的光谱特征,基于普朗克辐射定律与最小二乘法可实现煤粉燃烧火焰温度与辐射率的测量;煤粉燃烧火焰辐射光谱在590,766,769和779 nm附近可见明显的Na和K等碱金属痕量元素原子光谱发射谱线,并且这些原子谱线的出现与火焰温度有关;随着煤粉浓度的提高,虽然燃烧温度变化不大,但由于火焰辐射率的增加,造成辐射光谱强度的大幅提升。这对锅炉煤粉燃烧优化具有重要参考价值。     

多功能旋流燃烧器的工业性试验研究

秦皇岛热电厂2＃锅炉燃烧不稳定、燃烧效率低等问题主要是由于燃烧器的一次风管道结构不合理造成的。本文采用多功能旋流燃烧器的设计思想对旋流燃烧器进行了技术改造和工业性试验研究。结果表明,改造后的旋流燃烧器其着火点提前,并且仅改造6只主力燃烧器就可以使锅炉在50％负荷时达到不投油而稳定燃烧,排烟温度、飞灰含碳量和NOx排放量明显下降。     

Spectroscopic observations of methane-pulverized coal flames

A premixed laminar flame burner was used to study physical and chemical effects of burning methane and pulverized coal simultaneously. Spectral emissions obtained as a function of height in the flame, for OH, CH, C₂, and CO were used to calculate excited state species number densities. Premixed methane-air flames with a number of equivalence ratios and methane-air-coal dust flames with three equivalence ratios were studied and differences were noted. Spatial temperatures were measured in all flames by means of a thermocouple probe.The introduction of a pulverized coal additive (30mg/min) leads to changes in OH, Ch, C₂, and CO number densities and temperature at various heights, which depend on the stoichiometry of the methane-air flame. Possible chemical and physical mechanisms responsible for these changes are discussed qualitatively. The data pose a severe test for any quantitative model which includes the fluid dynamics, gas-phase chemistry, heterogeneous processes, and radiation transport.     

Soot formation characteristics in a lab-scale turbulent pulverized coal flame with simultaneous planar measurements of laser induced incandescence of soot and Mie scattering of pulverized coal

Soot formation characteristics of a lab-scale pulverized coal flame were investigated by performing carefully controlled laser diagnostics. The spatial distributions of soot volume fraction and the pulverized coal particles were measured simultaneously by laser induced incandescence (LII) and Mie scattering imaging, respectively. In addition, the radial distributions of the soot volume fraction were compared with the OH radical fluorescence, gas temperature and oxygen concentration obtained in our previous studies [1], [2]. The results indicated that the laser pulse fluence used for LII measurement should be carefully controlled to measure the soot volume fraction in pulverized coal flames. To precisely measure the soot volume fraction in pulverized coal flames using LII, it is necessary to adjust the laser pulse fluence so that it is sufficiently high to heat up all the soot particles to the sublimation temperature but also sufficiently low to avoid including a too large of a change in the morphology of the soot particles and the superposition of the LII signal from the pulverized coal particles on that from the soot particles. It was also found that the radial position of the peak LII signal intensity was located between the positions of the peak Mie scattering signal intensity and peak OH radical signal intensity. The region, in which LII signal, OH radical fluorescence and Mie scattering coexisted, expanded with increasing height above the burner port. It was also found that the soot formation in pulverized coal flames was enhanced at locations where the conditions of high temperature, low oxygen concentration and the existence of pulverized coal particles were satisfied simultaneously.     

Spherical turbulent flame propagation of pulverized coal particle clouds in an O2/N2 atmosphere

The present study aims to clarify the effects of turbulence intensity and coal concentration on the spherical turbulent flame propagation of a pulverized coal particle cloud. A unique experimental apparatus was developed in which coal particles can be dispersed homogeneously in a turbulent flow field generated by two fans. Experiments on spherical turbulent flame propagation of pulverized coal particle clouds in a constant volume spherical chamber in various turbulence intensities and coal concentrations were conducted. A common bituminous coal was used in the present study. The flame propagation velocity was obtained from an analysis of flame propagation images taken using a high-speed camera. It was found that the flame propagation velocity increased with increasing flame radius. The flame propagation velocity increases as the turbulence intensity increases. Similar trends were observed in spherical flames using gaseous fuel. The coal concentration has a weak effect on the flame propagation velocity, which is unique to pulverized coal combustions in a turbulent field. These are the first reports of experimental results for the spherical turbulent flame propagation behavior of pulverized coal particle clouds. The results obtained in the present study are obviously different from those of previous pulverized coal combustion studies and any other results of gaseous fuel combustion research.     

Effect of ammonia/oxygen/nitrogen equivalence ratio on spherical turbulent flame propagation of pulverized coal/ammonia co-combustion

Because ammonia is one of the most promising candidates for energy carrier in the future, various applications of ammonia as a fuel are currently considered. One medium for utilizing ammonia is by introducing it to coal-fired boilers. To the best of our knowledge, this paper is the first to report the fundamental mechanism of the flame propagation phenomenon for pulverized coal/ammonia co-combustion. The effects of the equivalence ratio of the ammonia-oxidizer mixture on the flame propagation velocity of pulverized coal/ammonia co-combustion in turbulent fields were clarified by the experiments employing a unique fan-stirred constant volume chamber. The flame propagation velocities of pulverized coal/ammonia co-combustion, pure ammonia combustion, and pure pulverized coal combustion were compared. As expected, the flame propagation velocity of pulverized coal/ammonia was higher than that of the pure pulverized coal combustion for all conditions. However, the comparison of the flame propagation velocities of pulverized coal/ammonia co-combustion and that of the pure ammonia combustion, revealed that whether the flame propagation of the pulverized coal/ammonia was higher than that of the pure ammonia combustion was dependent on the equivalence ratio of the ammonia-oxidizer. This unique feature was explained by a mechanism including three competing effects proposed by the authors. In the ammonia lean condition, the positive effects, which are the strong radiation from the luminous flame and the increment of local equivalence ratio by the addition of volatile matter, are larger than the negative effect, which is the heat absorption by coal particles in preheat zone. In the ammonia rich condition, the effect of an increment of the local equivalence ratio by the addition of volatile matter turns into a negative effect. Consequently, the negative effects overcome the positive effect in the ammonia rich condition resulting in a lower flame propagation velocity of pulverized coal/ammonia co-combustion.