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1.
粉尘火焰加速现象的实验研究   总被引:4,自引:1,他引:4  
浦以康  胡山 《爆炸与冲击》1995,15(2):97-106
粉尘火焰的发生、加速及由爆燃向爆轰转捩的机理是个至今尚未弄清的问题。需要解决的技术关键之一是在实验室实现弱点火条件下的粉尘火焰加速直至达到爆轰状态。着手发展了一种球形喷粉扬尘装置,令产生的扬尘湍流在水平实验管中形成空间均匀分布和维持秒级悬浮的粉尘云状态。采用以上扬尘装置的水平实验管,在6g黑火药的六点平面点火条件下获得了微细铝粉火焰经5m长的传播过程加速至1000m/s的实验结果。给出了扬尘湍流强度、粉尘粒度与浓度、点火能量及方式等因素对粉尘火焰加速过程中所起作用,及变截面效应(由小变大)对粉尘火焰减速的影响。  相似文献   

2.
大型水平爆轰管中悬浮铝粉爆炸过程的实验研究   总被引:1,自引:0,他引:1  
铝粉的燃烧与爆轰性能是粉尘爆炸领域研究的热点.利用长29.6m,内径199mm,配有40套喷粉扬尘系统的水平爆轰管,在40J电火花点火条件下,实现了悬浮铝粉-空气混和物火焰加速、爆燃、爆轰及其转捩过程,测得了爆炸波传播过程中的压力信号,并且观察到了爆轰波的稳定传播现象.实验结果表明,当铝粉浓度为300 g/m3时,在距离点火端10.15m(长径比L/D=51)处发生了DDT,测得的爆轰波传播过程中管内的最大爆速为1840m/s,最大峰值超压为10.5MPa.铝粉尘爆炸波在爆轰管内的传播过程可分为爆燃段、爆燃转爆轰(DDT)、爆轰增强以及稳态爆轰四个阶段.  相似文献   

3.
刘庆明  范宝春 《实验力学》1997,12(3):376-382
粉尘湍流火焰诱导激波问题是工业灾害研究中的重要课题.本文在自行设计的大型卧式燃烧管内,对铝粉火焰诱导激波现象进行了实验研究,测试了湍流火焰阵面前压缩波到激波的转捩过程,并将实验结果与数值模拟结果进行了比较.  相似文献   

4.
This paper summarizes the studies of DDT and stable detonation waves in dust-air mixtures at the Stosswellenlabor of RWTH Aachen. The DDT process and propagation mechanism for stable heterogeneous dust detonations in air are essentially the same as in the oxygen environment studied previously. The dust DDT process in tubes is composed of a reaction compression stage followed by a reaction shock stage as the pre-detonation process. The transverse waves that couple the shock wave and the chemical energy release are responsible for the propagation of a stable dust-air detonation. However, the transverse wave spacing of dust-air mixtures is much larger. Therefore, DDT and propagation of a stable detonation in most industrial and agricultural, combustible dust-air mixtures require a tube that has a large diameter between 0.1 m and 1 m and a sufficient length-diameter ratio beyond 100, when an appropriately strong initiation energy is used. Two dust detonation tubes, 0.14 m and 0.3 m in diameter, were used for observation of the above-mentioned results in cornstarch, anthraquinone and aluminum dust suspended in air. Smoked-foil technique was also used to measure the cellular structure of dust detonations in the 0.3 m detonation tube. Received 11 February 2000 / Accepted 1 August 2000  相似文献   

5.
障碍物对铝粉火焰加速作用的实验研究   总被引:12,自引:2,他引:12  
在沿火焰传播的通道上重复设置障碍物对粉尘火焰有明显加速作用,这种加速作用的机理可归功于障碍物诱导的湍流区对燃烧过程的正反馈。在封闭容器中,铝粉-空气混合物燃烧达到的最大压力p_(max)与障碍物的存在关系不大,而最大压力上升率(dp/dt)_(max)与障碍物的存在有关。因为p_(max)取决于容器内的总能量,(dp/dt)_(max)则取决于燃烧过程,即能量释放率。  相似文献   

6.
为了揭示煤粉尘爆炸过程中火焰传播特征,采用2种不同质量分数挥发分的煤粉在半封闭竖直燃烧管中进行实验。分别使用高速摄影装置和红外热成像装置记录火焰传播过程和空间的温度分布情况,并分析2种煤粉尘云的火焰传播速度和温度曲线。结果表明:在同等条件下,火焰在挥发分质量分数高的煤粉尘云中的传播速度和火焰温度要高于其在挥发分质量分数较低的煤粉尘云中的。煤粉尘云的体积质量和点火能量也影响着火焰的传播过程,随着煤粉尘云体积质量的增大,火焰的传播速度和火焰温度整体上呈现先增大后减小的趋势,在传播的后半段火焰速度出现震荡现象;随着点火能量的增大,火焰在煤粉尘云中的传播速度和最高温度也相应升高。通过大量的实验数据计算得到特定条件下火焰传播速度和温度的经验公式。  相似文献   

7.
为探索气流特征对水平长管内粉尘爆炸火焰结构的影响, 对采用加压送气传输方式形成的石松子粉尘云经静电引燃后其火焰在水平长管内的传播特性进行实验。利用热线风速仪测量不同气流条件下沿管径方向的速度分布和湍流强度分布, 采用高速摄像系统记录了火焰在水平管道内的传播过程。实验观察到, 即使管内石松子粉尘质量分数相同, 仍然会出现2种不同类型的火焰结构:一种类型火焰轮廓规则、清晰, 火焰中心为连续的黄色发光区并由红色边缘火焰包裹; 另一种类型火焰空间离散, 火焰发光区局部存在, 散乱地呈现不规则状态。详细分析不同气流条件对火焰结构的影响。  相似文献   

8.
Yu.V. Tunik 《Shock Waves》1999,9(3):173-179
In the present paper the direct initiation of a self supporting detonation and propagation of a low-speed combustion in methane-air-coal particles mixtures are solved. For particles, a heterogeneous regime of combustion is used, for methane one overall chemical reaction is taken into account: CH + 2O = CO + 2HO. The heat release rate is assumed to be defined as a delay time based on the well-known thermal theory of Frank-Kamenetsky (1967). The proposed model allows one to investigate the influence inert particles or coal dust on the explosion limits of methane-air mixtures. It is shown that the addition of a limited quantity of particles leads to detonation stability. In low speed combustion problems this method allows one to get a good correlation between theoretical and experimental velocities of steady flame propagation in carbon-hydrogen gaseous mixtures. Coal dust influence on gasdynamics of a methane-air mixture combustion is investigated in an unsteady problem by using of the global modelling. It is shown that limited coal dust concentration increases the flame wave intensity in lean methane-air mixtures in contrast to inert particles. In stoichiometric gas mixtures, sand and coal dusts decrease a flame velocity. Far from the ignition point flame, the velocity is largely defined by the dust mass concentration and not by the size of particles. Received 5 July 1997 / Accepted 13 July 1998  相似文献   

9.
给出了计算粉尘层流火焰速度的直接方法,此法简便易行,在粉尘浓度较低时,计算精度较高。实验结果表明:粉尘浓度对火焰传播速度和燃烧速度有很大的影响,粉尘浓度过大时,粒子运动轨迹就难观测,用直接法计算层流火焰速度的误差增大;管径大小也对燃烧速度有很大影响;小管径中的所得值比大管径中的所得值约低8%。  相似文献   

10.
本文报导了在1米爆炸泄压试验装置内完成的亚麻尘-空气混合物的一百多次试验结果,试验中研究了亚麻尘浓度,泄压面积(比例泄放比)、点火源位置及能量、泄压口封盖物等因素对泄放爆炸压力的影响。在比例泄放比A/V2/3=0.264,亚麻尘浓度0.080kg/m3情况下,爆炸压力测得为15kPa,而亚麻尘浓度为0.700kg/m3情况下,爆炸压力高达33.3kPa,甚至亚麻尘浓度低到0.050kg/m3时,仍能产生火焰传播。这表明如果厂房不采取合适的措施,亚麻尘爆炸可导致厂房倒塌的破坏。  相似文献   

11.
In the present paper, combustion of dust clouds from the discrete point heat source method has been addressed. Time-place temperature profile generated by single particle burning has been obtained to study the dust combustion. The summation of the temperature profiles of burned and burning particles predict the temperature in the preheating zone so that the ignition time of layer in flame front can be determined. Consequently the flame propagating speed was obtained based on the dust concentration corresponding to particles spacing and particle diameter. This method has been validated with aluminum dust cloud combustion. Decrease in the dust concentration leads to the lean limit of dust combustion. Increase in particles diameter or reduction in the dust concentration causes higher lean limit and also reduction in the flame propagating speed. Adding the ignition energy as igniter to this system, provides the path to study the effects of ignition energy in the dust combustion.  相似文献   

12.
The significance of experimental research on flame spectra of methane-coal dust explosions is explained. Weak explosions of methane-coal dust-air mixtures were carried out in a large-scale tube of Ø 200 cm×2900cm with one end open, and the absolute radiation intensities as well as their variation under different conditions for characteristic wavelengths of 0.8875, 1.000, 1.505, 2.801, and 4.346μm were obtained by using small angle of view and a multichannel detector developed by us. The experimental results are discussed and compared with those published abroad. Based on the absolute radiation intensity measured at wavelength 4.346μm and the selected blackbody radiation model, the temperature of explosion flame was determined. The results obtained are not only of great practical importance to the industry but may also be used in the study of flame and chemical kinetics.  相似文献   

13.
C. Wang  Z. Y. Han  M. Situ 《Shock Waves》2006,15(2):129-135
The high-speed combustible gas ignited by a hot gas jet, which is induced by shock focusing, was experimentally investigated. By use of the separation mode of shock tube, the test section of a single shock tube is split into two parts, which provide the high-speed flow of combustible gas and pilot flame of hot gas jet, respectively. In the interface of two parts of test sections the flame of jet was formed and spread to the high-speed combustible gas. Two kinds of the ignitions, 3-D “line-flame ignition” and 2-D “plane-flame ignition”, were investigated. In the condition of 3-D “line-flame ignition” of combustion, thicker hot gas jet than pure air jet, was observed in schlieren photos. In the condition of 2-D “plane-flame ignition” of combustion, the delay time of ignition and the angle of flame front in schlieren photos were measured, from which the velocity of flame propagation in the high-speed combustible gas is estimated in the range of 30–90m/s and the delay time of ignition is estimated in the range of 0.12–0.29ms. PACS 47.40.Nm; 82.40.FpPart of this paper was presented at the 5th International Workshop on Shock/Vortex Interaction, Kaohsiung, October 27–31, 2003.  相似文献   

14.
悬浮RDX炸药和铝颗粒混合粉尘爆轰的数值模拟   总被引:2,自引:0,他引:2  
采用两相流方法对炸药颗粒直径为20.0 m时与铝颗粒混合物的爆轰波的发展与传播过程及爆轰波参数进行了数值计算。结果表明,在炸药粉尘中加入铝颗粒,可以大大提高爆轰波参数。当铝颗粒直径为3.4 m时,尽管铝颗粒的直径较炸药颗粒直径小,但由于炸药颗粒的点火温度低,二者的点火时间相差不多。如果铝颗粒的直径为7.0 m,由于铝颗粒的点火滞后于炸药颗粒的点火,混合颗粒粉尘中可能形成双波阵面的爆轰波。  相似文献   

15.
为研究非金属粉末对管内瓦斯预混火焰传播的影响,选用煤粉和石粉2类煤矿井下常见粉末,采用微细热电偶、火焰传感器测试得出内铺2种粉末管内瓦斯火焰传播的瞬态温度、火焰阵面位置及火焰传播速度等参数,初步分析2种粉末影响瓦斯火焰传播机制的不同。实验表明:(1)煤粉能够加速管内瓦斯火焰的传播,而石粉则抑制管内瓦斯火焰的传播,但两者影响机制有本质不同;(2)内铺煤粉时,火焰温度瞬时值曲线呈现出明显的双峰结构,反应区宽度增加,表明活性煤粉与瓦斯形成了瓦斯 煤粉复合火焰;(3)内铺石粉时,火焰温度值整体下降,温度半峰宽度变窄,说明撒布岩粉法能有效抑制瓦斯煤尘爆炸发生。  相似文献   

16.
Experiments were conducted to investigate the DDT process of the oxyhydrogen gas in the rectangular detonation tube of 3 m long. The repeated obstacle was installed near the ignition plug and the effects of the obstacle on the DDT process were investigated. The behaviour of the combustion and detonation wave were visualized utilizing Imacon high-speed camera with the aid of Schlieren optics. As a result, DDT process was visualized, i.e. (i) multiple shock waves were induced by the expanding combustion wave, because the combustion flame played a role as a piston and compressed the unburned gases. (ii) The acceleration of the combustion wave was occurred and the distance between the shock wave and the combustion flame became shorter. (iii) Eventually, the local explosion was occurred and cause overdriven detonation wave to propagate at the velocity of about 3 kms−1. An abridged version of this paper was presented at the 15th Int. Colloquium on the Dynamics of Explosions and Reactive Systems at Boulder, Colorado, from July 30 to August 4, 1995  相似文献   

17.
球形封闭容器内一个简单的煤粉燃烧爆炸模型   总被引:1,自引:0,他引:1  
徐丰  浦以康 《爆炸与冲击》1998,18(2):112-117
在分析了大量球形封闭容器内煤粉燃烧爆炸实验数据基础上,考虑了煤粉燃烧爆炸机理所涉及的湍流燃烧、相变、各种化学反应动力学过程等复杂因素,并且对球形封闭容器内由于煤粉混合不均匀造成的燃烧不充分给予了考虑,得到了球形封闭容器内煤粉燃烧爆炸特征的数值计算结果,计算的压力-时间曲线与实验结果符合较好。  相似文献   

18.
Experiments were conducted to study flame acceleration in an orifice plate laden detonation tube. Orifice plate area blockage and spacing were varied to determine their affect on flame acceleration. The tube used in the study was 3.05 m long with an inner diameter of 14.0 cm. Experiments were primarily carried out with stoichiometric propane-air, however the affect of mixture reactivity was also investigated by varying the mixture equivalence ratio. The distance required for the flame to achieve a velocity equal to the speed of sound in the unburned gas mixture was measured. This run-up distance is used to characterize the early stage of the flame acceleration process. It was found that in all cases, the flame run-up distance decreased with increased blockage ratio and with increased mixture reactivity. It was found that for higher blockage ratios plates flame acceleration was greatest for a plate spacing of one tube diameter, but for lower blockage ratio plates the results obtained for one-half, one, and one and one-half tube diameter plate spacing were very similar. The most rapid flame acceleration was observed when the ratio of the orifice plate spacing and the orifice plate height (half of the difference between the tube and orifice plate diameter) is on the order of 5. It is proposed that this optimum acceleration corresponds to the condition where the plate spacing is roughly equal to the length of the unburned gas re-circulation zone downstream from the orifice plate. PACS 47.40.-x; 47.70.Fw This paper was based on work that was presented at the 19th Interna-tional Colloquium on the Dynamics of Explosions and Reactive Sys-tems, Hakone, Japan, July 27 - August 1, 2003  相似文献   

19.
球型密闭容器中铝粉爆炸机理的研究   总被引:3,自引:0,他引:3  
对中心点火球型密闭容器中的铝粉爆炸进行了实验和理论两方面的研究。实验采用20立升的球。除测量压力外,还通过系踪平均法测试了流场的湍流强度,并利用电子显微镜和X光衍射仪分析了铝粉及其燃烧后残渣的形状和组分。文中对20立升和50立升球型容器中铝粉燃烧的全过程进行了数值模拟。对于可测量的量如压力和压力上升速率,计算结果与实验结果基本相符。基于反应区外质点的熵几乎不变这一事实,对计算获得的参数剖面还进行了理论分析。  相似文献   

20.
A tailored interface shock tube and an over-tailored interface shock tube were used to measure the thermal energy radiated during diesel-spray combustion of light oil, α-methylnaphthalene and cetane by changing the injection pressure. The ignition delay of methanol and the thermal radiation were also measured. Experiments were performed in a steel shock tube with a 7 m low-pressure section filled with air and a 6 m high-pressure section. Pre-compressed fuel was injected through a throttle nozzle into air behind a reflected shock wave. Monochromatic emissive power and the power emitted across all infrared wavelengths were measured with IR-detectors set along the central axis of the tube. Time-dependent radii where soot particles radiated were also determined, and the results were as follows. For diesel spray combustion with high injection pressures (from 10 to 80 MPa), the thermal radiation energy of light oil per injection increased with injection pressure from 10 to 30 MPa. The energy was about 2% of the heat of combustion of light oil at P inj = about 30 MPa. At injection pressure above 30 MPa the thermal radiation decreased with increasing injection pressure. This profile agreed well with the combustion duration, the flame length, the maximum amount of soot in the flame, the time-integrated soot volume and the time-integrated flame volume. The ignition delay of light oil was observed to decrease monotonically with increasing fuel injection pressure. For diesel spray combustion of methanol, the thermal radiation including that due to the gas phase was 1% of the combustion heat at maximum, and usually lower than 1%. The thermal radiation due to soot was lower than 0.05% of the combustion heat. The ignition delays were larger (about 50%) than those of light oil. However, these differences were within experimental error.
An abridged version of this paper was presented at the 18th Int. Symposium on Shock Waves at Sendai, Japan during July 21 to 26, 1991 and at the 19th Int. Symposium on Shock Waves at Marseille, France during July 26 to 30, 1993.  相似文献   

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