共查询到18条相似文献,搜索用时 125 毫秒
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为了分析高压补燃液氧煤油发动机氧泵间管内气液两相掺混冷凝及其压力波传播过程,建立了可产生压力扰动的垂直管低温气液两相掺混实验系统,以氧气/液氧为实验工质,开展压力波对垂直管内低温气液两相掺混冷凝的影响研究,获得了不同压力波频率和氧气流量工况下的掺混图像,分析结果表明:压力波会使发散流型由微弱振荡冷凝向间歇振荡冷凝转变,使椭圆流型由稳定冷凝向振荡冷凝转变;在0~52 Hz不同频率压力波作用下,发散流型最大轴向冷凝长度与掺混孔径之比在10~30之间,椭圆流型的比值在8~15之间变化;压力波对气相摆动频率起主导性和正相关性的影响。 相似文献
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为找到煤油贮罐降温后的温度分层原因,通过分析煤油贮罐不同深度的温度,结合管道布置走向,发现煤油降温流动过程中存在上部滞流区,导致煤油贮罐形成上部热煤油和下部冷煤油分层。采用鼓泡与泵回流两种方式进行对比试验,结果表明鼓泡能较好消除煤油贮罐在垂直方向上的温度不均,泵回流方式无明显效果。为准确预估降温后的煤油温度,采用不同调温方式进行多次试验,构建了煤油调温目标温度计算模型,作为煤油降温停止的判断准则。鼓泡方法和调温模型已成功应用于天舟一号发射任务,有效保障了煤油推进剂的温度品质。 相似文献
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在脉冲爆震发动机工作过程中,爆震室压力处于强非定常状态。传统的型面不可调尾喷管与可调尾喷管都无法满足爆震室内压力的高频剧烈变化,进而导致较大的推力损失。为了提升现有脉冲爆震发动机型面不可调增推喷管性能,可以从爆震室中引出爆震燃气,通过无阀自适应控制将该二次流喷射在喷管扩张段,实时调节主流的有效扩张面积比,进而形成流体喷管。针对这种形式的流体喷管,在可爆混合物一定(当量比1.0,初始填充压力为0.1 MPa)的情况下,基于二维数值模拟,研究了不同二次流喷注条件(二次流喷注面积比、位置比)对主流流动状态及发动机推进性能的影响。计算结果表明:二次流的喷注改变了喷管有效流通面积;二次流在喷管扩张段喷注面积比越大,喷管的冲量提升率越大(相对于基准喷管冲量最大提升率为5.25%);二次流喷注位置越靠近喷管喉道处,喷管的冲量提升率越高。 相似文献
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Cylindrical heterogeneous detonation waves 总被引:1,自引:0,他引:1
Further experimental studies of blast wave initiated cylindrical heterogeneous (liquid fuel drops, gas oxidizer) detonation waves are described. A pie-shaped shock tube, used for these studies, was altered in certain ways so as to improve the modeling of cylindrical waves. These modifications, along with some operational aspects, are briefly discussed. The breech of the facility, where the blast wave is generated by an explosive, became distorted with usage. Results are presented which show that lower detonation velocities are realized with the damaged breech (other conditions being the same). A photographic and pressure switch wave time of arrival study was made to ascertain the wave shape. Photographs are shown which show that the waves, blast as well as detonation, are close to cylindrical. However, in some cases there is appreciable distortion of the wave front by debris ahead of the wave. Presumably this debris comes from the blasting cap used to ignite the condensed explosive. A series of experiments was conducted using kerosene drops of 388 μm diameter dispersed in air through use of a large number of hypodermic needles. Radial fuel void regions were established by cutting off the fuel flow to a number of needles. Preliminary results relating to the effect of the size of the cloud gap on detonation velocity, quenching, and the initiator energy levels required for detonation are discussed. 相似文献
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Critical conditions for detonation failure due to tube expansion have been observed in marginal detonations propagating in a
in. (6.35 × 76.2 mm) channel. In these experiments, a well established marginal detonation propagating in the narrow channel entered a test section in which one of the narrow walls was inclined to the central axis at positive angles which ranged from 10° to 45°. Experiments were performed at pressures ranging from 60 to 200 torr (8 to 26.7 kPa) in stoichiometric hydrogen-oxygen mixtures diluted with 20, 50 and 70% argon. Smoke track records obtained on the surface which is the major dimension of the tube, were used to determine failure, incipient failure or self-sustenance of the entering wave.Because of the narrow tube used in the studies the incident waves were marginal in that their velocity was below the expected CJ (Chapman-Jouguet) value, their transverse wave spacing was larger than one would see in a large tube, and the transverse waves were of greater strength than in an ordinary detonation. All of these indicators of marginal behavior became progressively more pronounced as the pressure dropped from 200 torr (26.7 kPa) to the limit pressure of approximately 58 torr (7.73 kPa).The most interesting result of this experimental investigation is that the theoretical analyses predicted that simple one-dimensional opening of the tube should not show a pressure dependence to failure, while the experiments showed a definite decrease in the opening angle required for failure as initial pressure decreased. This behavior is related to the marginality of the incident waves, which is observed to increase smoothly with decreased pressure. It is postulated that detonation failure in the hydrogen-oxygen system occurs when the shock velocity at the end of the cell drops to about 0.60 of the CJ value due either to marginal behavior or to an expansion of the cross section of the tube. 相似文献
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Two-phase flow effect on hybrid rocket combustion 总被引:1,自引:0,他引:1
This study numerically explores the aerodynamic and combustion processes in a hybrid rocket combustor, under a two-phase turbulent flow environment, considering the evaporation, combustion and drag of droplet and droplet ignition criterion. The predictions of temperature, reaction mode, reactant mass fraction, velocity, oxidizer consumption, fuel regression and droplet number distribution enhance understanding of the two-phase combustion aerodynamics inside the combustor. A parametric study of the inlet spray pattern, including spray cone angle, spray injection velocity and droplet size, is performed to improve the operation of reactant mixing and higher fuel regression rate. Analytical results indicate that both the oxidizer consumption and the fuel regression increase with increasing spray cone angle and spray injection velocity in the practical range of operation. However, for stoichiometric operation, the superior spray cone angle is within 20–60°, and spray injection velocity within 20–40 m/s, under a volume-mean droplet radius of 50 μm. The power dependence of solid-fuel regression on total mass flux is found to decrease with rising of droplet mean size. 相似文献
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In this study a flush wall scramjet combustor is tested in a supersonic incoming air flow with the Mach number of 3 which is generated by an air vitiation heater producing the stagnation temperature of 1505 K. Using liquid kerosene as the fuel, the flame is stabilized by means of a centrally mounted O2 pilot strut after being ignited by a plasma torch. During experimental measurements, the fuel is injected with a constant equivalence ratio of 0.8 according to specified strut/wall injection ratios, i.e., a portion of the fuel amount is injected from the strut while the rest is injected from the wall. The strut and wall injectors are arranged at the same axial position. The combustion performance and wall temperature gradients are evaluated with various fuel feeding ratios between the wall and the strut. Experimental results show, when the equivalence ratio is constant and the axial injection position is fixed, the combustion characteristics vary significantly with the strut/wall fuel feeding ratio, especially when this ratio is close to its lowest and highest limits. Among the four fuel feeding ratios examined, the strut only injection mode and the average distributed strut/wall injection mode show the best combustion performance. However, the strut/wall injection mode produces a smaller wall temperature gradient compared to the strut only injection mode, which is due to the significant film cooling effect caused by the wall injected liquid kerosene. 相似文献
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This paper briefly describes two attempts to utilize detonative combustion processes to MHD conversion of thermal energy of fuel to electrical energy and bonding of atmospheric nitrogen. For this purpose a continuous impulse detonation chamber with a frequency up to 200 cps was constructed. Using methane-oxygen-nitrogen mixtures the chamber was maintained in stable operation for several hundred hours. Oil was also employed as fuel.Estimates based on experimental data showed that up to 2% of chemical energy of the fuel may be converted into electrical energy. The use of an accelerating nozzle may improve this result.The concentration of nitrogen oxide in combustion products of the detonation wave was higher by 14% than that expected under usual combustion conditions.The advantages of this type of apparatus are: absence of compressors for fuel and oxidant, impulse current generation, low temperatures of chamber walls, and operation over a large range of operating conditions.Problems associated with the effect of the magnetic field on the propagation of the detonation wave are discussed and the possibility of applying the Zeldovich theory to the case of MHD interaction is described. It is shown that the detonation velocity may either increase or decrease depending on the relative orientation of the direction of magnetic field with respect to the detonation wave. 相似文献