Effect of evaporation chamber structure on flow characteristics and flame development mechanisms of V-gutter flameholder
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摘要:
针对一种蒸发腔V型火焰稳定器,研究了
Ma =0.15~0.35及320 K来流条件下蒸发腔结构参数对V型稳定器流动和火焰发展机理的影响,揭示了蒸发腔V型稳定器的火焰稳定机理,并总结了进气面积和蒸发孔总面积与进气面积比等蒸发腔结构参数对贫油点、熄火性能的影响规律。研究结果表明:点火过程中火焰不稳定造成的熄火与富油熄火相似,是高油量下点火瞬变带来的燃油蒸发积累所致。增加蒸发孔总面积与进气面积比虽然能扩大值班回流区、增强火焰稳定性,但会削弱燃油雾化、降低化学反应速率,导致火焰发展减缓、火焰强度降低。而增加进气面积能同时扩大值班回流区并改善燃油雾化效果,加速火焰发展并促使火焰稳定机制向贫油稳焰机制转变,更有利于提高贫油点、熄火性能。Abstract:The effect of evaporation chamber structure on flow characteristics and flame development mechanisms of a novel evaporating V-gutter flameholder at
Ma =0.15—0.35 and 320 K was studied by numerical simulation and experimental methods, and the flame stabilization mechanisms at lean and rich states were revealed. The effects of the structural parameters of the evaporation chamber, such as the intake area and the ratio of evaporation holes’ area to the intake area, on the performance of lean ignition and blowout were summarized. The results showed that the flame quenching caused by flame instability during ignition was similar to that at rich state, due to the enhanced fuel accumulation caused by ignition transience. Rising the ratio of evaporation holes’ area to the intake area can expand the pilot recirculation zone and enhance the flame stability, but it may weaken the fuel atomization and reduce the chemical reaction rate, resulting in a slower flame development and a lower flame intensity. Increasing the intake area can simultaneously expand the pilot recirculation zone and improve the fuel atomization, thereby accelerating the flame development and promoting the transition towards the flame stabilization mechanism at lean state, making it more conducive to improving the lean ignition and flame-holding performance of the evaporating V-gutter flameholder. -
表 1 V型稳定器蒸发腔结构参数
Table 1. Structural parameters of evaporation chamber for V-gutter flameholder
结构 D/mm r d/mm R D5.3R1.0 5.3 0.01 1.6 1.0 D5.3R1.5 5.3 0.01 2.0 1.5 D5.3R2.0 5.3 0.01 2.3 2.0 D6.0R1.5 6.0 0.015 2.5 1.5 D6.6R1.5 6.6 0.02 2.8 1.5 表 2 测量设备精度
Table 2. Accuracy of the measuring equipments
测量设备 测量误差 热式气体质量流量计 ±1.0%|Qg| 精密压力传感器 ±0.5%|Ps| K型热电偶 ±0.4%|Tt| 椭圆齿轮流量计 ±0.5%|Qf| 表 3 试验工况
Table 3. Experimental conditions
参数 数值 来流温度/K 320 来流马赫数 0.15~0.35 操作压力/kPa 101.0 燃油流量/(g/s) 0.1~12.0 表 4 数值计算边界条件
Table 4. Boundary conditions in the simulation
边界条件 位置 参数 速度进口 空气进口 V=100 m/s;
T=320 K压力出口 出口 pa=101 kPa 壁面 固壁 V=0;$\partial $T/$\partial $n=0 表 5 不同蒸发腔结构的V型稳定器内、外回流区的涡心位置(X, Y)
Table 5. Vortex centers (X, Y) of V-gutter flameholder with different evaporation chambers
结构 值班回流区涡心/mm 主流回流区涡心/mm 上涡 下涡 上涡 下涡 D5.3R1.0 (18.25, 8.35) (18.06, −8.12) (102.13, 12.78) (104.24, −12.41) D5.3R1.5 (18.9, 8.99) (18.05, −8.6) (109.56, 12.36) (104.47, −13.09) D5.3R2.0 (20.01, 10.29) (19.63, −9.84) (118.44, 13.16) (109.54, −14) D6.0R1.5 (18.21, 10.04) (18.71, −10.15) (105.16, 12.81) (105.22, −12.83) D6.6R1.5 (23.06, 11.57) (23.06, −11.48) (126.85, 12.14) (112.68, −13.47) 表 6 蒸发孔下游燃油平均粒径
Table 6. SMDs downstream evaporation-hole
结构 SMD/μm Ma=0.1 Ma=0.2 Ma=0.3 D5.3R1.0 248.69 78.89 45.29 D5.3R1.5 355.84 117.40 66.69 D5.3R2.0 394.34 126.04 77.20 D6.0R1.5 349.00 100.27 28.97 D6.6R1.5 278.07 77.34 29.15 -
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