Influence of Charge Structure on the Cook-off Temperature Distribution of Solid Rocket Motor
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摘要: 为研究装药结构对固体火箭发动机烤燃特性的影响,以装填HTPE推进剂的固体火箭发动机为研究对象,建立了复合、单孔管形及星孔形3种装药结构的固体发动机烤燃模型。以1和2℃/min的升温速率对小尺寸HTPE推进剂烤燃试样进行烤燃实验,以实验结果为基础,修正了推进剂材料参数。利用Fluent软件对3种装药结构在不同升温速率(β)下的烤燃行为进行了数值模拟。结果表明:装药结构对固体火箭发动机的烤燃响应时间、点火点和快/慢速烤燃的划分都有影响; 星孔形装药会导致点火点出现跳跃性变化的临界升温速率效应,而单孔管形装药不存在此现象。在本研究条件下,包含星孔段的复合装药发动机的临界升温速率为0.2℃/min,星孔形装药发动机的临界升温速率为0.3和0.5℃/min,即当0.3℃/min≤β≤0.5℃/min时点火点发生跳跃变化。Abstract: To investigate the influence of the charge structure on the cook-off characteristics of the solid rocket motor, we established 3 simplified cook-off models with 3 different charge structures, including the composite, the mono tube and the star tube, for the solid rocket motor with HTPE propellant.We conducted a cook-off test of small-size cook-off samples with HTPE propellant at the heating rate of 1℃/min and 2℃/min, and based on this experiment result, we adjusted the parameters of propellant material.By using the FLUENT software, we conducted the numerical simulation of the models' cook-off behaviors with 3 different charge structures at different heating rates (β).The results show that the charge structure has influence on the cook-off response time, the ignition point and the fast or slow cook-off division.The star tube charge leads to a critical heating rate effect, i.e. the jumping change of the ignition point, whereas the mono tube charge does not.Under the condition of this study, the critical heating rate of the composite charge motor with a star tube section is 0.2℃/min, and the critical heating rate of the star tube charge motor is 0.3 and 0.5℃/min, that is, when 0.3℃/min≤β≤0.5℃/min the ignition point jump changes.
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Key words:
- solid rocket motor /
- charge structure /
- HTPE propellant /
- numerical simulation
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表 1 HTPE推进剂烤燃实验结果
Table 1. Experiment result of cook-off of HTPE propellant
β/
(℃/min)tr/
(min)Tr/
(℃)1 139.8 165.0 2 73.3 171.6 表 2 推进剂材料参数
Table 2. Material parameters of HTPE propellant
ρ/
(kg/m3)cV/
(J/(kg·K))λ/
(J/(m·K·s))Q/
(MJ/kg)A/
(s-1)E/
(kJ/mol)R/
(J/(mol·K))1726 840 0.42 6.348 7.25×108 114.261 8.314 表 3 小尺寸试样仿真结果
Table 3. Simulation results of small-size sample
β/(℃/min) tr/(min) Tr/(℃) Temperature of ignition/(℃) δt/(%) 1 141.00 166.00 232.50 0.86 2 72.23 169.46 231.64 1.50 Note:δt is the relative error of response time (tr). 表 4 材料的物性参数
Table 4. Physical parameters of materials
Material ρ/
(kg/m3)cV/
(J/(kg·K))λ/
(J/(m·K·s))Case 7850 480 43 Insulation 870 1670 0.22 Air 1.225 1006.43 0.0242 表 5 不同升温速率下固体火箭发动机烤燃计算结果
Table 5. Results of cook-off of solid rocket motor at different heating rates
β/
(℃/min)Composite Mono tube Star tube tr/(h) Tr/(℃) tr/(h) Tr/(℃) tr/(h) Tr/(℃) 0.055 28.83 120.13 28.77 119.95 29.10 121.00 0.083 19.72 123.62 19.71 123.53 19.85 124.27 0.1 16.75 125.51 16.74 125.45 16.78 125.65 0.5 4.21 151.24 4.23 151.79 4.25 152.45 1.0 2.32 164.27 2.33 164.33 2.36 166.73 1.5 1.64 172.48 1.65 172.50 1.67 175.15 2.0 1.28 178.68 1.29 178.73 1.30 180.83 表 6 不同升温速率下发动机烤燃点火位置
Table 6. Ignition positions of cook-off at different heating rates
β/
(℃/min)Composite Mono tube Star tube l/(mm) r/(mm) l/(mm) r/(mm) l/(mm) r/(mm) 0.055 919.5-936.5 8 214.0-254.0 5 73-95 4.3 0.1 932.0-954.0 8 123.5-135.0 5 69-102 4.3 0.5 12.1-16.3 40 10.0-18.0 41 1290-1315 42.6 1.0 5.0-9.6 47 3.1-11.5 47 5-9 48.8 1.5 2.2-7.2 49 1.1-8.9 49 1-7 50.0 2.0 0-5.7 50 0-8.0 50 0-6 50.7 Note:l is the axial distance to the front face of the propellant grain, r is the radial distance to the internal surface of the propellant grain. -
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