真实气体效应下飞行/喷流参数对逆向喷流减阻降热特性的影响

Influence of flight/jet parameters on drag and heat reduction characteristics of opposing jet under real gas effect

  • 摘要: 高速飞行器飞行时会产生大量的气动阻力和气动热,周围气体分子的振动能和电子能激发并发生离解和电离等化学反应,真实气体效应变得不可忽略。逆向喷流技术作为一种新型的飞行器主动热防护方法,已受到学者们的广泛关注,因此有必要对真实气体效应下的逆向喷流减阻降热特性进行深入研究。采用二维可压缩Navier-Stokes方程和热化学非平衡气体模型模拟了钝体在不同飞行条件下喷流系统的流场分布,研究了真实气体效应下飞行/喷流参数对喷流流场结构、钝体气动阻力和气动热的影响。结果表明:飞行马赫数增大,钝体的总阻力和总热流显著增加,飞行马赫数从8增大到12,钝体的总阻力系数提高了29.30%,总热流增大了8.53倍。存在飞行攻角时流场的对称性会受到破坏,在攻角取10°时,迎风面和背风面的壁面压力相差2.57倍,热流甚至相差16.17倍。增大飞行高度会降低来流总压,使来流强度减弱和喷流穿透能力增强,飞行高度从32 km增加到36 km,钝体峰值压力降低了36.34 kPa,峰值热流降低了1.32 MW/m2。增大喷流压比对降低钝体总阻力和总热流具有显著的提升效果,当喷流压比为0.014时,系统展现出最佳的减阻降热效果,总阻力系数和总热流相较于无喷流时分别降低了41.32%和73.55%。喷流温度变化对近壁面温度分布的影响最大,增大喷流温度钝体总阻力系数基本不变,但钝体总热流增大,系统的减阻降热效率降低。

     

    Abstract: High-speed flight of hypersonic vehicles generates significant aerodynamic drag and thermal loads, where the vibrational and electronic energy excitation of surrounding gas molecules, along with chemical reactions such as dissociation and ionization, make the real gas effect non-negligible. The opposing jet technology, as a novel active thermal protection method for vehicles, has attracted considerable research attention. Thus, it is essential to conduct a detailed investigation of the drag and heat reduction capabilities of the opposing jet under real gas effects. This study employs two-dimensional compressible Navier-Stokes equations and a non-equilibrium thermochemical gas model to simulate the flow field of the opposing jet system under various flight conditions. The effects of real gas effects and flight/jet-flow parameters on the flow field structure, aerodynamic drag, and heat of a blunt body are investigated. The results indicate that an increase in flight Mach number significantly raises the total temperature and pressure, with the total drag coefficient increasing by 29.30% and the total heat flux increasing by 8.53 times when the flight Mach number increases from 8 to 12. The presence of a flight angle of attack disrupts the symmetry of the flow field, with a wall pressure difference of 2.57 times and a heat flux difference of up to 16.17 times between the windward and leeward sides at an angle of attack of 10°. Increasing flight altitude decreases the total pressure of the free-flow, resulting in reduced free-flow intensity and enhanced jet-flow penetration capability. As the flight altitude increases from 32 km to 36 km, the maximum pressure of the blunt body decreases by 36.34 kPa, and the maximum heat flux decreases by 1.32 MW/m². Increasing the jet pressure ratio significantly improves the total drag and heat flux. When the jet pressure ratio is 0.014, the system demonstrates optimal drag and heat flux reduction, with the total drag coefficient and heat flux reduced by 41.32% and 73.55%, respectively, compared to no-jet conditions. Changes in jet temperature have a significant impact on the near-wall temperature distribution. While increasing the jet temperature has little effect on the total drag coefficient, the total heat flux increases, reducing the overall drag and heat reduction efficiency of the system.

     

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