{"title":"推进喷管旁路质量喷射推力矢量的三维计算研究","authors":"Muhammad Abdun Nafi, A. Hasan","doi":"10.1063/1.5115900","DOIUrl":null,"url":null,"abstract":"For modern supersonic vehicles, thrust vector control is a conspicuous prerequisite to accomplish high performance aerospace applications. Thrust vector control chiefly falls into a few classifications, for example, mechanical thrust vector control and shock vector control. Shock vector control is outstanding amongst other approaches to achieve this thrust vector control. A bypass mass injection is used to generate shock vectoring in a planar supersonic Convergent-Divergent (CD) propulsion nozzle in this study and a 10×10 square mm bypass channel was used for the injection. This bypass mass injection is kept perpendicular at the diverging section of the studied nozzle. Overexpanded nozzle flow is achieved by carrying out the investigation at Nozzle Pressure Ratio (NPR) of 3.0. The flow conditions and size of the square injection channel ensures the bypass mass flow ratio around 5%. Reynolds-Averaged-Navier-Stokes (RANS) equations with k-ω SST turbulence model have been applied through numerical computations to capture the three-dimensional steady characteristics of the flow field. Results show that the shock structure becomes asymmetric due to the bypass mass injection along with the formation of recirculation zone near the bypass mass injection. Moreover, a considerable thrust vectoring can be achieved due to the asymmetric velocity distribution at the exit plane.For modern supersonic vehicles, thrust vector control is a conspicuous prerequisite to accomplish high performance aerospace applications. Thrust vector control chiefly falls into a few classifications, for example, mechanical thrust vector control and shock vector control. Shock vector control is outstanding amongst other approaches to achieve this thrust vector control. A bypass mass injection is used to generate shock vectoring in a planar supersonic Convergent-Divergent (CD) propulsion nozzle in this study and a 10×10 square mm bypass channel was used for the injection. This bypass mass injection is kept perpendicular at the diverging section of the studied nozzle. Overexpanded nozzle flow is achieved by carrying out the investigation at Nozzle Pressure Ratio (NPR) of 3.0. The flow conditions and size of the square injection channel ensures the bypass mass flow ratio around 5%. Reynolds-Averaged-Navier-Stokes (RANS) equations with k-ω SST turbulence model have been applied through numerical computatio...","PeriodicalId":423885,"journal":{"name":"8TH BSME INTERNATIONAL CONFERENCE ON THERMAL ENGINEERING","volume":"23 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2019-07-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":"{\"title\":\"3D computational study of thrust vectoring using bypass mass injection in a propulsion nozzle\",\"authors\":\"Muhammad Abdun Nafi, A. Hasan\",\"doi\":\"10.1063/1.5115900\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"For modern supersonic vehicles, thrust vector control is a conspicuous prerequisite to accomplish high performance aerospace applications. Thrust vector control chiefly falls into a few classifications, for example, mechanical thrust vector control and shock vector control. Shock vector control is outstanding amongst other approaches to achieve this thrust vector control. A bypass mass injection is used to generate shock vectoring in a planar supersonic Convergent-Divergent (CD) propulsion nozzle in this study and a 10×10 square mm bypass channel was used for the injection. This bypass mass injection is kept perpendicular at the diverging section of the studied nozzle. Overexpanded nozzle flow is achieved by carrying out the investigation at Nozzle Pressure Ratio (NPR) of 3.0. The flow conditions and size of the square injection channel ensures the bypass mass flow ratio around 5%. Reynolds-Averaged-Navier-Stokes (RANS) equations with k-ω SST turbulence model have been applied through numerical computations to capture the three-dimensional steady characteristics of the flow field. Results show that the shock structure becomes asymmetric due to the bypass mass injection along with the formation of recirculation zone near the bypass mass injection. Moreover, a considerable thrust vectoring can be achieved due to the asymmetric velocity distribution at the exit plane.For modern supersonic vehicles, thrust vector control is a conspicuous prerequisite to accomplish high performance aerospace applications. Thrust vector control chiefly falls into a few classifications, for example, mechanical thrust vector control and shock vector control. Shock vector control is outstanding amongst other approaches to achieve this thrust vector control. A bypass mass injection is used to generate shock vectoring in a planar supersonic Convergent-Divergent (CD) propulsion nozzle in this study and a 10×10 square mm bypass channel was used for the injection. This bypass mass injection is kept perpendicular at the diverging section of the studied nozzle. Overexpanded nozzle flow is achieved by carrying out the investigation at Nozzle Pressure Ratio (NPR) of 3.0. The flow conditions and size of the square injection channel ensures the bypass mass flow ratio around 5%. Reynolds-Averaged-Navier-Stokes (RANS) equations with k-ω SST turbulence model have been applied through numerical computatio...\",\"PeriodicalId\":423885,\"journal\":{\"name\":\"8TH BSME INTERNATIONAL CONFERENCE ON THERMAL ENGINEERING\",\"volume\":\"23 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2019-07-18\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"2\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"8TH BSME INTERNATIONAL CONFERENCE ON THERMAL ENGINEERING\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1063/1.5115900\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"8TH BSME INTERNATIONAL CONFERENCE ON THERMAL ENGINEERING","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1063/1.5115900","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 2
摘要
对于现代超声速飞行器来说,推力矢量控制是实现高性能航天应用的重要前提。推力矢量控制主要分为机械推力矢量控制和冲击矢量控制。在实现推力矢量控制的其他方法中,冲击矢量控制是突出的。在平面超声速会聚发散推进喷管中,采用旁通质量喷射来产生激波矢量,并采用10×10平方mm的旁通通道进行喷射。在所研究的喷管的发散部分保持这种旁路质量注入的垂直。在喷嘴压力比(NPR)为3.0时,研究了喷嘴过膨胀流动。方形注射通道的流动条件和尺寸保证了旁通质量流量比在5%左右。采用k-ω海温湍流模型的reynolds - average - navier - stokes (RANS)方程,通过数值计算捕捉了流场的三维稳态特征。结果表明:由于旁通质量注入,激波结构变得不对称,并在旁通质量注入附近形成再循环区;此外,由于出口平面的速度分布不对称,可以实现相当大的推力矢量。对于现代超声速飞行器来说,推力矢量控制是实现高性能航天应用的重要前提。推力矢量控制主要分为机械推力矢量控制和冲击矢量控制。在实现推力矢量控制的其他方法中,冲击矢量控制是突出的。在平面超声速会聚发散推进喷管中,采用旁通质量喷射来产生激波矢量,并采用10×10平方mm的旁通通道进行喷射。在所研究的喷管的发散部分保持这种旁路质量注入的垂直。在喷嘴压力比(NPR)为3.0时,研究了喷嘴过膨胀流动。方形注射通道的流动条件和尺寸保证了旁通质量流量比在5%左右。本文通过数值计算应用了具有k-ω海温湍流模型的reynolds - average - navier - stokes (RANS)方程。
3D computational study of thrust vectoring using bypass mass injection in a propulsion nozzle
For modern supersonic vehicles, thrust vector control is a conspicuous prerequisite to accomplish high performance aerospace applications. Thrust vector control chiefly falls into a few classifications, for example, mechanical thrust vector control and shock vector control. Shock vector control is outstanding amongst other approaches to achieve this thrust vector control. A bypass mass injection is used to generate shock vectoring in a planar supersonic Convergent-Divergent (CD) propulsion nozzle in this study and a 10×10 square mm bypass channel was used for the injection. This bypass mass injection is kept perpendicular at the diverging section of the studied nozzle. Overexpanded nozzle flow is achieved by carrying out the investigation at Nozzle Pressure Ratio (NPR) of 3.0. The flow conditions and size of the square injection channel ensures the bypass mass flow ratio around 5%. Reynolds-Averaged-Navier-Stokes (RANS) equations with k-ω SST turbulence model have been applied through numerical computations to capture the three-dimensional steady characteristics of the flow field. Results show that the shock structure becomes asymmetric due to the bypass mass injection along with the formation of recirculation zone near the bypass mass injection. Moreover, a considerable thrust vectoring can be achieved due to the asymmetric velocity distribution at the exit plane.For modern supersonic vehicles, thrust vector control is a conspicuous prerequisite to accomplish high performance aerospace applications. Thrust vector control chiefly falls into a few classifications, for example, mechanical thrust vector control and shock vector control. Shock vector control is outstanding amongst other approaches to achieve this thrust vector control. A bypass mass injection is used to generate shock vectoring in a planar supersonic Convergent-Divergent (CD) propulsion nozzle in this study and a 10×10 square mm bypass channel was used for the injection. This bypass mass injection is kept perpendicular at the diverging section of the studied nozzle. Overexpanded nozzle flow is achieved by carrying out the investigation at Nozzle Pressure Ratio (NPR) of 3.0. The flow conditions and size of the square injection channel ensures the bypass mass flow ratio around 5%. Reynolds-Averaged-Navier-Stokes (RANS) equations with k-ω SST turbulence model have been applied through numerical computatio...