发动机短舱泄压过程瞬态仿真

王晨臣; 冯诗愚; 彭孝天; 邓阳; 陈俊

doi:10.13700/j.bh.1001-5965.2019.0081

发动机短舱泄压过程瞬态仿真

doi: 10.13700/j.bh.1001-5965.2019.0081

1.
南京航空航天大学航空学院飞行器环境控制与生命保障工业和信息化部重点实验室, 南京 210016
2.
中国航空发动机集团商用航空发动机有限责任公司, 上海 200241

基金项目:

国家自然科学基金 U1933121

南京航空航天大学研究生创新基地（实验室）开放基金 kfjj20180108

江苏高校优势学科建设工程

详细信息

作者简介:
王晨臣男, 硕士研究生。主要研究方向:飞行器燃油系统

冯诗愚男, 博士, 副教授。主要研究方向:飞行器环境控制和燃油系统

通讯作者:
冯诗愚. E-mail:shiyuf@nuaa.edu.cn

中图分类号: V224⁺.2
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- 被引次数: 0
出版历程
- 收稿日期: 2019-03-04
- 录用日期: 2019-03-29
- 网络出版日期: 2019-11-20

Transient simulation on pressure relief process of engine nacelle

1.
Key Laboratory of Aircraft Environment Control and Life Support of Ministry of Industry and Information Technology, College of Aerospace Engineering, Nanjing University of Aeronautics and Astronautics, Nanjing 210016, China
2.
Commercial Aircraft Engine Co., Ltd., Aero Engine Corporation of China, Shanghai 200241, China

Funds:

National Natural Science Foundation of China U1933121

the Fundamental Research Funds for the Central Universities kfjj20180108

the Priority Academic Program Development of Jiangsu Higher Education Institutions

More Information

Corresponding author: FENG Shiyu. E-mail:shiyuf@nuaa.edu.cn

摘要

摘要:
发动机短舱泄压门的设计会影响到短舱的安全性，泄压是一个动态变化过程，与舱内外压力、外界气流马赫数及泄压门结构有关。基于Modelica语言建立了短舱泄压过程零维瞬态仿真数学模型，并通过计算流体力学（CFD）方法得到不同开启角度下所需泄压门排放质量流量和力矩系数，并将这些系数代入零维瞬态仿真数学模型，得到了短舱泄压过程中舱内压力、泄压门开启角度等关键参数随时间的变化关系，分析了泄压门开启舱内压力阈值及最大开启角度对泄压过程的影响。研究结果显示，降低泄压门开启舱内压力阈值会使泄压过程到达平衡阶段时间减小，但是对平衡阶段舱内压力和往复摆动角度/幅度无影响。适当降低最大开启角度可有效降低泄压平衡阶段往复摆动角度/幅度，而对初始阶段的泄压速率和平衡阶段的短舱内部压力基本无影响，但是随着最大开启角度进一步降低，则会导致泄压速率下降，并使平衡阶段短舱内部压力升高。
- 发动机短舱 /
- 泄压过程 /
- 瞬态模型 /
- 泄压门 /
- 计算流体力学(CFD)
Abstract:
The design of the engine nacelle pressure relief door will affect the safety of the nacelle. The pressure relief is a dynamic process, which is related to the pressure inside and outside the nacelle, the freestream Mach number and the structure of the pressure relief door. Based on the Modelica language, a zero-dimensional transient simulation mathematical model of the nacelle pressure relief process was established, and the pressure relief door (PRD) discharge and moment coefficient under different opening angles were calculated via computational fluid dynamics (CFD). Then those coefficients were substituted into the zero-dimensional transient simulation model, and the variation relationship of key parameters such as the plenum compartment pressure and opening angle of the PRD with time during the pressure relief process is obtained. The influence of the plenum compartment pressure threshold and the maximum opening angle of the PRD on the pressure relief process was analyzed. The study results show that reducing the plenum compartment pressure threshold for PRD opening will reduce the time required for the pressure relief process reaching to the equilibrium stage, but has no effect on the plenum compartment pressure and reciprocating swing angle/amplitude at equilibrium stage; properly reducing the maximum opening angle can effectively reduce the PRD reciprocating swing angle/amplitude in the equilibrium stage, and has no effect on the pressure relief rate in the initial stage and the plenum compartment pressure in the equilibrium stage, but excessive reduction of the maximum opening angle will decrease the pressure relief rate in the initial stage and increase plenum compartment pressure in the equilibrium stage.
- engine nacelle /
- pressure relief process /
- transient model /
- pressure relief door /
- computational fluid dynamics (CFD)

HTML全文

图 1 短舱泄压过程示意图

Figure 1. Schematic diagram of nacelle pressure relief process

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图 2 泄压门外形和结构示意图

Figure 2. Schematic diagram of PRD shape and structure

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图 3 泄压门几何模型

Figure 3. Geometry model of PRD

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图 4 网格划分

Figure 4. Mesh generation

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图 5 计算结果与试验数据对比

Figure 5. Comparison of calculation and test data

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图 6 计算结果与试验数据误差分析

Figure 6. Error analysis of calculation and test data

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图 7 排放质量流量随开启角度和舱内压力的变化

Figure 7. Discharge mass flow rate varies with opening angle and plenum compartment pressure

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图 8 流量系数随开启角度和舱内压力的变化

Figure 8. Discharge coefficient varies with opening angle and plenum compartment pressure

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图 9 力矩随开启角度和舱内压力的变化

Figure 9. Moment varies with opening angle and plenum compartment pressure

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图 10 不同开启阈值下舱内压力变化对比

Figure 10. Comparison of plenum compartment pressure changes under different opening thresholds

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图 11 不同开启阈值下开启角度变化对比

Figure 11. Comparison of opening angle changes under different opening thresholds

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图 12 不同最大开启角度下舱内压力变化对比

Figure 12. Comparison of plenum compartment pressure changes under different maximum opening angles

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图 13 不同最大开启角度下开启角度变化对比

Figure 13. Comparison of PRD opening angle changes under different maximum opening angles

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