固體燃料超燃沖壓發(fā)動機(jī)燃燒室工作過程理論與實(shí)驗(yàn)研究
[Abstract]:On the basis of the two-dimensional calculation results of the flow field in a solid fuel scramjet combustor, a quasi-one-dimensional calculation method is simplified and proposed in this paper. The common methods for calculating the burning surface regression rate are coupled into a quasi-one-dimensional equation, which takes into account the variation of the combustor area, friction, mass addition and heating. The burning surface regression rate is the flow field. The internal temperature, pressure, density and chamber diameter are functions of the burning surface regression rate in the flow equation, so that the burning surface regression rate and the internal flow field parameters can be calculated simultaneously. The boundary conditions of the combustor can be used to solve the unsteady flow, combustion and surface regression problems in the solid fuel combustor through the steady calculation at each moment. It provides a simple, fast and flexible numerical method.
Then, based on the characteristics of solid fuel combustor and the basic law of supersonic combustion flow, a basic theory for the design of solid fuel scramjet combustor is proposed. The theory includes that the combustor satisfies the conditions of self-ignition and flame stability, the mass flow rate of fuel and the mass flow rate of air satisfies an appropriate proportion, and the total pressure is reduced. According to the quasi-one-dimensional calculation program, a quasi-one-dimensional design method of combustion chamber is proposed, and the combustion flow in combustion chamber is further simplified as a heating pipe flow with constant cross-section and variable cross-section.
A small direct-connected test rig was designed and manufactured. The core component of the air heater is methane. It has the advantages of rapid start-up, stable operation and less pollutants. The maximum rate of burning surface regression occurs at the joint of the cavity and the equal straight section and the connection of the equal straight section and the expansion section. The back end of the straight section disappears slowly and the expansion section is connected with each other, and the expansion ratio of the expansion section decreases gradually. After the tip angle disappears, the burning surface regression rate decreases along the axis. At different times, the burning surface regression rate at the same position decreases with the working process of the combustor. With the increase of chamber, the Mach number of internal flow field increases gradually during the combustion chamber operation, which leads to the increase of total pressure loss of air flow and the decrease of engine thrust.
The matching problem of air flow parameters at the inlet and inlet outlet of a combustor is studied. Under certain flight conditions, the total pressure at the inlet of the combustor is increased, the total temperature at the inlet of the combustor is increased, the Mach number at the inlet of the combustor is decreased, the burning surface retreat rate is increased, the length of the combustor is reduced, and the specific thrust of the engine is increased. It is found that the total temperature has the greatest influence on the performance of the combustor.The effect of cavity size on the performance of the combustor is discussed.Under certain combustion efficiency conditions,increasing the relative diameter of the cavity outlet and the combustor inlet will increase the Mach number of the flow field in the combustor,increase the total pressure loss,reduce the rate of burning surface retreat and increase the length of the combustor. However, increasing the depth and length of the cavity does not affect the performance of the combustor. Finally, the performance variation of the combustor in the off-design state is studied. With the increase of flight altitude, the specific thrust of the engine increases first and then decreases, and the specific impulse increases slightly at the design point.
【學(xué)位授予單位】:北京理工大學(xué)
【學(xué)位級別】:博士
【學(xué)位授予年份】:2015
【分類號】:V435
【參考文獻(xiàn)】
相關(guān)期刊論文 前10條
1 楊明;孫波;;固體燃料超燃沖壓發(fā)動機(jī)燃燒室的數(shù)值仿真[J];兵工自動化;2012年01期
2 蔡毅;邢巖;胡丹;;敏感性分析綜述[J];北京師范大學(xué)學(xué)報(bào)(自然科學(xué)版);2008年01期
3 曾慧;白菡塵;朱濤;;X-51A超燃沖壓發(fā)動機(jī)及飛行驗(yàn)證計(jì)劃[J];導(dǎo)彈與航天運(yùn)載技術(shù);2010年01期
4 余勇,丁猛,劉衛(wèi)東,王振國;面向超音速燃燒室方案設(shè)計(jì)的一維流場分析模型[J];彈箭與制導(dǎo)學(xué)報(bào);2004年03期
5 解發(fā)瑜,李剛,徐忠昌;高超聲速飛行器概念及發(fā)展動態(tài)[J];飛航導(dǎo)彈;2004年05期
6 陳延輝 ,夏慧;超燃沖壓發(fā)動機(jī)在RJTF試驗(yàn)的推力性能真實(shí)程度[J];飛航導(dǎo)彈;2004年10期
7 陳英碩;葉蕾;蘇鑫鑫;;國外吸氣式高超聲速飛行器發(fā)展現(xiàn)狀[J];飛航導(dǎo)彈;2008年12期
8 楊向明;劉偉凱;陳林泉;鄭凱斌;;固體燃料超燃沖壓發(fā)動機(jī)原理性試驗(yàn)研究[J];固體火箭技術(shù);2012年03期
9 劉偉凱;陳林泉;楊向明;;固體燃料超燃沖壓發(fā)動機(jī)燃燒室摻混燃燒數(shù)值研究[J];固體火箭技術(shù);2012年04期
10 陶歡;魏志軍;武志文;王寧飛;;固體燃料超燃沖壓發(fā)動機(jī)燃燒室流動與摻混過程研究[J];飛航導(dǎo)彈;2012年08期
相關(guān)博士學(xué)位論文 前5條
1 夏強(qiáng);固體燃料沖壓發(fā)動機(jī)工作過程研究[D];南京理工大學(xué);2011年
2 吳先宇;超燃沖壓發(fā)動機(jī)一體化流道設(shè)計(jì)優(yōu)化研究[D];國防科學(xué)技術(shù)大學(xué);2007年
3 金亮;高超聲速飛行器機(jī)體/發(fā)動機(jī)一體化構(gòu)型設(shè)計(jì)與性能研究[D];國防科學(xué)技術(shù)大學(xué);2008年
4 王翼;高超聲速進(jìn)氣道啟動問題研究[D];國防科學(xué)技術(shù)大學(xué);2008年
5 劉凱禮;高超聲速進(jìn)氣道動/穩(wěn)態(tài)攻角特性研究[D];南京航空航天大學(xué);2012年
本文編號:2178720
本文鏈接:http://sikaile.net/kejilunwen/hangkongsky/2178720.html