中国电机工程学报
中國電機工程學報
중국전궤공정학보
ZHONGGUO DIANJI GONGCHENG XUEBAO
2014年
17期
2802-2807
,共6页
液体乙醇%小尺度燃烧%扩散燃烧%燃烧温度%稳燃极限
液體乙醇%小呎度燃燒%擴散燃燒%燃燒溫度%穩燃極限
액체을순%소척도연소%확산연소%연소온도%은연겁한
liquid ethanol%small-scale combustion%diffusion combustion%combustion temperature%stability limits
对自由射流和受限射流乙醇小尺度扩散火焰的燃烧温度及稳燃特性进行了实验研究。结果表明:火焰在静止空气中燃烧会经历淬熄前火焰、稳燃火焰、振荡前火焰、振荡火焰4个不同的状态。受限空间和自由空间下,火焰峰值温度随雷诺数增大均会经历增大,稳定和减小3个阶段,自由空间下,其温度最高可达1300K。尾部烟气温度随雷诺数先增大后保持稳定,其温度最高可达480K。只有当内径小到一定程度,玻璃管壁温才会随雷诺数有较大增加,其温度最高可达370K。随着受限空间内径的减小,火焰的燃烧上限明显降低,且均比自由空间时的低,而燃烧下限几乎均与自由空间时相同。在本实验范围内,热熄火是淬熄的主要因素,而燃料的不完全燃烧则是火焰由稳定燃烧转变为振荡燃烧的主要因素。
對自由射流和受限射流乙醇小呎度擴散火燄的燃燒溫度及穩燃特性進行瞭實驗研究。結果錶明:火燄在靜止空氣中燃燒會經歷淬熄前火燄、穩燃火燄、振盪前火燄、振盪火燄4箇不同的狀態。受限空間和自由空間下,火燄峰值溫度隨雷諾數增大均會經歷增大,穩定和減小3箇階段,自由空間下,其溫度最高可達1300K。尾部煙氣溫度隨雷諾數先增大後保持穩定,其溫度最高可達480K。隻有噹內徑小到一定程度,玻璃管壁溫纔會隨雷諾數有較大增加,其溫度最高可達370K。隨著受限空間內徑的減小,火燄的燃燒上限明顯降低,且均比自由空間時的低,而燃燒下限幾乎均與自由空間時相同。在本實驗範圍內,熱熄火是淬熄的主要因素,而燃料的不完全燃燒則是火燄由穩定燃燒轉變為振盪燃燒的主要因素。
대자유사류화수한사류을순소척도확산화염적연소온도급은연특성진행료실험연구。결과표명:화염재정지공기중연소회경력쉬식전화염、은연화염、진탕전화염、진탕화염4개불동적상태。수한공간화자유공간하,화염봉치온도수뢰낙수증대균회경력증대,은정화감소3개계단,자유공간하,기온도최고가체1300K。미부연기온도수뢰낙수선증대후보지은정,기온도최고가체480K。지유당내경소도일정정도,파리관벽온재회수뢰낙수유교대증가,기온도최고가체370K。수착수한공간내경적감소,화염적연소상한명현강저,차균비자유공간시적저,이연소하한궤호균여자유공간시상동。재본실험범위내,열식화시쉬식적주요인소,이연료적불완전연소칙시화염유은정연소전변위진탕연소적주요인소。
The experimental studies were carried out on the combustion temperature and stability of small-scale diffusion flames using ethanol as fuel both for free jet flow and confined jet flow. Results show that there are four conditions for the jet flow flames in the quiescent air, namely the quenching flames, stable combustion flames, quasi-oscillatory flames, and oscillatory flames. As Reynolds numbers increase, the flame peak temperatures increase firstly and then will decrease. For the free jet flow, the flame peak temperatures reach 1300K, and the exhaust gas temperatures increase, then keep stable, and may reach the maximum value of 480K. When using the quartz glass tube with a certain small diameter, the wall temperatures increase quickly with the increasing of Reynolds numbers, and may reach the maximum of 370K. The upper combustion limits of confined flow are all less than that of free flow, but the lower combustion limits are very close. As the inner diameters of the quartz glass tubes decrease, the upper combustion limits decrease sharply. In the present parameter ranges, thermal quenching is the main factor for flame quenching, and the main reason causing the transition from stable flames to oscillatory flames is the fuel incomplete combustion.