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Effect of jet velocity on LPG to flame stability and flame temperature distribution on Inverse Difusion Flame(IDF)

机译:喷射速度对逆转燃烧火焰稳定性和火焰温度分布的影响 - 逆扩散火焰(IDF)

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Liquid Pretolium Gas(LPG)experimental investigation used to Inverse Diffusion Flame(IDF)burners is presented.The effect of fuel jet velocity on the flame stability and flame temperature distribution of LPG Inverse Diffusion Flame(IDF)was investigated.Fuel jet speed(Vf)= 0.154 m/s and 0.330 m/s was chosen for analysis.Air jet velocity varies from Va = 7.431 m/s to Va = 15.924 m/s for V/= 0.154 m/s and Va = 8.493 m/s up to Va = 21.231 m/s for V/= 0.330 m/s.The results of the observation show that the velocity of the fuel jet affects the ratio of the velocity of the air-fuel jet which will ultimately have a significant effect on the flame.It was found that the stability of LPG IDF flame at Vf = 0.154 m/s occurred at Va = 11.677 m/s,the equivalence ratio(Φ)= 1.99.The stability of LPG IDF flame at Vf = 0.330 m/s occurs at Va = 14.862 m/s with an equivalence ratio(Φ)= 1.56.It was observed that the temperature along the IDF centerline increased when the distance from the burner(Z)exit increased.The nature of this temperature distribution shows that central cold air in the air jet is gradually heated towards the IDF downstream.The highest flame temperature is seen in Z between 90-110 mm.It was found that the length of the flame increased with increasing flow of fuel jets.At a constant fuel jet speed the flame length increases but will return again to a certain fuel-air ratio.At Vf = 0.154 m/s the highest flame height is 111 mm and at Vf = 0.330 m/s the highest flame height is 143 mm.
机译:呈上用于逆扩散火焰(IDF)燃烧器的液体预溶剂(LPG)实验研究。研究了燃料射流对LPG逆扩散火焰(IDF)的火焰稳定性和火焰温度分布的影响.FUEL射流速度(VF )= 0.154 m / s和0.330 m / s进行分析。航空公司从Va = 7.431 m / s变化到Va = 15.924 m / s,用于v / = 0.154 m / s和va = 8.493 m / s对于v / = 0.330 m / s的Va = 21.231 m / s。观察结果表明,燃料射流的速度影响了空气燃料射流的速度与最终对该产生显着影响的速度发现火焰。在VA = 11.677m / s,等效比(φ)= 1.99时发生vf = 0.154m / s的LPG IDF火焰的稳定性。LPG IDF火焰在VF = 0.330 m / s的稳定性在VA = 14.862 m / s的情况下,使用等效比(φ)= 1.56。观察到沿着IDF中心线的温度在燃烧器(Z)出口的距离增加时增加ED。该温度分布的性质表明,空气喷射中的中央冷空气逐渐向下游加热。最高的火焰温度在z之间看到90-110毫米。火焰的长度增加增加燃料喷射的流量。恒定的燃料喷射速度的火焰长度增加,但将再次返回到某个燃料空气比。vf = 0.154 m / s最高火焰高度为111 mm,在vf = 0.330 m / s处。最高的火焰高度为143毫米。

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