利用 NH3/H2-air 多点火源火焰相互作用对火焰形态和层流火焰评估的影响

Ahmed Yasiry , Jinhua Wang , Hongchao Dai , Xiao Cai , Ahmed A.A. Abdulraheem , Saba Y. Ahmed , Haroun A.K. Shahad , Zuohua Huang
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引用次数: 0

摘要

通过实验研究了使用多点火源的火焰-火焰相互作用和层流火焰演变的详细评估。为了了解火焰的相互作用,对集中点燃的火焰进行了测量和计算,以便与氢-氨/火焰多点火源进行比较。在 0.1 兆帕的初始压力下,外部点火源的位置、延迟时间、氢气混合和混合物当量比都会影响火焰的传播和形态。可以观察到,外部火焰压力波的推进会导致中央火焰前沿发生变形;这种变形甚至发生在火焰相互作用之前。变形可分为水平变形和垂直变形,水平变形是由于阻力使火焰前沿减速,而垂直变形则是由于流场对火焰前沿的推力使火焰前沿加速。同时,垂直变形受到阻力和推力-升力的影响。因此,等效火焰会随着时间的推移而减速。这种效应使膨胀火焰的形状变得不对称,从球形变为椭圆形,再变为三轴准椭圆形火焰(不规则形)。在所有延迟时间和点火源位置下,等效火焰速度和层流燃烧速度都在化学计量附近达到最大。随着化学计量氢氨/空气延迟时间的增加,等效层流火焰速度和层流燃烧速度单调下降,相互作用的时间和位置也单调下降。点火源 1 和点火源 2 的等效火焰速度和层流燃烧速度随延迟时间的增加而减小,这在富裕侧表现得很明显。而采用第三个点火源会随着延迟时间的增加而增加,因为阻力会从水平轴上消除。此外,氢气混合效应会增强并突出这些趋势。
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Flame morphology and laminar flame assessments affected by flames interaction using multi-ignition sources of NH3/H2-air flames

A detailed assessment of flame–flame interaction and laminar flame evolution using multi-ignition sources is experimentally studied. To understand the flame interaction, the centrally ignited flame is measured and calculated for comparison with multi-ignition sources hydrogen–ammonia/flame. The location of the external ignition source, the delay time, the hydrogen blending, and the mixture equivalence ratio at an initial pressure of 0.1 MPa affect the propagation and morphology of the flame. It can be observed that the advancement of the pressure wave of the external flame causes deformation to the central flame front; This deformation occurs even before the interaction of the flames. The deformation can be decomposed into horizontal deformation, which decelerates the flame front as a result of the drag or accelerates due to the thrust of the flow field on the flame front. At the same time, vertical deformation is influenced by drag and thrust-lift forces. Therefore, the equivalent flame decelerates with time. This effect gives a nonsymmetric shape for expanding flame, and the shape changes from spherical to ellipsoidal, then a triaxial quasi-ellipsoid flame (scalene). The equivalent flame speed and laminar burning velocity are maximized near stoichiometry for all delay times and locations of the ignition source. As the delay time of the stoichiometric hydrogen ammonia/air increases, the equivalent laminar flame speed and laminar burning velocity monotonously decrease, as well as the time and location of the interaction. The equivalent flame speed and laminar burning velocity for ignition sources 1 and 2 decreases with delay time, and this becomes evident on the rich side. While employing a third ignition source increases with delay time since the drag force get eliminated from the horizontal axis. Furthermore, the hydrogen blending effect enhances and highlights these tendencies.

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