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FLICKERING FREQUENCIES OF DIFFUSION FLAMES OBSERVED UNDER VARIOUS GRAVITY FIELDS

机译:在各种重力场下观察扩散火焰的闪烁频率

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Flame tip fluctuations observed in diffusion flames were investigated using thermal boundary layers. Particularly, flickering motion, which meant a periodic flame oscillation with low frequency (ranging from 10 to 20 Hz), was studied under various gravity levels. The artificial gravity level was changed from 1 G to 11 G with a centrifuge, where G was defined by a combined acceleration of the centrifuge and standard gravity. From the experimental results for wide conditions regarding the Reynolds number and gravity levels, it was found that there were two different modes of fluctuation. One was a "tip flickering," in which the top of a flame was merely oscillating or elongating periodically. The other was a "bulk flickering," which was accompanied by a fire plume separated from the top of the main flame. These two types of flickering were characterized by the Froude number coupling with the buoyant force. A relation for the Strouhal number, representing the dimensionless frequency St = 0.056Fr~(-0.41), was obtained for tip flickering in high Froude number conditions and St = 0.29Fr~(-0.50) was obtained for bulk flickering in low Froude number conditions. In schlieren images of thermal boundaries around the flames, it was observed that the thermal boundaries were also fluctuating with the flames, but the fluctuation scales differed between the two flickering modes. It seemed that bulk flickering was caused by a large-scale vortex which was driven by buoyancy, and tip flickering was caused by flame stretch due to the strong shear force around the fuel jet.
机译:使用热边界层研究在扩散火焰中观察到的火焰尖端波动。特别地,在各种重力水平下,研究了具有低频(范围为10至20Hz)的周期性火焰振荡的闪烁运动。用离心机将人工重力水平从1g变为11g,其中G由离心机和标准重力的组合加速来定义。从实验结果对于关于雷诺数和重力水平的广泛条件,发现有两种不同的波动模式。一个是“尖端闪烁”,其中火焰的顶部仅仅是周期性或周期性地振荡或伸长。另一个是“散装闪烁”,伴随着与主要火焰顶部分开的火羽流。这些两种闪烁的特征在于与浮力的浮动数耦合。代表无量纲频率ST = 0.056FR〜(-0.41)的Strouhal数的关系,用于在高弗劳德数局部条件下滴定闪烁,并在低FRoude数中获得ST = 0.29FR〜(-0.50),以便散装闪烁状况。在火焰周围的热边界的Schlieren图像中,观察到热边界也与火焰波动,但是两个闪烁模式之间的波动尺度不同。似乎散装闪烁是由浮力驱动的大规模涡旋引起的,并且由于燃料射流周围的强剪切力而导致火焰拉伸引起的尖端闪烁。

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