不同膨胀比下气体射流流场结构及脉动频率

Flow field structure and pulsation frequency of air jet under different pressure ratios

  • 摘要: 磨料气体射流的破岩情况决定于磨料加速效果,而气体流场的时空特征是决定磨料分布和加速的最重要因素。又根据膨胀比β(射流压力和环境压力的比值)会影响气体流场空间结构及脉动频率。因此,基于膨胀比β研究了超音速气体射流流场的时空演化规律。为研究气体射流流场时空特征,采用纹影试验获取了不同膨胀比下气体流场的灰度照片,并通过建立灰度值与密度值转换模型,计算了流场密度,得到了流场空间结构。又通过对纹影照片进行时域与频域转换,获取了流场频谱,得到了流场的脉动频率。结果表明:膨胀比β可显著影响超音速气体射流流场的空间结构及脉动强度。当膨胀比β=1时,气体射流处于完全膨胀状态,流场核心段没有明显的波节结构,气流密度变化平缓,脉动频率集中于100 Hz;随着膨胀比β增加至1.12时,超音速气流出现轻微的膨胀-压缩,气流密度沿射流轴线方向变化加剧,流场核心段出现明显波节结构,等速核长度较长,此时,流场脉动强,同时存在多个脉动主频率;继续增加膨胀比β至2时,气流密度沿射流轴线方向交替出现剧增、剧降,等速核长度快速衰减,但此时,流场的脉动受到抑制,脉动频率迅速减小。再继续增加膨胀比β,气体出喷嘴后,密度会迅速衰减为环境密度值,流场振荡性减弱,脉动频率再次稳定于100 Hz。

     

    Abstract: The rock breaking of the abrasive gas jet is determined by the abrasive acceleration effect, and the spatial and temporal characteristics of the air flow field are the most important factors in determining the distribution and acceleration of the abrasive. The pressure ratio β (the ratio of jet pressure to ambient pressure) affects the spatial structure of the air flow field and the pulsation frequency. Therefore, the temporal and spatial evolution of supersonic air jet flow field was studied based on the β. To study the spatial and temporal characteristics of the flow field, the Schlieren experiment was used to obtain the grayscale photos of the air flow field, the flow field density was calculated by establishing the conversion model between the grayscale value and the density value, and then the spatial structure of the flow field was obtained. The pulsation frequency of the flow field was obtained by converting the time domain and frequency domain of the grayscale photos. The results show that the β can significantly affect the spatial structure and pulsation intensity of the flow field. When the β=1, the air jet is in a fully expanded state, and there is no obvious wave node structure in the potential core of the flow field. The flow density changes gently, and the pulsation frequency is concentrated at 100 Hz. As the β increases to 1.12, the supersonic flow appears slight expansion and compression, and the flow density changes more rapidly along the axial direction of the jet. The potential core presents obvious nodal structure, and the length of potential core is longer. Meanwhile, the flow field pulsates strongly and multiple pulsating main frequencies exist simultaneously. When the β continues to increase to 2, the airflow density along the jet axis shows a sharp increase, a sharp drop, the length of potential core decreases rapidly. However, the pulsation of the flow field is suppressed and the pulsation frequency decreases rapidly. With the further increase of β, after the airflow is out of the nozzle, its density will quickly decay to the ambient density value, the flow field oscillatory weakens, the pulsation frequency is again stabilized at 100 Hz.

     

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