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Experimental Investigation of the Starting Behavior of a three-dimensional SCRamjet Intake with a Movable Cowl and Exchangeable Cowl Geometry at Different Mach Numbers

机译:不同马赫数可移动风帽和可交换风帽几何形状的三维SCRamjet进气口启动行为的实验研究

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In the current work we focused our research on the intake starting process which is crucial for proper performance of Supersonic Combustion Ramjet engines. To this date there is no generally valid method to accurately predict intake starting for a certain three-dimensional SCRamjet intake configuration. Therefore we conducted starting experiments at Mach 6 and 7 in a blow down wind tunnel on a three dimensional intake model, equipped with a movable cowl and therefore variable internal contraction. Our focus was on the influence of the cowl geometry, the free stream Mach number, the angle of attack and the ratio of total temperature in the free stream to model wall temperature on intake starting. While the influence of total temperature was minor in the temperature ranges considered, the effect of angle of attack was twofold: when the intake was pitched, that the leading edge shock decreased in strength, the intake showed improved starting characteristics. For a pitch angle in the opposite direction and for increasing yaw angles, intake starting was prevented. For a decrease in free stream Mach number from 7 to 6, the starting internal contraction ratio was delayed from 1.92 to 1.73, for the v-shaped lip configuration. Exchanging the v-shaped lip with a straight lip geometry, improved intake starting and at a constant free stream Mach number of 7, the maximum internal contraction for starting moved from 1.92 to 2.12.
机译:在当前的工作中,我们将研究重点放在进气启动过程上,这对于超音速燃烧冲压发动机的正常性能至关重要。迄今为止,还没有一种普遍有效的方法可以准确地预测某些三维SCRamjet进气装置的进气开始时间。因此,我们在三维进气模型上的排风管中以6马赫和7马赫的速度进行了启动实验,该模型配备了可移动的前围,因此内部收缩可变。我们的研究重点是前围几何形状,自由流马赫数,迎角以及自由流中总温度与进气口模型壁温的比值的影响。虽然在所考虑的温度范围内总温度的影响较小,但是迎角的影响却是双重的:当进气口倾斜时,前缘冲击强度降低,进气口的起动特性得到改善。对于相反方向的俯仰角和偏航角增加,防止了进气开始。对于V形唇形,自由流马赫数从7减少到6,起始内部收缩率从1.92延迟到1.73。用笔直的几何形状更换V形唇,改善了进气启动,在恒定的自由流马赫数为7的情况下,启动时的最大内部收缩从1.92变为2.12。

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