大气边界层对运载火箭地面风荷载的影响研究

Thomas G. Ivanco, Donald F. Keller, Jennifer L. Pinkerton
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引用次数: 2

摘要

一项运载火箭地面风载荷项目正在美国宇航局兰利跨音速动力隧道进行。目标是量化关键的空气动力学和结构特性,当发射前暴露在地面风中时,这些特性会影响运载火箭发生大的风致振荡。特别令人感兴趣的是,当一个von Kármán涡街在运载火箭的尾迹中形成时,运载火箭的动态响应导致准周期性升力和阻力。当涡流脱落的频率接近低阻尼结构模式的频率,从而激发共振响应时,载具对这些准周期性力的响应会变得相当大。接近车辆的风可以以随高度和湍流含量变化的速度为特征。变化的速度和湍流含量的组合在这里称为大气边界层。大气边界层对运载火箭风致振荡响应的重要性一直受到质疑,其影响也没有得到很好的理解。虽然世界上有几个设施致力于复制大气边界层,但在风洞中开发这样一个边界层,能够为气动弹性尺度的运载火箭模型产生飞行代表性的雷诺数,直到最近才完成。NASA兰利跨音速动力学隧道能够模拟发射台上运载火箭的飞行代表雷诺数,并且能够独特地复制许多气动弹性测试中典型的流体结构缩放参数。最近的测试工作成功地为跨音速动力隧道中的三个发射场开发了具有代表性的大气边界层,从而可以同时模拟这些发射场的所有已知气动和流固耦合参数。建立了具有代表性的大型运载火箭气动弹性动力学模型进行试验。气动弹性尺度包括匹配几何形状、模态振型、降低频率、阻尼、运行质量比和运行刚度比。模型在均匀光滑气流中进行了测试,然后浸入大气边界层中进行了效果比较。通过测量非定常压力、加速度和基础弯矩获得动态数据。研究发现,不论是在光滑均匀气流中还是在大气边界层中,共振风致振荡响应所产生的峰值动荷载是相似的。这表明共振锁定事件受代表性湍流和/或风廓线的影响最小。另外,在大气边界层中获得的非共振风致振荡响应事件更强。这表明,当暴露于增加的随机激励幅度时,低阻尼结构响应将增加,这与历史比较是一致的。共振响应事件产生的荷载比非共振响应事件产生的荷载强得多。因此,如果测试只是为了确定最坏情况和负载大小,那么平滑均匀流可能是一种适当的测试技术。然而,如果主要关注非共振响应载荷,则需要进行大气边界层模拟。
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Investigation of Atmospheric Boundary-Layer Effects on Launch-Vehicle Ground Wind Loads
A launch vehicle ground-wind-loads program is underway at the NASA Langley Transonic Dynamics Tunnel. The objectives are to quantify key aerodynamic and structural characteristics that impact the occurrence of large wind-induced oscillations of a launch vehicle when exposed to ground winds prior to launch. Of particular interest is the dynamic response of a launch vehicle when a von Kármán vortex street forms in the wake of the vehicle resulting in quasiperiodic lift and drag forces. Vehicle response to these quasiperiodic forces can become quite large when the frequency of vortex shedding nears that of a lowly-damped structural mode thereby exciting a resonant response. Wind approaching the vehicle can be characterized by a varying speed with height and turbulence content. The combination of both the varying speed and turbulence content is referred to herein as the atmospheric boundary-layer. The importance of the atmospheric boundary-layer upon launch vehicle wind-induced oscillation response has long been questioned, and its effects are not well understood. Although there are several facilities around the world dedicated to replicating atmospheric boundary layers, the development of such a boundary layer in a wind tunnel capable of producing flight-representative Reynolds numbers for aeroelastically-scaled launch vehicle models has only recently been accomplished. The NASA Langley Transonic Dynamics Tunnel is capable of simulating flight-representative Reynolds numbers of launch vehicles on the pad and is uniquely capable of replicating many fluid-structure scaling parameters typical of aeroelastic tests. Recent test efforts successfully developed representative atmospheric boundary-layers for three launch sites in the Transonic Dynamics Tunnel, thereby allowing all known aerodynamic and fluid-structure coupling parameters to be simultaneously simulated for those sites. Dynamic aeroelastically-scaled models representative of typical large launch vehicles were constructed for testing. Aeroelastic scaling includes matching geometry, mode shapes, reduced frequencies, damping, running mass ratios, and running stiffness ratios. The models were tested in smooth uniform flow and then immersed in the atmospheric boundary-layer for comparison of these effects. Dynamic data were acquired measuring unsteady pressure, acceleration, and base bending moment. It was discovered that peak dynamic loads resulting from resonant wind-induced oscillation response are similar when acquired in either smooth uniform flow or an atmospheric boundary-layer. This indicates that resonant lock-in events are minimally impacted by representative turbulence and/or wind profile. Alternately, nonresonant wind-induced oscillation response events are stronger when acquired in an atmospheric boundary-layer. This indicates that a lowly-damped structural response will increase when exposed to an increased magnitude of random excitation, which is consistent with historical comparisons. Loads created by the resonant response events were substantially stronger than those from the nonresonant response events. Therefore, if testing is done to simply identify worst-case conditions and load magnitude, then smooth uniform flow is likely an adequate test technique. However, if nonresonant response loads are of primary interest, then atmospheric boundary-layer simulation is required.
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