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Evaluating Shock-Tube Informed Biases for Shock-Layer Radiative Heating Simulations

机译:评估冲击管通知偏置用于冲击层辐射加热模拟

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A methodology for directly informing flight vehicle radiative heating simulations based on shock-tube measurements is developed. The differences between these shock-tube informed (STI) radiative heating values and the corresponding nominal values are typically the dominant contributor to the radiative heating margin. Previous approaches for evaluating the STI radiation were limited to the stagnation-point radiative flux, assumed optically-thin adjustments to the radiative flux, and were limited to tangent-slab radiation transport. The present approach removes these limitations. This approach relates differences between shock-tube measurements and their nominal simulations to the upper level number density of individual radiative processes. These upper level number density differences are compiled as a function of time behind the shock for all relevant shock tube measurements. By tracing the streamline from a point in a flight vehicle flowfield back to its crossing of the bow shock, the normal shock velocity and flow time since the shock are determined for that single flowfield point. This streamline tracing is repeated for all points in the flowfield computational grid. These normal shock velocities and times since the shock are used to evaluate the previously compiled differences in the upper level number densities of radiating species. These differences are applied during the radiation calculation to obtain the shock-tube informed bias to the radiative heating. Through the streamline mapping, the entire flowfield may be treated, which enables the use of ray-tracing radiative heating simulations and allows off-stagnation point surface regions to be considered. By adjusting the upper level number density prior to the radiative transport evaluation, the impact of optical thickness is captured. This approach may be automated within a flowfield and radiation code to enable routine analyses of the shock-tube informed biases. Examples of this capability are demonstrated for Titan and Earth entry cases.
机译:开发了一种基于冲击管测量的直接通知飞行车辆辐射加热模拟的方法。这些冲击管通知(STI)辐射加热值和相应的标称值之间的差异通常是辐射加热裕度的主要贡献者。以前用于评估STI辐射的方法限于停滞点辐射通量,假设对辐射通量的光学薄调整,并限于切线辐射传输。目前的方法消除了这些限制。该方法将震动管测量和其标称模拟之间的差异涉及各个辐射过程的上层数密度。这些上层数密度差异被编译为对所有相关冲击管测量的冲击后面的时间函数。通过将流线线追溯到飞行车辆流场中的光线回到其弓形冲击的交叉,由于该单流场的冲击以来,正常的冲击速度和流动时间。对于流场计算网格中的所有点重复该流程跟踪。这些正常冲击速度和时间以来用于评估辐射物种的上层数密度的先前编译的差异。在辐射计算期间应用这些差异以获得对辐射加热的冲击管通知偏置。通过流线映射,可以处理整个流场,这使得能够使用射线辐射加热模拟并允许考虑脱落点表面区域。通过在辐射传输评估之前调整上层数密度,捕获光学厚度的影响。该方法可以在流场和辐射码内自动化,以使触控管的常规分析能够通知偏差。对于泰坦和地球入学案件,证明了这种能力的示例。

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