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Numerical schemes for unsteady transonic flow calculation

机译:非定常跨音速流计算的数值方案

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摘要

An obvious reason for studying unsteady flows is the prediction of the effect of unsteady aerodynamic forces on a flight vehicle, since these effects tend to increase the likelihood of aeroelastic instabilities. This is a major concern in aerodynamic design of aircraft that operate in transonic regime, where the flows are characterised by the presence of adjacent regions of subsonic and supersonic flow, usually accompanied by weak shocks. It has been a common expectation that the numerical approach as an alternative to wind tunnel experiments would become more economical as computers became less expensive and more powerful. However even with all the expected future advances in computer technology, the cost of a numerical flutter analysis (computational aeroelasticity) for a transonic flight remains prohibitively high. Hence it is vitally important to develop an efficient, cheape r (in the sense of computational cost) and physically accurate flutter simulation technique which is capable of reproducing the data, which would otherwise be obtained from wind tunnel tests, at least to some acceptable engineering accuracy, and that it is essentially appropriate for industrial applications. This need motivated the present research work on exploring and developing efficient and physically accurate computational techniques for steady, unsteady and time-linearised calculations of transonic flows over an aircraft wing with moving shocks. This dissertation is subdivided into eight chapters, seven appendices and a bibliography listing all the reference materials used in the research work. The research work initially starts with a literature survey in unsteady transonic flow theory and calculations, in which emphasis is placed upon the developments in these areas in the last three decades. Chapter 3 presents the small disturbance theory for potential flows in the subsonic, transonic and supersonic regimes, including the required boundary conditions and shock jump conditions. The flow is assumed irrotational and inviscid, so that the equation of state, continuity equation and Bernoulli's equation formulated in Appendices A and B can be employed to formulate the governing fluid equation in terms of total velocity potential. Furthermore for transonic flow with free-stream Mach number close to unity, we show in Appendix C that the shocks that appear are weak enough to allow us to neglect the flow rotationality. The formulations are based on the main assumption that aerofoil slopes are everywhere small, and the flow quantities are small perturbations about their free-stream values. In Chapter 4, we developed an improved approximate factorisation algorithm that solves the two-dimensional steady subsonic small disturbance equation with nonreflecting far-field boundary conditions. The finite difference formulation for the improved algorithm is presented in Appendix D, with the description of the solver used for solving the system of difference equations described in Appendix E. The calculation of steady and unsteady nonlinear transonic flows over a realistic aerofoil are considered in Chapter 5. Numerical solution methods, based on the finite difference approach, for solving the two-dimensional steady and unsteady, general-frequency transonic small disturbance equations are presented, with the corresponding finite difference formulation described in Appendix F. The theories and solution methods for the time-linearised calculations, in the frequency and time domains, for the problem of unsteady transonic flow over a thin planar wing undergoing harmonic oscillation are presented in Chapters 6 and 7, respectively. The time-linearised calculations include the periodic shock motion via the shock jump correction procedure. This procedure corrects the solution values behind the shock, to accommodate the effect of shock motion, and consequently, the solution method will produce a more accurate time-linearised solution for supercritical flow. Appendix G presents the finite difference formulation of these time-linearised solution methods. The aim is to develop an efficient computational method for calculating oscillatory transonic aerodynamic quantities efficiently for use in flutter analyses of both two- and three-dimensional wings with lifting surfaces. Chapter 8 closes the dissertation with concluding remarks and future prospects on the current research work.
机译:研究非稳态流动的一个明显原因是对非恒定空气动力对飞行器的影响的预测,因为这些影响往往会增加气动弹性不稳定的可能性。这是在跨音速状态下运行的飞机的空气动力学设计中的一个主要问题,在该音速状态下,气流的特征是存在亚音速和超音速流的相邻区域,通常伴随着微弱的冲击。人们普遍希望,随着计算机变得更便宜,功能更强大,作为风洞实验的替代方法的数值方法将变得更加经济。然而,即使计算机技术有望在未来得到发展,跨音速飞行的数值颤动分析(计算气动弹性)的成本仍然过高。因此,开发一种高效,廉价(从计算成本的角度)和物理上精确的颤振仿真技术至关重要,该技术能够再现数据,否则该数据至少可以从风洞测试中获得,至少对于某些可接受的工程而言精度,并且基本上适合工业应用。这种需求激发了当前的研究工作,以探索和开发有效且物理上准确的计算技术,以对具有运动冲击的飞机机翼上的跨音速流动进行稳定,不稳定和时间线性化计算。本文分为八章,七个附录和一个参考书目,列出了研究工作中使用的所有参考资料。这项研究工作首先从关于非稳态跨音速流动理论和计算的文献调查开始,其中重点放在最近三十年来这些领域的发展。第3章介绍了亚音速,跨音速和超音速状态下势流的小扰动理论,包括所需的边界条件和冲击跳跃条件。假定流动是无旋的且无粘性的,因此可以使用附录A和附录B中公式化的状态方程,连续性方程和伯努利方程来以总速度势来公式化控制流体方程。此外,对于自由流马赫数接近于1的跨音速流,我们在附录C中显示,所出现的冲击足够弱,可以忽略流的旋转性。这些公式基于以下主要假设:机翼斜率到处都很小,并且流量对其自由流值的扰动很小。在第4章中,我们开发了一种改进的近似分解算法,该算法解决了具有非反射远场边界条件的二维稳态亚音速小扰动方程。附录D中给​​出了改进算法的有限差分公式,附录E中描述了用于求解差分方程组的求解器的描述。第三章考虑了在真实翼型上的稳态和非稳态非线性跨音速流的计算。 5.提出了一种基于有限差分方法的数值求解方法,用于求解二维稳态和非稳态通用频率跨音速小扰动方程,并在附录F中描述了相应的有限差分公式。第6章和第7章分别介绍了在频域和时域中的时间线性化计算,该问题用于在平面薄机翼上进行谐波振荡的跨音速不稳定流动问题。时间线性化的计算包括通过冲击跳跃校正程序进行的周期性冲击运动。此过程校正了冲击后的求解值,以适应冲击运动的影响,因此,该求解方法将为超临界流生成更准确的时间线性化解。附录G给出了这些时间线性化求解方法的有限差分公式。目的是开发一种有效地计算振动跨音速空气动力学量的有效计算方法,以用于具有升力面的二维和三维机翼的颤振分析。第八章在结语时对当前的研究工作进行了总结和展望。

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