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一种隐式预处理方法及其在定常和非定常流动数值模拟中的应用 总被引:1,自引:0,他引:1
将Choi-Merkle矩阵预处理方法与LU-SGS隐式方法、双时间法以及多重网格方法结合,发展适用于绕飞行器定常和非定常粘性流动的高效隐式预处理计算方法和程序.介绍一种针对定常和非定常流动的LU-SGS隐式预处理方法的统一表述方法.在不改变流动解的前提下,对Navier-Stokes方程的伪时间导数项实施Choi-Merkle矩阵预处理,从而改善可压缩控制方程在低速情况下的系统刚性,使基于LU-SGS时间推进格式的数值模拟方法同时适用于从极低马赫数到可压缩范围内的数值模拟.对Jameson中心格式的人工粘性进行相应的修改,以提高低速流动的计算精度.翼型、机翼以及翼身组合体绕流的数值模拟研究表明,隐式预处理方法获得了很高的计算效率,可使马赫数0.1左右的低速流动计算时间减少50%以上;通过对现有可压缩计算程序进行小量改动,便可使其均匀覆盖整个低速流动范围,提高CFD程序在飞行器绕流数值模拟中的实用性. 相似文献
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以压力为主变量求解喷管内的气体流动 总被引:1,自引:0,他引:1
一、引言 以压力为主变量求解气体流动问题的计算方法,早在七十年代,Hirt就证明是一种可有效地用于全马赫数的流动问题。但是由于一些技术上的困难,以压力为主变量的方法主要限于求解不可压的低速流动问题。本文将作者原有的非正交坐标下的,以压力为主变量求解不可压缩流动问题的计算方法和程序进行了改进。通过在动量方程中采用混合张量的形式而提高了计算的精度和稳定性,并通过在压力修正方程中隐式地引入密度的影响而将计算方法推广到用于求解可压缩流动问题。采用这种方法对两种喷管内的流动进行了计算,并将计算结果与实验结果进行了比较,结果是令人满意的。 相似文献
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本文用有限元法数值分析带二次流可调收—扩喷管跨音速流动,紊流粘性采用k—ε双方程模型来描述,并利用加权余量法中的Galerkin法建立有限元方程,求解可压缩粘性流体流动N-S方程,喷管壁面采用壁面函数。通过四种不同喷管、不同工况下尾喷管内部流场计算,并用实验数据进行对比表明:计算结果合理,程序可靠,可利用有限元法对喷管超音速流动进行数值研究。 相似文献
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本文利用κ-ε湍流模型方法和叶轮进出口测试结果计算离心叶轮内部流动。计算采用了SIMPLEC方法,对压力修正方法进行了适当改进。为适应可压缩流动计算的需要,利用局部摩擦损失建立了压力与密度的联系。文中给出了两个叶轮的计算结果。 相似文献
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可压缩流动离散涡方法 总被引:1,自引:0,他引:1
推导了可压缩流动旋涡动力学基本方程,并分析了其基本性质。如同不可压流动,在可压缩流动中旋涡同样具有场与物质两重特征。得出了可压缩流中的旋涡诱导速度公式,对Biot-Savart方程进行了可压缩修正。基于Lagrangian框架下的粒子方法,求解可压缩流中的胀量项,从而用离散涡模型求解了非定常、不稳定、可压缩流场。数值实验验证了提议的计算方法有效性。并分析了可压缩流动中旋涡运动的特征,与不可压流动的差别。 相似文献
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针对有壁面边界的可压缩流动问题,提出与基于非等距网格的高精度紧致型差分格式相结合的简化隐式迭代时间推进法,建立求解可压缩Navier-Stokes方程的直接数值模拟方法,提高了计算效率.应用该方法,直接数值模拟两种有壁面边界的二维可压缩流动问题,即可压缩平板边界层流动和可压缩槽道流动. 相似文献
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基于预处理HLLEW格式的全速域数值算法 总被引:2,自引:0,他引:2
基于HLLEW(Harten-Lax-Van Leer-Einfeldt-Wada)格式引入预处理技术发展适合求解全速域流场的三维Navier-Stokes求解器.引入低速预处理技术,重新构造HLLEW格式的耗散项,给出预处理后的HLLEW格式,并根据预处理后的雅克比矩阵构造相应的隐式时间推进方程.利用预处理方法求解NACA 4412低速不可压流动与RAE 2822跨声速可压缩流动,并与实验结果及原有方法的计算结果对比.结果表明:预处理HLLEW格式不仅提高低速不可压缩流动的计算效率和精度,也保持了对可压缩流动的处理能力,是一种适用于全速域流场数值模拟的有效方法. 相似文献
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Experimental investigations have indicated that electrode vapor can have a significant negative effect in thermal interruption speed for the gas-blast circuit breakers. This electrode vapor contamination can be minimized by the use of asymmetric dual-flow nozzle configuration. A computer program was developed to design the nozzle and electrode geometries of the asymmetric dual-flow interrupter and to calculate both the subsonic and supersonic cold flow fields. The Variational Principle of the finite element method, together with a Newton-Raphson iterative scheme, was used to solve the continuity equation for compressible flow. The supersonic flow field in the conical nozzle was calculated by the one-dimensional flow relationship. Two asymmetric dual-flow nozzle models were constructed to investigate the effects of orifice opening and nozzle divergent angle. The cold flow experiments were conducted in the Rensselaer Polytechnic Institute (RPI) Transonic and Supersonic Wind Tunnel Laboratory. Various upstream-to-downstream nozzle pressure ratios were used to obtain the subsonic and supersonic experimental flow-field data. The experimental flow measurements were correlated with the calculated values to validate the computer program. 相似文献
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Gas flow characteristics of argon inductively coupled plasma and advections of plasma species under incompressible and compressible flows 下载免费PDF全文
《中国物理 B》2018,(12)
In this work, incompressible and compressible flows of background gas are characterized in argon inductively coupled plasma by using a fluid model, and the respective influence of the two flows on the plasma properties is specified. In the incompressible flow, only the velocity variable is calculated, while in the compressible flow, both the velocity and density variables are calculated. The compressible flow is more realistic; nevertheless, a comparison of the two types of flow is convenient for people to investigate the respective role of velocity and density variables. The peripheral symmetric profile of metastable density near the chamber sidewall is broken in the incompressible flow. At the compressible flow, the electron density increases and the electron temperature decreases. Meanwhile, the metastable density peak shifts to the dielectric window from the discharge center, besides for the peripheral density profile distortion, similar to the incompressible flow.The velocity profile at incompressible flow is not altered when changing the inlet velocity, whereas clear peak shift of velocity profile from the inlet to the outlet at compressible flow is observed as increasing the gas flow rate. The shift of velocity peak is more obvious at low pressures for it is easy to compress the rarefied gas. The velocity profile variations at compressible flow show people the concrete residing processes of background molecule and plasma species in the chamber at different flow rates. Of more significance is it implied that in the usual linear method that people use to calculate the residence time, one important parameter in the gas flow dynamics, needs to be rectified. The spatial profile of pressure simulated exhibits obvious spatial gradient. This is helpful for experimentalists to understand their gas pressure measurements that are always taken at the chamber outlet. At the end, the work specification and limitations are listed. 相似文献
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在高声强下测量了微圆孔处声激发射流的速度和微圆孔的非线性声阻抗。随声压级的增加声激发射流的速度增大,实验中射流速度在 0-19m/s范围内变化,这表明出现一种强烈声整流现象;与此同时微圆孔声阻明显增大,而声抗减小,声抗最小值约是其线性值的0.7倍。此外实验结果还验证了一种微园孔声学非线性效应离散涡模型的合理性。 相似文献
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使用叶片排间隙混合平面概念,完成离心压气机级多叶片排三元N-S方程计算。每个动静叶片排内的流动被认为是定常的且由相对独立的程序段进行运算。这样的串行程序很容易被改造为在并行系统上运行的SPMD并行程序。 相似文献
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The purpose of this paper is to investigate the compressible turbulent synthetic jet flow characteristics of a dual diaphragm
piezoelectric actuator. Experimentally, a flow visualization system was established to obtain the particle streak images scattered
from 10-μm red fluorescent spheres for observing the synthetic jet flowfield produced by a dual diaphragm piezo actuator.
The centerline velocity of the synthetic jet was also measured by using a hot-wire anemometry system. In the analysis, the
computational approach adopted the transient three-dimensional conservation equations of mass and momentum with the moving
boundary specified to represent the piezo diaphragm motion. The standard k-∈ two-equation turbulent model was employed for
turbulence closure. For the actuator operating at the frequency of 648 Hz, the particle streakline images in the cross-sectional
plane visualized a turbulent jet flow pattern in the far-field area. The hot-wire anemometry data indicated that the measured
centerline velocity of synthetic jets reached 3.8 m/s at y/d= 50. The predictions were compared with the visualized particle
streak images and centerline velocity of the synthetic jet in order to validate the computer code. The numerical simulation
revealed the time-periodic formation and advection of discrete vortex pairs. Caused by the outward movement of the piezo diaphragms,
air near the orifice was entrained into the actuator cavity when the vortex pairs were sufficiently distant from the orifice. 相似文献
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A new finite volume-based numerical algorithm for predicting incompressible and compressible multi-phase flow phenomena is presented. The technique is equally applicable in the subsonic, transonic, and supersonic regimes. The method is formulated on a non-orthogonal coordinate system in collocated primitive variables. Pressure is selected as a dependent variable in preference to density because changes in pressure are significant at all speeds as opposed to variations in density, which become very small at low Mach numbers. The pressure equation is derived from overall mass conservation. The performance of the new method is assessed by solving the following two-dimensional two-phase flow problems: (i) incompressible turbulent bubbly flow in a pipe, (ii) incompressible turbulent air–particle flow in a pipe, (iii) compressible dilute gas–solid flow over a flat plate, and (iv) compressible dusty flow in a converging diverging nozzle. Predictions are shown to be in excellent agreement with published numerical and/or experimental data. 相似文献