王大磊, 朴 英. 某跨音速高压涡轮非定常流动数值模拟研究[J]. 工程力学, 2013, 30(2): 427-433. DOI: 10.6052/j.issn.1000-4750.2011.07.0437
引用本文: 王大磊, 朴 英. 某跨音速高压涡轮非定常流动数值模拟研究[J]. 工程力学, 2013, 30(2): 427-433. DOI: 10.6052/j.issn.1000-4750.2011.07.0437
WANG Da-lei, PIAO Ying. NUMERICAL STUDY OF 3-D UNSTEADY FLOW IN A TRANSONIC TURBINE STAGE[J]. Engineering Mechanics, 2013, 30(2): 427-433. DOI: 10.6052/j.issn.1000-4750.2011.07.0437
Citation: WANG Da-lei, PIAO Ying. NUMERICAL STUDY OF 3-D UNSTEADY FLOW IN A TRANSONIC TURBINE STAGE[J]. Engineering Mechanics, 2013, 30(2): 427-433. DOI: 10.6052/j.issn.1000-4750.2011.07.0437

某跨音速高压涡轮非定常流动数值模拟研究

NUMERICAL STUDY OF 3-D UNSTEADY FLOW IN A TRANSONIC TURBINE STAGE

  • 摘要: 通过求解三维非定常雷诺平均N-S方程模拟某跨音速高压涡轮非定常流场,研究涡轮内非定常流动特征。通过对静子尾迹及静子尾缘激波和转子叶排之间的相互干涉过程进行详细分析,发现定常/非定常模拟方法获得的涡轮总体性能参数基本一致但流场存在较大差异。静子尾迹是导致涡轮流场非定常性的重要因素之一:在转子叶栅通道中部和下部,静子尾迹和转子叶片附面层及下通道涡发生明显干涉,并导致通道中下部损失周期性波动幅度较大,此外尾迹和下通道涡间的干涉作用在转子尾缘处诱导出高频脱落涡。静子尾缘激波也是导致涡轮流场非定常性的原因之一,激波和转子叶片作用形成复杂的波系结构,对涡轮流场影响显著:一方面激波/附面层干涉导致转子和静子的吸力面产生周期性变化的高温区域;另一方面激波撞击叶片导致叶片表面的气流在激波后出现分离,对转子静压分布产生影响,使得转子叶片表面载荷出现明显的非定常性,进而导致涡轮输出功的周期性波动十分剧烈。

     

    Abstract: Three dimensional time-dependent Reynolds averaged Navier-Stokes equations were solved to investigate the unsteady flow in a transonic high pressure turbine stage. The influence of wake and shock waves of the stator vanes was analyzed. Results show that the aerodynamic performance parameters solved by steady/unsteady methods are similar, while the flow patterns are discrepant. The interaction between the upstream wake and downstream boundary and vortexes is marked and lead to the increase in the flow loss especially near the hub of the rotor. And high-frequency-shedding vortexes appear as a result of the interaction of the wake and hub passage vortexs. The stator wake is one of the major reasons that induce the unsteady effect of the rotor flow. The trailing edge shock waves of the stator vanes are considered as another reason. Due to the shock wave/boundary layer interaction phenomena, the distribution of static temperature on the surface of the rotor is influenced and high static temperature is produced periodically. Meanwhile, the distribution of static pressure on the rotor surface changes: the static pressure on the surface rising rapidly behind the shock waves; on the other hand, the shock wave/boundary layer interaction results in the flow separation on the suction side of the rotor. The rotor loading distribution changes periodically as well as the output power of the turbine.

     

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