SIMULATION OF UNSTATIONAL THERMO SHOCKED STATE GTU

A. Baranyuk, A. Rachinsky
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Abstract

The paper proposes a method of approximate calculation of the temperature field of the turbine blade in non-stationary mode by means of CFD-modeling. The academic version of the ANSYS-Fluent software package was used as a modeling tool. The local values of the heat transfer coefficient along the contour of the blade profile were calculated in the work. Previously, the gas flow velocity in the curved interscapular channel was calculated to determine the distribution of the gas flow velocity along the convex and concave surfaces of the blade. Comparison of the data thus obtained with the result of processing the experience conducted on the turbine, shows that in the conditions of the real rotating installation, the heat transfer to the surface of the blade was approximately 2 times higher. The most probable reason for this discrepancy is the earlier beginning of the transition to the turbulent boundary layer on the surface of the blade in real conditions of high turbulence of the oncoming flow. Calculations show that in the case of a sharp change in gas temperature, the largest temperature difference in the blade occurs after a few seconds and reaches 50 ... 90% of the change in gas temperature, and in blades with thin edges - close to this value. Increasing the thickness of the edges can significantly reduce the uneven temperature in the blades with sharp changes in gas temperature. In order to identify the nature of the stress state of the blades at different modes of operation of the gas turbine unit, the temperature stresses in the blade were calculated. The calculation was performed for Mises averaged stresses  in the cross section of an unevenly heated blade. When starting the installation, the maximum force occurred 30 ... 40 seconds after the start of the rotation of the rotor almost simultaneously with the maximum temperature difference between the edges and the central part of the section. The highest stress values occurred in the region of the inlet edge, where they exceeded 680 MPa per compression. In the future, the temperature stresses decreased and even changed sign due to the cooling process of the blade, overheated when throwing the gas temperature.
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非稳态热冲击状态gtu的模拟
本文提出了一种利用cfd模型近似计算涡轮叶片非静态温度场的方法。采用学术版的ANSYS-Fluent软件包作为建模工具。在工作中计算了沿叶片轮廓的局部换热系数。在此之前,通过计算弯曲肩胛间通道内的气体流速来确定叶片凹凸表面上气体流速的分布。将所得数据与对涡轮进行经验处理的结果进行比较,可以看出,在实际旋转安装条件下,叶片表面的换热量大约高出2倍。造成这种差异的最可能的原因是,在来流高湍流的实际条件下,叶片表面过渡到湍流边界层的时间较早。计算表明,在气体温度急剧变化的情况下,叶片的最大温差出现在几秒后,达到50…90%的气体温度变化,在边缘较薄的叶片中-接近这个值。增加叶片边缘厚度可以显著降低叶片内部温度不均匀,且气体温度变化剧烈。为了识别燃气轮机机组不同工况下叶片应力状态的性质,对叶片内的温度应力进行了计算。计算了不均匀加热叶片截面上的Mises平均应力。开始安装时,最大受力为30…开始转动后40秒转子几乎同时与边缘和截面中心部分之间的最大温差。最大的应力值出现在入口边缘区域,超过680 MPa /压缩。在未来,由于叶片的冷却过程,温度应力下降,甚至改变符号,过热时抛出的气体温度。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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