热声振荡中流体粒子的热力学性质和能量通量

S. Adachi
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摘要

用数值方法研究了气体氦在封闭直圆柱管内的热声塔康尼斯振荡。管受到沿管轴的强温度梯度的影响。热端部与冷中心部的温度之比为15,热部与冷部的长度之比为1.0。求解了轴对称可压缩Navier-Stokes方程,观察到驻波的基本反对称模态。利用得到的流场数据,对流体颗粒进行了跟踪,并计算了它们的热力学性质。流体粒子在管内振荡和漂移。为了得到能量转换的一般情况,我们考察了热增长率分布的演变。结果表明,在管内温度梯度较大的区域,该速率较大。用数值方法研究了气体氦在封闭直圆柱管内的热声塔康尼斯振荡。管受到沿管轴的强温度梯度的影响。热端部与冷中心部的温度之比为15,热部与冷部的长度之比为1.0。求解了轴对称可压缩Navier-Stokes方程,观察到驻波的基本反对称模态。利用得到的流场数据,对流体颗粒进行了跟踪,并计算了它们的热力学性质。流体粒子在管内振荡和漂移。为了得到能量转换的一般情况,我们考察了热增长率分布的演变。结果表明,在管内温度梯度较大的区域,该速率较大。
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Thermodynamic properties of fluid particles and energy fluxes in thermoacoustic oscillations
Thermoacoustic Taconis oscillations of gaseous helium in a closed straight cylindrical tube are numerically studied. The tube is subject to a strong temperature gradient along the tube axis. The ratio of the temperature of the hot end parts to that of the cold center part is 15, and the length ratio of the hot part to that of the cold part is 1.0. The axisymmetric compressible Navier-Stokes equations are solved and fundamental antisymmetric mode of a standing wave is observed. Using the obtained flow field data, we trace fluid particles and their thermodynamic properties are calculated. The fluid particles oscillate and drift in the tube. In order to obtain a general picture of the energy conversion, the evolution of the distribution of the increase rate of heat is examined. It is shown that the rate is large in the region where the temperature gradient is large in the tube.Thermoacoustic Taconis oscillations of gaseous helium in a closed straight cylindrical tube are numerically studied. The tube is subject to a strong temperature gradient along the tube axis. The ratio of the temperature of the hot end parts to that of the cold center part is 15, and the length ratio of the hot part to that of the cold part is 1.0. The axisymmetric compressible Navier-Stokes equations are solved and fundamental antisymmetric mode of a standing wave is observed. Using the obtained flow field data, we trace fluid particles and their thermodynamic properties are calculated. The fluid particles oscillate and drift in the tube. In order to obtain a general picture of the energy conversion, the evolution of the distribution of the increase rate of heat is examined. It is shown that the rate is large in the region where the temperature gradient is large in the tube.
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