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DARPA2潜艇模型非定常流动粘性流场和水动力计算 被引量:1
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作者 于向阳 姚凌虹 +2 位作者 孟庆昌 刘巨斌 张志宏 《舰船科学技术》 北大核心 2019年第7期19-24,共6页
采用基于非结构化网格的有限体积法数值求解非定常的DARPA2潜艇模型粘性流场和水动力,应用动网格技术处理含有动态边界问题的非稳态运动状态,通过调整边界条件和部分松弛因子,使初始流场变量达到收敛精度,并采用编译的UDF对模型运动进... 采用基于非结构化网格的有限体积法数值求解非定常的DARPA2潜艇模型粘性流场和水动力,应用动网格技术处理含有动态边界问题的非稳态运动状态,通过调整边界条件和部分松弛因子,使初始流场变量达到收敛精度,并采用编译的UDF对模型运动进行定义。为了得到较好的非定常结果,需要对初始流场进行讨论。用model-1对实验数据的拟合效果较好,数值计算结果稳定。要取得与实验一致的模拟效果,由实验中的不确定因素产生的误差是需要加以考虑的进行非定常数值模拟。 展开更多
关键词 数值模拟 非定常流动粘性流场计算 DARPA2
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椭球体定常流动粘性流场和水动力计算方法研究 被引量:2
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作者 于向阳 姚凌虹 +2 位作者 孟庆昌 刘巨斌 张志宏 《舰船电子工程》 2019年第7期187-193,共7页
潜艇等水下航行体粘性流场和水动力对其操纵性预报至关重要。而潜艇等水下航行体作操纵运动时,其水动力主要集中在主体部分,因此主体水动力预报的准确程度备受关注。6:1椭球体类似于潜艇等水下航行体的主体,对其流动预报的结果可以间接... 潜艇等水下航行体粘性流场和水动力对其操纵性预报至关重要。而潜艇等水下航行体作操纵运动时,其水动力主要集中在主体部分,因此主体水动力预报的准确程度备受关注。6:1椭球体类似于潜艇等水下航行体的主体,对其流动预报的结果可以间接检验数值计算模型对潜艇等水下航行体操纵性预报的能力。论文应用CFD软件对6:1椭球体水动力进行数值模拟。采用基于非结构化网格的有限体积法离散控制方程和湍流模式,对流项采用二阶迎风格式,速度-压力耦合采用SIMPLE方法处理,得到6个攻角的水动力数值计算结果。综合比较5种湍流模型对椭球体的水动力数值计算结果,并且分析了不同计算域,不同网格密度等对数值计算结果的影响。结果表明:SA和SST模型具有较好的计算效果,并且认为以牺牲1.5%网格密度相对偏差换取百万网格的代价值得考虑。论文的计算结果和结论为后续湍流模式、计算域范围和网格密度的研究提供了参考依据。 展开更多
关键词 椭球体 定常流动粘性流场计算 水动力数值计算
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求解跨音速粘性流反问题的有限体积法 被引量:3
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作者 海灏 陈乃兴 《工程热物理学报》 EI CAS CSCD 北大核心 1998年第6期702-705,共4页
In this paper a finite volume method for solving inverse problem of transonic viscousflow is preseflted. The method is based on a timermarching finite volume method and apressure residual correction formula. The resid... In this paper a finite volume method for solving inverse problem of transonic viscousflow is preseflted. The method is based on a timermarching finite volume method and apressure residual correction formula. The residual correction formula is an auxiliary partialdifferelltial equation that is solved for incremental changes in surface coordinates duringeach computational cycle. In the paper a transonic turbine cascade was calculated anddemonstrated. The inverse solution was agreed with the target well. 展开更多
关键词 气动热力学 粘性流动计算 透平叶栅 有限体积法
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Effects of groove on behavior of flow between hydro-viscous drive plates 被引量:1
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作者 黄家海 范毓润 +1 位作者 邱敏秀 方文敏 《Journal of Central South University》 SCIE EI CAS 2012年第2期347-356,共10页
The flow between a grooved and a flat plate was presented to investigate the effects of groove on the behavior of hydro-viscous drive. The flow was solved by using computational fluid dynamics (CFD) code, Fluent. Para... The flow between a grooved and a flat plate was presented to investigate the effects of groove on the behavior of hydro-viscous drive. The flow was solved by using computational fluid dynamics (CFD) code, Fluent. Parameters related to the flow, such as velocity, pressure, temperature, axial force and viscous torque, are obtained. The results show that pressure at the upstream notch is negative, pressure at the downstream notch is positive and pressure along the film thickness is almost the same. Dynamic pressure peak decreases as groove depth or groove number increases, but increases as output rotary speed increases. Consequently, the groove depth is suggested to be around 0.4 mm. Both the groove itself and groove parameters (i.e. groove depth, groove number) have little effect on the flow temperature. Circumferential pressure gradient induced by the groove weakens the viscous torque on the grooved plate (driven plate) greatly. It has little change as the groove depth increases. However, it decreases dramatically as the groove number increases. The experiment results show that the trend of experimental temperature and pressure are the same with numerical results. And the output rotary speed also has relationship with input flow rate and flow temperature. 展开更多
关键词 hydro-viscous drive variable viscosity groove effect numerical calculation
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