检索规则说明:AND代表“并且”;OR代表“或者”;NOT代表“不包含”;(注意必须大写,运算符两边需空一格)
检 索 范 例 :范例一: (K=图书馆学 OR K=情报学) AND A=范并思 范例二:J=计算机应用与软件 AND (U=C++ OR U=Basic) NOT M=Visual
作 者:王中[1] 王梦豪 彭远鸣 卢蕊[1] 周景军[1] WANG Zhong;WANG Menghao;PENG Yuanming;LU Rui;ZHOU Jingjun(The 705 Research Institute,China Shipbuilding Industry Corporation,Xi′an 710077,China)
机构地区:[1]中国船舶重工集团公司第705研究所,陕西西安710077
出 处:《西北工业大学学报》2024年第1期28-34,共7页Journal of Northwestern Polytechnical University
基 金:国家高层次人才特殊支持计划(W03070206)资助。
摘 要:超空泡航行体全沾湿航行阶段尾舵展开过程的流体动力载荷对于航行体稳定性分析以及尾舵机性能设计具有重要影响。建立了基于重叠网格技术和网格域间相对运动思想的尾舵展开过程数值计算方法;结合超空泡航行体设计需求,研究了尾舵不同展开速率、不同攻角状态展开以及尾舵展开前后的水动力载荷变化规律;通过对尾舵附近速度矢量场、压力场以及尾舵表面压力系数分析,揭示了尾舵不同状态的流体动力载荷变化原因。研究成果对超空泡航行体尾舵展开过程流场特性研究具有重要参考价值,同时为尾舵机性能设计提供了重要设计依据。In the state of navigating covered with liquid fluid,the hydrodynamics loads of the supercavitating vehicle during the deployment process of the tail rudder have an important impact on the stability analysis of the vehicle and the performance design of the tail rudder.In this study,a numerical simulation method for the deployment process of the rudder based on the overlapping grids technology and the concept of relative motion between grid domains is established.Combined with the design requirements of the supercavitating vehicle,the change law of hydrodynamics loads under different deployment rates,attack angles during the deployment process,before and after deployment of the tail rudder are researched in detail.Through the analysis of the velocity vector field,pressure field near the rudder and pressure coefficients of the rudder surface,the reasons for the changes of the hydrodynamic loads in different states are revealed.The results have important reference value for the research on the flow field characteristics of the deployment process of the tail rudder for the supercavitating vehicle,and provide an important design basis for the performance design of the tail rudder.
正在载入数据...
正在载入数据...
正在载入数据...
正在载入数据...
正在载入数据...
正在载入数据...
正在载入数据...
正在链接到云南高校图书馆文献保障联盟下载...
云南高校图书馆联盟文献共享服务平台 版权所有©
您的IP:216.73.216.222