导管螺旋桨与尾鳍运动参数对飞潜器水下流体动力特性影响研究

Investigation on the effects of ducted propeller and tail fin deflection parameters on the underwater hydrodynamic characteristics of trans-medium submersibles

  • 摘要:
    目的 旨在研究跨介质飞潜器水下直航和回转运动过程中的运动特性和流场特性。
    方法 基于计算流体力学数值模拟技术,并利用VOF多相流模型和SST k-ω湍流模型建立飞潜器水下航行数值计算模型。通过对比潜艇模型(DARPA Suboff)在不同航行速度下的总阻力试验结果和数值计算结果对数值方法的有效性进行了验证。在此基础上,分别对飞潜器水下直航和回转运动过程进行数值模拟和分析,重点研究了导管螺旋桨推进器旋转速度和尾鳍偏转角度对飞潜器水下直航和回转运动的影响。
    结果 结果表明:飞潜器水下直航时,航速与螺旋桨转速近似呈线性关系,如螺旋桨转速从600 r/min增加到4 800 r/min时,航速相应从1.1 m/s提升至8.1 m/s,同时负值俯仰力矩随螺旋桨转速增加而增大,但绝对值逐渐减小(俯仰力矩从−0.35 N·m提升至−0.17 N·m),表明高速航行时能够保持稳定姿态,螺旋桨转速对表面压力系数分布以及流场结构几乎不产生影响;飞潜器水下回转时,其回转半径的大小主要受尾鳍偏转角度的影响,几乎不受螺旋桨转速的影响,回转半径随着尾鳍偏转角的增大而减小(回转半径从3.35倍飞潜器长度减小到0.75倍),但减小趋势逐渐变缓,而飞潜器回转航速会受到螺旋桨转速及尾鳍偏转角的综合影响,两侧螺旋桨推力均随着螺旋桨转速和尾鳍偏转角的增大而增大,回转轨迹外侧螺旋桨推力始终大于内侧,两者差额也随着尾鳍偏转角的增大而增大;飞潜器回转过程中,尾鳍偏转引起的飞潜器回转运动导致其表面压力分布呈现明显的非对称性特征,随着尾鳍偏转角度的增加,飞潜器表面压力分布的非对称性特征逐渐明显,这种非对称性特征与其周围流场的非对称性流动密切相关。
    结论 该研究可为飞潜器构型设计及水下航行性能分析提供参考。

     

    Abstract:
    Objective  To investigate the dynamic behavior and flow field characteristics of trans-medium submersibles during underwater straight-line navigation and turning maneuvers.
    Method Computational fluid dynamics simulations were employed, using the VOF multiphase flow model and the SST k-ω turbulence model to establish a numerical model of the underwater navigation of the trans-medium submersibles. The accuracy of the numerical method was validated by comparing the experimental total drag data for the DARPA Suboff submarine model at various speeds with the numerical calculation results. On this basis, numerical simulations and analyses of underwater straight-line navigation and turning maneuvers of the trans-medium submersible were conducted, focusing on the effects of ducted propeller rotation speed and tail fin deflection angle on the underwater straight-line navigation and turning performance of the submersible.
    Results The research results indicate that during straight-line underwater navigation, the forward speed of the trans-medium submersible exhibits an approximately linear relationship with the propeller's rotational speed. For instance, as the propeller speed increases from 600 r/min to 4800 r/min, the forward speed rises from 1.1 m/s to 8.1 m/s. At the same time, the pitch moment becomes less negative with increasing propeller speed (from −0.35 N·m to −0.17 N·m), indicating that the submersible remains stable in pitch during high-speed navigation. The propeller speed has little effect on the surface pressure distribution and the structure of the surrounding flow field. During underwater turning, the turning radius is mainly determined by the tail fin deflection angle and is largely unaffected by the propeller speed. The turning radius decreases with increasing tail fin deflection angle (from 3.35 times the submersible's body length to 0.75 times), though the rate of decrease diminishes. In contrast, the turning speed is affected by both the propeller speed and the tail fin deflection angle. The thrust generated by both propellers increases with higher propeller speeds and larger tail fin deflection angles. During turning, the thrust of the outer propeller consistently exceeds that of the inner propeller, and the thrust difference increases with greater tail fin deflection. Furthermore, tail fin deflection during turning leads to a significantly asymmetric surface pressure distribution on the submersible. This asymmetry becomes more pronounced with increasing tail fin deflection and is closely associated with the asymmetric flow characteristics of the surrounding flow field.
    Conclusion This study provides a reference for the design and performance analysis of trans-medium submersible configurations.

     

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