受限水域船体周围时均流速分布规律试验研究

Experimental study on the time-averaged flow velocity distribution around a ship in restricted waters

  • 摘要: 船舶在限制水域航行时,运动船体与受限水体之间的复杂相互作用将形成独特的水流结构,船体附近时均流速的空间分布直接影响船舶操纵性和稳定性,对船舶运行安全具有重要影响。基于受限水域环境,利用高分辨率粒子图像测速技术(PIV),开展缩尺船模作用下的明槽湍流试验,研究船体周围时均流速的分布特征,探讨不同断面系数和来流条件下时均流速的分布规律,分析这两个关键因素对时均流速垂向分量和纵向分量的影响机制。结果表明:受限水域中纵向流速U最大值出现在船体底部,垂向流速V受船前形成的下潜水流以及船后形成的上升回流影响,最大值出现在船头处和船尾下游处,纵向及垂向流速均在贴近船头处变化最剧烈。船舶底部的无量纲纵向时均流速沿垂线呈非对称的“⊃”形分布,垂线流速从船体底部至水槽底部先增大后减小,船尾涡旋范围内近似呈“S”形分布;纵向时均流速随断面系数的增大而减小,最大纵向时均流速约为断面平均流速的1.35倍,但最大流速出现的位置基本不随断面系数发生变化。纵向时均流速随来流速度的增大而逐渐增加,无量纲纵向时均流速呈现明显分区现象,船前及船底最大流速区范围向外扩展,船头绕流低流速区缩小,船尾后部回流区范围扩大,而来流速度的变化基本未改变最大流速出现的位置。研究结果可为受限水域航道设计维护和船舶安全航行提供科学参考。

     

    Abstract: When a ship navigates in restricted waters, the complex interaction between the moving hull and the confined water body generates a distinctive flow structure. The spatial distribution of the time-averaged flow velocity near the hull directly affects the ship’s maneuverability and stability, and plays a critical role in ensuring operational safety. In this study, high-resolution Particle Image Velocimetry (PIV) technology was employed to conduct open-channel turbulence tests using a scaled ship model in a restricted water environment. The distribution characteristics of time-averaged velocity around the hull were examined, focusing on the effects of varying cross-sectional coefficients and inflow conditions. The influence of these two key factors on the longitudinal and vertical components of the time-averaged velocity was analyzed. Results show that the maximum longitudinal velocity U in restricted waters appears beneath the ship. Influenced by the descending flow at the bow and the ascending backflow behind the stern, the vertical velocity V peaks near the bow and downstream of the stern, with the most significant velocity changes occurring near the bow. The dimensionless longitudinal time-averaged velocity beneath the hull exhibits an asymmetric "⊃"-shaped distribution along the vertical axis. The vertical flow velocity initially increases and then decreases from the hull bottom to the channel bed, approximating an "S"-shaped pattern within the stern vortex region. The longitudinal time-averaged velocity decreases with an increasing cross-sectional coefficient, with its maximum value reaching approximately 1.35 times the average cross-sectional velocity. However, the position of the velocity peak remains largely unaffected. As the inflow velocity rises, the longitudinal time-averaged velocity increases accordingly, and the dimensionless profile reveals distinct zoning: the high-velocity zone beneath and in front of the hull expands, the low-velocity zone near the bow contracts, and the stern backflow zone enlarges. Nonetheless, variations in inflow velocity do not significantly alter the location of maximum flow velocity. These findings provide a scientific basis for the design and maintenance of restricted waterways and the safe navigation of vessels.

     

/

返回文章
返回