V型耦合板架截断模型动力边界等效规律

Dynamic boundary equivalence for the truncated V-shaped plate model: a new method and study on the effects of aligned plates

  • 摘要:
    目的 为了对船舶与海洋结构物局部板架的动力性能进行数值计算和实验测试,需要将局部结构从整体模型中截取出来,并采用适当的等效方法模拟与之相连的结构对局部板架结构动力性能的影响,探究板架结构截断模型的动力边界等效问题。
    方法 采用有限元法分析耦合角度和附板长度对V型板架自由振动特性的影响,研究弹性支撑刚度对一边弹性支撑、三边自由边界条件下正交加筋板自由振动特性的作用。对比分了不同耦合角度、不同附板长度的V型板架与弹性支撑正交加筋板固有频率与振型的对应关系,探寻弹性支撑刚度边界等效V型耦合板架截断边界的规律。
    结果 研究表明:V型板架前4阶板类模态的敏感耦合角度范围为140°~180°,模态较为稳定的附板长度区间为0.6~0.9 m。当弹性支撑刚度较小时,附加质量会显著降低正交加筋板的固有频率,提高各阶模态的敏感刚度,减小敏感刚度的频率范围;而当弹性支撑刚度较大时,附加质量对正交加筋板固有频率的影响甚微。V型板架前四阶板类模态的动力边界等效弹性刚度随耦合角度增大而减小,且V型耦合板架附板长度的变化会引起部分模态的转化现象和振型畸变现象。
    结论 采用弹性支撑边界模拟V型耦合板架的动力耦合条件,尽管在固有振型模态转换过程中存在细微不足,但整体上仍能实现有效等效。这一策略不仅为截断模型边界的模拟开辟新径,还提升了计算效率并维持了高精度。

     

    Abstract:
    Objective To conduct numerical analysis and experimental testing on the dynamic performance of stiffened plates truncated from naval and marine structures, it is necessary to address dynamic boundary equivalence to simulate the effects of surrounding coupled structures on the dynamic characteristics of the truncated structure.
    Method The finite element method is used to analyze the effects of the coupling angle and length of aligned plates on the free vibration behavior of a V-shaped stiffened plate, as well as the effects of elastic support stiffness on the free vibration behavior of an orthogonally stiffened plate with one elastically supported edge and three free edges. A comparison of the vibration characteristics between V-shaped stiffened plates with different coupling angles and aligned plate lengths and orthogonally stiffened plates with appropriate elastic support stiffness is conducted to establish a simulation method for achieving dynamic boundary equivalence of truncated stiffened plates.
    Results The results show that for the first four modes, the sensitivity range of the coupling angle of the V-shaped stiffened plate is between 140° and 180°, while the stable length range of the aligned plate is between 0.6 m and 0.9 m. When the elastic support stiffness is small, the additional mass significantly decreases the natural frequencies of the orthogonally stiffened plate, increases sensitivity to stiffness and narrows the frequency range over which the system is sensitive to stiffness variations. When the elastic support stiffness is large, the additional mass has little effect on the natural frequencies of the orthogonally stiffened plate. The equivalent elastic support stiffness of the first four modes of the V-shaped stiffened plate decreases as the coupling angle increases. Changes in the length of the aligned plate of the V-shaped stiffened plate lead to modal differentiation and distortion of the mode shapes.
    Conclusion The use of the elastic support boundaries to simulate the dynamic coupling conditions of the V-shaped stiffened plates, despite minor deficiencies during inherent mode transitions, can still achieve overall effective equivalence. This strategy not only provides a new approach for simulating truncated model boundaries but also improves calculation efficiency while maintaining high accuracy.

     

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