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船艇迎浪前进时,在风浪冲击下,艏部会高高翘起、而后又在波谷中跌落,形成纵摇、拍击、颠簸、失速、航速下降、稳定安全性降低等缺点。为了克服这样的不良航态,必须在水动力流场中,造成克服这些弱点的水动力和相应的水动力矩沿船体合理分布。为此,提出设置不同于常规船艇的船底浸湿面外形,使之产生足够强大的水动反冲击力、水动升力及相应的水动航向稳定扶正力矩,确保船艇不偏离目标;凭借足够强大的的水动升力和相应的船艇纵向稳定扶正力矩,消除船艇的纵摇拍击;以相应的船体横向稳定扶正力矩来克服船艇的横摇摆动。最终确保船艇平稳高速地破浪前进。而在风浪中转弯时所激起的强大水动离心力、水动反冲击力、水动升力和相应的水动助回转力矩、水动抗船体向心倾覆扶正力矩又能使船艇以很小的回转半径高速、稳定、安全地在风浪中转弯。 相似文献
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考虑到三维效应和重力影响,提出研究设置导流槽的船底在水面滑行激起的流场以及作用在槽和船底浸湿面上的水动力。该导流槽的顶部曲面前低后高,对船底基面形成倾角。运用严谨的数学物理方法解决问题,求得描绘三维流场状况的解析函数.由此获得船艇前进时出现在槽顶部曲面上推船艇前进的水动推进力和向上的水动升力定量值的解析表述式。将船底浸湿面设计成设置导流槽的外形,建成实船试航,通过卫星跟踪的GPS系统实测获得的数据证明了水动推进力的存在,且它随着航速的提高而迅速增大,于是船速以及稳定性、安全性均得以犬,幅提高。实船设计时,可通过合理调整表述式中的物理参数,设计建造整体性能远优于常规船艇的实船。 相似文献
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考虑到三维效应和重力影响,提出研究设置导流槽的船底在水面滑行激起的流场以及作用在槽和船底浸湿面上的水动力。该导流槽的顶部曲面前低后高,对船底基面形成倾角。运用严谨的数学物理方法解决问题,求得描绘三维流场状况的解析函数,由此获得船艇前进时出现在槽顶部曲面上推船艇前进的水动推进力和向上的水动升力定量值的解析表述式。将船底浸湿面设计成设置导流槽的外形,建成实船试航,通过卫星跟踪的GPS系统实测获得的数据证明了水动推进力的存在,且它随着航速的提高而迅速增大,于是船速以及稳定性、安全性均得以大幅提高。实船设计时,可通过合理调整表述式中的物理参数,设计建造整体性能远优于常规船艇的实船。 相似文献
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本文采用进退、横荡、摇首三个非线性运动方程,用龙格-库塔法在数字机上求解来预报船舶操纵性。船体上的横向水动力和力矩采用系列船模试验资料。进退方程中的纵向水动力是利用船体阻力曲线和螺旋桨敞水试验曲线等资料根据主机类型和工况计算的.计算是在 TQ-16机上进 相似文献
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为比较分析单船与两船并行航行的水动力差异,探讨静水中两船并行时漂角、船船相对位置对船体阻力、侧向力及摇首力矩的影响规律,文章基于RANS方程采用SST k-棕湍流模型,数值分析了某两船静水并行时船船相互作用。研究表明:不同漂角下两船中对中并行时,船体所受阻力均较单船航行时有所增大且受到指向两船中间的附加侧向力;当两船并行斜航的漂角相反时,同一船舶位于迎流侧较背流侧时船体受力存在一定差异;两船并行直航时,船船相对位置对船体受力有较大的影响,当两船纵向间距小于一倍船长时,船船相互作用较为显著,在不同横向间距下,船体受力随纵向间距的变化规律相同,在一定纵向间距下,船间横向间距越小船船相互作用越强。 相似文献
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本文应用细长体理论提供一个计及线型要素的船舶斜航时横向力和首摇力矩的计算方法。此方法原由不破提出,但本文对计算模型作了修改,即将分离涡布置在船体中心线上,使模型得到简化;同时还考虑了速度势的远场解,并将其计入水动力的修正中,使横向力和首摇力矩同时与试验相吻合,该方法在较广的船型范围内计算值与试验相吻合,适用于一般的民用船型(包括 C_B 在0.8以上的超肥大船型)。 相似文献
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利用计算流体力学方法对减摇鳍与船体之间的适配性问题进行研究。利用零航速减摇鳍的参数以及某型驱逐舰的船型型值表,分别建立在敞水条件下的减摇鳍模型以及加上减摇鳍的船体模型。首先,仿真分析在中、高航速下敞水条件的减摇鳍与受船体约束减摇鳍的静态水动力特性。其次,利用动网格技术分别分析在中、高航速和低航速下敞水条件的减摇鳍与受船体约束减摇鳍的动态水动力特性。计算结果分析表明:静态仿真时,虽然受船体约束减摇鳍的失速角没有敞水条件下的减摇鳍大,但在同样的攻角下,其升力系数却有较大的提高;在动态仿真中,无论是在中、高航速还是低航速下,受船体约束减摇鳍拍击产生的升力都要比敞水条件下的减摇鳍大,但同时产生的阻力以及所需的转鳍力矩也有较大的提高。 相似文献
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Takuya Ohmori Masataka Fujino Hideaki Miyata 《Journal of Marine Science and Technology》1998,3(1):22-29
To estimate the maneuvering ability of a ship, an accurate estimation of the hydrodynamic forces and moment acting on the ship's hull is indispensable. For the purpose of developing a numerical method of computing the viscous flow field around a hull and evaluating its validity, the hydrodynamic pressure on the hull and the velocity field were measured. Two full ship models with different hull forms in the aft part were used for the experiment. From the results of pressure measurements, the distribution of hydrodynamic lateral forces was obtained. The simulation method is a numerical solution of the Navier-Stokes equation based on a finitevolume method and applied to the maneuvering motion. The measured and computed results agree qualitatively well, and the method is a valuable tool for estimating the maneuvering ability of a ship. The typical characteristics of the flow field in the steady turning condition are revealed by the numerical simulation, and the mechanism of the relations between hull form, flow field, and hydrodynamic forces are clarified.Translation and combination of articles that appeared in the Journal of the Society of Naval Architects of Japan, vols. 176, 177, 179 (1994–1996): The original article won the SNAJ prize, which is awarded annually to the best papers selected from the SNAJ Journal, JMST, or other quality journals in the field of naval architecture and ocean engineering.This work was conducted as part of the joint SR221 project supported by JSRA (Shipbuilding Research Association of Japan). The authors express their sincere gratitude to the persons concerned, and especially to M. Kanai, S. Eguchi, S. Usami, K. Tatsumi, and T. Kawamura. 相似文献
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建立并求解高速排水艇稳定回转的运动方程。对运动方程中裸船体和附体的水动力导数、舵作用力和力矩、多个螺旋桨对回转的影响等进行估算。并以120t级渔政船为例,进行稳定回转直径和横倾角的计算,并与实船的试航结果进行比较。 相似文献
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Takuya Ohmori 《Journal of Marine Science and Technology》1998,3(2):82-93
A finite-volume method of computing the viscous flow field about a ship in maneuvering motion was developed. The time-dependent
Navier-Stokes equation discretized in the generalized boundary-fitted curvilinear coordinate system is solved numerically.
A third-order upwind differencing scheme, a marker and cell (MAC)-type explicit time marching solution algorithm and a simplified
subgrid scale (SGS) turbulence model are adopted. The simulation method is formulated, including the movement of a computational
grid fitted to the body boundary that allows computation of the flow field around a body under unsteady motion.
To estimate the maneuvering ability of a ship, the accurate prediction of the hydrodynamic forces and moments of the hull
is important. Therefore, experimental methods of finding the hydrodynamic forces of a ship in maneuvering motion, such as
the oblique towing test, the circular motion test (CMT) and planar motion mechanism (PMM) test, were established. Numerical
simulation methods for those captive model experiments were developed introducing computational fluid dynamics (CFD).
First, numerical methods for steady oblique tow and steady turn simulation were developed and then extended to unsteady forced
motion. Simulations were conducted about several realistic hulls, and the results were verified by comparisons with measured
results obtained in model experiments. Hydrodynamic forces and the moment, the longitudinal distribution of the hydrodynamic
lateral force, and the pressure distribution on the hull surface showed good agreement. 相似文献
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安装在潜艇上的首部水平舵位置对于潜艇在垂直方向的稳定性以及操纵性具有重大意义.本文首先通过Fluent 14.0计算Suboff模型的阻力以及DTMB舵型的升、阻力,仿真结果与实验结果吻合较好.然后计算带围壳舵Suboff潜艇和带首舵Suboff潜艇的阻力、升力特性,并比较了潜艇带首舵和围壳舵的升阻力特性差异,以及对艇体表面压力分布和尾部流场的影响.计算结果显示,相同舵角下,围壳舵和首舵阻力相差不大,围壳舵升力比首舵升力大.相同舵角下,潜艇总阻力相差不大,带首舵潜艇总升力、总力矩比带围壳舵潜艇总升力、总力矩大.围壳舵舵角的变化对艇体表面的压力变化影响相对首舵来说较小.围壳舵和首舵在较大舵角下,都会对尾水平舵产生显著影响. 相似文献