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Flow modelling around propeller for a deep drafted vessel in very shallow water

机译:深水条件下深吃水船螺旋桨周围的流动模型

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摘要

Computational fluid dynamics (CFD) codes, are recently used as efficient tools to understand flow characteristics such as wake development around propeller. This thesis presents numerical modelling of flow characteristics in the stern region for a deep drafted LNG carrier with the effect of propeller and rudder in shallow water. The modelling was conducted based on the B5-75 type propeller, with a diameter (D) of 7.7m, which was designed at MARIN in the Netherlands. The ANSYS Fluent version 12 software was used to solve the Reynold Averaged Navier Stokes (RANS) equations, and ICEM CFD as a mesh generator. The propeller was meshed using tetra unstructured mesh in a flow field based on 3D incompressible Navier-stokes solver. Two turbulent models were applied in the ANSYS Fluent; which are the standard k-epsilon (k-e) model for the steady simulation and transient shear stress transport (SST) k-omega (k-?) for the unsteady simulation. For the computational domain, the propeller blades were mounted on two finite long constant radius cylinders. The two types of cylinder domains, were developed; stator domain and rotor domain. For the stator domain, the inlet flow was 2D from blade, the outlet flow at 6D and the outer boundary was 3.6D. The upstream for the rotor domain was maintained at 0.2D but the downstream was extended between 0.4D and 0.7D, and the outer boundary at 1.4D. The turbulent model was simulated in the rotor domain by using the stator-rotor approaches such as the multiple reference frame (MRF) and the sliding mesh (SM) method. Comparisons with the published experiments were presented, and the dependence of the numerical solutions on the computational parameters was studied extensively. The thrust and torque of the propeller were generally predicted with a small error when it was compared with the published experiments. The difference in performance of propeller in the open water test is about 10 percent, likely due to mesh strategy as well as mesh resolution and quality. The performance of the propeller was also studied. It was found that the rudder placed in front of propeller increased the efficiency of the propeller and produced greater thrust increments when the rudder was deflected to -70 and -200. The presence of the rudder which acts by cancelling the trailing vortices from the tip of propeller slipstream leads to increase of thrust and torque of propeller. There was, as expected, a difference in the velocity concentration between propeller only and propeller-hull interaction. The effects of propeller and rudder on the velocity profiles in the region for the LNG carrier in shallow water are clearly identified. Especially in very shallow water, (h/T = 1.1), the extreme velocity profile is concentrated in vicinity of top part of the stern and seabed regions.
机译:计算流体动力学(CFD)代码最近被用作了解流量特性(例如螺旋桨周围尾流发展)的有效工具。本文提出了深吃水LNG船尾部螺旋桨和方向舵作用在浅水区船尾区流动特性的数值模型。建模是基于B5-75型螺旋桨进行的,该螺旋桨的直径(D)为7.7m,由荷兰MARIN设计。 ANSYS Fluent版本12软件用于求解Reynold平均Navier Stokes(RANS)方程,ICEM CFD作为网格生成器。螺旋桨在基于3D不可压缩Navier-stokes求解器的流场中使用四层非结构化网格进行了啮合。在ANSYS Fluent中应用了两个湍流模型。这是用于稳定模拟的标准k-ε(k-e)模型和用于非稳定模拟的瞬态剪应力传递(SST)k-ω(k-α)。对于计算领域,螺旋桨叶片安装在两个有限的长恒定半径圆柱体上。开发了两种类型的圆柱域:定子域和转子域。对于定子域,叶片的入口流量为2D,出口流量为6D,外边界为3.6D。转子域的上游保持在0.2D,下游保持在0.4D和0.7D之间,外边界在1.4D。通过使用诸如多参考框架(MRF)和滑动网格(SM)方法之类的定转子方法,在转子域中模拟了湍流模型。与已发表的实验进行了比较,并广泛研究了数值解对计算参数的依赖性。将螺旋桨的推力和扭矩与已发布的实验进行比较时,通常会预测出很小的误差。在开放水域测试中,螺旋桨的性能差异约为10%,这可能是由于网格策略以及网格分辨率和质量所致。还研究了螺旋桨的性能。结果发现,当舵偏向-70和-200时,置于螺旋桨前方的舵提高了螺旋桨的效率,并产生了更大的推力增量。通过抵消螺旋桨滑流尖端的尾随涡而起作用的舵的存在会导致螺旋桨的推力和扭矩增加。正如预期的那样,仅螺旋桨和螺旋桨-船体相互作用之间的速度集中存在差异。清楚地确定了螺旋桨和舵对浅水中LNG船所在区域的速度剖面的影响。特别是在非常浅的水中(h / T = 1.1),极端速度剖面集中在船尾和海底区域的顶部附近。

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