{"title":"基于流固耦合法的Savonius和Icewind风力机叶片设计非定常仿真","authors":"Z. Lillahulhaq, Vivien S. Djanali","doi":"10.1063/1.5138264","DOIUrl":null,"url":null,"abstract":"Wind turbine performance can be increased by using the optimum shape of the blade. Most of the previous numerical studies on Savonius wind turbine simulation used constant angular velocity as input data. Usually, the value of constant angular velocity was obtained from experimental data. In the actual case, the rotation of the rotor, i.e. the angular velocity of the blades, results from the interaction between fluids around the wind turbine with the turbine blades, in which there are changes of the moment of inertia. Rotation of the wind turbine can be simulated using the fluid-structure interaction method with one-degree of freedom. This study compares the performance of a rotor turbine using straight Savonius blades, to that using the Icewind turbine blades. In the steady and unsteady simulations, fluid was defined as incompressible, viscous, and uniform air which flow from inlet free stream. The simulation object rotates in one-degree of freedom in the overset mesh area. Icewind turbine generates higher coefficient power compares to the standard Savonius turbine, when it operates at very low wind speed, with the inlet free stream velocity below 4 m/s. This phenomenon is affected by the unsymmetrical shape of Icewind which allowed the fluid flow behind the reversing blade and sweep away the wake area, particularly effective at very low wind speed. The Savonius wind turbine, which is configured with endplates and overlap blades, rotates in high angular velocity and generates the highest peak coefficient of power. Fluid from the advancing blade is flowing through the overlap. The overlap flow fills the wake area and reduces backflow behind the reversing blade.Wind turbine performance can be increased by using the optimum shape of the blade. Most of the previous numerical studies on Savonius wind turbine simulation used constant angular velocity as input data. Usually, the value of constant angular velocity was obtained from experimental data. In the actual case, the rotation of the rotor, i.e. the angular velocity of the blades, results from the interaction between fluids around the wind turbine with the turbine blades, in which there are changes of the moment of inertia. Rotation of the wind turbine can be simulated using the fluid-structure interaction method with one-degree of freedom. This study compares the performance of a rotor turbine using straight Savonius blades, to that using the Icewind turbine blades. In the steady and unsteady simulations, fluid was defined as incompressible, viscous, and uniform air which flow from inlet free stream. The simulation object rotates in one-degree of freedom in the overset mesh area. 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引用次数: 6

摘要

风力涡轮机的性能可以通过使用最佳的叶片形状来提高。以往对Savonius风力机模拟的数值研究大多采用恒角速度作为输入数据。通常,恒角速度值是由实验数据得到的。在实际情况中,转子的转动,即叶片的角速度,是风力机周围流体与风力机叶片相互作用的结果,其中存在转动惯量的变化。采用一自由度流固耦合方法可以模拟风力机的转动。这项研究比较了使用直萨沃纽斯叶片的转子涡轮机和使用冰风涡轮叶片的转子涡轮机的性能。在定常和非定常模拟中,流体被定义为不可压缩的、粘性的、均匀的、从进口自由流流出的空气。仿真对象在偏移网格区域内以一个自由度旋转。在非常低的风速下,当入口自由流速度低于4 m/s时,冰风涡轮机比标准的Savonius涡轮机产生更高的系数功率。这种现象受冰风的不对称形状的影响,它允许流体在倒转叶片后面流动,并扫走尾迹区域,在非常低的风速下特别有效。Savonius风力涡轮机配置了端板和重叠叶片,以高角速度旋转,产生最高的峰值功率系数。流体从前进的叶片流过重叠部分。重叠流填充尾迹区域,减少倒转叶片后方的回流。风力涡轮机的性能可以通过使用最佳的叶片形状来提高。以往对Savonius风力机模拟的数值研究大多采用恒角速度作为输入数据。通常,恒角速度值是由实验数据得到的。在实际情况中,转子的转动,即叶片的角速度,是风力机周围流体与风力机叶片相互作用的结果,其中存在转动惯量的变化。采用一自由度流固耦合方法可以模拟风力机的转动。这项研究比较了使用直萨沃纽斯叶片的转子涡轮机和使用冰风涡轮叶片的转子涡轮机的性能。在定常和非定常模拟中,流体被定义为不可压缩的、粘性的、均匀的、从进口自由流流出的空气。仿真对象在偏移网格区域内以一个自由度旋转。冰风涡轮机产生高…
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Unsteady simulations of Savonius and Icewind turbine blade design using fluid-structure interaction method
Wind turbine performance can be increased by using the optimum shape of the blade. Most of the previous numerical studies on Savonius wind turbine simulation used constant angular velocity as input data. Usually, the value of constant angular velocity was obtained from experimental data. In the actual case, the rotation of the rotor, i.e. the angular velocity of the blades, results from the interaction between fluids around the wind turbine with the turbine blades, in which there are changes of the moment of inertia. Rotation of the wind turbine can be simulated using the fluid-structure interaction method with one-degree of freedom. This study compares the performance of a rotor turbine using straight Savonius blades, to that using the Icewind turbine blades. In the steady and unsteady simulations, fluid was defined as incompressible, viscous, and uniform air which flow from inlet free stream. The simulation object rotates in one-degree of freedom in the overset mesh area. Icewind turbine generates higher coefficient power compares to the standard Savonius turbine, when it operates at very low wind speed, with the inlet free stream velocity below 4 m/s. This phenomenon is affected by the unsymmetrical shape of Icewind which allowed the fluid flow behind the reversing blade and sweep away the wake area, particularly effective at very low wind speed. The Savonius wind turbine, which is configured with endplates and overlap blades, rotates in high angular velocity and generates the highest peak coefficient of power. Fluid from the advancing blade is flowing through the overlap. The overlap flow fills the wake area and reduces backflow behind the reversing blade.Wind turbine performance can be increased by using the optimum shape of the blade. Most of the previous numerical studies on Savonius wind turbine simulation used constant angular velocity as input data. Usually, the value of constant angular velocity was obtained from experimental data. In the actual case, the rotation of the rotor, i.e. the angular velocity of the blades, results from the interaction between fluids around the wind turbine with the turbine blades, in which there are changes of the moment of inertia. Rotation of the wind turbine can be simulated using the fluid-structure interaction method with one-degree of freedom. This study compares the performance of a rotor turbine using straight Savonius blades, to that using the Icewind turbine blades. In the steady and unsteady simulations, fluid was defined as incompressible, viscous, and uniform air which flow from inlet free stream. The simulation object rotates in one-degree of freedom in the overset mesh area. Icewind turbine generates highe...
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