Implementation of Tidal Stream Turbines and Tidal Barrage Structures in DG-SWEM

A. Schnabl, Túlio Marcondes Moreira, Dylan Wood, E. Kubatko, G. Houlsby, R. McAdam, T. Adcock
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引用次数: 7

Abstract

There are two approaches to extracting power from tides — either turbines are placed in areas of strong flows or turbines are placed in barrages enabling the two sides of the barrage to be closed off and a head to build up across the barrage. Both of these energy extraction approaches will have a significant back effect on the flow, and it is vital that this is correctly modelled in any numerical simulation of tidal hydrodynamics. This paper presents the inclusion of both tidal stream turbines and tidal barrages in the depth-averaged shallow water equation model DG-SWEM. We represent the head loss due to tidal stream turbines as a line discontinuity — thus we consider the turbines, and the energy lost in local wake-mixing behind the turbines, to be a sub-grid scale processes. Our code allows the inclusion of turbine power and thrust coefficients which are dependent on Froude number, turbine blockage, and velocity, but can be obtained from analytical or numerical models as well as experimental data. The barrage model modifies the existing culvert model within the code, replacing the original cross-barrier pipe equations. At the location of this boundary, velocities through sluice gates are calculated according to the orifice equation. For simulating the turbines, a Hill Chart for low head bulb turbines provided by Andritz Hydro is used. We demonstrate the implementations on both idealised geometries where it is straightforward to compare against other models and numerical simulations of real candidate sites for tidal energy in Malaysia and the Bristol Channel.
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潮汐能水轮机和潮汐能拦河坝结构在DG-SWEM中的实现
从潮汐中提取能量有两种方法——要么将涡轮机放置在水流强的区域,要么将涡轮机放置在拦河坝中,使拦河坝的两侧关闭,并在拦河坝上建立一个水头。这两种能量提取方法都会对水流产生明显的反向影响,在潮汐流体动力学的任何数值模拟中正确地模拟这种影响是至关重要的。本文提出了在深度平均浅水方程模型DG-SWEM中同时包含潮汐水轮机和潮汐坝。我们将潮汐流涡轮机的水头损失表示为线路不连续,因此我们认为涡轮机和涡轮机后面局部尾流混合的能量损失是一个亚电网尺度的过程。我们的规范允许包含涡轮功率和推力系数,这些系数取决于弗劳德数,涡轮堵塞和速度,但可以从分析或数值模型以及实验数据中获得。拦河坝模型修改了规范中现有的涵洞模型,取代了原有的跨障管方程。在该边界处,根据孔口方程计算通过水闸的速度。为了模拟涡轮机,使用了Andritz Hydro提供的低水头灯泡涡轮机的山图。我们展示了在理想的几何形状上的实现,它可以直接与其他模型和马来西亚和布里斯托尔海峡实际候选潮汐能地点的数值模拟进行比较。
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