Theoretical modelling of the three-dimensional wake of vertical axis turbines

IF 2.8 Q2 MECHANICS
P. Ouro, Maxime Lazennec
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引用次数: 4

Abstract

Graphical Abstract Vertical axis turbine (VAT) arrays can achieve larger power generation per land area than their horizontal axis counterparts, due to the positive synergy from clustering VATs in close proximity. The VATs generate a three-dimensional wake that evolves unevenly over the vertical and transverse directions according to two governing length scales, namely the rotor's diameter and height. Theoretical wake models need to capture such a complex wake dynamics to enable reliable array design that maximises energy output. This paper presents two new theoretical VAT wake models based on super-Gaussian and Gaussian shape functions, which account for the three-dimensional velocity deficit distribution in the wake. The super-Gaussian model represents the initial elliptical shape with the superposition of vertical and lateral shape functions that progressively converge into an axisymmetric circular-shaped wake at a downstream distance that depends on the rotor's height-to-diameter aspect ratio. Our Gaussian model improves the initial wake width prediction taking into account the rectangular rotor's cross-section. Our models were well validated with large-eddy simulations (LES) of single VATs with varying aspect ratios and thrust coefficients operating in an atmospheric boundary layer. The super-Gaussian model attained a good agreement with LES in both near and far wake, whilst the Gaussian model represented well the far-wake region.
垂直轴水轮机三维尾迹的理论建模
垂直轴涡轮机(VAT)阵列可以实现比水平轴更大的每土地面积发电量,这是由于近距离聚集的VAT的积极协同作用。VATs产生三维尾流,根据两个控制长度尺度,即转子的直径和高度,在垂直和横向方向上不均匀地发展。理论尾流模型需要捕捉如此复杂的尾流动力学,以实现可靠的阵列设计,最大限度地提高能量输出。本文提出了基于超高斯和高斯形状函数的两种新的增值尾流理论模型,它们解释了尾流中的三维速度亏缺分布。超高斯模型表示初始椭圆形状与垂直和横向形状函数的叠加,在下游距离逐渐收敛成轴对称圆形尾迹,这取决于转子的高径长弦比。考虑到矩形转子的横截面,我们的高斯模型改进了初始尾迹宽度预测。我们的模型通过在大气边界层中运行的具有不同展弦比和推力系数的单个VATs的大涡模拟(LES)得到了很好的验证。超高斯模型在近尾流和远尾流区域均与LES吻合较好,而高斯模型在远尾流区域表现较好。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
CiteScore
2.40
自引率
0.00%
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