{"title":"潮汐涡轮叶片涡发生器设计","authors":"M. Manolesos, Nicholas Kaufmann, George Papadakis","doi":"10.36688/ewtec-2023-343","DOIUrl":null,"url":null,"abstract":"Increasing tidal turbine performance through innovation is crucial if the cost of tidal energy is to become competitive compared to other sources of energy. The present investigation deals with the application of Vortex Generators (VGs) on tidal turbines in view of increasing their performance. The more mature wind energy industry uses passive VGs either as a retrofit or in the blade design process to reduce separation at the inboard part of wind turbine blades. Tidal turbine blades also experience flow separation and here we examine whether passive vane VGs can be used to reduce or suppress that separated flow. \nVortex generators (VGs) in various forms have been used and studied for flow separation control on wings since the 1940s [1]. Their working principle is relatively simple: they generate streamwise vortices that energise the boundary layer on the surface they are attached to, by bringing high momentum fluid closer to the surface [2]. This mechanism has been described by various researchers [3–6], while a number of studies have provided optimization guidelines under a variety of flow conditions [7–13]. \nIn the present investigation, a VG configuration is selected following a thorough wind tunnel campaign. It is found that sizing parameters for the tidal turbine profile are very similar to the wind turbine relevant literature [13,14]. The best performing vane VG configuration had a height of 0.007c, which corresponded to half the local boundary layer height (0.5δ) for operational Reynolds numbers. The results are also used to validate a Reynolds Averaged Navier Stokes (RANS) VG modelling approach using the BAY model [15]. The validated method is used to simulate the flow past a tidal turbine in both model size (1:8) and full scale, see Figure 1. The results show that VGs do suppress flow separation in both cases. However, and importantly, it is revealed that the significance of rotational effects is such that when deciding VG placement locations, only the full size blade should be considered. In the interest of brevity, the performance increase caused by a standard VG configuration is show in Figure 2, where a power coefficient improvement of 1.05% is predicted at λ=3. Figure 3 shows the effect on the normal and tangential forces on the blade. In the final paper and presentation, the results for different VG locations will be included and analysed in detail.","PeriodicalId":201789,"journal":{"name":"Proceedings of the European Wave and Tidal Energy Conference","volume":"29 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2023-09-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Designing Vortex Generators for Tidal Turbine Blades\",\"authors\":\"M. Manolesos, Nicholas Kaufmann, George Papadakis\",\"doi\":\"10.36688/ewtec-2023-343\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Increasing tidal turbine performance through innovation is crucial if the cost of tidal energy is to become competitive compared to other sources of energy. The present investigation deals with the application of Vortex Generators (VGs) on tidal turbines in view of increasing their performance. The more mature wind energy industry uses passive VGs either as a retrofit or in the blade design process to reduce separation at the inboard part of wind turbine blades. Tidal turbine blades also experience flow separation and here we examine whether passive vane VGs can be used to reduce or suppress that separated flow. \\nVortex generators (VGs) in various forms have been used and studied for flow separation control on wings since the 1940s [1]. Their working principle is relatively simple: they generate streamwise vortices that energise the boundary layer on the surface they are attached to, by bringing high momentum fluid closer to the surface [2]. This mechanism has been described by various researchers [3–6], while a number of studies have provided optimization guidelines under a variety of flow conditions [7–13]. \\nIn the present investigation, a VG configuration is selected following a thorough wind tunnel campaign. It is found that sizing parameters for the tidal turbine profile are very similar to the wind turbine relevant literature [13,14]. The best performing vane VG configuration had a height of 0.007c, which corresponded to half the local boundary layer height (0.5δ) for operational Reynolds numbers. The results are also used to validate a Reynolds Averaged Navier Stokes (RANS) VG modelling approach using the BAY model [15]. The validated method is used to simulate the flow past a tidal turbine in both model size (1:8) and full scale, see Figure 1. The results show that VGs do suppress flow separation in both cases. However, and importantly, it is revealed that the significance of rotational effects is such that when deciding VG placement locations, only the full size blade should be considered. In the interest of brevity, the performance increase caused by a standard VG configuration is show in Figure 2, where a power coefficient improvement of 1.05% is predicted at λ=3. Figure 3 shows the effect on the normal and tangential forces on the blade. 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引用次数: 0
摘要
如果要使潮汐能的成本与其他能源相比具有竞争力,通过创新来提高潮汐能涡轮机的性能是至关重要的。本文研究了涡发生器在潮汐水轮机上的应用,以期提高其性能。更成熟的风能行业使用被动VGs作为改造或在叶片设计过程中减少风力涡轮机叶片内侧部分的分离。潮汐涡轮叶片也经历了流动分离,在这里我们研究被动叶片VGs是否可以用来减少或抑制分离的流动。自20世纪40年代以来,各种形式的涡发生器(Vortex generator, vg)被用于机翼上的流动分离控制[1]。它们的工作原理相对简单:它们产生流向涡旋,通过使高动量流体更接近表面,从而为它们附着的表面边界层提供能量[2]。这一机制已被许多研究者描述[3-6],同时也有许多研究提供了各种流动条件下的优化指南[7-13]。在目前的研究中,在彻底的风洞运动之后选择了VG配置。研究发现,潮汐机剖面的尺寸参数与风力机相关文献[13,14]非常相似。表现最佳的叶片VG配置高度为0.007c,相当于工作雷诺数下局部边界层高度(0.5δ)的一半。研究结果还用于验证使用BAY模型的Reynolds average Navier Stokes (RANS) VG建模方法[15]。采用验证的方法在模型尺寸(1:8)和满尺尺寸下模拟潮汐涡轮机的水流,如图1所示。结果表明,在两种情况下,VGs都抑制了流动分离。然而,重要的是,它揭示了旋转效应的重要性,当决定VG放置位置时,只应该考虑全尺寸叶片。为了简洁起见,图2显示了标准VG配置带来的性能提升,其中在λ=3时,功率系数提升了1.05%。图3显示了对叶片上的法向力和切向力的影响。在最后的论文和演示中,将包括不同VG位置的结果并进行详细分析。
Designing Vortex Generators for Tidal Turbine Blades
Increasing tidal turbine performance through innovation is crucial if the cost of tidal energy is to become competitive compared to other sources of energy. The present investigation deals with the application of Vortex Generators (VGs) on tidal turbines in view of increasing their performance. The more mature wind energy industry uses passive VGs either as a retrofit or in the blade design process to reduce separation at the inboard part of wind turbine blades. Tidal turbine blades also experience flow separation and here we examine whether passive vane VGs can be used to reduce or suppress that separated flow.
Vortex generators (VGs) in various forms have been used and studied for flow separation control on wings since the 1940s [1]. Their working principle is relatively simple: they generate streamwise vortices that energise the boundary layer on the surface they are attached to, by bringing high momentum fluid closer to the surface [2]. This mechanism has been described by various researchers [3–6], while a number of studies have provided optimization guidelines under a variety of flow conditions [7–13].
In the present investigation, a VG configuration is selected following a thorough wind tunnel campaign. It is found that sizing parameters for the tidal turbine profile are very similar to the wind turbine relevant literature [13,14]. The best performing vane VG configuration had a height of 0.007c, which corresponded to half the local boundary layer height (0.5δ) for operational Reynolds numbers. The results are also used to validate a Reynolds Averaged Navier Stokes (RANS) VG modelling approach using the BAY model [15]. The validated method is used to simulate the flow past a tidal turbine in both model size (1:8) and full scale, see Figure 1. The results show that VGs do suppress flow separation in both cases. However, and importantly, it is revealed that the significance of rotational effects is such that when deciding VG placement locations, only the full size blade should be considered. In the interest of brevity, the performance increase caused by a standard VG configuration is show in Figure 2, where a power coefficient improvement of 1.05% is predicted at λ=3. Figure 3 shows the effect on the normal and tangential forces on the blade. In the final paper and presentation, the results for different VG locations will be included and analysed in detail.