| 研究生: |
陳泳齊 Chen, Yung-Chi |
|---|---|
| 論文名稱: |
以 OpenFOAM 平台中開發三種風機模型模擬單一風機後方尾流之大渦模擬研究 Large-Eddy Simulation of the Wake Flow behind a Standalone Turbine Using Three Turbine Models in OpenFOAM |
| 指導教授: |
吳毓庭
Wu, Yu-Ting |
| 學位類別: |
碩士 Master |
| 系所名稱: |
工學院 - 工程科學系 Department of Engineering Science |
| 論文出版年: | 2026 |
| 畢業學年度: | 114 |
| 語文別: | 英文 |
| 論文頁數: | 94 |
| 中文關鍵詞: | 計算流體力學 、OpenFOAM 、大渦模擬 、WALE 、致動圓盤模型 、致動線 模型 、風力機尾流 、紊流動能 |
| 外文關鍵詞: | Computational Fluid Dynamics, OpenFOAM, Large-Eddy Simulation, WALE, Actuator-Disk Method, Actuator-Line Method, Wind Turbine Wake, Turbulent Kinetic Energy |
| 相關次數: | 點閱:30 下載:2 |
| 分享至: |
| 查詢本校圖書館目錄 查詢臺灣博碩士論文知識加值系統 勘誤回報 |
本研究以 OpenFOAM 建立大渦模擬架構,探討時變入流條件下之風力機尾流特性,並比較不同致動器型風力機模型與網格解析度對尾流預測之影響。研究中採用 WALE 次網格尺度模型與 pimpleFoam 求解非穩態不可壓縮流場,並以體積力源項表示風力機氣動效應,包含 ADM-NR、ADM-R 與 ALM。所有案例皆採用相同時變入流條件,並以風洞實驗資料作為比較基準。分析物理量包含時間平均流向速度、流向紊流強度、垂直紊流動量通量,以及 resolved TKE budget terms。
結果顯示,ADM-R1 與最細網格 ADM-R0 具有相近之尾流預測結果,並可在計算成本與預測能力間取得較佳平衡。相較於 ADM-NR,ADM-R1 因考慮非均勻徑向載重與轉子誘導旋轉,可改善近尾流預測。ALM 結果顯示,nacelle 與 tower 源項主要影響 hub 附近與尾流下方之近尾流區域,而降低網格解析度會使紊流相關分布更為平滑。Resolved TKE budget 分析顯示,尾流紊流能量主要由剪切層中的 shear production 產生,並透過 advection 與 turbulent transport 重新分布。整體而言,ADM-R1 可提供合理且成本較低之尾流預測,而 ALM-1 則能提供較細緻之近尾流結構。
This study establishes an OpenFOAM-based large-eddy simulation framework to investigate wind turbine wake characteristics under time-varying inflow conditions and to compare the effects of actuator-type wind turbine models and grid resolution on wake prediction. The WALE subgrid-scale model and pimpleFoam solver are adopted for the unsteady incompressible flow simulation. The turbine-induced aerodynamic effects are introduced into the momentum equation through body-force source terms, including ADM-NR, ADM-R, and ALM. All cases use the same time-varying inflow condition and are compared with wind-tunnel experimental data. The wake characteristics are evaluated using the time-averaged streamwise velocity, streamwise turbulence intensity, vertical turbulent momentum flux, and resolved TKE budget terms.
The results show that ADM-R1 provides wake predictions close to the finest ADM-R0 case while achieving a better balance between computational cost and predictive capability. Compared with ADM-NR, ADM-R1 improves the near-wake prediction by considering non-uniform radial loading and rotor-induced rotation. The ALM results indicate that the nacelle and tower source terms mainly affect the near-wake region around the hub and lower wake, while reducing grid resolution smooths the turbulence-related distributions. The resolved TKE budget analysis shows that wake turbulence is mainly generated by shear production in the wake shear layer and redistributed by advection and turbulent transport. Overall, ADM-R1 provides reasonable wake predictions with lower computational cost, whereas ALM-1 gives a more detailed near-wake structure.
[1] Amiri, M. M., Shadman, M., and Estefen, S. F., “A review of physical and numerical modeling techniques for horizontal-axis wind turbine wakes,” Renewable and Sustainable Energy Reviews, Vol. 193, 2024, Article 114279.
[2] Eidi, A., Ghiassi, R., Yang, X. I. A., and Abkar, M., “Model-form uncertainty quantification in RANS simulations of wakes and power losses in wind farms,” Renewable Energy, Vol. 179, 2021, pp. 2212–2223.
[3] Wu, Y.-T., and Porté-Agel, F., “Large-Eddy Simulation of Wind-Turbine Wakes: Evaluation of Turbine Parametrisations,” Boundary-Layer Meteorology, Vol. 138, 2011, pp. 345–366.
[4] Porté-Agel, F., Meneveau, C., and Parlange, M. B., “A scale-dependent dynamic model for large-eddy simulation: application to a neutral atmospheric boundary layer,” Journal of Fluid Mechanics, Vol. 415, 2000, pp. 261–284.
[5] Arya, N., and De, A., “Effect of grid sensitivity on the performance of wall adapting SGS models for LES of swirling and separating–reattaching flows,” Computers & Mathematics with Applications, Vol. 78, No. 6, 2019, pp. 2035–2051.
[6] Naderi, S., Parvanehmasiha, S., and Torabi, F., “Modeling of horizontal axis wind turbine wakes in Horns Rev offshore wind farm using an improved actuator disc model coupled with computational fluid dynamic,” Energy Conversion and Management, Vol. 171, 2018, pp. 953–968.
[7] Sørensen, J. N., and Shen, W. Z., “Numerical Modeling of Wind Turbine Wakes,” Journal of Fluids Engineering, Vol. 124, No. 2, 2002, pp. 393–399.
[8] Martínez-Tossas, L. A., Churchfield, M. J., and Leonardi, S., “Large eddy simulations of the flow past wind turbines: actuator line and disk modeling,” Wind Energy, Vol. 18, No. 6, 2015, pp. 1047–1060.
[9] Jha, P. K., and Schmitz, S., “Actuator curve embedding – an advanced actuator line model,” Journal of Fluid Mechanics, Vol. 834, 2018, Article R2.
[10] Ali, N., Gatti, D., and Kornev, N., “Tailoring anisotropic synthetic inflow turbulence generator for wind turbine wake simulations,” Journal of Renewable and Sustainable Energy, Vol. 16, 2024, Article 043308.
[11] Munters, W., Meneveau, C., and Meyers, J., “Turbulent Inflow Precursor Method with Time-Varying Direction for Large-Eddy Simulations and Applications to Wind Farms,” Boundary-Layer Meteorology, Vol. 159, 2016, pp. 305–328.
[12] Chamorro, L. P., and Porté-Agel, F., “Effects of Thermal Stability and Incoming Boundary-Layer Flow Characteristics on Wind-Turbine Wakes: A Wind-Tunnel Study,” Boundary-Layer Meteorology, Vol. 136, 2010, pp. 515–533.
[13] Adedipe, T. A., Chaudhari, A., and Kauranne, T., “Impact of different forest densities on atmospheric boundary-layer development and wind-turbine wake,” Wind Energy, Vol. 23, No. 5, 2020, pp. 1165–1180.
[14] Stevens, R. J. A. M., Martínez-Tossas, L. A., and Meneveau, C., “Comparison of wind farm large eddy simulations using actuator disk and actuator line models with wind tunnel experiments,” Renewable Energy, Vol. 116, 2018, pp. 470–478.
[15] Hamlaoui, M. N., Smaili, A., Dobrev, I., Pereira, M., Fellouah, H., and Khelladi, S., “Numerical and experimental investigations of HAWT near wake predictions using Particle Image Velocimetry and Actuator Disk Method,” Energy, Vol. 238, 2022, Article 121660.
[16] Vermeer, L. J., Sørensen, J. N., and Crespo, A., “Wind Turbine Wake Aerodynamics,” Progress in Aerospace Sciences, Vol. 39, 2003, pp. 467–510.
[17] Sanderse, B., van der Pijl, S. P., and Koren, B., “Review of Computational Fluid Dynamics for Wind Turbine Wake Aerodynamics,” Wind Energy, Vol. 14, 2011, pp. 799–819.
[18] Bastankhah, M., and Porté-Agel, F., “A New Analytical Model for Wind-Turbine Wakes,” Renewable Energy, Vol. 70, 2014, pp. 116–123.
[19] Wu, Y.-T., and Porté-Agel, F., “Atmospheric Turbulence Effects on Wind-Turbine Wakes: An LES Study,” Energies, Vol. 5, 2012, pp. 5340–5362.
[20] Wu, Y.-T., and Porté-Agel, F., “Simulation of Turbulent Flow Inside and Above Wind Farms: Model Validation and Layout Effects,” Boundary-Layer Meteorology, Vol. 146, 2013, pp. 181–205.
[21] Revaz, T., and Porté-Agel, F., “Large-Eddy Simulation of Wind Turbine Flows: A New Evaluation of Actuator Disk Models,” Energies, Vol. 14, No. 13, 2021, Article 3745.
[22] Shapiro, C. R., Gayme, D. F., and Meneveau, C., “Filtered Actuator Disks: Theory and Application to Wind Turbine Models in Large Eddy Simulation,” Wind Energy, Vol. 22, No. 10, 2019, pp. 1414–1420.
[23] Martínez, L. A., Leonardi, S., Churchfield, M. J., and Moriarty, P. J., “A Comparison of Actuator Disk and Actuator Line Wind Turbine Models and Best Practices for Their Use,” 50th AIAA Aerospace Sciences Meeting including the New Horizons Forum and Aerospace Exposition, Nashville, Tennessee, 2012, AIAA 2012-0900.
[24] Yang, X., and Sotiropoulos, F., “A New Class of Actuator Surface Models for Wind Turbines,” Wind Energy, Vol. 21, No. 5, 2018, pp. 285–302.
[25] Jimenez, A., Crespo, A., Migoya, E., and Garcia, J., “Advances in Large-Eddy Simulation of a Wind Turbine Wake,” Journal of Physics: Conference Series, Vol. 75, 2007, Article 012041.
[26] Nicoud, F., and Ducros, F., “Subgrid-Scale Stress Modelling Based on the Square of the Velocity Gradient Tensor,” Flow, Turbulence and Combustion, Vol. 62, 1999, pp. 183–200.
[27] Lund, T. S., Wu, X., and Squires, K. D., “Generation of Turbulent Inflow Data for Spatially-Developing Boundary Layer Simulations,” Journal of Computational Physics, Vol. 140, 1998, pp. 233–258.
[28] Klein, M., Sadiki, A., and Janicka, J., “A Digital Filter Based Generation of Inflow Data for Spatially Developing Direct Numerical or Large Eddy Simulations,” Journal of Computational Physics, Vol. 186, 2003, pp. 652–665.
[29] Xie, Z.-T., and Castro, I. P., “Efficient Generation of Inflow Conditions for Large Eddy Simulation of Street-Scale Flows,” Flow, Turbulence and Combustion, Vol. 81, 2008, pp. 449–470.
[30] Calaf, M., Meneveau, C., and Meyers, J., “Large Eddy Simulation Study of Fully Developed Wind-Turbine Array Boundary Layers,” Physics of Fluids, Vol. 22, 2010, Article 015110.