Underlying data, figures and scripts of the publication: Wake Scaling of Actuator Discs in Different Aspect Ratios
doi: 10.4121/12923897.v4
Datacite citation style:
Fulvio Scarano; Simao Ferreira, Carlos; Huang, Ming; Andrea Sciacchitano (2021): Underlying data, figures and scripts of the publication: Wake Scaling of Actuator Discs in Different Aspect Ratios. Version 4. 4TU.ResearchData. dataset. https://doi.org/10.4121/12923897.v4
Other citation styles (APA, Harvard, MLA, Vancouver, Chicago, IEEE) available at Datacite
Dataset
choose version:
version 5 - 2022-11-04 (latest)
version 4 - 2021-10-15
version 3 - 2021-08-05
version 2 - 2021-07-06
version 1 - 2020-09-14
CC0
This online resource contains raw dataset, MATLAB scripts for some kinematic wake models, and underlying data for the rticle under revision, "Actuator disc diameter formulation for vertical-axis wind turbine kinematic wake modelling"
history
- 2020-09-14 first online
- 2021-10-15 published, posted
publisher
4TU.ResearchData
funding
- Delft University of Technology
- China scholarship council
organizations
TU Delft, Faculty of Aerospace Engineering, Department of Aerodynamics, Wind Energy, Flight Performance & Propulsion (AWEP)
DATA
files (55)
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1,568 bytesMD5:
dc0734735d419a30c81a95ce9192578eREADME.md -
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5b7a06f874d47caa8e90515d19d160a0BPA_HAWT.m -
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895e02d8bb029c8eb820af6f455f4580BPA_VAWT.m -
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eebd62b4b05417474d23e8fe931d35b9fig10_Stream-wise velocity contours and in-plane velocity vectors pattern at four cross sections downstream of the circular actuator..png -
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23d8c78a19db4f7400ffaeb44566e496fig11_Stream-wise velocity contours and in-plane velocity vectors at cross sections downstream of the square actuator..png -
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82fbfe605c81280aa8acb6e2fec315f2fig12_Stream-wise velocity contours and in-plane velocity vectors at cross sections downstream of the rectangular actuator.png -
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9230ef324ec9d9d25778843973deba7efig13Vorticity magnitude over four cross sections downstream of the circular actuator.png -
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373b222aba5bb6d969b0bcd73f9df434fig14_Vorticity magnitude over four cross sections downstream of the square actuator.png -
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1bca8f96b3bd093ed3c8f4a06f8d0312fig15_Vorticity magnitude contours over four cross sections downstream of the rectangular actuator..png -
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65323708236ad51d8d4c5b575dd3dd22fig16_Comparison of averaged stream-wise velocity deficit along X direction for the circular actuator.png -
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83f4c773cf7b0acc04cc24163912404ffig17_Comparison of stream-wise velocity profiles at different downstream locations for the case of a circle actuator.png -
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ae302db682db8954356116022a55ef07fig18_Comparison of cross-section averaged stream-wise velocity deficit along X direction.png -
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1e22d592d7fcc76f258bc17f300c9571fig19_Comparison of stream-wise velocity deficit averaged in upper half of the projected area along X direction (normalized by Deq).png -
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fb37379a880e893c827778e3e536fe34fig1_Schematic representation of a HAWT wake modelled according to Jensen (top), Larsen (middle) and the BPA (bottom), respectively. Colour-coded momentum deficit (blue fo.png -
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93437a678dd1bf6d81cf21688bc37253fig20_Comparison of stream-wise velocity deficit averaged in upper half of the projected area along X direction (normalized by D).png -
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72c40efd622604e54dcacb856e3e2596fig21_Representation of the experimental data (stream-wise velocity profile along Z), when normalized by Deq. (Labels follow legend from figure 20).png -
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3b8a0f7a4f870e4d9db7555b92c0fffafig22_Representation of the experimental data (stream-wise velocity profile along Y), when normalized by Deq. (Labels follow legend from figure 20).png -
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b9a8dced2839e597b3f4742eab2016c3fig23_Representation of the experimental data (stream-wise velocity profile along Z), when normalized by D. (Labels follow legend from figure 20).png -
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b7463e8a65891d64599bfc5e2f250af7fig24_Representation of the experimental data (stream-wise velocity profile along Y), when normalized by D (Labels follow legend from figure 20).png -
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613634df46561b7aac4c9ddbb48eaaa2fig25_Representation of the experimental data (stream-wise velocity profile along Z), when X is normalized by D, and Z is normalized by H. (Labels follow legend from figur.png -
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df8b40745c4eea57b5b20c4da53f9e9afig26_Representation of the experimental data (stream-wise velocity profile along Y), when X is normalized by D, and Y is normalized by D. (Labels follow legend from figur.png -
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c836ca81e7416d5f6de5cd77ac80b3b0fig27_Colour contours of the time-averaged and normalized stream-wise velocity of the circular actuator in the XY-plane at ZD = 0. Measurements by planar (left) and roboti.png -
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b60ef17daaff55e5428e048e460d7451fig2_Schematic plot of the Jensen-like rectangular wake characterisation based on both D and H (Abkar 2018), Deq (Shamsoddin & Porté-Agel, 2020) and D(present work).png -
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d2c006ca4f491afaf5d707a0aebf13eafig3_Geometrical details of circular, square and rectangular porous plates..png -
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1757e7b5cdb015c1be42dccb96acf44efig4_Layout of experiments wind tunnel and square actuator at its exit. Robotic arm and coaxial volumetric velocimeter, with an indication of measurement region..png -
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36d243c40f9a396a8d40935dca26a46afig5_Top- (up), and Front- (bottom) view of the porous plate (origin defined at the centre of the plate) and the IFOVs, the overall measurement domain is marked by the red.png -
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193e29ad8aae3144bde0836aa9232b09fig6_Raw (left) and pre-processed (right) CVV images of HFSB tracers, with the square actuator surface in view..png -
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0a1c6c461a7a2515329c85c340602cc3fig7_Thrust coefficient as a function of porosity; comparison between current results and literature. .png -
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7b5bbb69570ee8a8c80bae0993fb5715fig8_Contours of time-averaged and normalized stream-wise velocity in the XY-plane at ZD = 0. Circular (top), square (middle) and rectangular actuator (bottom)..png -
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be956ab39f76da5f4c195502ef8fe6c6fig9_Contours of time-averaged and normalized stream-wise velocity in the XZ-plane at YD = 0. Circular (top), square (middle) and rectangular actuator (bottom).png -
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ae21d3f165494be9addc57bb8d824111Figure10_btm.dat -
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