{"data":{"id":"10.4121/dbd831b5-8d6d-4ae2-9860-2d6a7a1be58e","type":"dois","attributes":{"doi":"10.4121/dbd831b5-8d6d-4ae2-9860-2d6a7a1be58e","prefix":"10.4121","suffix":"dbd831b5-8d6d-4ae2-9860-2d6a7a1be58e","identifiers":[],"alternateIdentifiers":[],"creators":[{"name":"Becker, Marcus","nameType":"Personal","givenName":"Marcus","familyName":"Becker","nameIdentifiers":[{"nameIdentifier":"0000-0003-4250-7654","nameIdentifierScheme":"https://orcid.org/"}],"affiliation":[]},{"name":"Lejeune, Maxime","givenName":"Maxime","familyName":"Lejeune","affiliation":[],"nameIdentifiers":[]}],"titles":[{"title":"FLORIDyn (OFF toolbox) Code and input files underlying the publication: Wind pattern clustering of high frequent field measurements for dynamic wind farm flow control"}],"publisher":"4TU.ResearchData","container":{},"publicationYear":2024,"subjects":[{"subject":"Mechanical Engineering","subjectScheme":"Australian and New Zealand Standard Research Classification (ANZSRC), 2008","classificationCode":"0913"},{"subject":"FOS: Mechanical engineering","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"Other Engineering","subjectScheme":"Australian and New Zealand Standard Research Classification (ANZSRC), 2008","classificationCode":"0999"},{"subject":"FOS: Other engineering and technologies","schemeUri":"http://www.oecd.org/science/inno/38235147.pdf","subjectScheme":"Fields of Science and Technology (FOS)"},{"subject":"Engineering","subjectScheme":"Australian and New Zealand Standard Research Classification (ANZSRC), 2008","classificationCode":"09"},{"subject":"FLORIDyn"},{"subject":"Wind Farm Flow Control"},{"subject":"Wake model"},{"subject":"Engineering wake model"},{"subject":"dynamic wind farm flow control"},{"subject":"wind farm simulation"}],"contributors":[{"name":"TU Delft, Faculty Of Mechanical Engineering, Delft Center For Systems And Control","nameType":"Organizational","affiliation":[],"contributorType":"Other","nameIdentifiers":[]}],"dates":[{"date":"2024-01-24","dateType":"Issued"}],"language":"en","types":{"ris":"COMP","bibtex":"misc","citeproc":"article","schemaOrg":"SoftwareSourceCode","resourceType":"Software","resourceTypeGeneral":"Software"},"relatedIdentifiers":[],"relatedItems":[],"sizes":[],"formats":[".py, .yaml, .csv, .graphml"],"version":"1","rightsList":[{"rights":"BSD 3-Clause \"New\" or \"Revised\" License","rightsUri":"https://opensource.org/licenses/BSD-3-Clause","schemeUri":"https://spdx.org/licenses/","rightsIdentifier":"bsd-3-clause","rightsIdentifierScheme":"SPDX"}],"descriptions":[{"description":"Python implementation of the FLORIDyn code [1] in the OFF toolbox, as well as the input files used for the publication \"Wind pattern clustering of high frequent field measurements for dynamic wind farm flow control\", M Becker, D Allaerts and JW van Wingerden, in preparation for the TORQUE 2024 conference.\u003cbr\u003eThe yaml files contain the baseline orientation (misalignment angle = 0 deg) and optimised angles. The C1 to C5 addition in the name refers to the wind direction change case that is investigated. The optimised angles have beed derived using FLORIS [2] and are given in separate files for convenience.\u003cbr\u003eTo run the code FLORIS [2] needs to be installed. In addition the DTU 10MW reference turbine [3] is used in the simulations. The required .yaml is provided with this code and needs to be added to the FLORIS turbine library. Go to 03_Code/main.py and run the selected case.\u003cbr\u003eThe farm power of all simulations in FLORIDyn in given in the files FarmPower*.csvTo use them in Matlab, call:\u003cbr\u003efarm_pow = readmatrix(\"FarmPowerNoYaw.csv\");farm_pow = reshape(farm_pow, 5, length(1:2:359), [] );\u003cbr\u003eDimension 1 is along the cases, dimension 2 along the wind directions and dimension 3 along time (4:4:2000).E.g. to plot the power for case C4 starting at 201deg callplot(4:4:2000, farm_pow(4, (201+1)/2, :))\u003cbr\u003e[1] https://iopscience.iop.org/article/10.1088/1742-6596/2265/3/032103/meta[2] https://github.com/NREL/floris[3] https://backend.orbit.dtu.dk/ws/portalfiles/portal/55645274/The_DTU_10MW_Reference_Turbine_Christian_Bak.pdf","descriptionType":"Abstract"}],"geoLocations":[],"fundingReferences":[],"xml":"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