FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W4365447492> ?p ?o ?g. }

• W4365447492 endingPage "556" @default.
• W4365447492 startingPage "535" @default.
• W4365447492 abstract "Abstract. The size of newly installed offshore wind farms increases rapidly. Planned offshore wind farm clusters have a rated capacity of several gigawatts and a length of up to 100 km. The flow through and around wind farms of this scale can be significantly different than the flow through and around smaller wind farms on the sub-gigawatt scale. A good understanding of the involved flow physics is vital for accurately predicting the wind farm power output as well as predicting the meteorological conditions in the wind farm wake. To date there is no study that directly compares small wind farms (sub-gigawatt) with large wind farms (super-gigawatt) in terms of flow effects or power output. The aim of this study is to fill this gap by providing this direct comparison by performing large-eddy simulations of a small wind farm (13 km length) and a large wind farm (90 km length) in a convective boundary layer, which is the most common boundary layer type in the North Sea. The results show that there are significant differences in the flow field and the energy budgets of the small and large wind farm. The large wind farm triggers an inertial wave with a wind direction amplitude of approximately 10∘ and a wind speed amplitude of more than 1 m s−1. In a certain region in the far wake of a large wind farm the wind speed is greater than far upstream of the wind farm, which can be beneficial for a downstream located wind farm. The inertial wave also exists for the small wind farm, but the amplitudes are approximately 4 times weaker and thus may be hardly observable in real wind farm flows that are more heterogeneous. Regarding turbulence intensity, the wake of the large wind farm has the same length as the wake of the small wind farm and is only a few kilometers long. Both wind farms trigger inertial gravity waves in the free atmosphere, whereas the amplitude is approximately twice as large for the large wind farm. The inertial gravity waves induce streamwise pressure gradients inside the boundary layer, affecting the energy budgets of the wind farms. The most dominant energy source of the small wind farm is the horizontal advection of kinetic energy, but for the large wind farm the vertical turbulent flux of kinetic energy is 5 times greater than the horizontal advection of kinetic energy. The energy input by the gravity-wave-induced pressure gradient is greater for the small wind farm because the pressure gradient is greater. For the large wind farm, the energy input by the geostrophic forcing (synoptic-scale pressure gradient) is significantly enhanced by the wind direction change that is related to the inertial oscillation. For both wind farms approximately 75 % of the total available energy is extracted by the wind turbines and 25 % is dissipated." @default.
• W4365447492 created "2023-04-15" @default.
• W4365447492 creator A5068241641 @default.
• W4365447492 date "2023-04-13" @default.
• W4365447492 modified "2023-09-26" @default.
• W4365447492 title "From gigawatt to multi-gigawatt wind farms: wake effects, energy budgets and inertial gravity waves investigated by large-eddy simulations" @default.
• W4365447492 cites W1158084216 @default.
• W4365447492 cites W1558567928 @default.
• W4365447492 cites W1667277804 @default.
• W4365447492 cites W1872576311 @default.
• W4365447492 cites W1966536410 @default.
• W4365447492 cites W1972960566 @default.
• W4365447492 cites W1985806137 @default.
• W4365447492 cites W1995088783 @default.
• W4365447492 cites W2016033830 @default.
• W4365447492 cites W2036274724 @default.
• W4365447492 cites W2038996062 @default.
• W4365447492 cites W2043392943 @default.
• W4365447492 cites W2051295969 @default.
• W4365447492 cites W2052170279 @default.
• W4365447492 cites W2056613470 @default.
• W4365447492 cites W2071357762 @default.
• W4365447492 cites W2075901111 @default.
• W4365447492 cites W2091430775 @default.
• W4365447492 cites W2096632151 @default.
• W4365447492 cites W2103587201 @default.
• W4365447492 cites W2108346476 @default.
• W4365447492 cites W2112043279 @default.
• W4365447492 cites W2112576193 @default.
• W4365447492 cites W2139417995 @default.
• W4365447492 cites W2144207130 @default.
• W4365447492 cites W2156096080 @default.
• W4365447492 cites W2159157859 @default.
• W4365447492 cites W2165553433 @default.
• W4365447492 cites W2165727159 @default.
• W4365447492 cites W2244503659 @default.
• W4365447492 cites W2278336330 @default.
• W4365447492 cites W2317753128 @default.
• W4365447492 cites W2511718092 @default.
• W4365447492 cites W2587622967 @default.
• W4365447492 cites W2594040502 @default.
• W4365447492 cites W2763985260 @default.
• W4365447492 cites W2779505942 @default.
• W4365447492 cites W2896743191 @default.
• W4365447492 cites W2979841977 @default.
• W4365447492 cites W3011128425 @default.
• W4365447492 cites W3012526672 @default.
• W4365447492 cites W3102151828 @default.
• W4365447492 cites W3168347726 @default.
• W4365447492 cites W3195705414 @default.
• W4365447492 cites W4213024732 @default.
• W4365447492 cites W4220966541 @default.
• W4365447492 cites W4281916809 @default.
• W4365447492 doi "https://doi.org/10.5194/wes-8-535-2023" @default.
• W4365447492 hasPublicationYear "2023" @default.
• W4365447492 type Work @default.
• W4365447492 citedByCount "1" @default.
• W4365447492 countsByYear W43654474922023 @default.
• W4365447492 crossrefType "journal-article" @default.
• W4365447492 hasAuthorship W4365447492A5068241641 @default.
• W4365447492 hasBestOaLocation W43654474921 @default.
• W4365447492 hasConcept C111603439 @default.
• W4365447492 hasConcept C118536763 @default.
• W4365447492 hasConcept C119599485 @default.
• W4365447492 hasConcept C121332964 @default.
• W4365447492 hasConcept C127413603 @default.
• W4365447492 hasConcept C135558025 @default.
• W4365447492 hasConcept C153294291 @default.
• W4365447492 hasConcept C154718420 @default.
• W4365447492 hasConcept C161067210 @default.
• W4365447492 hasConcept C199104240 @default.
• W4365447492 hasConcept C39432304 @default.
• W4365447492 hasConcept C48939323 @default.
• W4365447492 hasConcept C57879066 @default.
• W4365447492 hasConcept C78600449 @default.
• W4365447492 hasConcept C82313973 @default.
• W4365447492 hasConcept C8735168 @default.
• W4365447492 hasConcept C91586092 @default.
• W4365447492 hasConceptScore W4365447492C111603439 @default.
• W4365447492 hasConceptScore W4365447492C118536763 @default.
• W4365447492 hasConceptScore W4365447492C119599485 @default.
• W4365447492 hasConceptScore W4365447492C121332964 @default.
• W4365447492 hasConceptScore W4365447492C127413603 @default.
• W4365447492 hasConceptScore W4365447492C135558025 @default.
• W4365447492 hasConceptScore W4365447492C153294291 @default.
• W4365447492 hasConceptScore W4365447492C154718420 @default.
• W4365447492 hasConceptScore W4365447492C161067210 @default.
• W4365447492 hasConceptScore W4365447492C199104240 @default.
• W4365447492 hasConceptScore W4365447492C39432304 @default.
• W4365447492 hasConceptScore W4365447492C48939323 @default.
• W4365447492 hasConceptScore W4365447492C57879066 @default.
• W4365447492 hasConceptScore W4365447492C78600449 @default.
• W4365447492 hasConceptScore W4365447492C82313973 @default.
• W4365447492 hasConceptScore W4365447492C8735168 @default.
• W4365447492 hasConceptScore W4365447492C91586092 @default.
• W4365447492 hasIssue "4" @default.
• W4365447492 hasLocation W43654474921 @default.
• W4365447492 hasLocation W43654474922 @default.

• next