Matches in SemOpenAlex for { <https://semopenalex.org/work/W2808240116> ?p ?o ?g. }
- W2808240116 endingPage "820" @default.
- W2808240116 startingPage "788" @default.
- W2808240116 abstract "A group of three multiscale inhomogeneous grids have been tested to generate different types of turbulent shear flows with different mean shear rate and turbulence intensity profiles. Cross hot-wire measurements were taken in a wind tunnel with Reynolds number $Re_{D}$ of 6000–20 000, based on the width of the vertical bars of the grid and the incoming flow velocity. The effect of local drag coefficient $C_{D}$ on the mean velocity profile is discussed first, and then by modifying the vertical bars to obtain a uniform aspect ratio the mean velocity profile is shown to be predictable using the local blockage ratio profile. It is also shown that, at a streamwise location $x=x_{m}$ , the turbulence intensity profile along the vertical direction $u^{prime }(y)$ scales with the wake interaction length $x_{ast ,n}^{peak}=0.21g_{n}^{2}/(unicode[STIX]{x1D6FC}C_{D}w_{n})$ ( $unicode[STIX]{x1D6FC}$ is a constant characterizing the incoming flow condition, and $g_{n}$ , $w_{n}$ are the gap and width of the vertical bars, respectively, at layer $n$ ) such that $(u^{prime }/U_{n})^{2}unicode[STIX]{x1D6FD}^{2}(C_{D}w_{n}/x_{ast ,n}^{peak})^{-1}sim (x_{m}/x_{ast ,n}^{peak})^{b}$ , where $unicode[STIX]{x1D6FD}$ is a constant determined by the free-stream turbulence level, $U_{n}$ is the local mean velocity and $b$ is a dimensionless power law constant. A general framework of grid design method based on these scalings is proposed and discussed. From the evolution of the shear stress coefficient $unicode[STIX]{x1D70C}(x)$ , integral length scale $L(x)$ and the dissipation coefficient $C_{unicode[STIX]{x1D716}}(x)$ , a simple turbulent kinetic energy model is proposed that describes the evolution of our grid generated turbulence field using one centreline measurement and one vertical profile of $u^{prime }(y)$ at the beginning of the evolution. The results calculated from our model agree well with our measurements in the streamwise extent up to $x/Happrox 2.5$ , where $H$ is the height of the grid, suggesting that it might be possible to design some shear flows with desired mean velocity and turbulence intensity profiles by designing the geometry of a passive grid." @default.
- W2808240116 created "2018-06-21" @default.
- W2808240116 creator A5009998817 @default.
- W2808240116 creator A5048947797 @default.
- W2808240116 creator A5061174235 @default.
- W2808240116 creator A5076593652 @default.
- W2808240116 date "2018-06-13" @default.
- W2808240116 modified "2023-09-24" @default.
- W2808240116 title "Weakly sheared turbulent flows generated by multiscale inhomogeneous grids" @default.
- W2808240116 cites W121983332 @default.
- W2808240116 cites W1969164548 @default.
- W2808240116 cites W1980958362 @default.
- W2808240116 cites W1982022354 @default.
- W2808240116 cites W1983172941 @default.
- W2808240116 cites W1984152161 @default.
- W2808240116 cites W1991375939 @default.
- W2808240116 cites W1998898314 @default.
- W2808240116 cites W2004947645 @default.
- W2808240116 cites W2005916681 @default.
- W2808240116 cites W2006548175 @default.
- W2808240116 cites W2012503815 @default.
- W2808240116 cites W2024104838 @default.
- W2808240116 cites W2024431579 @default.
- W2808240116 cites W2026690725 @default.
- W2808240116 cites W2030427781 @default.
- W2808240116 cites W2032901867 @default.
- W2808240116 cites W2035093662 @default.
- W2808240116 cites W2037443308 @default.
- W2808240116 cites W2041352103 @default.
- W2808240116 cites W2041722657 @default.
- W2808240116 cites W2044192788 @default.
- W2808240116 cites W2044437516 @default.
- W2808240116 cites W2051589220 @default.
- W2808240116 cites W2056144693 @default.
- W2808240116 cites W2065067834 @default.
- W2808240116 cites W2067266183 @default.
- W2808240116 cites W2074967074 @default.
- W2808240116 cites W2079211394 @default.
- W2808240116 cites W2083702379 @default.
- W2808240116 cites W2084772634 @default.
- W2808240116 cites W2091540400 @default.
- W2808240116 cites W2094068548 @default.
- W2808240116 cites W2096149665 @default.
- W2808240116 cites W2105221613 @default.
- W2808240116 cites W2105802178 @default.
- W2808240116 cites W2117141276 @default.
- W2808240116 cites W2117385625 @default.
- W2808240116 cites W2117652238 @default.
- W2808240116 cites W2128565424 @default.
- W2808240116 cites W2128652407 @default.
- W2808240116 cites W2130927992 @default.
- W2808240116 cites W2141733977 @default.
- W2808240116 cites W2149217060 @default.
- W2808240116 cites W2170126284 @default.
- W2808240116 cites W2170994734 @default.
- W2808240116 cites W2751387434 @default.
- W2808240116 cites W2800853560 @default.
- W2808240116 cites W3103308842 @default.
- W2808240116 cites W328952167 @default.
- W2808240116 doi "https://doi.org/10.1017/jfm.2018.387" @default.
- W2808240116 hasPublicationYear "2018" @default.
- W2808240116 type Work @default.
- W2808240116 sameAs 2808240116 @default.
- W2808240116 citedByCount "1" @default.
- W2808240116 countsByYear W28082401162018 @default.
- W2808240116 crossrefType "journal-article" @default.
- W2808240116 hasAuthorship W2808240116A5009998817 @default.
- W2808240116 hasAuthorship W2808240116A5048947797 @default.
- W2808240116 hasAuthorship W2808240116A5061174235 @default.
- W2808240116 hasAuthorship W2808240116A5076593652 @default.
- W2808240116 hasBestOaLocation W28082401162 @default.
- W2808240116 hasConcept C121332964 @default.
- W2808240116 hasConcept C147196274 @default.
- W2808240116 hasConcept C150711758 @default.
- W2808240116 hasConcept C15476950 @default.
- W2808240116 hasConcept C189223162 @default.
- W2808240116 hasConcept C196558001 @default.
- W2808240116 hasConcept C204573209 @default.
- W2808240116 hasConcept C205904022 @default.
- W2808240116 hasConcept C24872484 @default.
- W2808240116 hasConcept C48939323 @default.
- W2808240116 hasConcept C57879066 @default.
- W2808240116 hasConcept C72117827 @default.
- W2808240116 hasConcept C72921944 @default.
- W2808240116 hasConcept C74650414 @default.
- W2808240116 hasConcept C87801597 @default.
- W2808240116 hasConceptScore W2808240116C121332964 @default.
- W2808240116 hasConceptScore W2808240116C147196274 @default.
- W2808240116 hasConceptScore W2808240116C150711758 @default.
- W2808240116 hasConceptScore W2808240116C15476950 @default.
- W2808240116 hasConceptScore W2808240116C189223162 @default.
- W2808240116 hasConceptScore W2808240116C196558001 @default.
- W2808240116 hasConceptScore W2808240116C204573209 @default.
- W2808240116 hasConceptScore W2808240116C205904022 @default.
- W2808240116 hasConceptScore W2808240116C24872484 @default.
- W2808240116 hasConceptScore W2808240116C48939323 @default.
- W2808240116 hasConceptScore W2808240116C57879066 @default.
- W2808240116 hasConceptScore W2808240116C72117827 @default.