Table 1.
Details of the various datasets used
| Case | Method | Acronym: Authors | H / h | |
|---|---|---|---|---|
| Staggered cubes | DNS | LC: Leonardi and Castro (2010) | 8.0 | 1/100 |
| Staggered and aligned cubes | DNS | CTCB: Coceal et al. (2006) | 8.0 | 1/32 |
| Staggered and aligned cubes | DNS | BCTB: Branford et al. (2011) | 8.0 | 1/32 |
| Staggered cubes, various angles | LES | CCTBBC: Claus et al. (2012) | 4.0 | 1/25 |
| Staggered, random height | LES | XCC: Xie et al. (2008) | 10.0 | 1/16 |
| Aligned cubes (b.layer) | LES | CP-A: Cheng and Porte-Agel (2015) | 1/16 | |
| Staggered and aligned cubes (b.layer) | LES | YSMM: Yang et al. (2016) | 1/8 | |
| Aligned blocks | DNS, LES | CXFRCHHC: Castro et al. (2016) | 12 | 1/12 |
Except for CP-A’s and YSMM’s LES, where H refers to the approximate boundary-layer depth, all cases were channel-flow computations, with H the channel half-height. All cases except CCTBBC and CXFRCHHC considered only arrays that were flow-aligned—i.e. wind direction normal to the faces of the obstacles. For the LES cases, the subgrid models used were either the standard Smagorinsky model (CCTBBC, XCC, CXFRCHHC), the modulated gradient model of Lu and Porte-Agel (2010) (CP-A), or the Vreman (2010) model (YSSM)