Articles | Volume 11, issue 6
https://doi.org/10.5194/wes-11-2093-2026
© Author(s) 2026. This work is distributed under the Creative Commons Attribution 4.0 License.
Generating high-fidelity wind fields from the wind speed correlation tensor
Download
- Final revised paper (published on 18 Jun 2026)
- Preprint (discussion started on 18 Nov 2025)
Interactive discussion
Status: closed
Comment types: AC – author | RC – referee | CC – community | EC – editor | CEC – chief editor
| : Report abuse
-
RC1: 'Comment on wes-2025-221', Anonymous Referee #1, 03 Dec 2025
- AC1: 'Reply on RC1', Matteo Faccioni, 12 Dec 2025
-
RC2: 'Comment on wes-2025-221', Anonymous Referee #2, 19 Jan 2026
- AC2: 'Reply on RC2', Matteo Faccioni, 22 Jan 2026
Peer review completion
AR – Author's response | RR – Referee report | ED – Editor decision | EF – Editorial file upload
AR by Matteo Faccioni on behalf of the Authors (30 Jan 2026)
Author's response
Author's tracked changes
Manuscript
ED: Referee Nomination & Report Request started (12 Feb 2026) by Sandrine Aubrun
RR by Anonymous Referee #3 (23 Mar 2026)
RR by Anonymous Referee #2 (25 Apr 2026)
ED: Publish subject to minor revisions (review by editor) (02 May 2026) by Sandrine Aubrun
AR by Matteo Faccioni on behalf of the Authors (05 May 2026)
Author's response
Author's tracked changes
Manuscript
ED: Publish as is (21 May 2026) by Sandrine Aubrun
ED: Publish as is (21 May 2026) by Julia Gottschall (Chief editor)
AR by Matteo Faccioni on behalf of the Authors (28 May 2026)
Manuscript
Review of lin
Generating high fidelity wind fields from the wind speed correlation tensor
Wind Energy Science
Summary
The proposed study presents a method for generating synthetic isotropic homogeneous turbulence (denoted the CBM method by the authors). It is based on the a priori knowledge of the two-point correlation tensor that is used to generate the corresponding velocity field first in Fourier space using a series of random number before going back to physical space via inverse Fourier transform. The performance of the proposed method is tested against a more standard method based on the a priori knowledge of the velocity spectrum (the so-called RPM method).
The manuscript is well organized and well written, quality of the English language is good overall. The authors present some interesting analysis and findings that might interest the community. However, some points need to be addressed before the paper can be considered for publication.
Comments
As pointed out by the authors, the CBM method they propose does not seem to be that new. The novelty they added to the previous correlation-based methods is not clear at all. Could the authors give the reader more details about that ?
Have the authors thought about addressing the more challenging issue of generating non-isotropic, non-homogeneous synthetic turbulence ?
L124: the authors point out the limitation of previous correlation based methods (Dietrich and
Newsam, 1997; Wood and Chan, 1994) due to the fact they “on the correlation matrix having a Toeplitz structure” To the reviewer’s limited knowledge, the Toeplitz structure of the correlation matrix is directly linked to the fact that one considers homogeneous (or stationary) directions, which is mandatory to be able to use Fourier transforms. As the authors have designed their method to generate isotropic homogeneous turbulence, their method has the same requirement: a correlation matrix with a Toeplitz structure. Could the authors comment on that please ?
L125: “This is not always the case in wind field generation problems.” could the authors give some example of cases were correlation matrices are not of Toeplitz type but which their method could handle anyway ?
Fig 1: how the ideal structure function is calculated ?
For the RPM, the authors prescribe a von Karman spectrum (I presume it is one-dimensional), whereas for the CBM, they prescribe the full 3D tensor B_pq. What is the impact of these difference ?
L156 and subsequent: the description and the origin of the problem related to PSD with negative values is not clear at all. Could the author elaborate on that ?
Could the authors show the spectra of the velocity field obtained using the CBM and compare it to the expected spectrum and that used with the RPM ?
Fig 5: could the author explain why the error of the RPM remains independent of the size of the spatial domain ? It seems to contradict the point they made in the last paragraph of page 4 (line 98) stating that the grid domain acts as a bandpass filter. One would expect the performance to increase as the bandwidth of the filter increases (with domain size).
It would interesting to show the structure functions computed for the various domain size for both methods RPM and CBM.