Articles | Volume 17, issue 1
https://doi.org/10.5194/gmd-17-143-2024
© Author(s) 2024. This work is distributed under the Creative Commons Attribution 4.0 License.
Development of inter-grid-cell lateral unsaturated and saturated flow model in the E3SM Land Model (v2.0)
Download
- Final revised paper (published on 10 Jan 2024)
- Preprint (discussion started on 05 Apr 2023)
Interactive discussion
Status: closed
Comment types: AC – author | RC – referee | CC – community | EC – editor | CEC – chief editor
| : Report abuse
-
RC1: 'Comment on egusphere-2023-375', Anonymous Referee #1, 09 May 2023
- AC1: 'Reply on RC1', Han Qiu, 01 Oct 2023
- AC2: 'Reply on RC1', Han Qiu, 01 Oct 2023
- AC3: 'Reply on RC1', Han Qiu, 01 Oct 2023
-
CC1: 'Comment on egusphere-2023-375', Xubin Zeng, 27 May 2023
- AC4: 'Reply on CC1', Han Qiu, 01 Oct 2023
-
RC2: 'Comment on egusphere-2023-375', Anonymous Referee #2, 01 Jun 2023
- AC5: 'Reply on RC2', Han Qiu, 01 Oct 2023
-
RC3: 'Comment on egusphere-2023-375', Zhenghui Xie, 15 Jun 2023
- AC6: 'Reply on RC3', Han Qiu, 01 Oct 2023
- AC2: 'Reply on RC1', Han Qiu, 01 Oct 2023
Peer review completion
AR – Author's response | RR – Referee report | ED – Editor decision | EF – Editorial file upload
AR by Han Qiu on behalf of the Authors (01 Oct 2023)
Author's response
Author's tracked changes
Manuscript
ED: Referee Nomination & Report Request started (13 Oct 2023) by Taesam Lee
RR by Anonymous Referee #2 (27 Oct 2023)
ED: Publish as is (02 Nov 2023) by Taesam Lee
AR by Han Qiu on behalf of the Authors (08 Nov 2023)
This is a review of "Development of Inter-Grid Cell Lateral Unsaturated and Saturated Flow Model in the E3SM Land Model (v2.0)" by Qiu et al.
The authors describe the development of a saturated lateral flow parameterization for between-gridcell water movement. The modified model is compared to a fully 3d subsurface flow model.
Derivation of equations
In general, I thought that the derivation of the moisture movement equations could be improved. Around line 105, the authors reference Oleson et al. [2013], which describes the conservation of mass in one dimension that is used in the CLM model. But their equation 7 is not what is found in Oleson et al., and instead is written in the general 3d form. The authors here use the index n to denote different control volumes, before switching to an index k used to describe the layers of the 1d soil structure. I think it would be more clear to either 1) describe the 3d equations first, then show how the specific 1d case leads to the ELM/CLM equations described in Oleson et al., or follow Oleson et al. and then show how the 3d equations are used to define the new term in equation 14.
Regarding the equations describing the lateral flux, e.g. 14 and following, the areas used to convert between fluxes and volumes should be clarified to show whether they are actual surface areas, or projected areas. The appropriate area is the area that is normal to the direction of the flux. This is why I found the description of equation 16 confusing. I don't think describing the fluxes relative to z' (the rotated z axis) make sense. This is still a 1d column model, with the nodes aligned verticaly, therefore the fluxes in the column are all in the vertical. Presumably the coupling to the atmosphere also occurs in the vertical. It would be more clear to me to note that a cosine arises in equation 16 due to the projected area of the surface being smaller than the surface area by a cosine factor.
I would also like to know if the presence of z in equation 15 is correct. I understood the gravity term in the modified Darcy equation to be the sin(theta) term.
Why does equation 17 not have a similar form as equation 15? Also, I would like to see the calculation of the transmissivity T described here rather than simply referenced.
What is the size of the contribution of the unsaturated lateral flow term, for both the benchmarking and application simulations? It would be useful to indicate the relative importance of this term, and whether this impacts the simulations significantly. It would seem to be straightforward to turn off this flux to test this issue.
Evaluation over lww
A comparison to a LWW PFLOTRAN simulation would have been interesting. Given that PFLOTRAN was used in the benchmarking section, why was it not used in the evaluation section?
The WTD map in figure 8 shows that the addition of lateral flow helps to better resolve the uphill/downhill differences in water table depth, but there are still significant differences relative to the Fan WTD map. The authors note that calibration of the f_d parameter to give a better match to the Fan WTD map may not be fruitful due to differences in climate forcing. But given the relatively large differences, it would be informative to do a sensitivity test for the f_d parameter. For example, is there a value of f_d that further lowers the water table depth, and better resolves the riparian areas as shown in the Fan map?
Statements such as "The effects of WTD changes on the energy fluxes were more pronounced at low elevation cells, especially at the stream and its surrounding cells. The delivery of the groundwater through the lateral flow to the valleys supported higher LH while reducing the SH compared with ELMv2.0 which has little spatial WTD variations" do not appear to be well supported by figure 9. Instead of highlighting the differences between the uphill and downhill areas apparent in figure 8, figure 9 shows spatial patterns having broad domain-wide patterns. Why do the water table patterns in figure 8 show much more structure? For example, larger LH values do not appear consistently in the riparian areas. Similarly, the patterns in the difference maps only show scattered points rather than a clear riparian pattern. Why is this?
The comparisons to observations (figures 10 and 11) do not seem to add much insight into the relative model behaviors. Given the authors choice to not calibrate the models, I don't think it can be stated that the differences between the observations are due to model structure. For example, the A121 differences in figure 10 might be smaller if the f_d parameter in ELMv2.0 model had been calibrated. The statement that both models "were able to capture the major fluctuations and wetting/drying cycles of soil moisture (SM)" seems over-stated. The rain events are generally captured, but the magnitude of the reponse, and the dry-down rate is generally poor. What information are the authors trying to give to the reader with these figures? Similarly for figure 12; one does not need to perform a model simulation to be aware that shallower water tables will typically have colder temperatures, higher LH, and lower SH than deeper water tables. Any two model versions having different water table depths would presumably show this behavior. I don't see that this figure adds any additional insight to the results.