Articles | Volume 18, issue 22
https://doi.org/10.5194/gmd-18-8855-2025
© Author(s) 2025. This work is distributed under the Creative Commons Attribution 4.0 License.
Optimizing physical scheme selection in RegCM5 for improved air–sea fluxes over Southeast Asia
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- Final revised paper (published on 21 Nov 2025)
- Preprint (discussion started on 15 May 2025)
Interactive discussion
Status: closed
Comment types: AC – author | RC – referee | CC – community | EC – editor | CEC – chief editor
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RC1: 'Comment on egusphere-2025-1579', Anonymous Referee #1, 25 Jun 2025
- AC1: 'Reply on RC1', Quentin Desmet, 13 Aug 2025
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RC2: 'Comment on egusphere-2025-1579', Anonymous Referee #2, 24 Jul 2025
- AC2: 'Reply on RC2', Quentin Desmet, 13 Aug 2025
Peer review completion
AR – Author's response | RR – Referee report | ED – Editor decision | EF – Editorial file upload
AR by Quentin Desmet on behalf of the Authors (13 Aug 2025)
Author's response
Author's tracked changes
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ED: Referee Nomination & Report Request started (15 Aug 2025) by Travis O'Brien
RR by Anonymous Referee #1 (13 Oct 2025)
ED: Publish subject to technical corrections (21 Oct 2025) by Travis O'Brien
AR by Quentin Desmet on behalf of the Authors (29 Oct 2025)
Author's response
Manuscript
General overview
The authors evaluate the performance of RegCM5 in simulating air-sea fluxes over the Southeast Asian region by testing different physical parametrizations: radiative transfer, planetary boundary layer, cumulus convection, parameterized microphysics, and cloud fraction.
To assess the performance of numerical simulations, the authors use a multicriteria decision-making framework to rank their ability in reproducing sea surface wind, latent and sensible heat fluxes, precipitation, and radiative heat fluxes..
The authors have not found a configuration that properly solves all criteria.
However, they found that using the Tiedtke cumulus convection scheme showed better results for precipitation and sea surface wind.
Comments:
The authors mention that the study focuses on the seasonal cycle and that they have chosen the year 2018 to perform the numerical simulations since it offers neutral conditions with respect to large-scale oscillations.
However, the authors remark that it is important to properly take into account the influence of upwellings, eddies, and meanders when forcing atmospheric models. This is the reason why they force RegCM5 with a high-resolution regional SYMPHONIE forced numerical simulation (5 km) instead of with an optimal-interpolation-based SST dataset.
With a 5 km spatial resolution, the ocean numerical simulation will be able to solve eddies of at least 20 km in diameter (effective spatial resolution).
When forcing the atmospheric model, the sea surface data, containing high-spatial resolution features, will be interpolated to the 25 km grid of RegCM5, passing from an effective spatial resolution of 20 km to 100 km.
At the end, there is no discussion about the role of mesoscale processes, such as upwelling, eddies, or meanders, in modulating heat fluxes, precipitation, or winds.
Following Frenger et al. (2013) and Villas Bôas et al. (2015), cold and warm eddies are important drivers of latent heat fluxes, and because of that, can modulate the cloud cover and precipitation.
In fact, Villas Bôas et al. (2015) showed that eddies can partially modulate 20% of latent heat fluxes.
When the authors compare the monthly SYMPHONIE sea surface temperature results with OSTIA estimations, there are no evident large-scale spatial pattern differences that indicate problems in representing the seasonal cycle.
Instead, the differences, which are larger than 2 oC, seem to be more related to a misaligned occurrence of warm and cold eddies in comparison with the observations.
Perhaps it would be easier to directly force RegCM5 with the GLORYS dataset, where mesoscale eddies should be in the proper location, because of the data assimilation.
Regarding the comparison of scores and rankings associated with the 36 experiments, it is difficult to identify which model aspect is more important or promotes more realistic results.
Perhaps it would be better to build a figure that resumes Figure 3, which highlights the model aspects that mostly occur in the top 10 ranks.
In this way, perhaps it would be easier to identify that experiment 12511 is the best performer.
Specific comments:
Line 182: Define all acronyms, like EBAF and IMERG.
In line 300, the authors mention that Tiedtke configurations “clearly” outperform the other configurations, but this is not easy to see.
In line 380, the authors highlight the weaker similarity along the equation in Figure 4, but the figure lacks coordinates, which makes it difficult to follow the text.
The authors commonly refer to correlation coefficients, but there is no figure or table to see them, as in line 415.