Articles | Volume 19, issue 10
https://doi.org/10.5194/gmd-19-4661-2026
© Author(s) 2026. This work is distributed under the Creative Commons Attribution 4.0 License.
ForEdgeClim v1.0: a 3D process-based microclimate model incorporating vertical and lateral radiative and thermal fluxes to simulate forest edge-to-core transitions
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- Final revised paper (published on 01 Jun 2026)
- Preprint (discussion started on 12 Feb 2026)
Interactive discussion
Status: closed
Comment types: AC – author | RC – referee | CC – community | EC – editor | CEC – chief editor
| : Report abuse
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RC1: 'Comment on egusphere-2026-649', Ilya Maclean, 17 Feb 2026
- AC1: 'Reply on RC1', Emma Van de Walle, 17 Apr 2026
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RC2: 'Comment on egusphere-2026-649', Anonymous Referee #2, 03 Mar 2026
- AC2: 'Reply on RC2', Emma Van de Walle, 17 Apr 2026
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RC3: 'Comment on egusphere-2026-649', Run Zhong, 04 Mar 2026
- AC3: 'Reply on RC3', Emma Van de Walle, 17 Apr 2026
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RC4: 'Comment on egusphere-2026-649', Vivienne Groner, 11 Mar 2026
- AC4: 'Reply on RC4', Emma Van de Walle, 17 Apr 2026
Peer review completion
AR – Author's response | RR – Referee report | ED – Editor decision | EF – Editorial file upload
AR by Emma Van de Walle on behalf of the Authors (17 Apr 2026)
Author's response
Author's tracked changes
Manuscript
ED: Referee Nomination & Report Request started (20 Apr 2026) by Dalei Hao
RR by Anonymous Referee #3 (01 May 2026)
RR by Anonymous Referee #2 (03 May 2026)
RR by Ilya Maclean (05 May 2026)
ED: Publish subject to minor revisions (review by editor) (05 May 2026) by Dalei Hao
AR by Emma Van de Walle on behalf of the Authors (11 May 2026)
Author's response
Author's tracked changes
Manuscript
ED: Publish as is (12 May 2026) by Dalei Hao
AR by Emma Van de Walle on behalf of the Authors (15 May 2026)
Manuscript
There is undoubtedly a strong and growing need for robust microclimate modelling approaches, particularly in forested systems where fine-scale thermal heterogeneity can strongly influence ecological processes. The manuscript addresses an important problem, and the attempt to develop a tractable, process-based framework is welcome.
However, the current presentation would benefit from greater physical clarity, closer engagement with the extensive microclimate modelling literature, and more precise definition of terms and units. Throughout the manuscript, model equations are presented without consistently specifying the units of each term. For a physically based model, dimensional consistency is important, and equations would benefit from explicit unit definitions (e.g. W m⁻², m s⁻¹, J m⁻³ K⁻¹, etc.) to avoid ambiguity and ensure reproducibility.
Specific comments:
Lines 100–109 – Iterative solution of the energy balanceIt is not made clear why the surface energy balance must be solved iteratively. In many comparable contexts, the system can be solved more efficiently using a Penman–Monteith formulation or related bulk-transfer approaches. The authors should clarify why iteration is necessary here, and whether a more computationally efficient analytical solution is possible.
Section 2.1.2 – Below-canopy air temperatureThe physical treatment of below-canopy air temperature is fairly questionable. It is now well established that Lagrangian approaches to fluid mechanics are required to rigorously describe scalar transport within and below plant canopies (see the seminal work of Raupach and subsequent developments). Air temperature at a given point below the canopy is not determined solely by local leaf temperature or local energy exchange. Rather, it reflects the cumulative influence of upstream canopy elements through advection and turbulent mixing. In other words, the temperature field represents an integrated effect of heat exchange along air parcel trajectories as they move through and downwind of the canopy. The current formulation appears to treat temperature as a locally determined variable, which risks neglecting this trajectory-dependent behaviour. The authors need to explain why a local formulation is sufficient in this context. In addition, foliage density does not appear to influence the formulation. If fluxes are expressed in standard units (e.g. W m⁻²), canopy leaf area density or LAI should explicitly affect the magnitude of exchange. As written, it is unclear how foliage density affects the flux exchange between the canopy and the air.
Sections 2.1.3 and 2.2.3 – Soil surface temperature and ground heat fluxThe soil surface temperature equation appears dimensionally inconsistent. If fluxes are expressed in W m⁻², there should be no need to introduce an explicit cross-sectional area term. Greater clarity on units is needed here. The assumption that temperature at 8 cm depth can be treated as fixed is problematic. At this depth, temperatures exhibit clear diurnal and seasonal variability. One typically needs to approach depths of ~2 m before assuming quasi-constant temperature. Without a multi-layer soil heat transfer model, soil surface temperature cannot be derived mechanistically. As written, the approach appears to depend on continuous measurement at 8 cm depth, which limits transferability. Thermal conductivity (k) is also treated as constant, yet it varies strongly with soil moisture content. I missed discussion of this issue.
In Section 2.2.3, the ground heat flux method will not reproduce the well-established quarter-cycle phase shift (diurnal or seasonal) between surface radiation forcing and subsurface heat flux. Instead, fluxes appear to mirror radiation directly, meaning the heat storage effect is not properly represented. It would be worth exploring the de Vries / Van Wijk method as described in Campbell & Norman, which provides a more physically consistent treatment of soil heat storage consistent with the framework presented in this paper
Section 2.2.4 – Sensible heat fluxThe terminology becomes imprecise with respect to thermal energy transfer from forest surfaces to the surrounding air. You introduce a forest–air convection coefficient, g, but in conventional notation g typically denotes leaf boundary layer conductance. The discussion also refers to molecular diffusion, whereas in forest environments free and forced laminer convection dominate at the leaf surface., and turbulent heat transfer is often critical within the air. Given the method used to compute air temperature, turbulent exchange likely needs to be explicitly accounted for sperate to leaf boundary layer conductance. The authors should clearly define the physical meaning of g, specify its units, and describe how it is parameterised and scaled.
Section 2.2.5 – Latent heat flux. This section is also problematic. The discussion focuses on evaporation, but in forest systems transpiration typically represents a substantial component of latent heat flux. Transpiration is controlled by stomatal conductance, which does not appear to be included in the formulation. The manuscript argues that evaporation is primarily driven by available radiative energy and surface humidity. However, radiative energy drives evapotranspiration both through direct surface energy availability and via its effects on PAR and stomatal conductance. Only the most direct pathway appears to be represented. Ignoring stomatal control risks substantial overestimation of latent heat flux, particularly under conditions where stomata are partially closed.Some of the limitations outlined above would be more easily reconciled if the model demonstrated strong predictive performance. Figure 3 is interesting, but the discrepancies between modelled and measured values appear large relative to the effect sizes being examined. In several cases, the measured differences between forest interior and core are smaller than the deviations between modelled and observed values. This raises concerns about whether the model can reliably resolve the spatial contrasts it seeks to quantify.
Overall assessmentThe model is not without merit and addresses an important problem and does seem to perform moderately well. However, it rests on several simplifying assumptions that limit its physical realism. Greater clarity on units, stronger engagement with existing microclimate modelling literature, and more rigorous treatment of canopy turbulence, soil heat storage, and stomatal control would substantially strengthen the manuscript.