Articles | Volume 29, issue 22
https://doi.org/10.5194/hess-29-6685-2025
© Author(s) 2025. This work is distributed under the Creative Commons Attribution 4.0 License.
Evolution of low-karstified rock-blocks and their influence on reservoir leakage: a modelling perspective
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- Final revised paper (published on 25 Nov 2025)
- Supplement to the final revised paper
- Preprint (discussion started on 03 Apr 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-2025-1320', Anonymous Referee #1, 20 May 2025
- AC1: 'Reply on RC1', Youjun Jiao, 02 Jul 2025
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RC2: 'Comment on egusphere-2025-1320', Anonymous Referee #2, 26 May 2025
- AC2: 'Reply on RC2', Youjun Jiao, 02 Jul 2025
Peer review completion
AR – Author's response | RR – Referee report | ED – Editor decision | EF – Editorial file upload
ED: Reconsider after major revisions (further review by editor and referees) (02 Jul 2025) by Heng Dai
AR by Youjun Jiao on behalf of the Authors (16 Jul 2025)
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ED: Referee Nomination & Report Request started (18 Jul 2025) by Heng Dai
RR by Anonymous Referee #1 (25 Jul 2025)
RR by Anonymous Referee #2 (23 Sep 2025)
ED: Publish subject to minor revisions (review by editor) (11 Oct 2025) by Heng Dai
AR by Youjun Jiao on behalf of the Authors (20 Oct 2025)
Author's response
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ED: Publish as is (22 Oct 2025) by Heng Dai
AR by Youjun Jiao on behalf of the Authors (28 Oct 2025)
This is a very interesting paper presenting a modeling approach aimed at showing how the coupling between dissolution, transport in fracture formations, and horizontal head forms a low-karstified rock-blocks which prevent water seepage, up to a threshold of head difference between reservoirs. I very much like the approach, the results, and the layout of the article, and I can see how it will be well suited to HESS. However, three aspects require attention in this study:
Introduction: The authors make an excellent case supporting their approach in the introduction, yet it will be beneficial to relate each aspect that is either added or missing in previous studies to the figure 1 illustration, thus providing a conceptual picture of the processes at hand.
Line 22: “One of the primary issues is the intensification of the natural karstification process due to artificial hydraulic gradients, which can result in persistent and uncontrollable leakage throughout the structure's lifespan”
This sentence exemplifies the narrow focus of the paper. In the second sentence of the introduction, we encounter jargon that is not properly explained. We have no idea what the artificial part is in these hydraulic gradients and why it leads to “persistent and uncontrollable leakage.” I suspect that not all potential readers remember exactly what the “karstification process” is. HESS aims at a broad readership; therefore, an effort should be made to address this broad readership by thoroughly explaining the terms and concepts.
Introducing Figure 1 earlier and including additional features, such as the permeability linked to fracture aperture changes and the chemical gradients that shape the LKB zone, can help rectify this. The latter will significantly aid in clarifying the cause-and-effect relationship that the authors seek to establish in their work. This approach will give readers a conceptual framework from the outset and elucidate the terms and concepts of the study.
Line 69: Explain what epikarst is.
Line 71: Not sure “aggressive” is clear in this context.
Line 87: Explain what “speleogenesis” is.
Line 95: add a space after “(4)”
While the criteria for transitioning between equations 1 and 2 are clear, the actual continuous transition between equations 1 and 2 or vice versa is not clear. How do we continuously transition from the laminar to the turbulent approximation without discontinuities in the flux? The flux mass balance presented in Eq. 4 should also be addressed in this context.
Addendum: at the end of the paper, we learn that equation 2 was not used throughout the simulations (or so I understood from the following sentence: “Turbulent flow did not occur throughout the simulations initiated with natural, original fractures.”). If that is the case, why present it?
Line 121: Is Figure 2 an illustration, actual layout, or sub-layout of the fractured domain? Also, the dimensions are critical in understanding the model framework (Reynolds number, head differences, etc.). Referring to boundary, seepage, and head without their dimensions seems inadequate.
Section 2.2.2: Please refer to Figure 2 when explaining the necessary steps in finding the water table.
Section 2.3: The “H₂O-CO₂-CaCO₃” system is heavily influenced by pH. Although the CO₂ concentration can provide an approximation, this is only valid within a limited range of pH values. Please address this aspect.
Furthermore, a convective approach for the laminar case must approximate the reactant depletion as it reaches the fracture surface by some rate law. Since eq. 9-11 do not consider the fracture thickness b_{ij} while the illustration in figure 3 does, I am a bit confused about this matter. Please provide clarity on this aspect.
Line 182: Is the mass removal term converted to a volume change from which the b_{ij} is updated? If so, what is the conversion constant from moles to volume?
Line 204: Correct grammar in “These analyses”
Figure 4: While we agree on the analytical solution deviation, the magnitude of the deviation between the numerical value and the analytical solution is around 50%, which necessitates further elaboration on why it is so large.
Section 2.4.2: It’s hard to understand how well the model performs since we do not have any specific case to compare it to, aside from the analytical solution, which we established as inadequate. How can we be sure that the model works as it should? In terms of numerical analysis, there is no mention of grid size sensitivity, convergence, or stability of the numerical code, which are standard practices. The authors should present these aspects of the code so that we can appreciate it accordingly.
Line 218: “on the both sides” should be “on both sides”
Line 219: “…the algorithm performed well in modeling the water table in heterogeneous network.” Well, compared to what? These statements appear throughout the paper, yet they are not supported by any comparison or measurement that helps us understand what “well” means. The only reference is to the ill-fitted analytical solution.
Table 1: What are the dimensions of the directional term? Angle?
Additionally, the mean length of the fractures is quite large. Is this realistic? Why was this length chosen? It appears that ten well-connected fractures may dominate the simulation.
Line 252: Please clarify the term “evolution time step.”
Line 255, figure 8 caption: What does “ka” stand for? I’m assuming it refers to time, but no dimensions have been provided. This should be clarified in Figure 8, not Figure 10. Additionally, the heat map for the aperture could be confused with the head heat map. It is unclear whether it is necessary.
Section 3.3: In this section, the authors relate the change in aperture to the location of the aquifer, as evident in Figure 11, and also relate the change in flux in a similar manner. However, the cause and effect suggest that the higher potential near the boundaries dictates higher fluxes, and as the flux increases, so does the reaction rate, which widens the aperture. This is a nucleation phenomenon observed in many studies on dissolution, specifically in the context of permeable structures.
Line 295: I find the K calculation very interesting. To begin with, the fact that there is only dissolution in this setup means that the LKB is a “residual” permeability, indicating that while some permeabilities have increased, the LKB remained unchanged. However, the K is calculated directly for a subsection, and figure 12, as well as a close examination of figure 8, shows that there is an anisotropic change in the aperture, where horizontal fractures experience more dissolution than the vertical fractures. This also leads to the formation of the LKB and the observed changes in flux. However, this structural anisotropy is not discussed or quantified in this context, although it is clear that the horizontal head difference drives the anisotropy. This emergence of anisotropy can be found in many studies on rock dissolution, where preferential flows arise due to these boundary conditions coupled with reactive transport. As this emergent behavior appears in similar fields, the connection should be made among them.
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