Articles | Volume 19, issue 1
https://doi.org/10.5194/tc-19-63-2025
© Author(s) 2025. This work is distributed under the Creative Commons Attribution 4.0 License.
A topographically controlled tipping point for complete Greenland ice sheet melt
Download
- Final revised paper (published on 09 Jan 2025)
- Preprint (discussion started on 10 Oct 2023)
Interactive discussion
Status: closed
Comment types: AC – author | RC – referee | CC – community | EC – editor | CEC – chief editor
| : Report abuse
-
RC1: 'Comment on tc-2023-154', Anonymous Referee #1, 31 Oct 2023
- AC1: 'Reply on RC2', Michele Petrini, 31 Dec 2023
-
RC2: 'Comment on tc-2023-154', Anonymous Referee #2, 10 Nov 2023
- AC1: 'Reply on RC2', Michele Petrini, 31 Dec 2023
-
RC3: 'Comment on tc-2023-154', Anonymous Referee #3, 30 Nov 2023
- AC1: 'Reply on RC2', Michele Petrini, 31 Dec 2023
Peer review completion
AR – Author's response | RR – Referee report | ED – Editor decision | EF – Editorial file upload
ED: Publish subject to revisions (further review by editor and referees) (18 Jan 2024) by Ruth Mottram
AR by Michele Petrini on behalf of the Authors (10 May 2024)
Author's response
Author's tracked changes
Manuscript
ED: Referee Nomination & Report Request started (12 Jul 2024) by Ruth Mottram
RR by Anonymous Referee #3 (28 Aug 2024)
ED: Publish subject to technical corrections (01 Nov 2024) by Ruth Mottram
AR by Michele Petrini on behalf of the Authors (06 Nov 2024)
Manuscript
Review of “A topographically-controlled tipping point for complete Greenland ice-sheet melt” by Michele Petrini et al.
In the manuscript under review, the authors run ice sheet model simulations of the Greenland Ice Sheet to test for it’s “tipping”. The surface mass balance is created by using elevation-class downscaling from CESM2. Since a temperature correction depending on surface elevation is included in this, the melt-elevation feedback is considered in the simulations. In addition, a simple model for earth deformation is included, which means that a bedrock-uplift feedback can be considered. For different levels of warming, the climate conditions are held constant and the long-term response of the ice sheet to this climate (including the feedbacks mentioned before) is simulated.
Main comment:
1) The usage of terminology in the draft is quite vague. A number of terms are used (“tpping”, “runaway”, “stabilising”, “topographically-controlled tipping point”, “pinning point”....) but they are never defined. As these can be used in different ways in different communities or are not known to me (e.g., topographically-controlled tipping point), it is essential that all these terms are defined and used consistently in the manuscript.
2) My impression is that the authors use “tipping point” as multistability shown by Robinson et al. (2010)? If this is true, however, they do not really show that the threshold they find is a “tipping point”, i.e., a bifurcation point. They show that at some level of SMB, the ice sheet eventually vanishes, but it remains unclear if this is reversible or not? Is there is hysteresis or not?
3) The study aims to analyse the “SMB threshold for complete melt” but does not include an uncertainty estimate for two essential processes, namely, the lapse-rate temperature correction and the bedrock uplift. At least a variation of these parameters would be expected to test for the robustness of the presented results.
4) The study claims that it identified a “topographically-controlled tipping point”, which I think refers to the “pinning point” that they mention the western margin of GrIS. Importantly, they find that this region deglaciates first in the “full melt” simulations, but stays in the “medium melt” simulations. This is however only an indication for a hypothesis, not a proof. If the authors wanted to prove this statement, they could for example prevent this region from deglaciating in the strong warming simulations (by not changing the SMB there for example) and showing that this means also the rest of the ice sheet does not vanish. Again, here the terminology is unclear: what do you mean here with tipping point? Which is exactly this region, it is only termed the GrIS western margin?
Further comments:
Abstract
- line 12: “highly nonlinear” → “nonlinear” as highly is not quantified.
- line 14 “runaway retreat”, runaway means that the feedback gain of this process if larger than 1, I don’t think that this has been shown yet. Rather, you can say “self-reinforcing”, “self-sustained”.
- line 14: if GIA only delays deglaciation, it does not “stabilise” the margin in the sense of stability analysis. It only affects the timescales.
- line 14-16: this sentence is not clear, reformulate.
- line 16-18: you do not show that this region is the trigger for tipping.
- line 19: what do you mean with “stabilising effect”?
Introduction
- in general the introduction is written as if you are intending to provide an estimate for a tipping point, however, this is not done in this manuscript (see main comments).
- line 24-25: Add a citation for “while until the late 1990s ice discharge has been the main source of ice loss”.
- GIA and it’s effect on GIS stability (papers like Zeitz et al.,2022) is directly relevant to this study and should be discussed in the introduction.
Methods
- A section on the model initialisation is missing. It is pointed to previous studies, but it would be useful to have a quick summary how you initialise and optimise model parameters here.
- lines 97 and following: does the downscaling mean that the SMB that the ice sheet model sees is not equivalent in mass to the fluxes in CESM2?
- line 129: How long does it take to reach the stable ice sheet configuration? What is your criterion for “stability”? Looking at Figure 2, it appears that quite a few runs are still changing (2.5 to 3.8K runs).
- How are the sensitivity runs done? You mention different till friction angle and switching off bedrock uplift – are new equilibrium initial states created for these conditions? If not, do you show the results in Fig A2 relative to a control run?
Results
The concept of a “topographic pinning point” is not clear to me. The results are meant to show that a region in west Greenland is such a “pinning point”, and if it is “un-pinned” the GrIS retreats in all other regions as well. However, the results shows only a correlation between this region being part of the maximum ice sheet extent during oscillations and regions in Greenland being glaciated. And it disappears first. This does not mean that this specific region has any control over other regions being glaciated further away. There is no physical process named through which this pinning point is “stabilising” the other regions of the ice sheet.
- line 139 “exhibits”
- line 139 how do you quantify “highly nonlinear”?
- line 146: please clarify “low GrIS melt is achieved for a decrease in SMB not exceeding 50% of the equilibrium pre-industrial SMB”. This sentence is quite complicated. And why is the pre-industrial SMB an equilibrium SMB?
- line 177: what do you mean with “more stable”?
- line 193: discharge is not included in your experiments except for a fixed
- line 197: please specify where this region is in the figures, e.g., show it in the figures.
- line 197: what is a topographic pinning point?
- line 201: what do you mean with “runaway”?
- line 203: How is this tipping point behaviour? You do not show irreversibility.
Discussion
- line 219: it might be worth giving the numbers here as they diverge quite a lot
- line 241: remove “highly”
Conclusions
- line 290: provide the “other studies”
- lines 291: you do not show that “tipping” depends on the margin – you show that the margin gets lost first.
- line 294: give the previous modelling studies
- line 297: “includes”, typo
Tables and Figures
- Table 1: The SMB related to the intial values at the start of the repeat-forcing runs, or? Where do the uncertainties in the final volume come from? Why are there no uncertainties in the Min. vol. Time then?
- Table 2: What are the CESM2-only runs? It appears to me that they are not relevant to this study here?
- Figure 2: How are the two axes GrIS integrated SMB (Gt/yr) and mm/yr linked? The GrIS extent changes drastically in the runs, and theoretically, this can cause a change of the integrated SMB while the average SMB remains the same.
- Figure A5, A6: I think these are never referenced.
- Table A1: does this mean you are using a spatially constant geothermal heat flux?