Articles | Volume 20, issue 7
https://doi.org/10.5194/cp-20-1559-2024
© Author(s) 2024. This work is distributed under the Creative Commons Attribution 4.0 License.
Climate and ice sheet dynamics in Patagonia throughout marine isotope stages 2 and 3
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- Final revised paper (published on 23 Jul 2024)
- Preprint (discussion started on 16 Jun 2023)
Interactive discussion
Status: closed
Comment types: AC – author | RC – referee | CC – community | EC – editor | CEC – chief editor
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RC1: 'Comment on cp-2023-47', Anonymous Referee #1, 18 Jul 2023
- AC1: 'Reply on RC1', Andrés Castillo, 20 Nov 2023
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RC2: 'Comment on cp-2023-47', Ilaria Tabone, 04 Oct 2023
- AC2: 'Reply on RC2', Andrés Castillo, 21 Nov 2023
Peer review completion
AR – Author's response | RR – Referee report | ED – Editor decision | EF – Editorial file upload
ED: Reconsider after major revisions (27 Nov 2023) by Pepijn Bakker
AR by Andrés Castillo on behalf of the Authors (11 Mar 2024)
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ED: Referee Nomination & Report Request started (19 Mar 2024) by Pepijn Bakker
RR by Ilaria Tabone (21 Mar 2024)
ED: Publish subject to minor revisions (review by editor) (06 Apr 2024) by Pepijn Bakker
AR by Andrés Castillo on behalf of the Authors (16 May 2024)
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ED: Publish as is (17 May 2024) by Pepijn Bakker
AR by Andrés Castillo on behalf of the Authors (27 May 2024)
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Castillo-Llarena and co-authors present numerical experiments to reconstruct the Patagonian ice sheet (PIS) at the last glacial maximum (LGM, 23-19 ka). They use an hybrid shallow ice / shelfy-stream model at 8 km resolution forced by PMIP outputs super-imposed to ERA5. They run 10 kyr under perpetual climate forcing to reach ice sheet equilibrium. Their major finding is that, using this methodology, the PMIP model ensemble does not reproduce the ice sheet extent inferred from geological evidence.
Numerical simulations of the Patagonian ice sheet are scarce, this is a nice motivation for this work. The methodology itself is sound, although not novel since it has been used multiple times, notably to simulate Northern Hemisphere ice sheets at the LGM. However, I have to admit that I am not convinced that it is appropriate in this case. The authors are trying to reproduce an ice field that is much smaller than the other LGM ice sheets (at max. 1/4th of present-day Greenland ice sheet). The topographic setup is also much more complex than in Greenland (for example) since the whole Patagonian ice sheet (PIS) is sitting over the Cordilleran mountains which display an extremely rough terrain. These lead to a spatially highly heterogeneous climate (altitude dependency, rain shadow effects etc.). The authors do not apply any specific corrections to the PMIP models (only a classical vertical lapse rate correction). Worse, they use ERA5 to get a “better” pre-industrial climate but in doing so they keep the imprint of ERA 5 (pretty much linked to present-day topography) at the LGM. With an ice sheet, the topography becomes necessarily much smoother so the complexities seen in ERA5 do no longer apply. The methodology used here has be followed for other much larger objects (e.g. Greenland), and even in this case it is generally accepted that the Eastern part of the Greenland ice sheet (which has a rough topography) is generally poorly represented with such “anomaly method”. I think that one reason for the small available numerical reconstruction of this ice sheet in the literature is due to the fact that it is a complex thing to model since it requires an adequate climate downscaling.
A second comment on spatial resolution is that the topography is very complex so we expect a LGM ice flow that displays strong horizontal gradients. The authors use a 8 km spatial resolution which seems very coarse given the spatial scales studied here. To my knowledge (even though I have not run the model in its latest revision), SICOPOLIS is not very demanding in terms of computational cost. If really the computing time is an issue I would suggest to reduce the vertical discretisation since 81 points in the ice (while SIA displays a relatively smooth profile) and 41 in the bedrock (where only temperature diffusion is solved!) seem a bit too much. Although I guess the computational cost is mostly linked to horizontal discretisation (since you might need to reduce the timestep to avoid numerical instabilities).
In summary, my major comment is on spatial resolution and, above all, climate downscaling. The authors conclusion (PMIP inability to reproduce LGM PIS) was pretty much expected. This study appears after the one of Yan et al. (2022) but it is much less thorough. Yan et al. (2022) used also the same, potentially controversial, method but they also tested climate sensitivities (temperature and precipitation alone, PMIP anomalies), climate parameters (PDD factors) and ice dynamics (sliding coefficient). I agree that it is better to have different studies on a single scientific question but here it does not bring any new piece of information since the methodology is the same (here with a coarser resolution) but with less discussion on the PMIP outputs.
Major comments
1) Climate downscaling & ice sheet resolution
As explained in the introduction of this review and I am not convinced that the methodology is suited for the LGM PIS. In addition this study arrives later than Yan et al. (2022). For this reason some additional work should have been done to bring some kind of novelty, such as for example, a proper discussion of the limitation of the employed method. It is possible that no regional atmospheric model simulation of Patagonia at the LGM has been run (I am not familiar with the literature) but maybe the authors could have suggested a few possible alternatives? Also, even given the huge biases of the PMIP model, why not running the ice sheet model forced by the PMIP outputs directly with no anomaly (or maybe some domain-wise correction). Or perhaps the authors could have smoothed the ERA 5 climatology to be compatible with the PMIP model resolution before applying the anomaly. Keeping the imprint of ERA5 does not make sense to me.
Also an ice sheet resolution of at least 2 km (preferably smaller) should have been employed given the rough topography.
2) Climate evaluation.
There is no map of temperature and precipitation under modern condition nor for the LGM. Is ERA5 good for the Patagonian region? Do you simulate the extent of present-day ice fields when using ERA5? If not, perhaps ERA5 needs also some correction. The LGM PMIP anomalies (January temperature and precip) should have been shown (in the supplement if too many maps). I liked the proxy data discussion but I found it too weak: where is located the pollen-based data? Have you selected a model grid point (outside of the LGM ice mask used) close to this site? This could have been a novelty compared to Yan et al. (2022) to include a more detailed proxy-data comparison (but I am not familiar with this data so perhaps it is qualitative than quantitative).
3) At several occasion in the text the authors mention the “chronology” of the PIS maximum. I generally agree with the authors about non-synchronicity of climate change. However I don’t think the present study brings any information about this. Instead of equilibrium simulations, it could have been possible to run transient ice model simulations using an index method (using an index representative of Southern Hemisphere temperature change). This would also have been a real improvement with respect to Yan et al. (2022).
4) Glacial erosion / sediments.
There was large glacial erosion during the last glacial cycle. So it is a simplification to use present-day topography. This is not discussed here. In addition, testing the model response with a different topography map could have been a novelty with respect to Yan et al. (2022). However, the main control here of ice sheet extent is the climate forcing so it is a much minor comment than the other first two.
Minor comments
- I do not agree with your sentence on P1L16: at the LGM the topography is much less complex than for present-day condition since the ice sheet is expected to drastically smooth the topography.
- Sentence P2L48-50 seems a bit out of context here since mostly EMICs use interactive ice sheets and the authors mostly describe GCM models through PMIP experiments (with no interactive ice sheets).
- Sec. 2.1: dragging law used?
- Sec. 2.2: how do you compute the anomalies? You should have put the LGM outputs and the PI outputs to the same topography (since the GCM sees different topographies). You mention the lapse rate on the previous section, is it also used to compute the PMIP anomalies? What has been done to precipitation do you account for the drying linked to temperature decrease?
- Sec. 2.2: show ERA 5 January temperature and annual precipitation. If there is a strong correlation with topography (which I expect) then the anomaly method is not suited (since the topography is much flatter at the LGM given the presence of the ice sheet).
- Sec. 2.2: resolution of ERA5 used?
- Sec. 2.2: should cite previous papers that use the anomaly method such as, e.g., Charbit et al. (2002)
- Sec. 3.x: I am not sure that Fig. 3 is the best illustrative figure. What we see in this figure is that the model strongly disagree, it is hard to see an emerging pattern. Some maps might help to understand the signal better. Maybe maps of surface mass balance for present-day topography or on ICE6G-C topography could have been useful.
- Sec. 3.2: the eastern extent is probably due to a combination of the strong rain shadow effect in ERA 5. Is this rain shadow effect is expected to be so strong at the LGM given the flatter topography and different zonal winds? This is something to discuss.
- P8 L148-150: should we need a model to draw this conclusion?
- Ice mask and topography used in PMIP models. I think this point is really important and it is good that it is brought forward. It should be clearly stated if the PMIP models use an ice mask in agreement with the reconstruction or not. Generally there is a strong albedo effect so the local temperature simulated by the model is strongly impacted by the presence of an ice sheet. If the GCM does not have an ice mask in its boundary conditions it will be hard to reconstruct an ice sheet there. Is this the case here? Do you have a strong correlation of the January temperature anomaly and the ice mask? It seems that the ice mask is shifted to the East in models that do have an ice mask. This is probably the reason of the too large simulated extent there?
Technical comments
- P5L86 Lambeck et al. (2014) have a drop of about 140 m of sea level.
- Fig. 1: it is hard to see the topography with this grey colour gradient (while we see fine the ocean, but we don’t need it). Generally the figures are a bit hard to read.
- Fig. 2: the green line is barely visible when there is a simulated ice sheet.
Reference
Charbit, S., Ritz, C., and Ramstein, G.: Simulations of Northern Hemisphere ice-sheet retreat: sensitivity to physical mechanisms involved during the Last Deglaciation, Quater. Sci. Rev., 21, 243–265, 2002.