Review of "Simulating the evolution of Hardangerjøkulen ice cap in southern Norway since the mid-Holocene and its sensitivity to climate change" by Åkesson et al.
The manuscript under consideration is a manuscript that has been substantially revised following recommendations of two reviewers. I have not read the original manuscript in detail but familiarized myself with the reviewers' comments and the authors' responses. In light of this, I'm trying to avoid pushing the manuscript into a new direction, however I do have a number of comments.
Hope it helps,
Andy Aschwanden
The manuscript is generally well written, flows nicely and is easy to follow and now has a clear(er) focus. The authors have carefully addressed the reviewers' comments. While the reviewer's comment "This setup, with a focus on the long-term evolution of the ice cap, is interesting to get an insight in the dynamics of this ice cap and the important role of the surface mass balance (SMB) and its feedback with elevation. However, the authors do not really dig into these concepts" still holds true, though to a lesser degree, the authors explicitly state their focus on long term reconstruction.
My main comment is that the manuscript could be made more relevant and broadly appealing by putting the results in a wider context and contrasting/comparing their findings with other recent work on ice caps and icefields. For example, recent publications assess the stability of the Juneau Icefield (Ziemen et al, 2016) and Yakutat Glacier (Truessel et al, 2015). Both glaciers are in south-east Alaska in a similar climate setting, but Yakutat Glacier is expected to disappear by the end of the 21st century while the Juneau Icefield is expected to survive. Ziemen et al (2016) have done many modeling experiments that are quite similar to this study (e.g. sensitivity to sliding, regrowth capability under different climate scenarios). I find it very interesting that for present-day climate, Hardangerjøkulen ice cap only grows to 20% to its current volume when starting from ice free conditions, while the Juneau Icefield's regrowth volumes are close to the steady-state volumes when starting from present-day (Fig 11 in Ziemen). Other similarities include the sparseness of the ice thickness data. Ziemen showed, using a very crude sensitivity experiment, that uncertainties in ice thickness have a strong impact on the simulated volume evolution. Very recently, Gilbert et al (2016) studied the evolution of the Barnes Ice Cap on Baffin Island, corroborating some of the findings of Mahaffy's seminal 1976 paper, and concluded that the ice cap will disappear within this millennium. I hope this will help expand on the concluding statement (P20,L14) "We expect that ice caps with comparable geometry elsewhere may display similar sensitivity and hysteresis".
Figure 2, SMB-altitude profile and P15, L19-20: I'm not quite able to figure out how the profile was derived from observations without reading all the underlying literature, so this might be a red herring: looking at the geographical setting, I can imagine that the ice cap experiences orographic precipitation at least to some degree, where the windward side receives higher precipitation than the lee side. If more high-altitude area is in the lee side, averaging could lead to a decrease in SMB at high altitude. Schuler et al (2008) studied orographic precipitation effects on the Svartisen ice cap further north using the Smith and Barstad (2004) linear theory of orographic precipitation model.
A side note: The authors' statement in the response letter "In addition, we think that the dependency of initial conditions for ice caps (hysteresis), illustrated in Fig. 11, has not received much attention in the literature and is relevant for modeling and reconstructing paleo-ice caps and predicting future ice cap evolution." may be true for small(er) glaciers, but not for ice sheets. We've been pushing this idea for more than 5 years now; see Aschwanden, Aðalgeirsdóttir, and Khroulev (2013) and Aðalgeirsdóttir et al (2014).
Detailed comments:
P1, L13-14: "... that the surface mass balance-altitude feedback and ice cap hypsometry are essential to this sensitivity." The surface mass balance-altitude feedback and the glacier hypsometry are not independent of each other (or am I missing something?), the hypsometry of a glacier determines how strong the surface mass balance-altitude feedback is. If memory serves me well, this was beautifully illustrated by Rivera and Cassa (1999)
P2, L3: their sea level equivalents (e.g. Grinsted, 2013; Bahr et al., 2015). It's a good practice to also cite the first manuscript that introduces a new concept (here V-A scaling).
P3, L7: ...ranges form 1020 to 1865 m a.s.l....
P6, L21: ...on a scaling analysis of the Stokes equations... ("full Stokes" still makes me cringe)
P7, L15-20: I do not want to go off on a tangent, but why do you acknowledge that SIA is only valid for no-slip conditions and then go on and combine it with Weertman sliding? See Appendix in Bueler and Brown (2009) why this should be avoided. I do not expect this to influence your general conclusions though (in fact, you will most likely get very similar sensitivities when strictly using no-slip). Along the same lines, I agree with the discussion in the previous reviews that using a more complex stress balance is not needed here.
P7, L23-24: "In this study, the basal sliding parameter β is assumed spatially and temporally constant. In reality, sliding likely varies in space and time according aforementioned factors." This two sentences do not make sense the way they are written, one gets the impression that using a constant β leads to a constant in time and space sliding, which is not true. I think you can just delete the second sentence.
P7, L25-27: There is a much stronger argument against deriving the basal friction parameter from surface properties. Inversions for β are only valid at or around the time stamp of the data sets used for inversion. Consequently, β fields are snap shots and should not used for prognostic simulations at all, but this would be all the more severe for the long time scales (millennia) considered in this study.
P8, L22: Define your steady-state. See Ziemen et al (2016) near Eq. 4 why this is important to correctly interpret your results.
P10, L2: ...sensitivity to the choice of...
P12, L19,22: should be Figure 11a,b not 10
P12, 31: Our Holocene simulations shows...
P19, L2-5: This is a rather broad brush over a large field. At least provide references (there is a wealth of literature on simple, analytical models by glaciologists including, but not limited, to: J. Oerlemans, G. Roe, W. Harrison, M. Luethi).
References:
@article{Aschwanden2013,
abstract = {Validation is a critical component of model devel- opment, yet notoriously challenging in ice sheet modeling. Here we evaluate how an ice sheet system model responds to a given forcing. We show that hindcasting, i.e. forcing a model with known or closely estimated inputs for past events to see how well the output matches observations, is a viable method of assessing model performance. By simulat- ing the recent past of Greenland, and comparing to obser- vations of ice thickness, ice discharge, surface speeds, mass loss and surface elevation changes for validation, we find that the short term model response is strongly influenced by the initial state. We show that the thermal and dynamical states (i.e. the distribution of internal energy and momentum) can be misrepresented despite a good agreement with some observations, stressing the importance of using multiple obser- vations. In particular we identify rates of change of spatially dense observations as preferred validation metrics. Hindcast- ing enables a qualitative assessment of model performance relative to observed rates of change. It thereby reduces the number of admissible initial states more rigorously than validation efforts that do not take advantage of observed rates of change.},
author = {Aschwanden, Andy and Aðalgeirsd{\'{o}}ttir, G. and Khroulev, Constantine},
doi = {10.5194/tc-7-1083-2013},
file = {:Users/andy/pdfs//Aschwanden, Aðalgeirsd{\'{o}}ttir, Khroulev - 2013 - Hindcasting to measure ice sheet model sensitivity to initial states.pdf:pdf;:Users/andy/pdfs//Aschwanden, Aðalgeirsd{\'{o}}ttir, Khroulev - 2013 - Hindcasting to measure ice sheet model sensitivity to initial states.pdf:pdf},
journal = {The Cryosphere},
pages = {1083--1093},
title = {{Hindcasting to measure ice sheet model sensitivity to initial states}},
volume = {7},
year = {2013}
}
@article{Adalgeirsdottir2014,
author = {Aðalgeirsd{\'{o}}ttir, G. and Aschwanden, Andy and Khroulev, Constantine and Boberg, Frederik and Mottram, Ruth and Lucas-Picher, P.},
doi = {10.3189/2014JoG13J202},
issn = {00221430},
journal = {Journal of Glaciology},
keywords = {ice and climate,ice-sheet modeling},
number = {222},
pages = {782--794},
title = {{Role of model initialization for projections of 21st-century Greenland ice sheet mass loss}},
url = {http://www.igsoc.org/journal/60/222/t13j202.html},
volume = {60},
year = {2014}
}
@article{Bueler2009,
author = {Bueler, E. and Brown, J},
doi = {10.1029/2008JF001179},
journal = {J. Geophys. Res.},
number = {F3},
pages = {1--21},
title = {{The shallow shelf approximation as a ``sliding law'' in a thermomechanically coupled ice sheet model}},
volume = {114},
year = {2009}
}
@article{Gilbert2016,
author = {Gilbert, A. and Flowers, G. E. and Miller, G. H. and Rabus, B. T. and {Van Wychen}, W. and Gardner, A. S. and Copland, L.},
doi = {10.1002/2016JF003839},
issn = {21699003},
journal = {Journal of Geophysical Research: Earth Surface},
keywords = {10.1002/2014JF003232 and erosion,climate impacts,geomorphology,modeling},
number = {8},
pages = {1516--1539},
title = {{Sensitivity of Barnes Ice Cap, Baffin Island, Canada, to climate state and internal dynamics}},
volume = {121},
year = {2016}
}
@article{Mahaffy1976,
author = {Mahaffy, M W},
doi = {10.1029/JC081i006p01059},
issn = {01480227},
journal = {Journal of Geophysical Research},
keywords = {doi:10.1029/JC081i006p01059,http://dx.doi.org/10.1029/JC081i006p01059},
month = {feb},
number = {6},
pages = {1059--1066},
title = {{A three-dimensional numerical model of ice sheets: Tests on the Barnes Ice Cap, Northwest Territories}},
url = {http://doi.wiley.com/10.1029/JC081i006p01059},
volume = {81},
year = {1976}
}
@article{Rivera1999,
author = {Rivera, A. and Casassa, Gino},
journal = {Global and Planetary Change},
keywords = {ela,glaciers,hypsometry,patagonia,volume change},
pages = {233--244},
title = {{Volume changes on Pio XI glacier, Patagonia : 1975--1995}},
volume = {22},
year = {1999}
}
@article{Schuler2008,
author = {Schuler, T V and Crochet, P and Hock, R and Jackson, M and Barstad, I and J{\'{o}}hannesson, T.},
doi = {10.1002/hyp.7073},
issn = {08856087},
journal = {Hydrological Processes},
keywords = {accepted 2 april 2008,downscaling,era-40,glacier mass balance,modelling,orographic precipitation,received 1 november 2007,snow distribution},
month = {sep},
number = {19},
pages = {3998--4008},
title = {{Distribution of snow accumulation on the Svartisen ice cap, Norway, assessed by a model of orographic precipitation}},
url = {http://doi.wiley.com/10.1002/hyp.7073},
volume = {22},
year = {2008}
}
@article{Truessel2015,
author = {Tr{\"{u}}ssel, Barbara L. and Truffer, Martin and Hock, Regine and Motyka, Roman J and Huss, Matthias and Zhang, Jing},
doi = {10.3189/2015JoG14J125},
journal = {J. Glaciol.},
keywords = {climate change,glacier mass balance,glacier modeling,ice and climate,mountain glaciers},
number = {225},
pages = {65--75},
title = {{Runaway thinning of the low-elevation Yakutat Glacier, Alaska, and its sensitivity to climate change}},
volume = {61},
year = {2015}
}
@article{Ziemen2016,
abstract = {We study the evolution of the Juneau Icefield, one of the largest icefields in North America (>3700 km 2 ), using the Parallel Ice Sheet Model (PISM). We test two climate datasets: 20 km Weather Research and Forecasting Model (WRF) output, and data from the Scenarios Network for Alaska Planning (SNAP), derived from spatial interpolation of observations. Good agreement between simulated and observed surface mass balance was achieved only after substantially adjusting WRF precipitation to account for unresolved orographic effects, while SNAP's climate pattern is incompatible with observations of surface mass balance. Using the WRF data forced with the RCP6.0 emission scenario, the model projects a decrease in ice volume by 58–68% and a 57–63% area loss by 2099 compared with 2010. If the modeled 2070–99 climate is held constant beyond 2099, the icefield is eliminated by 2200. With constant 1971–2010 climate, the icefield stabilizes at 86% of its present-day volume. Experiments started from an ice-free state indicate that steady-state volumes are largely independent of the initial ice volume when forced by identical scenarios of climate stabilization. Despite large projected volume losses, the complex high-mountain topography makes the Juneau Icefield less susceptible to climate warming than low-lying Alaskan icefields.},
author = {ZIEMEN, FLORIAN A. and HOCK, REGINE and ASCHWANDEN, ANDY and KHROULEV, CONSTANTINE and KIENHOLZ, CHRISTIAN and MELKONIAN, ANDREW and ZHANG, JING},
doi = {10.1017/jog.2016.13},
issn = {0022-1430},
journal = {Journal of Glaciology},
month = {feb},
number = {231},
pages = {199--214},
title = {{Modeling the evolution of the Juneau Icefield between 1971 and 2100 using the Parallel Ice Sheet Model (PISM)}},
url = {http://www.journals.cambridge.org/abstract_S0022143016000137},
volume = {62},
year = {2016}
} |