Kent A. Peacock (12 Sep 2018) "A Different Kind of Rigor: What Climate Scientists Can Learn from Emergency Room Doctors", Ethics, Policy & Environment, Volume 21, 2018 - Issue 2, Pages 194-214, https://doi.org/10.1080/21550085.2018.1509483
https://www.tandfonline.com/doi/full/10.1080/21550085.2018.1509483
Peacock says:
"There is a genuine possibility, however, remote, that the whole contents of the Bentley trench could shatter in a matter of weeks or months, raising global mean sea level by 3 m or more almost immediately."
What peer-reviewed publication supports this statement? I think Pollard, DeConto & Alley 2015 have said they can't rule out this is possible in a matter of "decades" (3m in 3 decades?):
https://www.sciencedirect.com/science/article/pii/S0012821X14007961
"In summary, applying a simple Pliocene-like warming scenario to our model, the combined mechanisms of MISI, melt-driven hydrofracturing and cliff failure cause a very rapid collapse of West Antarctic ice, on the order of decades."
I have not seen "weeks or months". Anyone else?
Lennart,
First, the Peacock paper is peer-reviewed, but that said, I have not seen another comparable statement about the stability of the ice above the Bentley Subglacial Trench.
Second, the statement from Pollard, DeConto & Alley (2015) addresses a collapse of the entire WAIS within decades; while the Peacock (2018) comment was limited to the Bentley trench. Also, Pollard, DeConto & Alley (2015) limited the rate of ice-cliff retreat to less than half (i.e. 5 km/a) of the maximum observed for the Jakobshavn Glacier of about 13 km/a (see the Youtube video & Reply #268):
https://www.youtube.com/watch?time_continue=3029&v=aqVPlBf4ydoHowever:
a. Jakobshavn ice flow is restrained on both sides by the wall of the fjord; while the ice in the Bentley trench does not have comparable side restraints.
b. Jakobshavn is currently retreating up a positively sloped ice bed; while this would not be the case for an ice cliff with the Bentley trench formed some years after the initiation of a MICI collapse triggered at the threshold of the Thwaites Glacier.
c. The current height of the Jakobshavn ice face is in the 100 to 120m range, while after a few tens of kilometers of retreat, the ice face for the Thwaites Glacier could be several hundred meters high and with a relative water depth w = D/H (water dept/ice face height) of 0.6 to 0.8; for such a case Schlemm & Levermann (2018) indicates that the actual retreat rate would be well (likely by many times) over 60 km/a (see also Reply #278).
Tanja Schlemm and Anders Levermann (2018), "A simple stress-based cliff-calving law", The Cryosphere Discuss.,
https://doi.org/10.5194/tc-2018-205https://www.the-cryosphere-discuss.net/tc-2018-205/tc-2018-205.pdfFourth, the linked Ivanovic et al. (2018) reference indicates that paleo-signals from meltwater pulse events in the NH override any such paleo-signals from SH meltwater pulse events. Thus one would not likely able to find any evidence of a meltwater pulse event in the paleo-record from a meltwater pulse event associate with the Bentley Subglacial Trench.
R. F. Ivanovic et al. (04 June 2018), "Climatic Effect of Antarctic Meltwater Overwhelmed by Concurrent Northern Hemispheric Melt", Geophysical Research Letters 45, Issue 11
https://doi.org/10.1029/2018GL077623https://agupubs.onlinelibrary.wiley.com/doi/full/10.1029/2018GL077623Abstract
Records indicate that 14,500 years ago, sea level rose by 12–22 m in under 340 years. However, the source of the sea level rise remains contentious, partly due to the competing climatic impact of different hemispheric contributions. Antarctic meltwater could indirectly strengthen the Atlantic Meridional Overturning Circulation (AMOC), causing northern warming, whereas Northern Hemisphere ice sheet meltwater has the opposite effect. This story has recently become more intriguing, due to increasing evidence for sea level contributions from both hemispheres. Using a coupled climate model with freshwater forcing, we demonstrate that the climatic influence of southern‐sourced meltwater is overridden by northern sources even when the Antarctic flux is double the North American contribution. This is because the Southern Ocean is quickly resalinized by Antarctic Circumpolar water. These results imply that the pattern of surface climate changes caused by ice sheet melting cannot be used to fingerprint the hemispheric source of the meltwater.
Plain Language Summary
The fastest major sea level rise ever recorded took place 14,500 years ago, when sea level rose by 12–22 m in under 340 years. The extra water came from melting ice sheets, which stretched across North America and northern Europe as well as Greenland and Antarctica. We ran a climate model to test the impact of different meltwater contributions from Antarctica and the Northern Hemisphere ice sheets (North America, Greenland, and Eurasia). Our simulations demonstrate that northern meltwater has a much stronger and longer lasting effect on ocean circulation and climate than Southern Hemisphere melt. Consequently, northern melting overrides the impact of southern melting even when the flux of water from North America is only half the magnitude of the Antarctic flux. This means that past climate records cannot be used to identify the contribution of meltwater from different ice sheets: the northern signal can override the southern signal.
Fifth, the two images from Bassis & Walker (2011) show that any ice cliff in the Bentley trench would inherently be unstable and would collapse with the slightest perturbation.
J. N. Bassis & C. C. Walker (23 November 2011), "Upper and lower limits on the stability of calving glaciers from the yield strength envelope of ice", Proceedings of the Royal Society A,
https://doi.org/10.1098/rspa.2011.0422https://royalsocietypublishing.org/doi/full/10.1098/rspa.2011.0422Abstract
Observations indicate that substantial changes in the dynamics of marine-terminating ice sheets and glaciers are tightly coupled to calving-induced changes in the terminus position. However, the calving process itself remains poorly understood and is not well parametrized in current numerical ice sheet models. In this study, we address this uncertainty by deriving plausible upper and lower limits for the maximum stable ice thickness at the calving face of marine-terminating glaciers, using two complementary models. The first model assumes that a combination of tensile and shear failure can render the ice cliff near the terminus unstable and/or enable pre-existing crevasses to intersect. A direct consequence of this model is that thick glaciers must terminate in deep water to stabilize the calving front, yielding a predicted maximum ice cliff height that increases with increasing water depth, consistent with observations culled from glaciers in West Greenland, Antarctica, Svalbard and Alaska. The second model considers an analogous lower limit derived by assuming that the ice is already fractured and fractures are lubricated by pore pressure. In this model, a floating ice tongue can only form when the ice entering the terminus region is relatively intact with few pre-existing, deeply penetrating crevasses.
Caption for the first image: "Contours showing maximum stable ice thickness as a function of water depth for different crevasse penetration depths for a constant yield strength of 1 MPa. The contours represent different crevasse penetration ratios r, ranging from 0 (no crevasses) to 1 (completely fractured). The arrows indicate the maximum dry calving cliff thickness when crevasse depths are computed according to the Nye theory (110 m) and when the ice is assumed to be intact with no pre-existing crevasses (221 m). The dashed black line shows the thickness at buoyancy for a given ice thickness. Inset: the maximum floating termini thickness for different fractions of intact ice."
Caption for second image: "Comparison of observed height-above-buoyancy and water depth against predicted bounds. The shaded region shows allowed values for the height-above-buoyancy determined using S3 (C0=1 MPa,α=0) with no crevasses. The dashed black line shows the maximum height-above-buoyancy permitted when surface and bottom crevasses are included. The dotted line shows a constant height-above-buoyancy of 50 m. Density of ice ρi=920 kg m−3 and density of water ρw=1020 kg m−3. CG, Columbia Glacier, Alaska; AK, Alaska; Sb, Svalbard; WG, West Greenland; HG, Helheim Glacier, Greenland."
Best,
ASLR
For ease of reference, I provide the third attached image from Schlemm and Levermann (2018)