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Saturday, May 25, 2013

Chris Reynolds: Acceleration of summer Arctic sea ice loss

Posted on 4:39 PM by Unknown

Summer Acceleration

by Chris Reynolds, Dosbat, May 23, 2013

I have recently outlined the changes in the Cryosphere Today Area index (CT Area), using anomalies to examine the changes from the long-term-average seasonal cycle. I've shown the changes in the CT Area anomalies (link), the autumn response to increasing open water in the summer season (link), and the recent June anomaly crashes (link). I have also covered research showing the majority of surface-based Arctic Amplification is a response to summer ice loss (link), and that this amplification is probably being understated by the GISS dataset (link). However, I have not addressed a substantial issue -- that of the summer acceleration loss of area when compared to the loss of winter area.

The ice edges within the Arctic at minimum and outside the Arctic at maximum are set by different regions at opposing times in the seasonal cycle; until recently the recession of the ice edge had been proceeding at very nearly the same rate, leading to only a small increase in annual range. 2007 changed that, as can be seen from Cryosphere Today (link), where 2007 is seen to usher in a steep increase in the annual range.



In the graphic to the left, the green trace (annual daily maximum) is read on the left-hand axis, and the red trace (annual daily minimum) is read on the right-hand axis. However, both axes are 6M km^2 across, and are merely offset to match the earlier period. From this it can be seen that, for much of the period, both maximum and minimum follow each other relatively closely. In other words, whatever caused the reduction in area in March and September, it seemed to be applied equally to regions geographically remote and removed in time by 6 months. The most reasonable cause of this, backed up by other reasoning, is that Anthropogenic Global Warming has been causing the loss; to argue for separate processes makes things get rather complicated very quickly. This period of decline of sea ice also covers a period of substantial volume loss; September lost 7,800 cubic kilometres of sea ice from 1979 to 2006.

However, since the 1990s, and to a far more marked degree since 2007, the two plots have diverged markedly. This is the Summer Acceleration.



Using the data I've previously calculated, I have broken down the April PIOMAS volume into the volume contribution from grid box cells with an effective thickness of less than 2-m thick, and the volume contribution from those cells whose effective thickness is more than 2-m thick. April is chosen as the peak volume month, a 2-m-thick demarcation is chosen because ice thinner than 2 m thick is typically thermodynamically-grown first-year ice and that over 2 m thick is typically mechanically-thickened multi-year ice. The graph covers 1978 to 2012.

It can be seen that while ice under 2 m thick has remained the same (growing in recent years), the volume decrease is from ice over 2 m thick. Furthermore, when the declining ice over 2 m thick is superimposed over a plot of daily minimum in CT Area, they match reasonably closely. I don't think this is accidental.

The peripheral seas outside the Arctic Ocean are where the sea ice maximum is set; during the period of the above graph they have always been seasonal, with no surviving multi-year ice, so their ice falls into the under-2-m-thick category. So whilst it may seem odd that ice volume in April would relate closely to conditions 5 months later within the Arctic, it is not odd at all because the ice over 2 m thick is all within the Arctic Ocean. The loss of thicker ice has been directly impacting the initial conditions for seasonal melt within the Arctic Ocean.

So it seems that volume in April is driving the loss of area in September. I don't think the reverse is true because volume has been declining from the thickest ice, away from the ice edge. This is shown by the decline from ice over 2 m thick, not from the first-year ice (2 m thick and under) that would form after the September minimum in the periphery of the pack (around the coasts of the Arctic Ocean). Furthermore, as can be seen in recent years, with the increase in volume from ice less than 2 m thick; thin ice is able to 'bounce back' from perturbations, which is a strong negative feedback (e.g., Tietsche et al., Bitz & Roe), whereas, having a longer persistence (being many years old), thicker older ice has more of a 'memory' of impacts and hence carries forward the forcing of anthropogenic warming.

Volume loss drives thickness loss because volume loss represents thinning and, as I've discussed previously, thinning increases open-water-formation efficiency (link). This can be appreciated using the same approach as Figure 2 of Keen et al. (2013), "A Case Study of a Modelled Episode of Low Arctic Sea Ice." However, I have calculated the following graphic from gridded PIOMAS data (link).



The grey plots are for all years 1978 to 2012, lighter greys for more recent years, darker for earlier. Red is the average of that full period, green is the post 2007 average, blue is the average for 2010 to 2012. The large swings for some years of thicker ice are due to transport of thicker ice in those years, leading to open water.

Going along the horizontal axis are thicknesses of PIOMAS modelled sea ice in April; these are broken down into 5-cm bands, then for each band I calculated the percentage of ice in that thickness band that melts out to give open water in September -- this percentage is given in the vertical axis. It is perhaps easiest to understand if I take a simple case where all the ice is only one thickness and use the red line as the long-term average.

If we had an ice pack that was uniformly 3.5 m thick, then using the graph, finding the 3.5-m increment on the horizontal axis, we can go across from there to find that we'd expect about 7% of the pack to melt out to open water by the end of the melt season in September. Now if we thin this imaginary ice pack to 2.5 m thick, we can use the red line to scan across and see that about 12% would melt out by September. But if we thin this pack by just 1 m more, to 1.5 m, now a massive 80% of the ice area melts out by September.

I have used gridded PIOMAS data to calculate the average thickness of the April ice pack north of 70N -- this is to bias the result in favour of conditions within the Arctic Ocean.



With average ice thickness dropping to below 2 m, we are now firmly in the region where the percentage melt increases rapidly, and non-linearly, with further reductions in April grid box thickness. What this means is that we can expect strong volatility in the sea ice in the years to come, and without some stabilisation of the April thickness, we will see this volatility manifesting itself as a succession of crashes in area and volume.


Whether or not we face a rapid transition still bothers me. I haven't changed my opinion back to being sceptical of a rapid transition, but I may still do so dependent on events. However, I don't think the case for it is much more persuasive than the case against.


The decline in volume has hit a critical phase; where compared with past decades virtually all the MYI volume has been eliminated from the Arctic Ocean. Will we see autumn ice growth stabilise the pack, or will further declines in volume cause such winter thinning that we will see a virtually sea-ice-free state in the pack within years? I don't know.


Because area and extent are readily obtained from satellite data, public attention tends to be focused on these metrics. However, the acceleration of the summer decline in area and extent is a result of the decline in volume. 


http://dosbat.blogspot.fi/2013/05/summer-acceleration.html
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