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International Polar Year 2007–2008 - WMO

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Fig. 3.2-6. Composite<br />

changes in the polar<br />

troposphere in<br />

October-December<br />

2002-8 as the ice<br />

retracted from the<br />

western Arctic. Top<br />

left: vertical section<br />

of air temperature<br />

anomalies (ºC) from<br />

the Bering Strait to<br />

the Pole. Top right:<br />

corresponding plot of<br />

geopotential height<br />

anomalies (dynamic<br />

metres). Lower<br />

left: the 500-1000<br />

hPa thickness field<br />

anomaly showing, in<br />

particular, the band<br />

of greater thickness<br />

from the E. Siberian<br />

Sea to N Alaska,<br />

the main region of<br />

diminished sea-ice<br />

cover. Gradients in this<br />

field are the baroclinic<br />

contribution to the<br />

flow field. Lower<br />

right: the zonal wind<br />

anomaly field (ms-1)<br />

at 700 hPa showing<br />

the reduction in zonal<br />

wind component<br />

north of Alaska and<br />

western Canada.<br />

(Images: Overland and Wang<br />

(2010)<br />

378<br />

IPY 20 07–20 08<br />

three times the ocean cooling rate and 10 times the<br />

mechanical work of the standard winter model runs<br />

were applied to the mixed layer. It thus seems most<br />

likely to Toole et al., that if PSW heat is vented upwards<br />

in the central Canada Basin in the near future, that flux<br />

will be accomplished by a relatively weak, small-scale<br />

turbulent diffusive process. John Toole (WHOI) will<br />

lead on the two main questions that underlie this issue:<br />

What are the intensities and the physical mechanisms<br />

supporting turbulent diapycnal heat and fresh water<br />

fluxes between the Arctic surface mixed layer and the<br />

waters immediately underlying, and how might those<br />

fluxes change in future if we transition to a seasonal<br />

ice pack?<br />

Q: How might the ice-free polar ocean alter the regional<br />

atmospheric circulation?<br />

A: As the ice in the Pacific sector of the Arctic melted<br />

back to its record minimum in summer 2007 and the<br />

heat storage of the underlying ocean increased, the<br />

release of this heat in autumn eroded the stratification<br />

of the atmosphere to progressively higher levels<br />

leading to a clear change in the regional atmospheric<br />

circulation.<br />

As Fig. 3.2-6 reveals, the retraction of sea-ice cover<br />

from the western Arctic in summer 2002-08 was<br />

accompanied by a warming throughout the Arctic<br />

troposphere and an increase in geopotential height<br />

anomaly in fall leading to a weakening of the poleward<br />

geopotential gradient. It is this weakening of the thermal<br />

wind that reduces the jet stream winds, according to<br />

Overland and Wang (2010). [“The consequences of<br />

increased September open water in the western Arctic<br />

and increased 1000–500 hPa thickness is an anomalous<br />

late autumn easterly zonal wind component, especially<br />

north of Alaska and Canada on the order of 40%”. (op<br />

cit, P8)]. If so, this will be a highly significant result for the<br />

IPY. It therefore makes sense to inquire, in planning an<br />

observational legacy phase for the IPY, what continued<br />

coverage of the upper watercolumn would be needed<br />

to keep track of ocean-atmosphere heat exchange<br />

as the sea-ice dwindles away. It precisely this is the<br />

question that will be addressed by Jim Overland and<br />

Muyin Wang (NOAA-PMEL).

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