1
Core 2003 y = -0.31x + 1100 Core 2005 y = -0.77x + 2000 Core 2004 y = -1.28x + 3050 300 350 400 450 500 550 600 650 700 1850 1870 1890 1910 1930 1950 1970 1990 2010 2030 Elevation m Denstiykgm -3 Difference between gradients: 2003 and 2004 -99% significant 2004 and 2005 -97.5% significant 2003 and 2005 -97.5% significant T4 T5 T6 Variations in mass balance and snow and firn densities along a transect in the percolation zone of the Greenland Ice Sheet Vicki Parry (1), Peter Nienow (1), Douglas Mair (2), Julian Scott (3), Duncan Wingham (4) 1 – School of Geosciences, University of Edinburgh, UK, 2 – School of Geography and the Environment, University of Aberdeen, UK, 3 – British Antarctic Survey, Cambridge, UK, 4 –Centre for Polar Observation and Modelling, University College London, UK. INTRODUCTION Accurate elevation changes over large areas of the polar ice sheets can be measured using satellite radar altimetry, from which mass balance can be derived. In the percolation zone seasonal changes in snow pack density ensure that changes in surface elevation cannot be directly correlated with changes in mass. We aim to determine the influences of summer densification along a 57 km transect in the percolation zone of the Greenland Ice Sheet (GIS). The field sites are located along a 57 km transect on the EGIG line in the percolation zone on the west of the GIS (Fig 1.). Fig. 1 Location Time Retrieved from and to Results from: 2006 Pit T1 – T7 Spring 2006 Spring 2006 surface to Last Summer Surface (LSS) 2005 2005-2006 pre- melt accumulation 2005 Core T1 – T7 Spring 2006 2005 LSS (beneath 2005 winter accumulation) 1.5 m 2005 post-melt accumulation 2004 Core T4 – T6 Autumn 2004 LSS 2004 (current surface) 2004 post-melt accumulation 2003 Core T4 – T6 Spring 2004 LSS 2003 (beneath 2003 winter accumulation) 2003 post-melt accumulation METHODS Density measurements were made by measuring volume and mass of samples from visually identified stratigraphic layers in snowpits and shallow cores. The shallow cores may extend through more than one years accumulation, so the bottom part may include part of the previous years accumulation. FIELD SITES •The average Core 2005 (post-melt) density is 20% greater than Pit 2006 (pre-melt) (Fig. 2) from T1 to T7. •Pre-melt (Pit 2006) density shows no change with elevation. Post-melt (Core 2005) density decreases by 36 kg m -3 for every 100 m elevation increase from T1 to T7 (Fig. 2). The transect extends from T1 (69 o 44 N, 48 o 7 W) at 1680 m elevation to T7 (69 o 56 N, 46 o 48 W) at 2050 m elevation (Fig 1). •Density decreases with increasing elevation from T4 to T6 for Cores 2003, 2004 and 2005 (Fig. 3). •The gradients of densification with elevation for Cores 2003, 2004 and 2005 are all statistically significantly different at or above 97.5% (Fig. 3). RESULTS =404 kg m - 3 WE=0.4 m 1 m =524 kg m -3 WE=0.4 m 0.76 m If densification due to meltwater percolation and refreezing is not accounted for, changes in elevation may be misinterpreted as a change in mass. E.G. Assuming no mass change, and applying the average densification from the transect, 120 kg m -3 , there is a surface lowering of 0.24 m in a 1 m thick snowpack. DISCUSSION: Implications for mass balance measurements derived from elevation changes measured by satellite radar altimetry: Fig. 3 Pit2006 y = -0.03x + 470 R 2 = 0.05 Core 2005 y = -0.36x + 1200 R 2 = 0.79 300 350 400 450 500 550 600 650 1600 1650 1700 1750 1800 1850 1900 1950 2000 2050 2100 Elevation m Densitykgm -3 2006 pit 2005 core M ean S.D CoeffVariation kg m -3 kg m -3 % 404 20 5 524 56 11 T1 T7 CONCLUSION In order for accurate mass balance measurements to be derived from accurate elevation change measurements, future changes in rates of densification must be considered. We have found that in the percolation zone of the Greenland ice sheet, elevation changes may not directly relate to mass change due to seasonal variations in densification of the snowpack associated with processes of surface melt, percolation and refreezing. As expected, densification decreases with increasing elevation, but this gradient changes annually. Firn density is related to annual melt and accumulation (Braithwaite 1994), both of which vary. With projected rising temperatures, rates of densification will increase with a subsequent impact on elevation change but not necessarily on mass balance at higher elevations in the percolation zone. However, if temperatures change so will densification rates and elevation changes will occur without any change in mass. JAR 1 962 m Swiss Camp 1149 m JAR 3 323 m JAR 2 568 m 0 100 200 300 400 500 600 1996 1998 2000 2002 2004 2006 Years Fig 4. Fig 2. Fig 4. shows the number of Positive Degree Days (PDD) at 4 AWS stations (Steffen and others 1996) down glacier from T1 from 1996 to 2005. There is a modest positive correlation showing that since 1996 the number of PDDs per year have been increasing by 17 PDDs per year at 323 m, and 6 PDDs per year approximately at the ELA (1149 m). Using a lapse rate of 1 o C for every 142 m (Hanna and others 2005) for Core 2005 results, there is an increase in density of 51 kg m -3 for every 1 o C warming. With predicted increases in temperature in the Arctic of 2 to 3 o C by 2040 (ACIA 2005), for a 1 m snowpack, pre-melt density of 404 kg m -3 , there will be an increase in post-melt density of 102 – 204 kg m -3 and a decrease in elevation of 0.21 – 0.34 m, with no mass loss. Thus, changing temperatures in the Arctic also need to be considered. Our thanks for help in the field go to Yenz, and for logistical support go to Kristian Keller and Rene Forsberg of KMS and DNSC, Copenhagen, Malcolm Davidson of the European Space Agency, Robin Abbot of VECO Polar Resources, Kate Bar Friis of Kangerlussuaq International Science Support and the Danish Polar Centre. REFERENCES Braithwaite, R., M. Laternser, W. Pfeffer. 1994. Variations of near-surface firn density in the lower accumulation area of the Greenland ice sheet, Patkitsoq, West Greenland. J. Glaciol., 40(136), 477-485. Pfeffer, W., M. Meier, and T. Illangasekare. 1991. Retention of Greenland runoff by refreezing: Implications for projected future sea level change. J Geophys. Res. 96(C12), 22,117-22,124. Steffen, K., J. Box, and W. Abdalati, 1996 Greenland LCimate Network: GC-Net , in Colbeck, S. C. Ed. CREEL 96-27 Special Report on Glaciers, Ice Sheets and Volcanoes, trib. To M. Meier, pp. 98-103. ACIA. 2005: Arctic Climate Impact Assesment. Cambridge university press, New York, pp.27 ACKNOWLEDGEMENTS This work is a contribution to the validation of the ESA CryoSat. The work is funded by NERC through grant NER/O/S/2003/00620.

Vicki Parry (1), Peter Nienow (1), Douglas Mair (2), Julian Scott (3), Duncan Wingham (4)

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600. JAR 3 323 m. 500. JAR 2 568 m. 400. 300. JAR 1 962 m. 200. 100. Swiss Camp 1149 m. 0. 1996. 1998. 2000. 2002. 2004. 2006. Years. Vicki Parry (1), Peter Nienow (1), Douglas Mair (2), Julian Scott (3), Duncan Wingham (4) - PowerPoint PPT Presentation

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Page 1: Vicki Parry (1), Peter Nienow (1), Douglas Mair (2), Julian Scott (3), Duncan Wingham (4)

Core 2003y = -0.31x + 1100 Core 2005

y = -0.77x + 2000

Core 2004y = -1.28x + 3050

300

350

400

450

500

550

600

650

700

1850 1870 1890 1910 1930 1950 1970 1990 2010 2030

Elevation m

Dens

tiy kg

m-3

Difference between gradients:2003 and 2004 - 99% significant2004 and 2005 - 97.5% significant2003 and 2005 - 97.5% significant

T4T5

T6

Variations in mass balance and snow and firn densities along a transect in the percolation zone of the Greenland Ice Sheet

Vicki Parry (1), Peter Nienow (1), Douglas Mair (2), Julian Scott (3), Duncan Wingham (4)

1 – School of Geosciences, University of Edinburgh, UK, 2 – School of Geography and the Environment, University of Aberdeen, UK, 3 – British Antarctic Survey, Cambridge, UK, 4 –Centre for Polar Observation and Modelling, University College London, UK.

INTRODUCTION

Accurate elevation changes over large areas of the polar ice sheets can be measured using satellite radar altimetry, from which mass balance can be derived.

In the percolation zone seasonal changes in snow pack density ensure that changes in surface elevation cannot be directly correlated with changes in mass.

We aim to determine the influences of summer densification along a 57 km transect in the percolation zone of the Greenland Ice Sheet (GIS).

The field sites are located along a 57 km transect on the EGIG line in the percolation zone on the west of the GIS (Fig 1.).

Fig. 1

Location Time Retrieved from and to Results from:

2006 Pit T1 – T7 Spring 2006

Spring 2006 surface to Last Summer Surface (LSS) 2005

2005-2006 pre-melt accumulation

2005 Core T1 – T7 Spring 2006

2005 LSS (beneath 2005 winter accumulation) 1.5 m

2005 post-melt accumulation

2004 Core T4 – T6 Autumn 2004

LSS 2004 (current surface) 2004 post-melt accumulation

2003 Core T4 – T6 Spring 2004

LSS 2003 (beneath 2003 winter accumulation)

2003 post-melt accumulation

METHODS

Density measurements were made by measuring volume and mass of samples from visually identified stratigraphic layers in snowpits and shallow cores.

The shallow cores may extend through more than one years accumulation, so the bottom part may include part of the previous years accumulation.

FIELD SITES

•The average Core 2005 (post-melt) density is 20% greater than Pit 2006 (pre-melt) (Fig. 2) from T1 to T7.

•Pre-melt (Pit 2006) density shows no change with elevation. Post-melt (Core 2005) density decreases by 36 kg m-3 for every 100 m elevation increase from T1 to T7 (Fig. 2).

The transect extends from T1 (69o 44 N, 48o 7 W) at 1680 m elevation to T7 (69o 56 N, 46o 48 W) at 2050 m elevation (Fig 1).

•Density decreases with increasing elevation from T4 to T6 for Cores 2003, 2004 and 2005 (Fig. 3).

•The gradients of densification with elevation for Cores 2003, 2004 and 2005 are all statistically significantly different at or above 97.5% (Fig. 3).

RESULTS

=404 kg m-3

WE=0.4 m

1 m =524 kg m-3

WE=0.4 m0.76 m

If densification due to meltwater percolation and refreezing is not accounted for, changes in elevation may be misinterpreted as a change in mass.

E.G. Assuming no mass change, and applying the average densification from the transect, 120 kg m-3, there is a surface lowering of 0.24 m in a 1 m thick snowpack.

DISCUSSION: Implications for mass balance measurements derived from elevation changes measured by satellite radar altimetry:

Fig. 2 Fig. 3

Pit 2006y = -0.03x + 470

R2 = 0.05

Core 2005y = -0.36x + 1200

R2 = 0.79

300

350

400

450

500

550

600

650

1600 1650 1700 1750 1800 1850 1900 1950 2000 2050 2100

Elevation m

Dens

ity kg

m-3

2006 pit 2005 core

Mean S.D Coeff Variationkg m-3 kg m-3 %

404 20 5 524 56 11

T1 T7

CONCLUSION

In order for accurate mass balance measurements to be derived from accurate elevation change measurements, future changes in rates of densification must be considered. We have found that in the percolation zone of the Greenland ice sheet, elevation changes may not directly relate to mass change due to seasonal variations in densification of the snowpack associated with processes of surface melt, percolation and refreezing. As expected, densification decreases with increasing elevation, but this gradient changes annually. Firn density is related to annual melt and accumulation (Braithwaite 1994), both of which vary. With projected rising temperatures, rates of densification will increase with a subsequent impact on elevation change but not necessarily on mass balance at higher elevations in the percolation zone.

However, if temperatures change so will densification rates and elevation changes will occur without any change in mass.

JAR 1 962 m

Swiss Camp 1149 m

JAR 3 323 m

JAR 2 568 m

0

100

200

300

400

500

600

1996 1998 2000 2002 2004 2006

Years

Fig 4.

Fig 2.

Fig 4. shows the number of Positive Degree Days (PDD) at 4 AWS stations (Steffen and others 1996) down glacier from T1 from 1996 to 2005.

There is a modest positive correlation showing that since 1996 the number of PDDs per year have been increasing by 17 PDDs per year at 323 m, and 6 PDDs per year approximately at the ELA (1149 m).

Using a lapse rate of 1 oC for every 142 m (Hanna and others 2005) for Core 2005 results, there is an increase in density of 51 kg m-3 for every 1 oC warming.

With predicted increases in temperature in the Arctic of 2 to 3 oC by 2040 (ACIA 2005), for a 1 m snowpack, pre-melt density of 404 kg m-3, there will be an increase in post-melt density of 102 – 204 kg m-3 and a decrease in elevation of 0.21 – 0.34 m, with no mass loss.

Thus, changing temperatures in the Arctic also need to be considered.

Our thanks for help in the field go to Yenz, and for logistical support go to Kristian Keller and Rene Forsberg of KMS and DNSC, Copenhagen, Malcolm Davidson of the European Space Agency, Robin Abbot of VECO Polar Resources, Kate Bar Friis of Kangerlussuaq International Science Support and the Danish Polar Centre.

REFERENCES

Braithwaite, R., M. Laternser, W. Pfeffer. 1994. Variations of near-surface firn density in the lower accumulation area of the Greenland ice sheet, Patkitsoq, West Greenland. J. Glaciol., 40(136), 477-485.

Pfeffer, W., M. Meier, and T. Illangasekare. 1991. Retention of Greenland runoff by refreezing: Implications for projected future sea level change. J Geophys. Res. 96(C12), 22,117-22,124.

Steffen, K., J. Box, and W. Abdalati, 1996 Greenland LCimate Network: GC-Net, in Colbeck, S. C. Ed. CREEL 96-27 Special Report on Glaciers, Ice Sheets and Volcanoes, trib. To M. Meier, pp. 98-103.

ACIA. 2005: Arctic Climate Impact Assesment. Cambridge university press, New York, pp.27

ACKNOWLEDGEMENTS

This work is a contribution to the validation of the ESA CryoSat. The work is funded by NERC through grant NER/O/S/2003/00620.