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Ice2sea Open Forum 2 - 19, March 2011 Vincent Favier, Christophe Genthon, Gerhard Krinner, Hubert Gallée Evolution of Antarctic Surface Mass Balance by high-resolution downscaling of LMDZ4 AGCM and contribution to sea-level change Cécile AGOSTA

Evolution of Antarctic Surface Mass Balance by high ...€¦ · Sublimation HIDEP Melting HiDEP Refreezing HiDEP HiDEP Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

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Ice2sea Open Forum 2 - 19, March 2011

Vincent Favier, Christophe Genthon, Gerhard Krinner, Hubert Gallée

Evolution of Antarctic Surface Mass Balance by high-resolution downscaling of LMDZ4 AGCM

and contribution to sea-level change

Cécile AGOSTA

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

1

Antarctic Surface Mass Balance

(van de Berg et al., 2006)

Coastal areas : snowy and windy

Antarctic Plateau :cold and dry

4000

2000

1000

700

500

300

200

100

50

20

0

-400

mm w.e. a-1

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

1

Antarctic Surface Mass Balance

(van de Berg et al., 2006)

4000

2000

1000

700

500

300

200

100

50

20

0

-400

mm w.e. a-1

Climate models: major SMB changes expected in coastal areas

Coastal areas : snowy and windy

Antarctic Plateau :cold and dry

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

SMB Downscaling : Why ?

Spatial extentAntarctica (5600 km x 5600 km)

➙ Reduced computation time needed

Time extent~800 yrs (1980-2200 * 2 Scenarios * 2 Boundary conditions)

SMB estimationPrecipitation, Sublimation, Melting, Refreezing, Blowing snow

GCM resolution : ~ 60 km Required resolution : ≤ 15 km

2

HiDEP

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

3

The HiDEP modelHigh-Resolution Downscaling of surface Energy balance and Precipitation

GCM Outputs :P, T, Qv, U, V, W

3D FieldsTime step : 6H

Surface FieldsTime step : 3H

High-resolution topography

INPUTS (~50 KM RESOLUTION)

HiDEP

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

GCM Outputs :P, T, Qv, U, V, W

3D FieldsTime step : 6H

Surface FieldsTime step : 3H

OUTPUTS (15 KM RES.)Precipitation

High-resolution topography

The HiDEP modelHigh-Resolution Downscaling of surface Energy balance and Precipitation

INPUTS (~50 KM RESOLUTION)

3

HiDEP

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

GCM Outputs :P, T, Qv, U, V, W

3D FieldsTime step : 6H

Surface FieldsTime step : 3H

RainHIDEP

SnowHiDEP

Precipitation

High-resolution topography

The HiDEP modelHigh-Resolution Downscaling of surface Energy balance and Precipitation

OUTPUTS (15 KM RES.)

INPUTS (~50 KM RESOLUTION)

3

HiDEP

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

GCM Outputs :P, T, Qv, U, V, W

3D FieldsTime step : 6H

Surface FieldsTime step : 3H

RainHIDEP

SnowHiDEP

Precipitation

Surface Energy Balance

High-resolution topography

The HiDEP modelHigh-Resolution Downscaling of surface Energy balance and Precipitation

OUTPUTS (15 KM RES.)

INPUTS (~50 KM RESOLUTION)

3

SublimationHIDEP

MeltingHiDEP

RefreezingHiDEP

HiDEP

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

GCM Outputs :P, T, Qv, U, V, W

3D FieldsTime step : 6H

Surface FieldsTime step : 3H

RainHIDEP

SnowHiDEP

Precipitation

Surface Energy Balance

High-resolution topography

The HiDEP modelHigh-Resolution Downscaling of surface Energy balance and Precipitation

OUTPUTS (15 KM RES.)

INPUTS (~50 KM RESOLUTION)

3

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

4

Upward wind ➙ Adiabatic cooling ➙ ρsat ↓

Integration of the Clausius-Clapeyron equation at saturation :

ρ=ρsat(t1)

z

W ⇒Δρsat = precipitation

when ρ≥ρsat and W upwardρ=ρsat(t2)

Δρsat

Precipitation downscaling : an orographic precipitation model

Δρsat/Δt = F (ρsat,T,P) × Wwhen ρ≥ρsat and W upward

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

Precipitation downscaling : an orographic precipitation model

4

Upward wind ➙ Adiabatic cooling ➙ ρsat ↓

Integration of the Clausius-Clapeyron equation at saturation :

ρ=ρsat(t1)

z

W ⇒Δρsat = precipitation

when ρ≥ρsat and W upwardρ=ρsat(t2)

Δρsat

Δρsat/Δt = F (ρsat,T,P) × Wwhen ρ≥ρsat and W upward

➙ Feedback on ρsat,T,P➙ Time-delay for hydrometeor formation➙ Hydrometeor advection

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

Precipitation downscaling : an orographic precipitation model

4

Upward wind ➙ Adiabatic cooling ➙ ρsat ↓

Integration of the Clausius-Clapeyron equation at saturation :

ρ=ρsat(t1)

z

W ⇒Δρsat = precipitation

when ρ≥ρsat and W upwardρ=ρsat(t2)

Δρsat

Δρsat/Δt = F (ρsat,T,P) × Wwhen ρ≥ρsat and W upward

➙ Feedback on ρsat,T,P➙ Time-delay for hydrometeor formation➙ Hydrometeor advection

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

5

Orographic precipitation :Determination of the vertical wind W

At the surface : the wind is tangent to the topography

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

Orographic precipitation :Determination of the vertical wind W

At the surface : the wind is tangent to the topography➙ new vertical wind at the surface

5

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

Orographic precipitation :Determination of the vertical wind W

At the surface : the wind is tangent to the topography➙ new vertical wind at the surface

➙ Computation for W : resolution of mountain gravity wave

5

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

Total precipitation : Orographic + Non-Orographic

GCM Grid (~50 km res.) HiDEP Grid (15 km res.)GCM

Topography

GCM Precipitation6

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

Total precipitation : Orographic + Non-Orographic

GCM Grid (~50 km res.) HiDEP Grid (15 km res.)GCM

Topography

GCM Precipitation

Interpolation

6

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

Total precipitation : Orographic + Non-Orographic

GCM Grid (~50 km res.) HiDEP Grid (15 km res.)GCM

TopographyGCM

InterpolatedTopography

GCM Precipitation

Interpolation

6

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

Total precipitation : Orographic + Non-Orographic

GCM Grid (~50 km res.) HiDEP Grid (15 km res.)GCM

TopographyGCM

InterpolatedTopography

GCM Precipitation

Interpolation

6

Low-res. Oro. Precip.

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

Total precipitation : Orographic + Non-Orographic

GCM Grid (~50 km res.) HiDEP Grid (15 km res.)GCM

TopographyGCM

InterpolatedTopography

GCM Precipitation

Interpolation

6

High-res.Topography

Low-res. Oro. Precip.

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

Total precipitation : Orographic + Non-Orographic

GCM Grid (~50 km res.) HiDEP Grid (15 km res.)GCM

TopographyGCM

InterpolatedTopography

GCM Precipitation

Interpolation

6

High-res.Topography

High-res. Oro. Precip.

Low-res. Oro. Precip.

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

Total precipitation : Orographic + Non-Orographic

GCM Grid (~50 km res.) HiDEP Grid (15 km res.)GCM

TopographyGCM

InterpolatedTopography

GCM Precipitation

Interpolation

6Interpolation

High-res.Topography

High-res. Oro. Precip.

Low-res. Oro. Precip.

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

Total precipitation : Orographic + Non-Orographic

GCM Grid (~50 km res.) HiDEP Grid (15 km res.)GCM

TopographyGCM

InterpolatedTopography

GCM Precipitation

Interpolation

6Interpolation

High-res.Topography

High-res. Oro. Precip.

Low-res. Oro. Precip.

Low-res. Total Precip. (Oro. + Non-Oro.)

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

7

High-resolution Total Precip.

Low-res. Total Precip. (Interpolated from GCM)

+ High-resolution Orographic Precip.

Low-res. NON-Orographic Precipitation

− Low-resolution Orographic Precip.

Total precipitation : Orographic + Non-Orographic

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

8

Surface Energy Balance

×

z

Var

×

Extrapolation of GCM surface fields against the topography

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

8

Surface Energy Balance

Surface Scheme

×

z

Var

×

Extrapolation of GCM surface fields against the topography

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

8

Surface Energy Balance

×

z

Var

×

Extrapolation of GCM surface fields against the topography

Surface Scheme

SublimationMelting

Refreezing

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

9

Application to LMDZ4 : 1980-2007

HiDEP-LMDZ4LMDZ44000

2000

1000

700

500

300

200

100

50

20

0

-400

mm w.e. a-1SMB

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

10

Application to LMDZ4 : 1980-2007

4000

2000

1000

700

500

300

200

100

50

20

0

-400

mm w.e. a-1van de Berg et al, 2006Arthern et al, 2006

HiDEP-LMDZ4

SMB

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

Validation with a quality-controlled SMB data-set (Magand et al., 2007) : 90° – 180°E

0

200

400

600

800

0 200 400 600 800Observed SMB (mm w.e. a-1)

Mod

eled

SM

B (m

m w

.e. a

-1)

LMDZ4 vs. ObsHiDEP-LMDZ4 vs. Obs

HiDEP grid box

LMDZ4 grid box

Obs. Point

Average :in each LMDZ4 Box

1 Obs ↔1 HiDEP Box

R2 = 0.68Slope = 1.10

R2 = 0.73Slope = 0.97

11

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

Validation with a quality-controlled SMB data-set (Magand et al., 2007) : 90° – 180°E

00,20,40,60,81,0

0 500 1000 1500 2000 2500 3000 3500 4000

R2 weighted by the number of observation in LMDZ4 grid boxes

Elevation range of Observations (m)

0306090120

0 500 1000 1500 2000 2500 3000 3500080160240320

R2N

b. o

f Obs

.C

um. N

b. of Obs.

LMDZ4 vs. ObsHiDEP-LMDZ4 vs. Obs

12

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

Validation with a quality-controlled SMB data-set (Magand et al., 2007) : 90° – 180°E

Elevation bins of Observations (m)

0

200

400

600

800

0 500 1000 1500 2000 2500 3000 3500 4000

SMB

(mm

w.e

. a-1

)

0306090120

0 500 1000 1500 2000 2500 3000 3500080160240320

Nb.

of O

bs.

Cum

. Nb. of O

bs.

ObsLMDZ4HiDEP-LMDZ4

13

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

Validation with a quality-controlled SMB data-set (Magand et al., 2007)

14

Extension of the data quality-control to the rest of Antarctica :Work in progress at LGGE

For further information, you can contact Soazig Parouty

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

15

Grounded SMB 1980-2007

208 mm a -1 = kg m -2 a -1

⇔ 2410 Gt a -1

⇔ 6.7 mm a -1 sea level equivalent

Present SMB (1950-2000) : ‣ Range : 1475 à 2331 Gt a -1 [Monaghan et al., 2006]

175.2 mm a-1 = kg m-2 a -1

⇔ 2159 Gt a -1

⇔ 6.0 mm a -1 sea level equivalent

LMDZ4P-E

HiDEP-LMDZ4SMB

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

16

Conclusion

• High-resolution SMB (15 km) obtained from LMDZ4 downscalingPartial validation for present :

✦ Downscaled SMB close to LMDZ4 SMB performance✦ Increase the wet bias of LMDZ4 in coastal areas

BUT lack of field data in (crucial) coastal areas

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

16

Conclusion

• High-resolution SMB (15 km) obtained from LMDZ4 downscalingPartial validation for present :

✦ Downscaled SMB close to LMDZ4 SMB performance✦ Increase the wet bias of LMDZ4 in coastal areas

BUT lack of field data in (crucial) coastal areas

Runing :• HiDEP-LMDZ4 for :

ScenarioScenarioA1B E1

LMDZ4 Boundary Conditions

HadCM3 21C 21C & 22CLMDZ4 Boundary Conditions ECHAM5 21C 21C

Just Finished

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

17

Outlook

Further validation :• Extended quality-controlled data set over all Antarctica• Coastal-to-plateau transects

Model development in progress :• MAR Surface Scheme• Humidity advection

Thank you

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

Validation with a quality-controlled SMB data-set (Magand et al., 2007)

Quality criteria defined of the basis of :1 - Essential information available : location, time period, method2 - Quality rating of SMB measurement methods

11

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

Validation with a quality-controlled SMB data-set (Magand et al., 2007)

Quality criteria defined of the basis of :1 - Essential information available : location, time period, method2 - Quality rating of SMB measurement methods

Applied to the 90° – 180°E Antarctic sector :Review of references compiled by Vaughan and Russell (1997)+ New results from recent field campaigns

11

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

Validation with a quality-controlled SMB data-set (Magand et al., 2007)

Quality criteria defined of the basis of :1 - Essential information available : location, time period, method2 - Quality rating of SMB measurement methods

Applied to the 90° – 180°E Antarctic sector :Review of references compiled by Vaughan and Russell (1997)+ New results from recent field campaigns

➜ Quality-controlled data set for the 1950–2005 time period - Reduction in density and coverage- BUT reduced uncertainties compared to other compilations

11

400

800

600

400

1000

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

11

Law Dome

Climatologie SMB van Ommen et al., 2004

LMDZ4SMB 1980-2007

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

11

Law Dome

Climatologie SMB van Ommen et al., 2004

400

800

600

1000

600

HiDEP-LMDZ4SMB 1980-2007

Snow Sublimation

Melt

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

9

Application to LMDZ4 : 1980-2007

4000

2000

1000

700

500

300

200

100

50

20

0

-400

mm w.e. a-1LMDZ4

Snow-Sublim.

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

9

Application to LMDZ4 : 1980-2007

4000

2000

1000

700

500

300

200

100

50

20

0

-400

mm w.e. a-1HiDEP-LMDZ4

Snow Sublimation

Melt SMB

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

29

Désagrégateur de précipitationLimites du désagrégateur de précipitation

Pas de dynamique (coûteux en temps de calculs)• Pas de rétro-action de la physique sur la dynamique• Pas de contournement du relief• Pas d’effet de blocage

+ Hypothesis to simplify and linearize the equations :• Small perturbations around the hydrostatic equilibrium• Horizontal wind >> Vertical wind• Mean values slowly varying horizontally• 2D• Scorer parameter l(z)=f (T(z),P(z)) slowly varying

Cécile AGOSTA - LGGE Ice2sea - Open Forum 2011 19, March 2011

5

W : nouvelle vitesse verticale Momentum equation+ Continuity equation+ Thermal dynamic equation+ Steady adiabatic, inviscid, no-rotating flow

Orographic precipitation :Determination of the vertical wind W

➙ Wave equation on W (Mountain gravity wave) : WG