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Impact of atmospheric variability on soil moisture-precipitation coupling Jiangfeng Wei with support from Paul Dirmeyer, Zhichang Guo, and Li Zhang Center for Ocean-Land-Atmosphere Studies Maryland, USA
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Page 1: Jiangfeng Wei with support from Paul Dirmeyer, Zhichang Guo, and Li Zhang Center for Ocean-Land-Atmosphere Studies Maryland, USA.

Impact of atmospheric variability on soil moisture-precipitation coupling

Jiangfeng Weiwith support from Paul Dirmeyer, Zhichang Guo, and Li Zhang

Center for Ocean-Land-Atmosphere StudiesMaryland, USA

Page 2: Jiangfeng Wei with support from Paul Dirmeyer, Zhichang Guo, and Li Zhang Center for Ocean-Land-Atmosphere Studies Maryland, USA.
Page 3: Jiangfeng Wei with support from Paul Dirmeyer, Zhichang Guo, and Li Zhang Center for Ocean-Land-Atmosphere Studies Maryland, USA.

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MotivationUncertainty of land surface models

• significantly different output at the same forcing (e.g., PILPS, GSWP)

Complexity of land-atmosphere interaction

• full of nonlinear processes

• uncertainties in land simulations may be brought to atmosphere

Sources of the signals are hard to trace in the complex system

• e.g. GLACE “hotspots”

Page 4: Jiangfeng Wei with support from Paul Dirmeyer, Zhichang Guo, and Li Zhang Center for Ocean-Land-Atmosphere Studies Maryland, USA.

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Global Land-Atmosphere Coupling Experiment

16-member ensembles for 1 June- 31 August of 1994 (SST prescribed)Ensemble W: control integrationsEnsemble S: soil moisture is given the same as one member of W

Ω=16σ 2

<X > − σ 2X

15σ 2X

(0 ≤ Ω ≤ 1)

Ω measures the similarity (or predictability) of the time series in 16 ensemble members, and is equivalent to the percentage of variance caused by the slowly varying oceanic, radiative, and land surface processes.

Ω(S)-Ω(W) is the predictability come from the prescribed subsurface soil moisture, and is a measure of land-atmosphere coupling strength in GLACE.

Koster, R. D., and Coauthors 2004: Regions of strong coupling between soil moisture and precipitation, Science, 305, 1138-1140.Koster, R. D., and Coauthors, 2006: GLACE: The Global Land-Atmosphere Coupling Experiment. Part I: Overview, J. Hydrometeorol., 7, 590–610.

Page 5: Jiangfeng Wei with support from Paul Dirmeyer, Zhichang Guo, and Li Zhang Center for Ocean-Land-Atmosphere Studies Maryland, USA.

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Models

Each AGCM is coupled to the three land models.

Totally six model configurations (combinations): COLA-SSiB, COLA-CLM, COLA-Noah, GFS-SSiB, GFS-CLM, GFS-Noah .

Page 6: Jiangfeng Wei with support from Paul Dirmeyer, Zhichang Guo, and Li Zhang Center for Ocean-Land-Atmosphere Studies Maryland, USA.

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Results from GLACE-type experiments

Values for COLA AGCM are larger than for GFS, showing the dominant impact of the AGCM.

Ω(W), Ω(S), and Ω(S)-Ω(W) have similar patterns, with larger values over tropical land.

Spatial correlations among Ω are 0.43-0.71, and among Ω(S)-Ω(W) are 0-0.29.

Results indicate that the land-atmosphere coupling strength may be strongly influenced by the external forcing (e.g. SST).

Page 7: Jiangfeng Wei with support from Paul Dirmeyer, Zhichang Guo, and Li Zhang Center for Ocean-Land-Atmosphere Studies Maryland, USA.

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Decompose of precipitation variance using Fourier transform

All the model simulations underestimate the high-frequency (fast synoptic) variance and overestimate the low-frequency (intraseasonal) variance.

More low-frequency variance in COLA AGCM.

The percentages for the theoretical white noise are 69%, 21%, and 10%, indicating that the precipitation time series follow a red spectrum.

Page 8: Jiangfeng Wei with support from Paul Dirmeyer, Zhichang Guo, and Li Zhang Center for Ocean-Land-Atmosphere Studies Maryland, USA.

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frequency

Power

White noise

precipitation

Page 9: Jiangfeng Wei with support from Paul Dirmeyer, Zhichang Guo, and Li Zhang Center for Ocean-Land-Atmosphere Studies Maryland, USA.

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Decompose of precipitation variance using Fourier transform

global mean

spatial correlation with Ω(S)-Ω(W)

spatial correlation with Ω(W)

Good correspondence between low-frequency intraseasonal variability and precipitation predictability (Ω).

Page 10: Jiangfeng Wei with support from Paul Dirmeyer, Zhichang Guo, and Li Zhang Center for Ocean-Land-Atmosphere Studies Maryland, USA.

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JJA lag-2-pentad autocorrelation of precipitation (ACR)

global mean

spatial correlation with Ω(W)

ACR has higher spatial correlation with Ω than intraseasonal variance.

Page 11: Jiangfeng Wei with support from Paul Dirmeyer, Zhichang Guo, and Li Zhang Center for Ocean-Land-Atmosphere Studies Maryland, USA.

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Conceptual relationships

Ω =F(α 0+α )

Based on the above analysis, we can build a conceptual relationship:

α0 is a constant, and α0>>α. Thus, Ω is largely determined by F. Then the coupling strength

Ω(S) − Ω(W ) = F(α (S) − α (W ))

α(S)-α(W) is the difference of α between the two ensembles, and is the impact of soil moisture on the coupling strength.

F: the impact of low-frequency external forcing (F≈ACR)α: the impact of soil moisture

Page 12: Jiangfeng Wei with support from Paul Dirmeyer, Zhichang Guo, and Li Zhang Center for Ocean-Land-Atmosphere Studies Maryland, USA.

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S’ experiment:

COLA-SSiB reads soil moisture from GFS-SSiBGFS-SSiB reads soil moisture from COLA-SSiB

Exchange prescribed soil moisture to separate the impact of soil moisture and atmosphere

Difference in soil moisture variability has some impact on land-atmosphere coupling, but the characteristics of the atmosphere appear to be more important.

Page 13: Jiangfeng Wei with support from Paul Dirmeyer, Zhichang Guo, and Li Zhang Center for Ocean-Land-Atmosphere Studies Maryland, USA.

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Physical mechanisms

More low-frequency variation of precipitation

More sustained dry and wet

period

Stronger impact of soil moisture on precipitation

Larger soil moisture memory and more

sustained ET

Lan

d p

ath

Atm

osp

heric

path

Page 14: Jiangfeng Wei with support from Paul Dirmeyer, Zhichang Guo, and Li Zhang Center for Ocean-Land-Atmosphere Studies Maryland, USA.

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Conceptual relationships

Ω =F(α 0+α )

Based on the above analysis, we can build a conceptual relationship:

α0 is a constant, and α0>>α. Thus, Ω is largely determined by F. Then the coupling strength

Ω(S) − Ω(W ) = F(α (S) − α (W ))

α(S)-α(W) is the difference of α between the two ensembles, and is the impact of soil moisture on the coupling strength. α(S)-α(W) can be further expanded to SM->ET and and ET->P

F: the impact of low-frequency external forcing (F≈ACR)α: the impact of soil moisture

Ω(S) − Ω(W ) = F ⋅SM → ET(F) ⋅ET → P

Page 15: Jiangfeng Wei with support from Paul Dirmeyer, Zhichang Guo, and Li Zhang Center for Ocean-Land-Atmosphere Studies Maryland, USA.

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Lag-2-pentad ACR for GLACE models

Page 16: Jiangfeng Wei with support from Paul Dirmeyer, Zhichang Guo, and Li Zhang Center for Ocean-Land-Atmosphere Studies Maryland, USA.

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Lag-2-pentad ACR

Page 17: Jiangfeng Wei with support from Paul Dirmeyer, Zhichang Guo, and Li Zhang Center for Ocean-Land-Atmosphere Studies Maryland, USA.

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Correlation across 12 GLACE models

Page 18: Jiangfeng Wei with support from Paul Dirmeyer, Zhichang Guo, and Li Zhang Center for Ocean-Land-Atmosphere Studies Maryland, USA.

18

Conceptual relationships

Ω =F(α 0+α )

Based on the above analysis, we can build a conceptual relationship:

α0 is a constant, and α0>>α. Thus, Ω is largely determined by F. Then the coupling strength

Ω(S) − Ω(W ) = F(α (S) − α (W ))

α(S)-α(W) is the difference of α between the two ensembles, and is the impact of soil moisture on the coupling strength. α(S)-α(W) can be further expanded to SM->ET and and ET->P

F: the impact of low-frequency external forcing (F≈ACR)α: the impact of soil moisture

Ω(S) − Ω(W ) = F ⋅SM → ET(F) ⋅ET → P

(Ω(S) − Ω(W ))calibrated = (Ω(S) − Ω(W ))ACR(obs)

ACR(models)

Page 19: Jiangfeng Wei with support from Paul Dirmeyer, Zhichang Guo, and Li Zhang Center for Ocean-Land-Atmosphere Studies Maryland, USA.

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Coupling strength Ω(S)-Ω(W)

Page 20: Jiangfeng Wei with support from Paul Dirmeyer, Zhichang Guo, and Li Zhang Center for Ocean-Land-Atmosphere Studies Maryland, USA.

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SummaryFor our six model configurations, the choice of AGCMs is the

main reason for the substantially different precipitation variability, predictability, and land-atmosphere coupling strength among the configurations. The impact of different land models is secondary.

Intraseasonal precipitation variability, which is mainly a property of the AGCM, can impact land-atmosphere coupling both directly in the atmosphere and indirectly through soil moisture response to precipitation.

Models generally overestimate the low-frequency component of precipitation. The calibrated coupling strength shows a similar global pattern, but is significantly weaker over some regions.

Page 21: Jiangfeng Wei with support from Paul Dirmeyer, Zhichang Guo, and Li Zhang Center for Ocean-Land-Atmosphere Studies Maryland, USA.

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References Wei, J., P. A. Dirmeyer, and Z. Guo, 2010: How much do different land models

matter for climate simulation? Part II: A decomposed view of land-atmosphere coupling strength. J. Climate. 23, 3135-3145.

Wei, J. and P. A. Dirmeyer, 2010: Toward understanding the large-scale land-atmosphere coupling in the models: Roles of different processes, Geophys. Res. Lett., 37, L19707, doi:10.1029/2010GL044769.

Wei, J., P. A. Dirmeyer, Z. Guo, and Li Zhang, 2011: Impact of atmospheric variability on soil moisture-precipitation coupling, in Climate Variability, published by Intech.

Questions or comments to [email protected].


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