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Groundwater – SM – climate interactions:

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1 Groundwater – SM – climate interactions:
EGU 2016 – CL4.11 – April 21st, 2016 16/09/2018 Groundwater – SM – climate interactions: Lessons from idealized model experiments with forced water table depth Agnès Ducharne1, Min-Hui Lo2, Bertrand Decharme3, Rong-You Chien2, Fuxing Wang4, Josefine Ghattas5, Frédérique Cheruy4, Jeanne Colin3 , Sophie Tyteca3, Chia-Wei Lan2 1 METIS/IPSL, Paris, France 2 Department of Atmospheric Science, NTU, Taiwan 3 GAME, CNRM, Toulouse, France 4 LMD/IPSL, Paris, France 5 IPSL, Paris, France

2 GW with long residence times  buffering effects
1. Introduction 2/12 Kollet & Maxwell, 2008 GW with long residence times  buffering effects on stream flow on SM and LA coupling where the water table is close enough to the surface As an introduction, I’d like to remind you that GW tends to flow horizontally in river catchments, with rather long residence times, and this comes with important buffering effects Objective Identify where the WT can influence SM, ET, and LA coupling through idealized model experiments

3 3 state-of-the-art LSMs: CLM4, ISBA/SURFEX, ORCHIDEE
2. The numerical experiment 3/12 3 state-of-the-art LSMs: CLM4, ISBA/SURFEX, ORCHIDEE Off-line or coupled to their parent climate model following LMIP/AMIP-like protocols for intercomparability Off-line forcing = PGF (1°, 3-hourly, , Sheffield et al. 2006) + GPCC bias corrrection Reference simulations with standard configuration + 7 simulations with forced water table depth (WTD) between 0.5 and 10 m CLM SUR ORC Point at the underground !!

4 3 state-of-the-art LSMs: CLM4, ISBA/SURFEX, ORCHIDEE
2. The numerical experiment 3/12 3 state-of-the-art LSMs: CLM4, ISBA/SURFEX, ORCHIDEE Off-line or coupled to their parent climate model following LMIP/AMIP-like protocols for intercomparability Off-line forcing = PGF (1°, 3-hourly, , Sheffield et al. 2006) + GPCC bias corrrection Reference simulations with standard configuration + 7 simulations with forced water table depth (WTD) between 0.5 and 10 m CLM SUR ORC Point at the underground !!

5 3 state-of-the-art LSMs: CLM4, ISBA/SURFEX, ORCHIDEE
2. The numerical experiment 3/12 3 state-of-the-art LSMs: CLM4, ISBA/SURFEX, ORCHIDEE Off-line or coupled to their parent climate model following LMIP/AMIP-like protocols for intercomparability Off-line forcing = PGF (1°, 3-hourly, , Sheffield et al. 2006) + GPCC bias corrrection Reference simulations with standard configuration + 7 simulations with forced water table depth (WTD) between 0.5 and 10 m CLM SUR ORC Point at the underground !!

6 3 state-of-the-art LSMs: CLM4, ISBA/SURFEX, ORCHIDEE
2. The numerical experiment 3/12 3 state-of-the-art LSMs: CLM4, ISBA/SURFEX, ORCHIDEE Off-line or coupled to their parent climate model following LMIP/AMIP-like protocols for intercomparability Off-line forcing = PGF (1°, 3-hourly, , Sheffield et al. 2006) + GPCC bias corrrection Reference simulations with standard configuration + 7 simulations with forced water table depth (WTD) between 0.5 and 10 m CLM SUR ORC Point at the underground !!

7 3 state-of-the-art LSMs: CLM4, ISBA/SURFEX, ORCHIDEE
2. The numerical experiment 3/12 3 state-of-the-art LSMs: CLM4, ISBA/SURFEX, ORCHIDEE Off-line or coupled to their parent climate model following LMIP/AMIP-like protocols for intercomparability Off-line forcing = PGF (1°, 3-hourly, , Sheffield et al. 2006) + GPCC bias corrrection Reference simulations with standard configuration + 7 simulations with forced water table depth (WTD) between 0.5 and 10 m CLM SUR ORC Point at the underground !!

8 3 state-of-the-art LSMs: CLM4, ISBA/SURFEX, ORCHIDEE
2. The numerical experiment 3/12 3 state-of-the-art LSMs: CLM4, ISBA/SURFEX, ORCHIDEE Off-line or coupled to their parent climate model following LMIP/AMIP-like protocols for intercomparability Off-line forcing = PGF (1°, 3-hourly, , Sheffield et al. 2006) + GPCC bias corrrection Reference simulations with standard configuration + 7 simulations with forced water table depth (WTD) between 0.5 and 10 m CLM SUR ORC Point at the underground !!

9 3 state-of-the-art LSMs: CLM4, ISBA/SURFEX, ORCHIDEE
2. The numerical experiment 3/12 3 state-of-the-art LSMs: CLM4, ISBA/SURFEX, ORCHIDEE Off-line or coupled to their parent climate model following LMIP/AMIP-like protocols for intercomparability Off-line forcing = PGF (1°, 3-hourly, , Sheffield et al. 2006) + GPCC bias corrrection Reference simulations with standard configuration + 7 simulations with forced water table depth (WTD) between 0.5 and 10 m CLM SUR ORC Point at the underground !!

10 3 state-of-the-art LSMs: CLM4, ISBA/SURFEX, ORCHIDEE
2. The numerical experiment 3/12 3 state-of-the-art LSMs: CLM4, ISBA/SURFEX, ORCHIDEE Off-line or coupled to their parent climate model following LMIP/AMIP-like protocols for intercomparability Off-line forcing = PGF (1°, 3-hourly, , Sheffield et al. 2006) + GPCC bias corrrection Reference simulations with standard configuration + 7 simulations with forced water table depth (WTD) between 0.5 and 10 m CLM SUR ORC Point at the underground !!

11 3 state-of-the-art LSMs: CLM4, ISBA/SURFEX, ORCHIDEE
2. The numerical experiment 3/12 3 state-of-the-art LSMs: CLM4, ISBA/SURFEX, ORCHIDEE Off-line or coupled to their parent climate model following LMIP/AMIP-like protocols for intercomparability Off-line forcing = PGF (1°, 3-hourly, , Sheffield et al. 2006) + GPCC bias corrrection Reference simulations with standard configuration + 7 simulations with forced water table depth (WTD) between 0.5 and 10 m CLM SUR ORC Modifier SURFEX : rajouter le drainage libre !!!

12 Land averages – Sensitivity to WTD
3. Off-line results 4/12 Land averages – Sensitivity to WTD REF (Rodell et al., 2015) REF REF REF Total runoff  -Qforce Dynamic LAI in ORCHIDEE, which increases with SM, and contributes to the slower increase in ET via a complex interplay with soil evaporation and transpiration

13 The critical WTD 3. Off-line results Qle = f(WTD) Variation rate
5/12 The critical WTD Qle = f(WTD) Variation rate Variation rate in % of Qle(REF) To map the spatial variations of this sensitivity, we introduced a new variable : the critical WTD, which I will illustrate here based on land averages. All values are land averages

14 The critical WTD 3. Off-line results Qle = f(WTD)
5/12 The critical WTD Qle = f(WTD) WTDc = depth at which Qle response becomes small Variation rate in % of Qle(REF) 5% WTDc similar to extinction depth of Shah et al 2007 WTDc = 2.5m WTDc = 4m WTDc = 6.5m Deeper WTDc  higher sensitivity to WTD All values are land averages

15 The critical WTD : 5% threshold Strong inter-model difference
3. Off-line results 6/12 The critical WTD : 5% threshold Patterns // aridity Strong inter-model difference DIRECTLY MOVE TO 1% !!!

16 The critical WTD : 1% threshold Strong inter-model difference
3. Off-line results 7/12 The critical WTD : 1% threshold Patterns // aridity Strong inter-model difference VG vs Brooks Corey ?

17 3. Off-line results REF: Aridity index P/Rn 1% WTDc CLM ORC SUR 8/12
Arid zones ORC Transition zones SUR Arid zones

18 3. Off-line results 1% WTDc
9/12 1% WTDc The reasons for inter-model differences are not clear yet but may involve: Dynamic LAI in ORC, combined with different sensitivities of soil evaporation and transpiration Different models of unsaturated hydraulic parameters (BC for CLM & SUR, VG for ORC) cf. Decharme et al. 2011 Different ways to link the soil and deep WTs CLM Arid zones ORC Transition zones We’ve also started to compare with many other possible explanatory factors, and the reasons for the inter-model differences are not clear yet. But we think they may involve… SUR Arid zones

19 3. Off-line results 1% WTDc Simulated WTD (Fan et al., 2013) CLM
10/12 1% WTDc Simulated WTD (Fan et al., 2013) CLM Major aquifer systems (Whymap, 2008) ORC We also compared our WTDc maps to the simulated WTD map published at the global scale by Fan et al in 2013, which shows that the WTD is deep in arid zones, which is a well known fact. The map of the major aquifer systems, just below, tells us that in many part of the world, these deep simulated WTD do not correspond to an aquifer formation so there is no WTD… Yet, there are also many places where deep WTD exist in unconfined aquifers, and the critical WTD diagnostic suggests they can influence the surface fluxes by capillary rise. SUR

20 3. Off-line results 1% WTDc Simulated WTD (Fan et al., 2013) CLM
10/12 1% WTDc Simulated WTD (Fan et al., 2013) CLM Major aquifer systems (Whymap, 2008) ORC We also compared our WTDc maps to the simulated WTD map published at the global scale by Fan et al in 2013, which shows that the WTD is deep in arid zones, which is a well known fact. The map of the major aquifer systems, just below, tells us that in many part of the world, these deep simulated WTD do not correspond to an aquifer formation so there is no WTD… GREY, like in central Asia and parts of Sahara Yet, there are also many places where deep WTD exist in unconfined aquifers, and the critical WTD diagnostic suggest they can influence the surface fluxes by capillary rise. SUR

21 We miss simulations with deeper WTD to define the WTDc
4. Coupled simulations 11/12 Short overview Only 3 1, 2, 3m Variation rates around 1.5 and 2.5m CLM and ORC have a larger reference Qle in coupled mode than offline CLM shows smaller variations rates to shallow WTD in coupled mode We miss simulations with deeper WTD to define the WTDc All values are land averages

22 5. Conclusion and perspectives
12/12 Off-line results The critical WTD helps comparing the sensitivity of surface fluxes to GW between different regions and models Models need WTDs down to m to represent the effect of GW on SM and ET in arid and semi-arid zones Coupled results « Deeper » analysis is needed Limits and perspectives Fixed WTD over the entire grid-cells  highly unrealistic Same experiments with forced WTD over fractions of grid-cells (coupled mode) Comparison of the three LSMs with dynamic WTD parametrization

23 Thank you for your attention Thank you for your attention
EGU 2016 – CL4.11 – April 21st, 2016 16/09/2018 Thank you for your attention Thank you for your attention Whymap 2008 Thank you ! Myself My talk today is about…

24 Thank you for your attention Complementary slides
EGU 2016 – CL4.11 – April 21st, 2016 16/09/2018 Thank you for your attention Complementary slides Whymap 2008 Thank you ! Myself My talk today is about…

25 Land averages – Reference simulations
3. Off-line results 4 Land averages – Reference simulations Evapotranspiration Total runoff Point at the underground !! OBS from Rodell et al. (2015)

26 Land averages – Reference simulations
3. Off-line results Land averages – Reference simulations Point at the underground !! Total ET has two major components: transpiration & soil evaporation: In CLM and SURFEX, the changes of total ET are driven by soil evaporation. In ORCHIDEE, the changes of total ET are driven by the transpiration (until WTD1)

27 ESoil TVeg ORCHIDEE WTD1-WTD2 Esoil and TVeg in mm/d LAI

28 ESoil TVeg ORCHIDEE WTD05-WTD1 Esoil and TVeg in mm/d LAI

29 SM-ET coupling strength (from Dirmeyer, 2013)
3. Off-line results SM-ET coupling strength (from Dirmeyer, 2013) C(REF) Annual, W/m² C(WTD1) Annual, W/m² Coupling strength decreases with 1m because it reduces the SM and ET variability ORC keeps more coupling strength because ET increases less, meaning that it keeps more water stress than the other models

30 C(WTD1) – C(REF) Annual, W/m²
3. Off-line results C(WTD1) – C(REF) Annual, W/m² 1% WTDc CLM ORC Striking similarity between patterns of WTDc and change in C SUR

31 3. Off-line results 9 1% WTDc CLM ORC VG vs Brooks Corey ? SUR

32 3. Off-line results 9 1% WTDc CLM ORC VG vs Brooks Corey ? SUR

33 3. Off-line results 9 1% WTDc CLM ORC VG vs Brooks Corey ? SUR

34 In arid zones, sandy soils exhibit a shallower WTDc
3. Off-line results 9 1% WTDc ORCHIDEE CLM ORC The sensitivity to sandy soil is opposite to what’s reported in Shah et al 2007 for the extinction depth, but with climate from Florida. In arid zones, sandy soils exhibit a shallower WTDc SUR


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