DSD-NL 2014 - iMOD Symposium - 11. High resolution global scale groundwater modelling, Rens van Beek, Universiteit Utrecht
1. High Resolution Global Scale
Groundwater Modelling
Department of Physical Geography β Faculty of Geosciences
Rens van Beek
Inge de Graaf, Edwin Sutanudjaja, Yoshi Wada & Marc Bierkens
Limits to global groundwater
consumption: effects on low
flows and groundwater levels
4. Towards a high resolution global hydrological model
4
Global-scale simulations at 5 arc minutes (~10 x 10 km at equator)
River discharge Domestic water use
5. What has been the effect of abstractions on groundwater levels?
5
β’ Simulation of groundwater head
dynamics;
β’ Lateral flow (exchange between cells)
cannot be ignored at finer spatial
resolutions.
Challenges to the construction of a
physically based global-scale groundwater
model:
β’ Quality of available global datasets:
- Surficial hydro-lithology;
- Aquifer thickness estimates.
6. 6
Model lay-out
β’ 5β resolution;
β’ Steady-state;
β’ Offline coupling to MODFLOW;
β’ Coupling to iMOD under construction.
Sutanudjaja et al., 2011
7. Land-surface model
Available global datasets
Gleeson et al. 2010
Hartmann and Moosdorf 2012
Hydro-lithology
Conductivity
Model Input
Groundwater recharge
Surface water levels
β’ Imposed as average long-term levels for
lakes, reservoirs and lakes;
β’ Based on discharge for rivers and imposed
by means of the RIVER package using
uniform conductivity;
β’ DRAIN package is used where no main river
channel is available.
8. 8
range
Land surface
Sediment basin
50 m
Floodplain elevation
range
1) πΉβ² π₯ = 1 β
πΉ π₯ β πΉπππ
πΉπππ₯ β πΉπππ
Fβ(x) is spatial frequency
distribution of elevation above
the floodplain
2) Associated Z-score
π π₯ = πΊβ1(πΉβ² π₯ )
Where G-1 is the inverse of the
standard normal distribution.
Sediment basin aquifers: delineation and depth (1)
9. 9
3) Using case studies in the US
β’ range of aquifer thickness
β’ average coefficent of variation
β’ Aquifer thickness is assumed
to be log-normally distributed
(positive skew)
4) πππ· = π(πππ; πππ₯)
π π₯ = πππ· Γ (1 + πΆπ£πππ·Z x )
π· π₯ = π π(π₯)
dmax
dmin
Sediment basin aquifers: delineation and depth (2)
16. 16
0.01 0.1 1 10 100 1000 Years
- Months years decades centuries millennia
Flow paths and travel times
17. β’ Suitable method to develop aquifer schematization and properties for data
poor environments;
β’ The large scale-distribution of groundwater levels is captured; starting
point to assess groundwater level fluctuations;
β’ Confirms the relevance of including lateral flow in global scale hydrological
models at finer resolutions.
17
Conclusions
ο What is the effect of past and future abstractions on
groundwater levels?
Major limitations, currently being addressed:
β’ Steady-state;
β’ Single, unconfined layer;
β’ Coupling of surface and groundwater.
18. 18
Thank you for your attention
http://www.hydrol-earth-syst-sci-discuss.net/11/5217/2014/hessd-11-5217-2014.pdf