Title: On the dialog between experimentalist and modeler in catchment hydrology
1On the dialog between experimentalist and modeler
in catchment hydrology
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- Jeff McDonnell
- Department of Forest Engineering
Oregon State University
2How the experimentalist and modeler view the
rainfall runoff process
3The experimentalist
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has described a morass of process
complexity! has done little to whittle down
complexity or identify first order controls
4The modeler
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- has been guilty of a having a disparity between
the scale of measurements and the scale of model
sub-units.
http//hydrology.pnl.gov/forest.asp
- Or if a conceptual model, parameters
represented are often not physically-based or
related to physical properties, and therefore
cannot be established prior to a model
calibration.
5If the experimentalist was to build a model
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After much whittling down, this is my most
parsimonious model structure.
6If the modeler went into the field
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?????
as my subgrid scale parameterization
7Outline
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- Experimental evidence how complex is it?
- Some recent work on how to use process knowledge
for model calibration - Some new thoughts on residence time and how it
might subsume much flowpath heterogeneity - Residence time as a model state variable
- Residence time as a scalable value
8A note on my examples todaywhere P Q E
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Your AZ sites
My examples
9How complex is it?
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10How complex is it?
Weiler and McDonnell, in prep
11How complex is it?
Freer et al., 2002 WRR
12How complex is it?
Tromp van Meerveld and McDonnell, 2004 WRR
13Hillslope to catchmentHow complex is it?
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McGlynn and McDonnell, 2003a WRR
14Hillslope to catchmentHow complex is it?
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McGlynn and McDonnell 2003b WRR
15Catchment to catchment How complex is it?
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Parshall Flumes
16Catchment to catchment How complex is it?
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Weiler and McDonnell, in prep
17This is the PUB problem
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Wagener et al., in press EOS
18U. Arizona Dialog
Soft data
Evaluation rules
Experimentalist
Modeler
Values for evaluation rules (ai)
a2
a3
1
a4
a1
0
Degree of acceptability
Seibert and McDonnell, 2002 AGU Monograph
Seibert and McDonnell, 2002 WRR Freer et al.
2004 JoH
19Soft data
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Seibert and McDonnell, 2002 WRR
20U. Arizona Dialog
Virtual Experiments
Weiler and McDonnell 2004 JoH
21A posteriori parameter rejection
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- A poorly gauged watershed in Chile
- An example of an additional criterion
- Percent new water in a storm hydrograph
Efficiency
22A posteriori parameter rejection
- Red dots new water gt 50
- Black dots new water lt 50
- Identifies parameter sets that produce the
efficient results for the wrong reasons
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Efficiency
Vache et al., 2004 GRL
23New work in a new direction
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24A case for water residence time
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25What is residence time?
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remember from your shower this morning
Temperature (deg C)
Flow rate (L/s)
A very different type of information!
t1 residence time t2
Time (seconds)
26U. Arizona Dialog
Residence time distributions in watersheds
- As an experimentalist, I concede that the
subsurface is unknowable (with current meas.) - - There are an infinite array of flowpaths
- The distribution quantifies the flowpath
heterogeneity - For models that link water quantity and water
quality, flowpath reasonableness is key
27Mean residence time
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- Simply the mean of these distributions
x
28Some reported mean residence times
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- Small Experimental Watersheds
- Dischma Catchment, AU, 33 km2, 4.1 yr
- Pukemanga Catchment, NZ, 0.3 km2, 12 yr
- Panola, GA, 0.4 km2, 4.5 yr
- Rietholzbach, CH 3.5 km2, 1.1 yr
- Large River Basins
- Colorado R, UT, 75,000 km2, 14 yr
- Mississippi R., MN, 253,000 km2, 10 yr
- Neuse R., NC, 11,000 km2, 11, yr
- Sacramento R, CA, 277,000 km2, 10 yr
Sources Michel, 1992 Burns et al. 1999 McGlynn
et al., 2003 Vitvar et al., in press Stewart
and Mehlhorn, in press
29Why mean residence time is important?
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Burns et al., 2003 Groundwater
30How do we compute residence time?
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31Tracers and Age Ranges
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- Environmental tracers
- added (injected) by natural processes, typically
conservative (no losses, e.g., decay, sorption),
or ideal (behaves exactly like traced material)
We will focus on this
32A quick stable isotope primer
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- Isotopes are atoms of the same element that have
different numbers of neutrons. - 18O and 2H are constituent part of natural water
moleculesthey are the water molecule - Applied naturally during precipitation events
- Conservative at ambient temperatures
- Only mixing can alter concentration
33U. Arizona Dialog
The crazy parts per mil nomenclature
Ratio sample
Ratio standard
-
Delta Isotope (i.e. d in o/oo )
x 1000
Ratio standard
Dont let this throw you off they could have
used ppm!
3418O Natures tracer
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Convolution Integral
Plummer et al., Chem. Geology 2001
35U. Arizona Dialog
Convolution integral
Input Function Derived from precipitation d18O
signal Represents d18O in water that contributes
to recharge
System Response Function Time distribution of
water flow paths
Predicted or simulated output d18O signature
36The rest of the talk in a nutshell
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37A model proof- of-concept
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38Maimai The simplest of our various experimental
watersheds
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Planar slope
hollow
3 ha catchment
17 ha catchment
Hillslope throughflow trench
Stream and riparian zones
Downstream
39U. Arizona Dialog
The simplest of models to start
Grid-based, highly simplified with 3 tunable
parameters
The volume of water within each reservoir is
accounted for using the familiar continuity
equation
Vache et al., 2004 GRL
40Model output
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Nash Suttcliffe Efficiency 0.83
1750 runs, cutoff 0.75
41Tracer in the model
NATO ARW Moscow
Then defined as a mass balance of some arbitrary
conserved tracer
The mean residence time is derived by the
concentration breakthrough
i.e. time averaged C normalized by total mass of
the tracer
42Simulated tracer breakthrough
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Directly simulated MRT over the prior parameter
range varied from 30 to 95 days.
43U. Arizona Dialog
the tradeoff between between high discharge
efficiency and more realistic MRT
44Spatial model output
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45Soil water sampling for residence time computation
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46Modeling residence time a lysimeter near the
divide
NATO ARW Moscow
MRT 13 days
Stewart and McDonnell, 1991 WRR
47MRT and distance from the divide
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48Regionalized MRT to the entire basin based on a 2
meter elevation grid using a single direction D8
algorithm
49Model output from before
We reject this simple model
50Adding more model complexity Simulated values
incorporating soil depth
51MRT A scalable value?
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52Residence time as a scalable parameter
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- Is residence time related to basin area?
- .a recent breakthrough weve had from the HJ
Andrews (0.1 to 64 km2)
PhD work of Kevin McGuire at HJA
53Model Input Precipitation and d18O
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54Model Simulations
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s0.13
s0.18
s0.27
s0.34
s0.11
s0.23
s0.14
McGuire et al. 2004 WRR
55Topographic Distributions
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56Topographic Distributions
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McGuire et al. WRR in review
57Mean Residence Time and Topography Relationships
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McGuire et al. 2004 WRR
58MRT as a scalable value
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21 ha
6200 ha
500 m/y (1.6E-05 m/s)
581 ha
60 ha
101 ha
10 ha
59Conclusions 1
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- Hillslope processes are complex
- Highly threshold dependent, not steady state
- Networks dominate subsurface flux during events
- Residence time is something that can be
quantified with data - Residence time represents flowpath heterogeneity
and makes sense across all scales - Residence time probes a different axis in
different information spaceit is non-redundant - Our recent work in Oregon suggests that MRT
scales with readily available terrain indices - This may help to define the connection between
the headwater catchments and their mesoscale
basin.
60Conclusions 2
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- Residence time is a measurable observable that
can be a good system constraint - Provides a rationale for making the model more
complex - We are now exploring spatial variation in soil
properties, explicit inclusion of an immobile
domain, unsaturated zone coupling - Perhaps we need to
- Move beyond the status quo where we go into the
field, collect data, build a model and declare
victory. - Deal with the disparity between the scale of
measurements and the scale of our physically
based model sub-units.