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PROCESS-BASED, DISTRIBUTED WATERSHED MODELS •New generation •Source waters and flowpaths •Physically based

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Page 1: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

PROCESS-BASED,DISTRIBUTED

WATERSHED MODELS

•New generation•Source waters and flowpaths•Physically based

Page 2: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

Objectives• Use distributed hydrologic modeling to improve

understanding of the hydrology, water balance and streamflow variability.

– Test and validate model components and complete model against internal and spatially distributed measurements.

– Evaluate the level of complexity needed to provide adequate characterization of streamflow at various scales.

– Quantify spatial heterogeneity of inputs (rainfall, topography, soils - where data exist) and relate this to heterogeneity in streamflow.

– Role of groundwater? Fracture flow?

Page 3: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

Distributed models incorporate the effects of topography through direct used of the digital elevation data during computation, along with process-level knowledge.

Page 4: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

Hydrological processes within a catchment are complex, involving:

• Macropores

• Heterogeneity

• Fingering flow

• Local pockets of saturation

The general tendency of water to flow downhill is however subject to macroscale conceptualization

Page 5: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based
Page 6: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

TOP_PRMS

PRMS

National Weather Service - Hydro17

TOPMODEL

Page 7: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

PRECIPITATION-RUNOFF MODELING SYSTEM

(PRMS)

MODELING OVERVIEW

&

DAILY MODE COMPONENTS

http://wwwbrr.cr.usgs.gov/projects/SW_precip_runoff/

Page 8: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

3rd HRU DIMENSION

Page 9: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

BASIC HYDROLOGIC MODEL

Q = P - ET S

Runoff Precip Met Vars Ground Water

Soil Moisture Reservoirs

Basin Chars Snow & Ice

Water use Soil Moisture

Components

Page 10: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

Distributed Parameter Approach

Hydrologic Response Units - HRUs

HRU Delineation Based on:

- Slope - Aspect

- Elevation - Vegetation

- Soil - Precip Distribution

Page 11: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

HRUs

Page 12: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

PRMS Parameters

original version

Page 13: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

PRMS

Page 14: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

Darcy’s Law Applied to Profile

depth

h

x

p

Total head = h + x + p

di/dt = K [(h + x + p) / x]

i

I = x (mt -m0) h<<p

mtm0

[Green & Ampt]

Page 15: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

PRMS

Page 16: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

Relation of HRUs and Subsurface and GW Reservoirs

Surface ( 6 hrus )

Subsurface ( 2 reservoirs )

Ground water (1 reservoir)

Page 17: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

PRMS

• HANDLES DISTRIBUTED PRECIPITATION WELL

• HANDLES INFILTRATION WELL

• DOES NOT DO SO WELL WITH GROUNDWATER COMPONENT

• SOLUTION: ADD TOPMODEL TO PRMS

Page 18: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

Terrain Based Runoff Generation Using TOPMODEL

Beven, K., R. Lamb, P. Quinn, R. Romanowicz and J. Freer, (1995), "TOPMODEL," Chapter 18 in Computer Models of Watershed Hydrology, Edited by V. P. Singh, Water Resources Publications, Highlands Ranch, Colorado, p.627-668.

“TOPMODEL is not a hydrological modeling package. It is rather a set of conceptual tools that can be used to reproduce the hydrological behaviour of catchments in a distributed or semi-distributed way, in particular the dynamics of surface or subsurface contributing areas.”

Page 19: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

TOPMODEL and GIS

• Surface saturation and soil moisture deficits based on topography– Slope– Specific Catchment Area– Topographic Convergence

• Partial contributing area concept• Saturation from below (Dunne) runoff

generation mechanism

Page 20: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

Saturation in zones of convergent topography

Page 21: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

Topographic index is used to compute the depth to the water table, which in turn influences runoff generation: ln(A /tan )where ln is the natural logarithm, A is the area drained per unit contour or the specific area, and tan is the slope

Regions of the landscape that drain large upstream areas or that are very flat give rise to high values of the index; thus areas with the highest values are most likely to become saturated during a rain or snowmelt event and thus are most likely to be areas that contribute surface runoff to the stream.

Page 22: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

Flowdirection.

Steepest directiondownslope

α1

α2

1

234

5

67

8

Proportionflowingtoneighboringgridcell3isα2/(α1+α

2)

Proportionflowingtoneighboringgridcell4isα

1/(α1+α2)

Numerical Evaluation with the D Algorithm

Upslope contributing area a

Stream line

Contour line

Topographic DefinitionSpecific catchment area a is the upslope area per unit contour length [m2/m m]

Tarboton, D. G., (1997), "A New Method for the Determination of Flow Directions and Contributing Areas in Grid Digital Elevation Models," Water Resources Research, 33(2): 309-319.) (http://www.engineering.usu.edu/cee/faculty/dtarb/dinf.pdf)

Page 23: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

TOPMODEL assumptions• The dynamics of the saturated zone can be approximated

by successive steady state representations.

• The hydraulic gradient of the saturated zone can be approximated by the local surface topographic slope, tan.

• The distribution of downslope transmissivity with depth is an exponential function of storage deficit or depth to the water table

m/SoeTT −= fz

oeTT −=- To lateral transmissivity [m2/h]- S local storage deficit [m]- z local water table depth [m]- m a parameter [m]- f a scaling parameter [m-1]

Page 24: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

Topmodel - Assumptions

• The soil profile at each point has a finite capacity to transport water laterally downslope.

∫== dzKTwhereSTqcap

f

KdzeKT

KDT

o

0

fzo =∫=

=∞ −

e.g.

or

UnitsD mz mK m/hrf m-1

T m2/hrS dimensionlessq m2/hr = m3/hr/m

S

DwD

Page 25: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

a/TS or a/S or ln(a/S) or ln(a/tan)[tan=S]isawetnessindexthatdeterminesthelocationsofsaturationfrombelowandsoilmoisturedeficit.

WithuniformKandfiniteDassumption

'S/a

wSTaR

== where

( )∫=λ dAS/aA1

'

)w1(Dz −=

With exponential K assumption

⎟⎠⎞

⎜⎝⎛ λ−−=⎟

⎠⎞

⎜⎝⎛−=

Sa

lnf1

zTSaR

lnf1

z where

( )∫=λ dAS/alnA1 and

)TR

ln(f1

z +λ−=

Soil moisture deficit = z times porosity

Topmodel

Specific catchment area a [m2/m m] (per unit coutour length)

S

DwD

z

Page 26: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

zfoeKK −=

Hydraulic conductivity (K) decreases with depth

where z is local water table depth (m) f is a scaling parameter (m-1):

shape of the decrease in K with depth

Page 27: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

ALGORITHM FOR OVERLAND AND SUBSURFACE FLOW

Subsurface Flow (Darcy Law)qi = T0 tan exp(-Si/m)

Si =S0 +m[γ- ln(ai/T0 tan)]whereγ isthemeanvalueofwetnessindexoverthebasin

OverlandFlow(Green-AmptProcedure)qi=f(p,K0)

wherepisprecipitation(snowmelt)intensityandK0 issaturatedhydraulicconductivity

Page 28: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

GL4 CASE STUDY: OBJECTIVES

• to test the applicability of the TOP_PRMS model for runoff simulation in seasonally snow-covered alpine catchments

• to understand flowpaths determined by the TOP_PRMS model

• to validate the flowpaths by comparing them with the flowpaths determined by tracer-mixing model

Page 29: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

RESAERCH SITE

Page 30: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

GIS WEASEL

• Simplify the treatment of spatial information in modeling by providing tools (a set of ArcInfo 8 commands) to:

(1) Delineate the basin from GRID DEM

(2) Characterize stream flow direction, stream channels, and modeling response unit (MRU)

(3) Parameterize input parameters for spatially distributed models such as TOPMODEL and TOP_PRMS model

Page 31: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

PROCEDURES FOR DELINEATION AND PARAMETERIZATION

• DEM (10 m) was converted from TIN to GRID format using ArcInfo 8 commands

• a pour-point coverage was generated using location information of gauging stations

• DEM and the pour-point coverage were overlaid to delineate the basin

• DEM slope and direction were re-classified to extract the drainage network

• a base input parameter file and re-classified DEM were used to derive parameters needed for TOP_PRMS model

Page 32: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

DELINEATION FOR GREEN LAKE 4

• Delineated basin area: 220ha

• Matches the real basin

• Three HRU (MRU) delineated (one stream tributary one MRU)

Page 33: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

INPUT DATA

• Measured discharge

• Measured precipitation

• Measured temperature

• Measured solar radiation

Maximum Daily Temperature at GL4-40-30-20-10

0102030

136 256 11 131 251 6 126 246 1 121 241 361 116 236

Calendar Days

Temperature (

o C)

1997 1998 1999 20001996

Daily Precipitation at D1

0

2

4

6

8

10

12

Precipitation (cm)

Minimum Daily Temperature at GL4

-40

-30

-20

-10

0

10

20

Temperature (

oC)

Page 34: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

SIMULATED SNOWMELT VS. RUNOFFMartinelli

0

1

2

3

4

5

6

7

136 256 11 131 251 6 126 246 1 121 241 361 116 236

Calendar Days

Runoff (cm)

ObservedModeled

1997 1998 1999 20001996

Martinelli Daily Modeled Snowmelt

0

1

2

3

4

5

Snowmelt (cm)

Page 35: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

SENSITIVITY ANALYSIS AND PARAMETER CALIBRATION

• Sensitivity controlled by optimization function of observed and modeled runoff

• Sensitive parameters in snow module: snowmelt factor and sublimation rate

• Sensitive parameters in topographic module: scaling factor and transmissivity

• Rosenbrock optimization

• Same optimization function as sensitivity analysis

• Parameters in snow module control magnitude of modeled runoff

• Parameters in topographic module control shape of rising and receding limbs

• Improvement evaluated by modeling efficiency

Sensitivity Analysis Parameter Calibration

Page 36: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

SENSITIVITY ANALYSIS AND PARAMETER CALIBRATION

Martinelli Green Lake 4Parameter Module Description Unit Range

Initial Optimized Initial Optimized

MFMAX snow maximum non-rain melt factor mm/(6hrs. oC) 0.5-2.0 1.2 0.8 1.2/1.2/1.2 1.2/1.2/1.2

MFMIN snow minimum non-rain melt factor mm/(6hrs.oC) 0.2-1.0 0.1 0.1 0.1/0.1/0.1 0.1/0.1/0.1

NMF snow maximum value of negative melt factor mm/(6hrs.oC) 0.05-0.5 0.15 0.05 0.15/0.15/0.15 0.15/0.15/0.15

PLWHC snow snow liquid water holding capacity none 0.01-0.3 0.05 0.05 0.05/0.05/0.05 0.05/0.05/0.05

SUBRATE snow average daily snowpack sublimation rate In/day 0-0.2 0.01 0.00065 0.01/0.01/0.01 0.01/0.01/0.01

TIPM snow antecedent temperature index none 0.2-0.6 0.3 0.3 0.3/0.3/0.3 0.3/0.3/0.3

WEI snow initial snow water equivalent in 0-1000 65 97 5/20/20 25/25/25

Tmax_lap temp monthly maximum temperature lapse rate oC (or F) -10-10 * * * *

Tmin_lap temp monthly minimum temperature lapse rate oC (or F) -10-10 * * * *

Tmax_adj temp MRU maximum temperature adjustment oC (or F) -10-10 0 0.0782 0/0/0 1/1/-1

Tmin_adj temp MRU minimum temperature adjustment oC (or F) -10-10 0 0.484 0/0/0 1/1/-1

hamon_adj potet monthly temperature coefficient-Hamon none 0.04-0.008 0.0055 0.00486 0.0055 0.0055

xko topc surface vertical hydraulic conductivity mh-1 0.01-5 0.02 0.02 0.02/0.02/0.02 0.02/0.02/0.02

szm topc value of M in recession equation m 0-10 0.04 0.0539 0.04/0.05/0.05 0.19/0.23/0.23

to topc mean MRU value of ln(To) ln(m2h-1) -6-4 -2 -2.44 -2/-2/-4 -3/-3/-6

srmax topc available water capacity of root zone m 0-5.0 1.0 0.0051 1/1/2 0.56/0.56/1.12

sro topc initial value of root zone deficit m 0-1.0 0.05 0.0 0.05/0.05/0.05 0.05/0.05/0.05

Page 37: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

SIMULATED SNOWMELT VS. RUNOFFGreen Lake 4

0

1

2

3

4

134 254 9 129 249 4 124 244 364 119 239 359 114 234

Calendar Day

Runoff (cm)

Observed

Modeled

1997 1998 1999 20001996

Modeled Daily Snowmelt at GL4

0

1

2

3

4

5

SNowmelt (cm)

Page 38: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

MONTHLY WATER BUDGET

-20

-10

0

10

20

30

40

50

60

70

5 8 1 2 5 8 1 2 5 8 1 2 5 8 1 2 5 8Water Balance Components (cm)

Runoff ETStorage Snowmelt

Martinelli

-20

-10

0

10

20

30

40

50

60

70

5 8 1 2 5 8 1 2 5 8 1 2 5 8 1 2 5 8

Year/Month

Water Balance Components (cm)

Runoff ETStorage Snowmelt

1996 1997 1998 1999 2000

Green Lake 4

Page 39: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

PROBLEM ON RUNOFF SIMULATION

• Runoff peaks in May and June failed to be captured by the model

• The modeled runoff tells us that a large amount of snowmelt was infiltrated into soil to increase soil water storage

• However, the reality is that there were runoff peaks in May and June as observed

• It is hypothesized that a large amount of the snowmelt produced in May and June may contribute to the stream flow via overland and topsoil flowpaths due to impermeable barrier of frozen soils and basal ice

Page 40: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

Summary and Conclusions

• Modeling system centered on TOPMODEL for representation of spatially distributed water balance based upon topography and GIS data (vegetation and soils).

• Capability to automatically set up and run at different model element scales.

• Encouraged by small scale calibration, though physical interpretation of calibrated parameters is problematic.

• Large scale water balance problem due to difficulty relating precipitation to topography had to be resolved using rather empirical adjustment method.

• Results provide hourly simulations of streamflow over the entire watershed.

Page 41: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

MODFLOW

• THE IDEAL SITUATION FOR GROUNDWATER TYPES WOULD BE TO COMBINE PRMS WITH MODFLOW

• MODFLOW-PRMS CONNECTION IS BEING DONE TODAY

• BETA VERSIONS NOT YET AVAILABLE, BUT SOON

Page 42: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

Are there any questions ?

AREA 1AREA 1

AREA 2AREA 2

3

12

Page 43: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

DON’T HAVE TOO MUCHCONFIDENCE IN MODELS!

WARNING: TAKE ALLMODELS WITH A GRAIN OF SALT!

Page 44: PROCESS-BASED, DISTRIBUTED WATERSHED MODELS New generation Source waters and flowpaths Physically based

REFERENCES

• Leavesley, G.H., Lichty, R.W., Troutman, B.M., and Saindon, L.G., 1983, Precipitation-runoff modeling system--Users manual: U.S. Geological Survey Water-Resources Investigations Report 83-4238, 207 p.

• Leavesley, G.H., Restrepo, P.J., Markstrom, S.L., Dixon, M., and Stannard, L.G., 1996, The modular modeling system (MMS)--User's manual: U.S. Geological Survey Open-File Report 96-151, 142 p.

• Mastin, M.C., and Vaccaro, J.J., in press, Watershed models for decision support in the Yakima River Basin, Washington: U.S. Geological Survey Open-File Report..

• Ryan, Thomas, 1996, Global climate change response program--Development and application of a physically based distributed parameter rainfall runoff model in the Gunnison river basin: United States Department of Interior, Bureau of Reclamation, 64 p.