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Precipitation-Runoff and Streamflow-Routing Models for the ...

Precipitation-Runoff and Streamflow-Routing Models for the ...

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in<strong>for</strong>mation to <strong>the</strong> model. Reaction kinetics <strong>for</strong> nonconservativeconstituents can be supplied by <strong>the</strong> user.One-dimensional transport <strong>the</strong>ory is thoroughlyexplained in <strong>the</strong> BLTM user’s manual (Jobson <strong>and</strong>Schoellhamer, 1987). The advantages of a Lagrangianapproach are (1) <strong>the</strong> scheme accurately models <strong>the</strong>convection <strong>and</strong> dispersion terms in comparison to <strong>the</strong>usual Eulerian approach (Jobson, 1980; Thomson <strong>and</strong>o<strong>the</strong>rs, 1984), <strong>and</strong> (2) <strong>the</strong> model directly represents <strong>the</strong>actual transport processes by using <strong>the</strong> concept of afluid parcel, where chemical <strong>and</strong> biological reactionsoccur <strong>and</strong> move with <strong>the</strong> flow. The solution schemestarts with a series of parcels in <strong>the</strong> river (initial conditionsat various input locations) <strong>and</strong> adds a new parcelat each external boundary node with flow into <strong>the</strong> systemduring each time step (boundary conditions).Model CalibrationData were collected from time-of-travel studiesthat defined <strong>the</strong> travel <strong>and</strong> dispersion of dye in <strong>the</strong>Pudding River <strong>for</strong> July 7–12, 1993 (Lee, 1995). Thesedata were used to calibrate a solute transport model <strong>for</strong><strong>the</strong> transport of conservative constituents. Figures 37–39 show simulation results of <strong>the</strong> calibrated BLTMmodel compared to observed data. Appendix 14 lists<strong>the</strong> input files used in DAFLOW <strong>and</strong> BLTM modeling.For model calibration, DAFLOW input flows on<strong>the</strong> main stem <strong>and</strong> tributaries were interpolated frommeasurements of discharge made at <strong>the</strong> time of <strong>the</strong> dyestudies. These discharge measurements were usedra<strong>the</strong>r than discharge simulations from PRMS precipitation-runoffmodeling (table 13) because <strong>the</strong>y provideda more accurate calibration of <strong>the</strong> BLTM model.On July 2, a convection storm occurred that was notlogged on all precipitation-gage records used in <strong>the</strong>PRMS simulation. The differences between <strong>the</strong> measured<strong>and</strong> PRMS simulated flows shown in table 13are typical of what can be expected from simulationswhen convection storms dominate <strong>the</strong> wea<strong>the</strong>r <strong>and</strong>irrigation occurs within <strong>the</strong> basin. Simulated flowswere lower than measured flows at most locationsbecause <strong>the</strong> rainfall distribution was not accuratelyportrayed by data from <strong>the</strong> precipitation-gage networkused in modeling. Simulated flows were higher thanmeasured flows on Mill <strong>and</strong> Zollner Creeks becausesimulations were not adjusted <strong>for</strong> irrigation of agriculturalcrops (Appendix 14 contains <strong>the</strong> FLOW.IN fileused in calibration <strong>and</strong> lists <strong>the</strong> WDM files of interpolatedflows that were used).Table 13. Measured <strong>and</strong> <strong>Precipitation</strong>-<strong>Runoff</strong> ModelingSystem simulated discharge used to define flowdistribution in <strong>the</strong> main stem of <strong>the</strong> Pudding River <strong>for</strong>Branch Lagrangian Transport Model modeling[ft 3 /s, cubic feet per second; RM, river mile]____________________________________________________Measured SimulatedRiver Stream Date of discharge, discharge, 1mile name measurement in ft 3 /s in ft 3 /s____________________________________________________6.2 Mill Creek atRM 0.1 07/08/93 6.2 19.48.1 Pudding Riverat Aurora(14202000) 07/07/93 279 21507/08/93 259 21020.2 Butte Creek atRM 2.3 07/07/93 52.8 32.207/09/93 35.7 31.427.0 Pudding Riverat bridge 07/07/93 187 13029.1 Zollner Creek atRM 0.4 07/07/93 2.1 6.335.8 Pudding Riverat bridge 07/08/93 135 11845.5 Abiqua Creek atRM 1.0 07/09/93 68.2 30.348.7 Pudding Riverat bridge 07/09/93 57.8 53.0____________________________________________________1 Simulated by rainfall-runoff modeling using <strong>Precipitation</strong>-<strong>Runoff</strong>modeling System. Flows were underestimated because <strong>the</strong> source of <strong>the</strong>rain was a convection storm that affected only part of <strong>the</strong> basin.Dye concentrations were simulated <strong>for</strong> threereaches on <strong>the</strong> main stem of <strong>the</strong> Pudding River fromRM 45.5 to 31.5, RM 31.5 to 17.6, <strong>and</strong> RM 17.6 to5.4 to coincide with <strong>the</strong> observed dye-study data.Observed dye-concentration data were adjusted tosimulate a conservative substance by applying a recoveryratio. The recovery ratio was computed by techniquesdescribed by Hubbard <strong>and</strong> o<strong>the</strong>rs (1982). The15-minute flow data needed in BLTM modeling werelinearly interpolated in <strong>the</strong> BLTM.FLW file from dailydata. This is an appropriate method if flows are not rapidlychanging. The input boundary used in modeling isnot <strong>the</strong> point at which dye is injected, but ra<strong>the</strong>r <strong>the</strong>first downstream location where <strong>the</strong> dye is mixed laterally.This input is used because BLTM is a one-dimensionalmodel that assumes total mixing in <strong>the</strong> crosssection. In model calibration, peak timing is matchedbetween observed <strong>and</strong> simulated values by adjustmentof <strong>the</strong> A 0 parameter (cross-section area storage) in <strong>the</strong>59

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