A NONLINEAR OPTIMIZATION MODEL FOR ESTIMATING MANNING S ROUGHNESS COEFFICIENT

Similar documents
Estimating of Manning s Roughness Coefficient for Hilla River through Calibration Using HEC-RAS Model

IMPLICIT NUMERICAL SCHEME FOR REGULATING UNSTEADY FLOW IN OPEN CHANNEL Mohamed. T. Shamaa 1, and Hmida M. Karkuri 2

FLOOD ROUTING FOR A SPECIFIC ORIENTATION OF PLANNED DEVELOPMENTS FOR AL-SHAMIYA RIVER IN IRAQ AS CASE STUDY

Calibration of Manning s Friction Factor for Rivers in Iraq Using Hydraulic Model (Al-Kufa River as Case study)

EFFECT OF BAFFLE BLOCKS ON THE PERFORMANCE OF RADIAL HYDRAULIC JUMP

Guo, James C.Y. (1999). "Critical Flow Section in a Collector Channel," ASCE J. of Hydraulic Engineering, Vol 125, No. 4, April.

EFFECT OF SPATIAL AND TEMPORAL DISCRETIZATIONS ON THE SIMULATIONS USING CONSTANT-PARAMETER AND VARIABLE-PARAMETER MUSKINGUM METHODS

OPEN CHANNEL FLOW. Computer Applications. Numerical Methods and. Roland Jeppson. CRC Press UNIVERSITATSB'BUOTHEK TECHNISCHE. INFORMATlONSBiBUOTHEK

Flood Routing by the Non-Linear Muskingum Model: Conservation of Mass and Momentum

MACRODISPERSION AND DISPERSIVE TRANSPORT BY UNSTEADY RIVER FLOW UNDER UNCERTAIN CONDITIONS

Abstract. 1 Introduction

This file was downloaded from Telemark Open Research Archive TEORA -

PERFORMANCE OF A CENTRAL-TYPE JET PUMP II- EXPERIMENTAL STUDY ON WATER FLOW

Flood routing. Prof. (Dr.) Rajib Kumar Bhattacharjya Indian Institute of Technology Guwahati

THE HYDRAULIC PERFORMANCE OF ORIENTED SPUR DIKE IMPLEMENTATION IN OPEN CHANNEL

Application of the Muskingum-Cunge method for dam break flood routing F. Macchione Dipartimento di Difesa del Suolo, Universita delta Calabria,

EXPERIMENTAL STUDY OF BACKWATER RISE DUE TO BRIDGE PIERS AS FLOW OBSTRUCTIONS

Lecture Note for Open Channel Hydraulics

VARIATION OF MANNING S ROUGHNESS COEFFICIENT WITH SEEPAGE IN SAND-BED CHANNEL *Satish Patel 1 and Bimlesh Kumar 2

Application of Mathematical Modeling to Study Flood Wave Behavior in Natural Rivers as Function of Hydraulic and Hydrological Parameters of the Basin

Optimal Control of Open-Channel Flow Using Adjoint Sensitivity Analysis

Computation of gradually varied flow in compound open channel networks

39.1 Gradually Varied Unsteady Flow

MATHEMATICAL MODELING OF FLUVIAL SEDIMENT DELIVERY, NEKA RIVER, IRAN. S.E. Kermani H. Golmaee M.Z. Ahmadi

Numerical Hydraulics

Fluid Mechanics Prof. S.K. Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur

Reservoir Oscillations with Through Flow

Gradually Varied Flow I+II. Hydromechanics VVR090

Simulation of Transcritical Flow in Hydraulic structures

International Journal of Scientific & Engineering Research, Volume 6, Issue 3, March ISSN

EFFECT OF VERTICAL CURVATURE OF FLOW AT WEIR CREST ON DISCHARGE COEFFICIENT

1.060 Engineering Mechanics II Spring Problem Set 8

Minimum Specific Energy and Critical Flow Conditions in Open Channels

Accuracy of Muskingum-Cunge flood routing

A note on critical flow section in collector channels

Correction methods for dropping of simulated water level utilising Preissmann and MOUSE slot models

MODELING FLUID FLOW IN OPEN CHANNEL WITH HORSESHOE CROSS SECTION

Transactions on Modelling and Simulation vol 10, 1995 WIT Press, ISSN X

MODELING OF LOCAL SCOUR AROUND AL-KUFA BRIDGE PIERS Saleh I. Khassaf, Saja Sadeq Shakir

Design of Stilling Basins using Artificial Roughness

Hydraulics Part: Open Channel Flow

Simulation of flow discharge on Danube River

9. Flood Routing. chapter Two

Transactions on Ecology and the Environment vol 8, 1994 WIT Press, ISSN

Prediction of bed form height in straight and meandering compound channels

BACKWATERRISE DUE TO FLOW CONSTRICTION BY BRIDGE PIERS

NUMERICAL MODEL FOR MOVABLE BED AS A TOOL FOR THE SIMULATION OF THE RIVER EROSION A CASE STUDY

Lecture 10: River Channels

The Sensitivity Analysis of Runoff from Urban Catchment Based on the Nonlinear Reservoir Rainfall-Runoff Model

SPRAY LOSSES IN SPRINKLER IRRIGATION SYSTEMS IN IRAQ

International Journal of Scientific & Engineering Research, Volume 6, Issue 3, March ISSN

River Current Resource Assessment and Characterization Considering Ice Conditions

Investigation of Flow Profile in Open Channels using CFD

Presented by: Civil Engineering Academy

Introduction to BASEMENT Basic Simulation Environment for Computation of Environmental Flow and Natural Hazard Simulation

OPEN CHANNEL FLOW. One-dimensional - neglect vertical and lateral variations in velocity. In other words, Q v = (1) A. Figure 1. One-dimensional Flow

CHAPTER 2- BACKGROUND. INVESTIGATIONS OF COMPOSITE ROUGHNESS COEFFICIENT IN A RIVER WITH LOW FLOW

Analysis of dynamic wave model for flood routing in natural rivers

Fluvial Dynamics. M. I. Bursik ublearns.buffalo.edu October 26, Home Page. Title Page. Contents. Page 1 of 18. Go Back. Full Screen. Close.

D. MATHEMATICAL MODEL AND SIMULATION

Hydraulics for Urban Storm Drainage

H3: Transition to Steady State Tidal Circulation

28.2 Classification of Jumps

presented by Umut Türker Open Channel Flow

Rating Curves: Part 1 Correction for Surface Slope

Uniform Channel Flow Basic Concepts Hydromechanics VVR090

Hydraulics Prof. Dr. Arup Kumar Sarma Department of Civil Engineering Indian Institute of Technology, Guwahati

CRITERIA FOR THE CHOICE OF FLOOD ROUTING METHODS IN

Hydromechanics: Course Summary

Morphological Changes of Reach Two of the Nile River

Study on river-discharge measurements with a bottom-mounted ADCP

Modelling Breach Formation through Embankments

Volume Conservation Controversy of the Variable Parameter Muskingum Cunge Method

DEPARTMENT OF CIVIL AND ENVIRONMENTAL ENGINEERING Urban Drainage: Hydraulics. Solutions to problem sheet 2: Flows in open channels

LOSSES DUE TO PIPE FITTINGS

= Q:An Qn% icx=zv. A, with Bn = T- n. Modelling of irrigation channel dynamics for controller design

Minimum Cost Design of Lined Canal Sections

State of the Art Two- Dimensional Hydraulic Modeling Tools Model Benchmark Testing

Modelling fluid flow JAGST Vol. 13(2) 2011 MODELING FLUID FLOW IN OPEN CHANNEL WITH CIRCULAR CROSS-SECTION

A fuzzy dynamic wave routing model

Computation of Gradually Varied Flow in Channel Networks with Hydraulic Structures

Beaver Creek Corridor Design and Analysis. By: Alex Previte

NUMERICAL SIMULATION OF OPEN CHANNEL FLOW BETWEEN BRIDGE PIERS

Engineering Hydrology (ECIV 4323) CHAPTER FOUR. Stream flow measurement. Instructors: Dr. Yunes Mogheir Dr. Ramadan Al Khatib

PREDICTION OF THE CHARACTERISTCS OF FREE RADIAL HYDRAULIC B-JUMPS FORMED AT SUDDEN DROP USING ANNS

H4: Steady Flow through a Channel Network

Implementation of Bridge Pilings in the ADCIRC Hydrodynamic Model: Upgrade and Documentation for ADCIRC Version 34.19

NPTEL Quiz Hydraulics

Open Channel Flow I - The Manning Equation and Uniform Flow COURSE CONTENT

Abstract. 1. Introduction

Advanced Hydraulics Prof. Dr. Suresh A. Kartha Department of Civil Engineering Indian Institute of Technology, Guwahati

BOUSSINESQ-TYPE MOMENTUM EQUATIONS SOLUTIONS FOR STEADY RAPIDLY VARIED FLOWS. Yebegaeshet T. Zerihun 1 and John D. Fenton 2

Birecik Dam & HEPP Downstream River Arrangement R. Naderer, G. Scharler Verbundplan GmbH, 5021 Salzburg, Austria

Model for Dredging a Horizontal Trapezoidal Open Channel with Hydraulic Jump

Advanced Hydraulics Prof. Dr. Suresh A. Kartha Department of Civil Engineering Indian Institute of Technology, Guwahati

1.060 Engineering Mechanics II Spring Problem Set 4

Reverse stream flow routing by using Muskingum models

New computation method for flood flows and bed variations in a low-lying river with complex river systems

UNIFORM FLOW CRITICAL FLOW GRADUALLY VARIED FLOW

Thelongwaveequations

Transcription:

Twelfth International Water Technology Conference, IWTC2 2008, Alexandria, Egypt 299 A NONLINEAR OPTIMIZATION MODEL FOR ESTIMATING MANNING S ROUGHNESS COEFFICIENT Maysoon Kh. Askar and K. K. Al-Jumaily * Dr., University of Salahaddin, Erbil, Iraq ** Prof. Dr., University of Technology, Baghdad, Iraq ABSTRACT The present research formulated mathematical model for estimating Manning's roughness coefficient in open canal networks. The inverse problem was formulated as a nonlinear optimization model with n value as an unknown variable by embedding the finite difference approximation of the Saint-Venant equations for unsteady flow in an open canal as equality constraints. The Sequential Quadratic Program was used to solve the optimization model and to minimize least square objective function. The Hilla-Kifl irrigation project was selected as a field case study for this work. The project was situated in the southern sector of Iraq. Six sections on Hilla Main Canal and Three sections on Distributary canal were chosen. The Root Mean Square Error of n values is found between 0.00075 and 0.0030 for different time increment. Optimization model showed a deviation between calculated and designed n values of about 6.4%. INTRODUCTION The objective of the present research is to formulate a new approach to estimate Manning's roughness in a canal network with different types of hydraulic structures such as: gates, drops, tail and side escapes, sudden change in cross sections, and combination of such structures which are performed by embedding the implicit finite difference method of the Saint-Venant equations for flow into a nonlinear optimization model. The determination of an optimum value of the flow resistance coefficient and other parameters such as weighting factor, and distance increment (x) are the primary task in the calibration of one-dimensional unsteady flow model. An obvious and widely used method to determine the parameters is by a trial and error technique in which the continuity and momentum equations (Saint-Venant equations) can be repeatedly solved by a finite difference technique with certain boundary conditions for different assumed function of the parameters.

300 Twelfth International Water Technology Conference, IWTC2 2008, Alexandria, Egypt The best fit between observed and calculated values of discharge or depth is the optimum value. The literature relevant to estimate or calibrate n values for unsteady open-channel flow is sparse. In the present research, the sequential quadratic programming algorithm description by Nash et al. (996) was used to solve the nonlinear optimization model to estimate value of Manning's roughness coefficient. GOVERNING EQUATIONS An optimization model was formulated by using Sequential quadratic programming with inverse problem to estimate the Manning's roughness coefficient as unknown variable. The Saint-Venant equations for trapezoidal canal with external and internal boundary conditions as discussed by Askar (2005) by a single weighted roughness coefficient at each cross section were used as governing equations. The governing equations can be written as follows: y v y B + A + vb = t x x q () g y x + v v x + v t = g ( S S ) o f q. v A (2) where B is the free surface flow width; x = distance along the longitudinal axis of the canal; A = active cross-sectional area; t = time; y = depth of flow; q = lateral inflow (positive) or outflow (negative); g = acceleration due to gravity; S f = the energy line slope computed from Manning equation; S o = the canal bed slope and v = velocity. MODEL FORMULATION The inverse problem is formulated as a nonlinear optimization model with Manning's roughness coefficient as the unknown variable. The formulation of the inverse problem for canal network can be summarized as follows: - Objective Function The objective function is to minimize the sum of squares of the difference between the simulated and observed values of the flow depth.

Twelfth International Water Technology Conference, IWTC2 2008, Alexandria, Egypt 30 Minimize f ( y) = N m j= i= y (3) j+ j+ si+ yoi+ j+ yoi+ where y s = simulated depth values at several observation stations; y o = observed depth at the corresponding points; i = grid point in space; m = total number of sections for every channel; j = time level; and N = total number of times. The finite difference method was used to solve the inverse problem by using n values as the unknown. However, the simulated depth used in the objective function can be calculated from the equation: 2 y k + s = y k s y + dn n (4) where n = Manning's roughness coefficient. 2- Nonlinear Constraints In this research, the Saint-Venant continuity and momentum equations for a trapezoidal canal were used as nonlinear constraint. The Saint-Venant equations are written as shown in equations (), and (2), respectively. The downstream boundary condition is used also as nonlinear constrains. It can be written as follows: Where J + J + J + G N = v N R n S f = 0 (5) n S f = friction slope of canal which is given by Manning's equation: 4 2 2 3 S f = v n / R (6) Internal boundary conditions such as gates, drops, escapes, looped, divergent, etc used the empirical equation of each control structure, flow and conservation equations as nonlinear constraint also, Askar (2005). The specified upstream boundary condition is included as a linear constraint. This can be given as follows: + ( ) f ( t ) Q j = (7)

302 Twelfth International Water Technology Conference, IWTC2 2008, Alexandria, Egypt where f ( t) = specified inflow hydrograph. The nonlinear optimization problem described in this section was solved using the Sequential Quadratic Programming (SQP) algorithm. The basic idea for (SQP) framework for equality constraints is analogous to Newton's method for unconstraint minimization: At each step, a local model of optimization problem is constructed and solved, yielding a step towards the solution of the original problem. In the nonlinear optimization programming both the objective function and constraints must be modeled as: Minimize f ( x) (8) Subject to ( x ) = 0 g (9) FIELD INVESTIGATIONS The following constituents of canals network, Fig. (), were chosen to be used in the measurements: Main canal: a part of the Hilla Main Canal, HC was chosen from km 2 + 000 up to km 3+500 with base width of 2.5m, side slope of.5h: V, design longitudinal slope of 5 cm/km, design Manning's n of 0.05, design discharge of 4.2 m 3 /s, and design depth of 3.5 m. The Hilla Main Canal takes off from the Kifl Main Canal about 4.9 km downstream of the main intake structure of the project. Distributary canal: a part of distributary canal, R from km 0+035 to 0+500 was chosen with base width of.5 m, side slope of.5h: V, design longitudinal slope of 0 cm/km, design discharge of 2.5 m 3 /s, design depth of 2m, and design Manning's n of 0.05. The following steps were followed in gathering the field data:. Six sections on the main canal were selected as shown in Fig. (). The first and sixth sections represent the upstream and downstream boundary conditions, respectively. 2. Three sections were chosen at distributary canal, the first one at km 0+035, the second at km 0+250, and the third at km 0+500. 3. The rating curves were plotted for sections No., 3, 5, 6, 7, and 9, using a set of measurements of discharge and depth of the flow. These measurements were made over a period from 2/2/2002 up to 5//2003 so as to obtain an

Twelfth International Water Technology Conference, IWTC2 2008, Alexandria, Egypt 303 accurate relationship between the discharge and depth of flow. The depth of water was measured with a graduated rod. 4. The water level at each section was measured instantaneously (every 5 minutes over a period up to six hrs) at fixed time from 6//2002 up to 22//2003 for calibration purposes; this was achieved by changing the height of the head gate (h g ). 5. The discharge was determined by using the rating curve for each cross section. 6. For verification purposes, the discharges and the depths at section, 3, 5, 6, and 9 were measured every hr up to 6 hr and continued for several days from 23//2003 to 30//2003. km 0 + 500 Q U/s t Hilla main canal Canal no 2 Canal no 3 km 0 + 750 km 0+ 035 km 0 + 250 km 0 +500 km + 000 Canal no 3 km + 250 3 4 5 7 8 9 Q D/s t 6 km +500 Q t D/s Fig. () Schematic layout of Hilla-Kifl network EVALUATION OF THE MODEL Performance of the proposed optimization model for the calibration of Manning's roughness coefficient was evaluated using hypothetical open canal network.

304 Twelfth International Water Technology Conference, IWTC2 2008, Alexandria, Egypt This example problem, as shown in Fig. (2), includes flow in simple hypothetical dendritic canals with multiple n values corresponding to different reaches. The observation data for these cases were calculated by using model development (Canal Network Optimization Program), Askar (2005) for assumed true values of n. These calculated observation data for discharge and flow depth were then used in the optimization model to estimate the actual Manning's roughness coefficient. Identical initial and boundary conditions were applied while obtaining the calculated observation data and while solving the optimization model. This approach was used to evaluate the performance of the methodology. The advantage of using observation data is that to know the actual deviation between the true values and calculated values of n. The characteristics of simple hypothetical network are shown in Table (). The calculated (simulated) flow measurement data were used in the objective function of the optimization model to correct n values for all three canals. The initial estimates of n for all three canals were specified to be 0.02. Optimization program was carried out to estimate n values applied to Al-Kifl canal system. The arrangement shown in Fig. (2) was used for this purpose. The initial assumed n value was taken in the optimization model equal to 0.0. The root mean square error of n values were taken as indicator to comparison between estimated and observed n value Table (2) shows the Root Mean Square Error (RMSE) of Manning's roughness coefficient with different time increment for the arrangement of Fig. (2). It can be observed from Table (2) that errors in estimated values of n increase as t was increased. Identical results were obtained when the initial estimates for n was taken equal to 0.05. The result of the optimization program showed that the values of n = 0.0432, 0.04, 0.0379 for canals no., 2, 3 which were calculated respectively, concerning Fig. (). The Root Mean Square Error (RMSE) of n values in sections 3 and 5 = 0.054, and 0.057 respectively. Canal No.2 Q t Fig. (2) Schematic layout of simple network

Twelfth International Water Technology Conference, IWTC2 2008, Alexandria, Egypt 305 Identical initial and boundary conditions were applied while obtaining the calculated observation data and while solving the optimization model. This approach was used to evaluate the performance of the methodology. The advantage of using observation data was that to know the actual deviation between the true values and calculated values of n. Table () Characteristics of simple network Characteristic Canal Canal 2 Canal 3 Length of canal (m) 000 500 500 Bed width (m) 2.8.6 Side slope (Z).5.5.5 Longitudinal slope (cm/km) 0 0 0 Manning's Roughness Coefficient (n) 0.06 0.022 0.08 Table (2) Root Mean Square Error (RMSE) of n values in canals with different time increment X t RMSE of Manning's Roughness Coefficient (m) (min) Canal Canal 2 Canal 3 00 5 0.030 0.035 0.035 00 30 0.037 0.043 0.047 00 60 0.038 0.04 0.049 00 20 0.048 0.044 0.052 SUMMARY AND CONCLUSIONS In this research, the Sequential Quadratic Programming was used for estimating the Manning's roughness coefficient from unsteady flow measurement data in open canal network. Four-point implicit finite difference method was used to solve the governing equations. Performance of the proposed model was evaluated for small dendritic network and for Al-Kifl canal. Results of these evaluations showed that potential applicability of the proposed model for estimating Manning's roughness coefficient in open canal network with different types of hydraulic structures as internal boundary conditions. It was found that the model performs satisfactorily when discharge measurements were available. Further testing of the methodology using field data is necessary to establish its practical utility for natural channels.

306 Twelfth International Water Technology Conference, IWTC2 2008, Alexandria, Egypt REFERENCES. Askar, M. Kh., 2005, "A Hydrodynamic Model for Simulation of Flow in Open Canal Network", Ph.D. Thesis, University of Technology, Baghdad. 2. Backer, L., and Yeh, W.W.G., 972, "The Identification of Parameters in Unsteady Open Channel Flows", Water Resource Research, Vol. 8, No. 4, pp. 956-965. 3. Backer, L., and Yeh, W.W.G., 973, "The Identification of Multiple Reach Channel Parameters", Water Resource Research, Vol. 9, No. 2, pp. 326-335. 4. Fread, D.L., and Smith, G.F., 978, "Calibration Technique for -D Unsteady Flow Models", Journal of the Hydraulics Division, ASCE, Vol. 04, No. 7, pp. 027-044. 5. Nash, S.G., and Sofer, A., 2000, "Linear and Nonlinear Programming", McGraw- Hill Company, Inc., New York. 6. Powell, M.J.D., 974, "Introduction to Constrained Optimization", Numerical Methods for Constrained Optimization, P.E. Gill and W. Murray, eds., Academic Press, London, pp. -28. 7. Ramesh, R., Datta, B., Bhallamudi, M., and Narayana, A., 2000, "Optimal Estimation of Roughness in Open Channel Flows", Journal of Hydraulic Engineering, Vol. 26, No. 4, pp. 299-303. 8. Venutelli, M., 2002, "Stability and Accuracy of Weighted Four-Point Implicit Finite Difference Schemes for Open Channel Flow", Journal of Hydraulic Engineering, ASCE, Vol. 28, No. 3, pp. 28-288.