1 Numerical Hydraulics Numerical solution of the St. Venant equation, FD-method Wolfgang Kinzelbach with Marc Wolf and Cornel Beffa.

Slides:



Advertisements
Similar presentations
OPEN-CHANNEL FLOW Introduction Ch-10 of HH
Advertisements

Change of the flow state
Advective Flows. Watershed & Water Quality Modeling Technical Support Center Surface Water Flow Options 1.Specified river, tributary flows (net flow)
Modelling tools - MIKE11 Part1-Introduction
Chapter 13: Momentum Principles in Open-Channel
End of Chapter 4 Movement of a Flood Wave and begin Chapter 7 Open Channel Flow, Manning’s Eqn. Overland Flow.
1 Numerical Hydraulics W. Kinzelbach with Marc Wolf and Cornel Beffa Lecture 4: Computation of pressure surges continued.
Numerical Hydraulics W. Kinzelbach with Marc Wolf and Cornel Beffa Lecture 3: Computation of pressure surges.
Open Channel Flow.
Open Channel Flow Part 2 (cont)
1 Numerical Hydraulics Classification of the equations Wolfgang Kinzelbach with Marc Wolf and Cornel Beffa.
Gates. Gates Gates are used to control the discharge and also to stop the flow if required. Gates are used to control the discharge and also to stop the.
Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Open Channel Flow June 12, 2015 
Open Channel Flow.
Pertemuan Open Channel 2. Bina Nusantara VARIED FLOW IN OPEN CHANNELS.
Wolfgang Kinzelbach with Marc Wolf and Cornel Beffa
Shallow water equations in 1D: Method of characteristics
Tutorial for CIVL252 Hydraulics
HEC-RAS US Army Corps of Engineers Hydrologic Engineering Center
Hydraulic Jump as an application of Momentum Equation
1 Numerical Hydraulics Open channel flow 1 Wolfgang Kinzelbach with Marc Wolf and Cornel Beffa.
MECH 221 FLUID MECHANICS (Fall 06/07) Chapter 10: OPEN CHANNEL FLOWS
HEC-RAS.
1 Numerical Hydraulics Open channel flow 2 Wolfgang Kinzelbach with Marc Wolf and Cornel Beffa.
Open channel hydraulics
Numerical Hydraulics Wolfgang Kinzelbach with Marc Wolf and Cornel Beffa Lecture 1: The equations.
Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Open Channel Flow July 15, 2015 
FUNDAMENTAL EQUATIONS, CONCEPTS AND IMPLEMENTATION
St Venant Equations Reading: Sections 9.1 – 9.2.
GRADUALLY VARIED FLOW CVE 341 – Water Resources
ArGEnCo – MS²F - Hydrologie, Hydrodynamique Appliquée et Constructions Hydrauliques (HACH) Experimental and numerical investigations.
SPN7 Numerical investigations on the influence of hydraulic boundary conditions on the efficiency of sewer flushing Dr.-Ing. Joerg Schaffner
Modeling Drop Structures in HEC-RAS Version 3.1
Chapter 7 continued Open Channel Flow
CH 7 - Open Channel Flow Brays Bayou Concrete Channel Uniform & Steady
Hydraulic Routing in Rivers
Solution of the St Venant Equations / Shallow-Water equations of open channel flow Dr Andrew Sleigh School of Civil Engineering University of Leeds, UK.
Feb 2003HEC-RAS Version 3.11 Slides adapted from HEC Unsteady Flow Course Unsteady Flow Course.
FLOOD ROUTING.
Channel Routing Simulate the movement of water through a channel
Engineering Low-Head Dams for Function and Safety Fritz R. Fiedler Department of Civil Engineering University of Idaho.
Solution of the St Venant Equations / Shallow-Water equations of open channel flow Dr Andrew Sleigh School of Civil Engineering University of Leeds, UK.
Distributed Flow Routing Surface Water Hydrology, Spring 2005 Reading: 9.1, 9.2, 10.1, 10.2 Venkatesh Merwade, Center for Research in Water Resources.
Dynamic Channel Routing Preissmann Scheme. Dynamic Channel Routing Preissmann Scheme unconditionally stable for  >=0.5 second-order accurate if 
Mathematical Background
MIKE 11 IntroductionNovember 2002Part 1 Introduction to MIKE 11 Part 1 General Hydrodynamics within MIKE 11 –Basic Equations –Flow Types Numerical Scheme.
ERT 349 SOIL AND WATER ENGINEERING
Overview of Open Channel Flow Definition: Any flow with a free surface at atmospheric pressure Driven entirely by gravity Cross-section can vary with location.
Finding the S vs. Q relationship By: Cody Hudson.
School of Civil Engineering/Linton School of Computing, Information Technology & Engineering 1 CE 3205 Water and Environmental Engineering Stilling Basins.
Hydraulic Routing in Rivers Reference: HEC-RAS Hydraulic Reference Manual, Version 4.1, Chapters 1 and 2 Reading: HEC-RAS Manual pp. 2-1 to 2-12 Applied.
Basic Hydrology & Hydraulics: DES 601 Module 16 Open Channel Flow - II.
Surface Water Virtual Mission Dennis P. Lettenmaier, Kostas Andreadis, and Doug Alsdorf Department of Civil and Environmental Engineering University of.
Watershed Modeling using HEC-HMS and EPA-SWMM ©T. G. Cleveland, Ph.D., P.E. 25 July 2012 Lesson 14.
Basic Hydraulics: Open Channel Flow – II
Basic Hydrology: Rainfall-runoff based methods – III
Basic Hydrology & Hydraulics: DES 601
Routing-Hydrologic and Hydraulic
EXAMPLE Water flows uniformly in a 2m wide rectangular channel at a depth of 45cm. The channel slope is and n= Find the flow rate in cumecs.
ERT 349 SOIL AND WATER ENGINEERING
May, 1999 Bridges This module will cover bridges and how they are input into HEC-RAS. 9/21/2018.
Distributed Flow Routing
Modelling tools - MIKE11 Part1-Introduction
Hydrodynamic Concepts
Instituto Superior Técnico instituto superior técnico
HEC-RAS US Army Corps of Engineers Hydrologic Engineering Center
Fluvial Hydraulics CH-3
Design of a Pipe Runoff Link Inflow
BAE 6333 – Fluvial Hydraulics
Example 3.E - Graf Assume a channel with uniform flow at a depth of 5.03 m. Channel is rectangular with a width of 9 m and average velocity of 12 m/s.
Presentation transcript:

1 Numerical Hydraulics Numerical solution of the St. Venant equation, FD-method Wolfgang Kinzelbach with Marc Wolf and Cornel Beffa

2 Basic equations of open channel flow in variables h and v for rectangular channel Continuity („Flux-conservative form“) Momentum equation

3 Basic equations of open channel flow in variables h and q for rectangular channels Continuity Momentum equation

4 Basic equations of open channel flow for general cross-section in variables A and Q Continuity Momentum equation

5 Boundary conditions At inflow boundary usually the inflow hydrograph should be given At the outflow boundary we can use –water level (also time variable e.g. for tide) –water level-flow rate relation (e.g. weir formula) –slope of water level or energy In supercritical flow it can happen that two boundary conditions are necessary for one boundary (for both v and h)

6 Boundary conditions Number of boundary conditions from number of characteristics In 1D: subcritical flow: IB: 1, OB: 1 supercritical flow: IB: 2, OB: 0 IB = Inflow boundary, OB = Outflow boundary t t

7 Discretized basic equations in variables h and v for rectangular channels Continuity Momentum equation Finite differences: Explicit method („Flux-conservative“ form) i = 2,…,Nx

8 Discretized basic equations in variables h and v for rectangular channels Boundary conditions (i = 1) example Explicit method Boundary conditions (i = Nx+1) example or weir formula

9 Discretized basic equations in variables h and v for rectangular channels Explicit method requires stability condition Courant-Friedrichs-Levy (CFL) criterium must be fulfilled: Explicit method c is the relative wave velocity with respect to average flow

10 Assignment: Determine the wave propagation (water surface profile, maximum water depth, outflow hydrograph) for a rectangular channel with the following data: width b = 10 m, k str = 20 m -1/3 /s length L = 10‘000 m, bottom slope I S =0.002 Inflow before wave, base flow Q 0 = 20 m 3 /s Boundary condition downstream: Weir with water depth 2.2 m Boundary condition upstream: Inflow hydrograph Inflow hydrograph  Q (is added to base flow Q 0 ): Zeit (h)  Q (m 3 /s)

11 Inflow/Outflow hydrographs time steps in 10s Q (m 3 /s) about 4 h