Boundary Conditions of the First Kind (Dirichlet Condition)

Size: px
Start display at page:

Download "Boundary Conditions of the First Kind (Dirichlet Condition)"

Transcription

1 Groundwater Modeling Boundary Conditions Boundary Conditions of the First Kind (Dirichlet Condition) Known pressure (velocity potential or total heard) head, e.g. constant or varying in time or space. Since total head, h, is known, an equation for head is not needed along the boundary. Boundary conditions of the Second Kind (Neumann Condition) Known flux or specific discharge (mass per unit volume per unit time. Express in terms of flux exiting a boundary cell. For a no flow boundary, δφ/dn = 0. Boundary conditions of the Third Kind (mixed Boundary condition or Cauchy Condition) Flux normal to a boundary can be expressed in terms of the head along the boundary and a known constant. Phreatic surface with accretion The pressure is equal to atmospheric and it is necessary to know the flux. The phreatic surface can vary if enough information on the aquifer properties are known. Can be an unconfined or confined aquifer. Surface of seepage Pressure is equal to zero so the velocity potential is a function of elevation. Boundary Between Two Porous Media The pressure or total head is equal along the boundary. Continuity must be assured along the boundary. For MODFLOW, use constant-head, inactive or variable head cells. Groundwater Modeling

2 ASTM Standard Guide for... Defining Boundary Conditions in Ground-Water Flow Modeling (D ) Specific Head or Dirichlet Boundary Type General-Specified-Head Boundary - head specified as a function of position and time Constant-Head Boundary - head specified as a function of position Specific Flux or Neumann Boundary Type - flux specified as a function of position and time No-Flow Boundary - material of very low permeability Streamline Boundary - ground-water divide Head Dependent Flux or Cauchy Type Boundary - flux varies dependent on head gradient between aquifer and boundary Constant Flux Boundary - base of a confining layer after head is drawn down into confined/unconfined aquifer Head Dependent Boundary - rate of evapotranspiration specified as a function of depth to a cutoff depth Free-Surface Boundary Type 6-2

3 - moveable boundary where the head is equal to the elevation of the boundary - water table or top flow line where the location may not be known initially Seepage-Face Boundary - surface of seepage associated with a free surface boundary - location is predetermined but length is unknown - can be ignored for regional modeling Defining Initial Conditions in Ground-Water Flow Modeling (D ) Defining Steady-State Initial Conditions for a Transient-State Simulation of Head Distribution - field conditions that represent approximately an equilibrium condition - initial conditions might include model head adjustment to offset unknowns lack of definite information on boundary conditions, aquifer hydraulic properties and initial head values Defining Transient-State Initial Condition for a Transient-State Simulation of Absolute Head - the simulation boundary conditions and hydraulic properties are simulated over a long period of time so that stresses before the simulations are insignificant Defining the Initial Head for Steady or Transient-State Simulation of Head Change in Response to a Stress - models only the water-level changes related to the application of a stress - applies the principle of superposition, if applicable 6-3

4 Model Calibration - Process of evaluating initial and boundary conditions and aquifer hydraulic properties to verify that the model can reproduce measured heads or fluxes - There is a package in GMS capable of performing inverse modeling, but it is not available under the present UT liscense. - Inverse modeling is the process of adjusting model inputs until the optimum set of inputs are determined for a partiticular condition. - The inputs are optimized by comparing the residuals computed using a number of pairs of predicted and measured values. - Residuals are usually computed by squaring the differences between the predicted and measured values so that positive and negative residuals do not produce a false optimum. - After a model is calibrated, then the model can be used to simulate other conditions. Conducting a Sensitivity Analysis for a Ground-Water Flow Model Application (D ) - used to calculate the sensitivity of a system when evaluating a model for initial and boundary conditions and for aquifer hydraulic properties - used to calculate the sensitivity with respect to a future prediction Process Identify inputs to be varied Identify variations of the inputes Perform simulations Compare predicted values with measured values Calculate residuals Determine sensitivity type (Type I, II, III, IV) Type I sensitivity occurs whtn variation of an input causes insignificant changes in the residuals as well as the model s conclusions. Type I senstitivity is of no concern because, regardless of the value of the input, the conclusion will remain the same. 6-4

5 Type II sensitivity occurs when variation of an input causes significant changes in the residuals but insignificant changes in the model s conclusions. Tkype II sensitivity is of no concern because, regardless of the value of the input, the conclusion will remain the same. Type III sensitivity occurs when variation of an input causes significant changes to both the residuals and the model s conclusions. Type III sensitivity is of no concern because, even though the model s conclusions change as a result of variation of the input, the parameters used in those simulations cause the model to become uncalibrated. Type IV sensitivity occurs when variation of an input causes in the residuals but significant changes in the model s conclusions. Type IV sensitivity can invalidate model results because, over the range of the that parameter in which the model can be considered calibradted, the conclusions of the model can change significantly. CHANGE IN RESIDUALS CHANGE IN CONCLUSIONS Insignificant Significant Insignificant Type I Type II Significant Type IV Type III 6-5

ALL GROUND-WATER HYDROLOGY WORK IS MODELING. A Model is a representation of a system.

ALL GROUND-WATER HYDROLOGY WORK IS MODELING. A Model is a representation of a system. ALL GROUND-WATER HYDROLOGY WORK IS MODELING A Model is a representation of a system. Modeling begins when one formulates a concept of a hydrologic system, continues with application of, for example, Darcy's

More information

Principles of groundwater flow

Principles of groundwater flow Principles of groundwater flow Hydraulic head is the elevation to which water will naturally rise in a well (a.k.a. static level). Any well that is not being pumped will do for this, but a well that is

More information

ATTACHMENT 8: Quality Assurance Hydrogeologic Characterization of the Eastern Turlock Subbasin

ATTACHMENT 8: Quality Assurance Hydrogeologic Characterization of the Eastern Turlock Subbasin ATTACHMENT 8: Quality Assurance Hydrogeologic Characterization of the Eastern Turlock Subbasin Quality assurance and quality control (QA/QC) policies and procedures will ensure that the technical services

More information

Barometric Effects on Transducer Data and Groundwater Levels in Monitoring Wells D.A. Wardwell, October 2007

Barometric Effects on Transducer Data and Groundwater Levels in Monitoring Wells D.A. Wardwell, October 2007 Barometric Effects on Transducer Data and Groundwater Levels in Monitoring Wells D.A. Wardwell, October 2007 Barometric Effects on Transducer Data Barometric Fluctuations can Severely Alter Water Level

More information

GROUNDWATER FLOW NETS Graphical Solutions to the Flow Equations. One family of curves are flow lines Another family of curves are equipotential lines

GROUNDWATER FLOW NETS Graphical Solutions to the Flow Equations. One family of curves are flow lines Another family of curves are equipotential lines GROUNDWTER FLOW NETS Graphical Solutions to the Flow Equations One family of curves are flow lines nother family of curves are equipotential lines B C D E Boundary Conditions B and DE - constant head BC

More information

LAPLACE'S EQUATION OF CONTINUITY

LAPLACE'S EQUATION OF CONTINUITY LAPLACE'S EQUATION OF CONTINUITY y z Steady-State Flow around an impervious Sheet Pile Wall Consider water flow at Point A: v = Discharge Velocity in Direction Figure 5.11. Das FGE (2005). v z = Discharge

More information

Period #16: Soil Compressibility and Consolidation (II)

Period #16: Soil Compressibility and Consolidation (II) Period #16: Soil Compressibility and Consolidation (II) A. Review and Motivation (1) Review: In most soils, changes in total volume are associated with reductions in void volume. The volume change of the

More information

3D-Groundwater Modeling with PMWIN

3D-Groundwater Modeling with PMWIN Wen-Hsing Chiang 3D-Groundwater Modeling with PMWIN A Simulation System for Modeling Groundwater Flow and Transport Processes Second Edition With 242 Figures and 23 Tables 4y Springer Contents 1 Introduction

More information

The University of Toledo Soil Mechanics Laboratory

The University of Toledo Soil Mechanics Laboratory The University of Toledo Soil Mechanics Laboratory Permeability Testing - 1 Constant and Falling Head Tests Introduction In 1856 the French engineer Henri D arcy demonstrated by experiment that it is possible

More information

Modelling the Discharge Rate and the Ground Settlement produced by the Tunnel Boring

Modelling the Discharge Rate and the Ground Settlement produced by the Tunnel Boring Modelling the Discharge Rate and the Ground Settlement produced by the Tunnel Boring Giona Preisig*, Antonio Dematteis, Riccardo Torri, Nathalie Monin, Ellen Milnes, Pierre Perrochet *Center for Hydrogeology

More information

CHAPTER: 6 FLOW OF WATER THROUGH SOILS

CHAPTER: 6 FLOW OF WATER THROUGH SOILS CHAPTER: 6 FLOW OF WATER THROUGH SOILS CONTENTS: Introduction, hydraulic head and water flow, Darcy s equation, laboratory determination of coefficient of permeability, field determination of coefficient

More information

Lecture 6 - Boundary Conditions. Applied Computational Fluid Dynamics

Lecture 6 - Boundary Conditions. Applied Computational Fluid Dynamics Lecture 6 - Boundary Conditions Applied Computational Fluid Dynamics Instructor: André Bakker http://www.bakker.org André Bakker (2002-2006) Fluent Inc. (2002) 1 Outline Overview. Inlet and outlet boundaries.

More information

Fluid-Induced Material Transport: A Volume Averaged Approach to Modelling in SPH

Fluid-Induced Material Transport: A Volume Averaged Approach to Modelling in SPH Fluid-Induced Material Transport: A Volume Averaged Approach to Modelling in SPH Vinay Kumar SPH Workshop, 30.06. 01.07.2014, Karlsruhe www.baw.de Outline Motivation Model concept Groundwater model SPH

More information

1.72, Groundwater Hydrology Prof. Charles Harvey Lecture Packet #2: Aquifers, Porosity, and Darcy s Law. Lake (Exposed Water Table)

1.72, Groundwater Hydrology Prof. Charles Harvey Lecture Packet #2: Aquifers, Porosity, and Darcy s Law. Lake (Exposed Water Table) 1.72, Groundwater Hydrology Prof. Charles Harvey Lecture Packet #2: Aquifers, Porosity, and Darcy s Law Precipitation Infiltration Lake (Exposed Water Table) River Water table Saturated zone - Aquifer

More information

MODFLOW-2000, THE U.S. GEOLOGICAL SURVEY MODULAR GROUND-WATER MODEL USER GUIDE TO MODULARIZATION CONCEPTS AND THE GROUND-WATER FLOW PROCESS

MODFLOW-2000, THE U.S. GEOLOGICAL SURVEY MODULAR GROUND-WATER MODEL USER GUIDE TO MODULARIZATION CONCEPTS AND THE GROUND-WATER FLOW PROCESS MODFLOW-2000, THE U.S. GEOLOGICAL SURVEY MODULAR GROUND-WATER MODEL USER GUIDE TO MODULARIZATION CONCEPTS AND THE GROUND-WATER FLOW PROCESS By Arlen W. Harbaugh 1, Edward R. Banta 2, Mary C. Hill 3, and

More information

4. Right click grid ( ) and select New MODFLOW, then select Packages, enabling both the optional Well and Recharge option.

4. Right click grid ( ) and select New MODFLOW, then select Packages, enabling both the optional Well and Recharge option. Groundwater Hydrology CE 40460 Example 1 -- Grid Approach Building a grid is the first step in creating a groundwater model using GMS, and it requires the following components: top and bottom elevations,

More information

Fluids and Solids: Fundamentals

Fluids and Solids: Fundamentals Fluids and Solids: Fundamentals We normally recognize three states of matter: solid; liquid and gas. However, liquid and gas are both fluids: in contrast to solids they lack the ability to resist deformation.

More information

Understanding Complex Models using Visualization: San Bernardino Valley Ground-water Basin, Southern California

Understanding Complex Models using Visualization: San Bernardino Valley Ground-water Basin, Southern California Understanding Complex Models using Visualization: San Bernardino Valley Ground-water Basin, Southern California Zhen Li and Wesley R. Danskin U.S. Geological Survey, [email protected], [email protected],

More information

ESSENTIAL COMPONENTS OF WATER-LEVEL MONITORING PROGRAMS. Selection of Observation Wells

ESSENTIAL COMPONENTS OF WATER-LEVEL MONITORING PROGRAMS. Selection of Observation Wells ESSENTIAL COMPONENTS OF WATER-LEVEL MONITORING PROGRAMS Before discussing the uses and importance of long-term water-level data, it is useful to review essential components of a water-level monitoring

More information

Use of OpenFoam in a CFD analysis of a finger type slug catcher. Dynaflow Conference 2011 January 13 2011, Rotterdam, the Netherlands

Use of OpenFoam in a CFD analysis of a finger type slug catcher. Dynaflow Conference 2011 January 13 2011, Rotterdam, the Netherlands Use of OpenFoam in a CFD analysis of a finger type slug catcher Dynaflow Conference 2011 January 13 2011, Rotterdam, the Netherlands Agenda Project background Analytical analysis of two-phase flow regimes

More information

Revised Multi-Node Well (MNW2) Package for MODFLOW Ground-Water Flow Model

Revised Multi-Node Well (MNW2) Package for MODFLOW Ground-Water Flow Model Revised Multi-Node Well (MNW2) Package for MODFLOW Ground-Water Flow Model Techniques and Methods 6 A30 U.S. Department of the Interior U.S. Geological Survey Cover: Schematic cross section showing flow

More information

By Michael L. Merritt and Leonard F. Konikow. U.S. Geological Survey. Water-Resources Investigations Report 00-4167

By Michael L. Merritt and Leonard F. Konikow. U.S. Geological Survey. Water-Resources Investigations Report 00-4167 Documentation of a Computer Program to Simulate Lake-Aquifer Interaction Using the MODFLOW Ground-Water Flow Model and the MOC3D Solute-Transport Model By Michael L. Merritt and Leonard F. Konikow U.S.

More information

Processing Modflow A Simulation System for Modeling Groundwater Flow and Pollution. Wen-Hsing Chiang and Wolfgang Kinzelbach

Processing Modflow A Simulation System for Modeling Groundwater Flow and Pollution. Wen-Hsing Chiang and Wolfgang Kinzelbach Processing Modflow A Simulation System for Modeling Groundwater Flow and Pollution Wen-Hsing Chiang and Wolfgang Kinzelbach December 1998 Contents Preface 1. Introduction... 1 System Requirements... 4

More information

When the fluid velocity is zero, called the hydrostatic condition, the pressure variation is due only to the weight of the fluid.

When the fluid velocity is zero, called the hydrostatic condition, the pressure variation is due only to the weight of the fluid. Fluid Statics When the fluid velocity is zero, called the hydrostatic condition, the pressure variation is due only to the weight of the fluid. Consider a small wedge of fluid at rest of size Δx, Δz, Δs

More information

Coupling micro-scale CFD simulations to meso-scale models

Coupling micro-scale CFD simulations to meso-scale models Coupling micro-scale CFD simulations to meso-scale models IB Fischer CFD+engineering GmbH Fabien Farella Michael Ehlen Achim Fischer Vortex Factoria de Càlculs SL Gil Lizcano Outline Introduction O.F.Wind

More information

FLUID DYNAMICS. Intrinsic properties of fluids. Fluids behavior under various conditions

FLUID DYNAMICS. Intrinsic properties of fluids. Fluids behavior under various conditions FLUID DYNAMICS Intrinsic properties of fluids Fluids behavior under various conditions Methods by which we can manipulate and utilize the fluids to produce desired results TYPES OF FLUID FLOW Laminar or

More information

For Water to Move a driving force is needed

For Water to Move a driving force is needed RECALL FIRST CLASS: Q K Head Difference Area Distance between Heads Q 0.01 cm 0.19 m 6cm 0.75cm 1 liter 86400sec 1.17 liter ~ 1 liter sec 0.63 m 1000cm 3 day day day constant head 0.4 m 0.1 m FINE SAND

More information

Advanced tools in water management in The Netherlands

Advanced tools in water management in The Netherlands Advanced tools in water management in The Netherlands Modelling for system knowledge, effective operational management, and policy making Gé van den Eertwegh Rivierenland Water Board The Netherlands PR

More information

CONSTANT HEAD AND FALLING HEAD PERMEABILITY TEST

CONSTANT HEAD AND FALLING HEAD PERMEABILITY TEST CONSTANT HEAD AND FALLING HEAD PERMEABILITY TEST 1 Permeability is a measure of the ease in which water can flow through a soil volume. It is one of the most important geotechnical parameters. However,

More information

Review of Soil Moisture Calculation Method. 2. Conceptual Model of Soil Moisture Over a Shallow Water Table

Review of Soil Moisture Calculation Method. 2. Conceptual Model of Soil Moisture Over a Shallow Water Table 1 Review of Soil Moisture Calculation Method 1. Introduction In accordance with the Habitats Directive, the Environment Agency is required to carry out an appropriate assessment when considering applications

More information

Groundwater flow systems theory: an unexpected outcome of

Groundwater flow systems theory: an unexpected outcome of Groundwater flow systems theory: an unexpected outcome of early cable tool drilling in the Turner Valley oil field K. Udo Weyer WDA Consultants Inc. [email protected] Introduction The Theory of

More information

MIKE 21 FLOW MODEL HINTS AND RECOMMENDATIONS IN APPLICATIONS WITH SIGNIFICANT FLOODING AND DRYING

MIKE 21 FLOW MODEL HINTS AND RECOMMENDATIONS IN APPLICATIONS WITH SIGNIFICANT FLOODING AND DRYING 1 MIKE 21 FLOW MODEL HINTS AND RECOMMENDATIONS IN APPLICATIONS WITH SIGNIFICANT FLOODING AND DRYING This note is intended as a general guideline to setting up a standard MIKE 21 model for applications

More information

Distinguished Professor George Washington University. Graw Hill

Distinguished Professor George Washington University. Graw Hill Mechanics of Fluids Fourth Edition Irving H. Shames Distinguished Professor George Washington University Graw Hill Boston Burr Ridge, IL Dubuque, IA Madison, Wl New York San Francisco St. Louis Bangkok

More information

Open channel flow Basic principle

Open channel flow Basic principle Open channel flow Basic principle INTRODUCTION Flow in rivers, irrigation canals, drainage ditches and aqueducts are some examples for open channel flow. These flows occur with a free surface and the pressure

More information

LECTURE 9: Open channel flow: Uniform flow, best hydraulic sections, energy principles, Froude number

LECTURE 9: Open channel flow: Uniform flow, best hydraulic sections, energy principles, Froude number LECTURE 9: Open channel flow: Uniform flow, best hydraulic sections, energy principles, Froude number Open channel flow must have a free surface. Normally free water surface is subjected to atmospheric

More information

SWAT INPUT DATA:.GW CHAPTER 24

SWAT INPUT DATA:.GW CHAPTER 24 CHAPTER 24 SWAT INPUT DATA:.GW SWAT partitions groundwater into two aquifer systems: a shallow, unconfined aquifer which contributes return flow to streams within the watershed and a deep, confined aquifer

More information

Express Introductory Training in ANSYS Fluent Lecture 1 Introduction to the CFD Methodology

Express Introductory Training in ANSYS Fluent Lecture 1 Introduction to the CFD Methodology Express Introductory Training in ANSYS Fluent Lecture 1 Introduction to the CFD Methodology Dimitrios Sofialidis Technical Manager, SimTec Ltd. Mechanical Engineer, PhD PRACE Autumn School 2013 - Industry

More information

IMPACT ASSESSMENT OF SOLUTION MINING ON GROUNDWATER RESOURCES IN KAZAN TRONA FIELD, ANKARA-TURKEY

IMPACT ASSESSMENT OF SOLUTION MINING ON GROUNDWATER RESOURCES IN KAZAN TRONA FIELD, ANKARA-TURKEY IMPACT ASSESSMENT OF SOLUTION MINING ON GROUNDWATER RESOURCES IN KAZAN TRONA FIELD, ANKARA-TURKEY Hasan Yazicigil, Department of Geological Engineering Middle East Technical University, 06531, Ankara,

More information

Embankment Consolidation

Embankment Consolidation Embankment Consolidation 36-1 Embankment Consolidation In this tutorial, RS2 is used for a coupled analysis of a road embankment subject to loading from typical daily traffic. Model Start the RS2 9.0 Model

More information

2D Modeling of Urban Flood Vulnerable Areas

2D Modeling of Urban Flood Vulnerable Areas 2D Modeling of Urban Flood Vulnerable Areas Sameer Dhalla, P.Eng. Dilnesaw Chekol, Ph.D. A.D. Latornell Conservation Symposium November 22, 2013 Outline 1. Toronto and Region 2. Evolution of Flood Management

More information

SOUTHWEST FLORIDA WATER MANAGEMENT DISTRICT RESOURCE REGULATION TRAINING MEMORANDUM

SOUTHWEST FLORIDA WATER MANAGEMENT DISTRICT RESOURCE REGULATION TRAINING MEMORANDUM SOUTHWEST FLORIDA WATER MANAGEMENT DISTRICT RESOURCE REGULATION TRAINING MEMORANDUM DATE: December 04, 1996 This document is subject to change. If in doubt, verify current status with Technical Services

More information

ANNEX D1 BASIC CONSIDERATIONS FOR REVIEWING STUDIES IN THE DETAILED RISK ASSESSMENT FOR SAFETY

ANNEX D1 BASIC CONSIDERATIONS FOR REVIEWING STUDIES IN THE DETAILED RISK ASSESSMENT FOR SAFETY ANNEX D1 BASIC CONSIDERATIONS FOR REVIEWING STUDIES IN THE DETAILED RISK ASSESSMENT FOR SAFETY ANNEX D1: BASIC CONSIDERATIONS FOR REVIEWING STUDIES IN DRA FOR SAFETY D1-1 ANNEX D1 BASIC CONSIDERATIONS

More information

2.016 Hydrodynamics Reading #2. 2.016 Hydrodynamics Prof. A.H. Techet

2.016 Hydrodynamics Reading #2. 2.016 Hydrodynamics Prof. A.H. Techet Pressure effects 2.016 Hydrodynamics Prof. A.H. Techet Fluid forces can arise due to flow stresses (pressure and viscous shear), gravity forces, fluid acceleration, or other body forces. For now, let us

More information

COST AND PERFORMANCE REPORT

COST AND PERFORMANCE REPORT COST AND PERFORMANCE REPORT Pump and Treat of Contaminated Groundwater at the United Chrome Superfund Site Corvallis, Oregon September 1998 Prepared by: SITE INFORMATION Identifying Information: United

More information

Mathematics and Computation of Sediment Transport in Open Channels

Mathematics and Computation of Sediment Transport in Open Channels Mathematics and Computation of Sediment Transport in Open Channels Junping Wang Division of Mathematical Sciences National Science Foundation May 26, 2010 Sediment Transport and Life One major problem

More information

Hydraulics Laboratory Experiment Report

Hydraulics Laboratory Experiment Report Hydraulics Laboratory Experiment Report Name: Ahmed Essam Mansour Section: "1", Monday 2-5 pm Title: Flow in open channel Date: 13 November-2006 Objectives: Calculate the Chezy and Manning coefficients

More information

Water Supply. Simulation of Water Distribution Networks. Mohammad N. Almasri. Optimal Design of Water Distribution Networks Mohammad N.

Water Supply. Simulation of Water Distribution Networks. Mohammad N. Almasri. Optimal Design of Water Distribution Networks Mohammad N. Water Supply Simulation of Water Distribution Networks The Use of EPANET Mohammad N. Almasri 1 Introduction This presentation focuses on two issues: The simulation of water distribution networks (WDNs)

More information

Experiment (13): Flow channel

Experiment (13): Flow channel Introduction: An open channel is a duct in which the liquid flows with a free surface exposed to atmospheric pressure. Along the length of the duct, the pressure at the surface is therefore constant and

More information

USER S GUIDE FOR MODTOOLS: COMPUTER PROGRAMS FOR TRANSLATING DATA OF MODFLOW AND MODPATH INTO GEOGRAPHIC INFORMATION SYSTEM FILES

USER S GUIDE FOR MODTOOLS: COMPUTER PROGRAMS FOR TRANSLATING DATA OF MODFLOW AND MODPATH INTO GEOGRAPHIC INFORMATION SYSTEM FILES USER S GUIDE FOR MODTOOLS: COMPUTER PROGRAMS FOR TRANSLATING DATA OF MODFLOW AND MODPATH INTO GEOGRAPHIC INFORMATION SYSTEM FILES U.S. GEOLOGICAL SURVEY Open-File Report 97 240 MODFLOW MODPATH MODTOOLS

More information

STATE OF VERMONT AGENCY OF NATURAL RESOURCES DEPARTMENT OF ENVIRONMENTAL CONSERVATION WASTE MANAGEMENT DIVISION SOLID WASTE MANAGEMENT PROGRAM

STATE OF VERMONT AGENCY OF NATURAL RESOURCES DEPARTMENT OF ENVIRONMENTAL CONSERVATION WASTE MANAGEMENT DIVISION SOLID WASTE MANAGEMENT PROGRAM STATE OF VERMONT AGENCY OF NATURAL RESOURCES DEPARTMENT OF ENVIRONMENTAL CONSERVATION WASTE MANAGEMENT DIVISION SOLID WASTE MANAGEMENT PROGRAM Solid Waste Management Program Waste Management Division 103

More information

Ground-Water-Level Monitoring and the Importance of Long-Term Water-Level Data U.S. Geological Survey Circular 1217

Ground-Water-Level Monitoring and the Importance of Long-Term Water-Level Data U.S. Geological Survey Circular 1217 Ground-Water-Level Monitoring and the Importance of Long-Term Water-Level Data U.S. Geological Survey Circular 1217 by Charles J. Taylor William M. Alley Denver, Colorado 2001 U.S. DEPARTMENT OF THE INTERIOR

More information

O.F.Wind Wind Site Assessment Simulation in complex terrain based on OpenFOAM. Darmstadt, 27.06.2012

O.F.Wind Wind Site Assessment Simulation in complex terrain based on OpenFOAM. Darmstadt, 27.06.2012 O.F.Wind Wind Site Assessment Simulation in complex terrain based on OpenFOAM Darmstadt, 27.06.2012 Michael Ehlen IB Fischer CFD+engineering GmbH Lipowskystr. 12 81373 München Tel. 089/74118743 Fax 089/74118749

More information

VISCOSITY OF A LIQUID. To determine the viscosity of a lubricating oil. Time permitting, the temperature variation of viscosity can also be studied.

VISCOSITY OF A LIQUID. To determine the viscosity of a lubricating oil. Time permitting, the temperature variation of viscosity can also be studied. VISCOSITY OF A LIQUID August 19, 004 OBJECTIVE: EQUIPMENT: To determine the viscosity of a lubricating oil. Time permitting, the temperature variation of viscosity can also be studied. Viscosity apparatus

More information

Maximizing volume given a surface area constraint

Maximizing volume given a surface area constraint Maximizing volume given a surface area constraint Math 8 Department of Mathematics Dartmouth College Maximizing volume given a surface area constraint p.1/9 Maximizing wih a constraint We wish to solve

More information

Soil Suction. Total Suction

Soil Suction. Total Suction Soil Suction Total Suction Total soil suction is defined in terms of the free energy or the relative vapor pressure (relative humidity) of the soil moisture. Ψ = v RT ln v w 0ω v u v 0 ( u ) u = partial

More information

Appendix 4-C. Open Channel Theory

Appendix 4-C. Open Channel Theory 4-C-1 Appendix 4-C Open Channel Theory 4-C-2 Appendix 4.C - Table of Contents 4.C.1 Open Channel Flow Theory 4-C-3 4.C.2 Concepts 4-C-3 4.C.2.1 Specific Energy 4-C-3 4.C.2.2 Velocity Distribution Coefficient

More information

GEOS 4430 Lecture Notes: Darcy s Law

GEOS 4430 Lecture Notes: Darcy s Law GEOS 4430 Lecture Notes: Darcy s Law Dr. T. Brikowski Fall 2013 0 file:darcy law.tex,v (1.24), printed October 15, 2013 Introduction Motivation: hydrology generally driven by the need for accurate predictions

More information

Physics 9e/Cutnell. correlated to the. College Board AP Physics 1 Course Objectives

Physics 9e/Cutnell. correlated to the. College Board AP Physics 1 Course Objectives Physics 9e/Cutnell correlated to the College Board AP Physics 1 Course Objectives Big Idea 1: Objects and systems have properties such as mass and charge. Systems may have internal structure. Enduring

More information

Emergency Spillways (Sediment basins)

Emergency Spillways (Sediment basins) Emergency Spillways (Sediment basins) DRAINAGE CONTROL TECHNIQUE Low Gradient Velocity Control Short-Term Steep Gradient Channel Lining Medium-Long Term Outlet Control Soil Treatment Permanent [1] [1]

More information

Chapter 9. Steady Flow in Open channels

Chapter 9. Steady Flow in Open channels Chapter 9 Steady Flow in Open channels Objectives Be able to define uniform open channel flow Solve uniform open channel flow using the Manning Equation 9.1 Uniform Flow in Open Channel Open-channel flows

More information

ME6130 An introduction to CFD 1-1

ME6130 An introduction to CFD 1-1 ME6130 An introduction to CFD 1-1 What is CFD? Computational fluid dynamics (CFD) is the science of predicting fluid flow, heat and mass transfer, chemical reactions, and related phenomena by solving numerically

More information

NUMERICAL ANALYSIS OF THE EFFECTS OF WIND ON BUILDING STRUCTURES

NUMERICAL ANALYSIS OF THE EFFECTS OF WIND ON BUILDING STRUCTURES Vol. XX 2012 No. 4 28 34 J. ŠIMIČEK O. HUBOVÁ NUMERICAL ANALYSIS OF THE EFFECTS OF WIND ON BUILDING STRUCTURES Jozef ŠIMIČEK email: [email protected] Research field: Statics and Dynamics Fluids mechanics

More information

INTRODUCTION TO FLUID MECHANICS

INTRODUCTION TO FLUID MECHANICS INTRODUCTION TO FLUID MECHANICS SIXTH EDITION ROBERT W. FOX Purdue University ALAN T. MCDONALD Purdue University PHILIP J. PRITCHARD Manhattan College JOHN WILEY & SONS, INC. CONTENTS CHAPTER 1 INTRODUCTION

More information

Hydraulic Transients used for Leakage Detection in Water Distribution Systems

Hydraulic Transients used for Leakage Detection in Water Distribution Systems Hydraulic Transients used for Leakage Detection in Water Distribution Systems Dídia Covas and Helena Ramos Instituto Superior Técnico, Dept. Civil Engineering, Lisbon, Portugal ABSTRACT The current paper

More information

Differential Balance Equations (DBE)

Differential Balance Equations (DBE) Differential Balance Equations (DBE) Differential Balance Equations Differential balances, although more complex to solve, can yield a tremendous wealth of information about ChE processes. General balance

More information

2.0 BASIC CONCEPTS OF OPEN CHANNEL FLOW MEASUREMENT

2.0 BASIC CONCEPTS OF OPEN CHANNEL FLOW MEASUREMENT 2.0 BASIC CONCEPTS OF OPEN CHANNEL FLOW MEASUREMENT Open channel flow is defined as flow in any channel where the liquid flows with a free surface. Open channel flow is not under pressure; gravity is the

More information

EXPERIMENT 10 CONSTANT HEAD METHOD

EXPERIMENT 10 CONSTANT HEAD METHOD EXPERIMENT 10 PERMEABILITY (HYDRAULIC CONDUCTIVITY) TEST CONSTANT HEAD METHOD 106 Purpose: The purpose of this test is to determine the permeability (hydraulic conductivity) of a sandy soil by the constant

More information

CHAPTER 9 CHANNELS APPENDIX A. Hydraulic Design Equations for Open Channel Flow

CHAPTER 9 CHANNELS APPENDIX A. Hydraulic Design Equations for Open Channel Flow CHAPTER 9 CHANNELS APPENDIX A Hydraulic Design Equations for Open Channel Flow SEPTEMBER 2009 CHAPTER 9 APPENDIX A Hydraulic Design Equations for Open Channel Flow Introduction The Equations presented

More information

Chapter 13 OPEN-CHANNEL FLOW

Chapter 13 OPEN-CHANNEL FLOW Fluid Mechanics: Fundamentals and Applications, 2nd Edition Yunus A. Cengel, John M. Cimbala McGraw-Hill, 2010 Lecture slides by Mehmet Kanoglu Copyright The McGraw-Hill Companies, Inc. Permission required

More information

Customer Training Material. Lecture 2. Introduction to. Methodology ANSYS FLUENT. ANSYS, Inc. Proprietary 2010 ANSYS, Inc. All rights reserved.

Customer Training Material. Lecture 2. Introduction to. Methodology ANSYS FLUENT. ANSYS, Inc. Proprietary 2010 ANSYS, Inc. All rights reserved. Lecture 2 Introduction to CFD Methodology Introduction to ANSYS FLUENT L2-1 What is CFD? Computational Fluid Dynamics (CFD) is the science of predicting fluid flow, heat and mass transfer, chemical reactions,

More information

Hydrologic Modeling System HEC-HMS

Hydrologic Modeling System HEC-HMS Hydrologic Engineering Center Hydrologic Modeling System HEC-HMS Release Notes Version 4.0 December 2013 Approved for Public Release Distribution Unlimited Hydrologic Modeling System HEC-HMS, Release Notes

More information

Numerical Modelling of Water Flow (Seepage) in the Karun 4 Dam and Abutments (Steady State)

Numerical Modelling of Water Flow (Seepage) in the Karun 4 Dam and Abutments (Steady State) Numerical Modelling of Water Flow (Seepage) in the Karun 4 Dam and Abutments (Steady State) Mohammad Hosseiny Sohi 03 November 2015 Contents: Objectives Karun River & Karun 4 Dam in Iran Geology of dam

More information

LNAPL Distribution and Recovery Model (LDRM) Volume 2: User and Parameter Selection Guide. Regulatory and Scientific Affairs Department

LNAPL Distribution and Recovery Model (LDRM) Volume 2: User and Parameter Selection Guide. Regulatory and Scientific Affairs Department LNAPL Distribution and Recovery Model (LDRM) Volume 2: User and Parameter Selection Guide Regulatory and Scientific Affairs Department API PUBLICATION 4760 JANUARY 2007 LNAPL Distribution and Recovery

More information

Lecture L2 - Degrees of Freedom and Constraints, Rectilinear Motion

Lecture L2 - Degrees of Freedom and Constraints, Rectilinear Motion S. Widnall 6.07 Dynamics Fall 009 Version.0 Lecture L - Degrees of Freedom and Constraints, Rectilinear Motion Degrees of Freedom Degrees of freedom refers to the number of independent spatial coordinates

More information

du u U 0 U dy y b 0 b

du u U 0 U dy y b 0 b BASIC CONCEPTS/DEFINITIONS OF FLUID MECHANICS (by Marios M. Fyrillas) 1. Density (πυκνότητα) Symbol: 3 Units of measure: kg / m Equation: m ( m mass, V volume) V. Pressure (πίεση) Alternative definition:

More information

How To Build An Effluent Recovery Scheme

How To Build An Effluent Recovery Scheme NGEST Effluent Recovery Scheme tekopohjavettä jätevedestä 6.10.2010 / Suvi Niini NGEST Effluent Recovery Scheme Part of a larger Northern Gaza Emergency Sewage Treatment Project (NGEST) with several donors

More information

Chapter 5 MASS, BERNOULLI AND ENERGY EQUATIONS

Chapter 5 MASS, BERNOULLI AND ENERGY EQUATIONS Fluid Mechanics: Fundamentals and Applications, 2nd Edition Yunus A. Cengel, John M. Cimbala McGraw-Hill, 2010 Chapter 5 MASS, BERNOULLI AND ENERGY EQUATIONS Lecture slides by Hasan Hacışevki Copyright

More information

6-1 Introduction. 1. Storm drain that does not require pressure testing. 2. Lateral that does not require pressure testing.

6-1 Introduction. 1. Storm drain that does not require pressure testing. 2. Lateral that does not require pressure testing. Chapter 6 Storm Drains 6-1 Introduction A storm drain (storm sewer) is a network of pipes that conveys surface drainage from a surface inlet or through a manhole, to an outfall. Storm drains are defined

More information

SOIL GAS MODELLING SENSITIVITY ANALYSIS USING DIMENSIONLESS PARAMETERS FOR J&E EQUATION

SOIL GAS MODELLING SENSITIVITY ANALYSIS USING DIMENSIONLESS PARAMETERS FOR J&E EQUATION 1 SOIL GAS MODELLING SENSITIVITY ANALYSIS USING DIMENSIONLESS PARAMETERS FOR J&E EQUATION Introduction Chris Bailey, Tonkin & Taylor Ltd, PO Box 5271, Wellesley Street, Auckland 1036 Phone (64-9)355-6005

More information

Fundamentals of Fluid Mechanics

Fundamentals of Fluid Mechanics Sixth Edition. Fundamentals of Fluid Mechanics International Student Version BRUCE R. MUNSON DONALD F. YOUNG Department of Aerospace Engineering and Engineering Mechanics THEODORE H. OKIISHI Department

More information

F1 Fuel Tank Surging; Model Validation

F1 Fuel Tank Surging; Model Validation F1 Fuel Tank Surging; Model Validation Luca Bottazzi and Giorgio Rossetti Ferrari F1 team, Maranello, Italy SYNOPSIS A Formula One (F1) car can carry more than 80 kg of fuel in its tank. This has a big

More information

Drinking Water Source Protection Area Delineation Guidelines and Process Manual

Drinking Water Source Protection Area Delineation Guidelines and Process Manual Drinking Water Source Protection Area Delineation Guidelines and Process Manual Division of Drinking and Ground Waters Source Water Assessment and Protection Program Revised December 2014 Table of Contents

More information

Chapter 4 Atmospheric Pressure and Wind

Chapter 4 Atmospheric Pressure and Wind Chapter 4 Atmospheric Pressure and Wind Understanding Weather and Climate Aguado and Burt Pressure Pressure amount of force exerted per unit of surface area. Pressure always decreases vertically with height

More information

Domain decomposition techniques for interfacial discontinuities

Domain decomposition techniques for interfacial discontinuities Domain decomposition techniques for interfacial discontinuities Geordie McBain Institut Jean le Rond d Alembert December 5, 2012 Connexion and substructuring Two ways to look at domain decomposition Decomposing

More information

oil liquid water water liquid Answer, Key Homework 2 David McIntyre 1

oil liquid water water liquid Answer, Key Homework 2 David McIntyre 1 Answer, Key Homework 2 David McIntyre 1 This print-out should have 14 questions, check that it is complete. Multiple-choice questions may continue on the next column or page: find all choices before making

More information

STANDARD CLEANING AND CALIBRATION PROCEDURE FOR TGA-50(H) AND TGA-51(H)

STANDARD CLEANING AND CALIBRATION PROCEDURE FOR TGA-50(H) AND TGA-51(H) STANDARD CLEANING AND CALIBRATION PROCEDURE FOR TGA-50(H) AND TGA-51(H) by Joseph F. Greenbeck, Jr. And Courtney W. Taylor INTRODUCTION The following procedure is to be used for the maintenance and calibration

More information

AP1 Waves. (A) frequency (B) wavelength (C) speed (D) intensity. Answer: (A) and (D) frequency and intensity.

AP1 Waves. (A) frequency (B) wavelength (C) speed (D) intensity. Answer: (A) and (D) frequency and intensity. 1. A fire truck is moving at a fairly high speed, with its siren emitting sound at a specific pitch. As the fire truck recedes from you which of the following characteristics of the sound wave from the

More information

STATE OF TENNESSEE DEPARTMENT OF ENVIRONMENT AND CONSERVATION DIVISION OF UNDERGROUND STORAGE TANKS TECHNICAL GUIDANCE DOCUMENT - 008

STATE OF TENNESSEE DEPARTMENT OF ENVIRONMENT AND CONSERVATION DIVISION OF UNDERGROUND STORAGE TANKS TECHNICAL GUIDANCE DOCUMENT - 008 STATE OF TENNESSEE DEPARTMENT OF ENVIRONMENT AND CONSERVATION DIVISION OF UNDERGROUND STORAGE TANKS TECHNICAL GUIDANCE DOCUMENT - 008 Effective Date - January 13, 1992 Revised Date - November 19, 1993

More information

Lecture 5 Hemodynamics. Description of fluid flow. The equation of continuity

Lecture 5 Hemodynamics. Description of fluid flow. The equation of continuity 1 Lecture 5 Hemodynamics Description of fluid flow Hydrodynamics is the part of physics, which studies the motion of fluids. It is based on the laws of mechanics. Hemodynamics studies the motion of blood

More information