GEO-SLOPE International Ltd, Calgary, Alberta, Canada Salt Flow Example

Similar documents
Lecture 3 Activated sludge and lagoons

Investigation of a Dual-Bed Autothermal Reforming of Methane for Hydrogen Production

THE EFFECT OF SHEAR STRENGTH NORMALISATION ON THE RESPONSE OF PILES IN LATERALLY SPREADING SOILS

The impact of velocity on thermal energy storage performance of tube type thermocline tank

Hybrid Model of Existing Buildings for Transient Thermal Performance Estimation

DESIGN OF OPTIMAL WATER DISTRIBUTION SYSTEMS

Production Policies of Perishable Product and Raw Materials

Head versus Volume and Time

A Three-dimensional Coupled Thermo-hydro Model for Enhanced Geothermal Systems

Adjoint Modeling to Quantify Stream Flow Changes Due to Aquifer Pumping

COMPUTER MODELLING AND FINITE ELEMENT ANALYSIS OF TUBE FORMING OPERATIONS Dr.S.Shamasundar, Manu Mathai, Sachin B M

Demulsification of Water-in-Oil Emulsions by Microwave Heating Technology

Quantitative Models to Study the Soil Porosity

CONE PERMEAMETER IN-SITU PERMEABILITY MEASUREMENTS WITH DIRECT PUSH TECHNIQUES

Surface Water Hydrology

SANITARY ENGINEERING ASSISTANT, 7866 SANITARY ENGINEERING ASSOCIATE, 7870 SANITARY ENGINEER, 7872

Theoretical Investigation on Condensing Characteristics of Air and Oil Vapor Mixtures

Analysis of the Internal Pressure in Tube Hydroforming and Its Experimental Investigation

MODELING AND SIMULATION OF A FUEL CELL REFORMER FOR CONTROL APPLICATIONS

Progress towards Modeling Red Tides and Algal Blooms

Numerical Simulation of Transient 3-D Surface Deformation of a Completely Penetrated GTA Weld

GenomeLab GeXP. Troubleshooting Guide. A53995AC December 2009

MIAMI-DADE COUNTY PRODUCT CONTROL SECTION DEPARTMENT OF REGULATORY AND ECONOMIC RESOURCES (RER)

OPTIMIZATION OF FILLER METALS CONSUMPTION IN THE PRODUCTION OF WELDED STEEL STRUCTURES

Optimum Design of Pipe Bending Based on High- Frequency Induction Heating Using Dynamic Reverse Moment

Quick Reference: Amplifier Equations

Global Energy Trade Flows and Constraints on Conventional and Renewable Energies A Computable Modeling Approach

KINEMATICS OF RIGID BODIES. y Copyright 1997 by The McGraw-Hill Companies, Inc. All rights reserved. KINEMATICS OF RIGID BODIES

Learning and Technology Spillover: Productivity Convergence in Norwegian Salmon Aquaculture

DEFECT ASSESSMENT ON PIPE USED FOR TRANSPORT OF MIXTURE OF HYDROGEN AND NATURAL GAS

CONICAL PIPE ENVELOPE FORMATION PROCESS

Quantifying the First-Flush Phenomenon: Effects of First-Flush on Water Yield and Quality

SCHEDULING FOR YARD CRANES BASED ON TWO-STAGE HYBRID DYNAMIC PROGRAMMING

Cross-Roller Ring Series

Fuzzy evaluation to parkour social value research based on AHP improved model

MODELING THE TAPPING OF SILICON MELT FROM THE SUBMERGED ARC FURNACES

Evaluating the Effectiveness of a Balanced Scorecard System Implemented in a Functional Organization

Report of significant findings--las Vegas Bay/ Boulder Basin investigations

Theoretical model and experimental investigation of current density boundary condition for welding arc study

Optimal Spatial Design of Capacity and Quantity of Rainwater Harvesting Systems for Urban Flood Mitigation

Analysis of a Mesoscale Fuel Reformer with Heat Recirculation and Porous Surface Stabilized Flame

SURFACE TENSION OF LIQUID MARBLES, AN EXPERIMENTAL APPROACH

AN IDEA BASED ON HONEY BEE SWARM FOR NUMERICAL OPTIMIZATION (TECHNICAL REPORT-TR06, OCTOBER, 2005) Dervis KARABOGA

A biomechanical model for the study of plant morphogenesis: Coleocheate orbicularis, a 2D study species.

An Approach to Classify the Risk of Operating Nuclear Power Plants Case Study: Neckarwestheim Unit 1 and Unit 2

Lectures on: Introduction to and fundamentals of discrete dislocations and dislocation dynamics. Theoretical concepts and computational methods

Quantitative [3-glucuronidase assay in transgenic plants

r r r r r r r r r REPORT ON THE EDWARDS AQUIFER SAN ANTONIO REGION, TEXAS DONALD G. RAUSCHUBER & ASSOCIATES, INC. AUSTIN, TEXAS MAY 18, 1995

Pass-Through and Consumer Search: An Empirical Analysis. by Timothy J. Richards, Miguel I Gómez and Jun Lee

DISPLACEMENT-BASED DESIGN OF CONCRETE TILT-UP FRAMES ACCOUNTING FOR FLEXIBLE DIAPHRAGMS

The effect of hitch-hiking on genes linked to a balanced polymorphism in a subdivided population

Super Precision Bearings for Machine Tools

Arch. Min. Sci., Vol. 61 (2016), No 4, p

Occurrence and spatial pattern of water repellency in a beech forest subsoil

PcBn for cast iron Machining

Managing Accounting Information Quality: An Australian Study

APPENDIX A RAINFALL LOSSES. (Draft of section of Maricopa County, Arizona, Hydrologic Design Manual)

A Model for Dissolution of Lime in Steelmaking Slags

Ru Bbar and Shansep Soil Strength

Nucleation and crystallisation kinetics of a Na-fluorrichterite based glass by differential scanning calorimetry (DSC)

Steam Turbine Seminar -17 Lund University

direction and point of application.

W. M. Clearman, S. M. Ghiaasiaan, J. S. Cha, C. S. Kirkconnell 1, P. V. Desai

A two-level discount model for coordinating a decentralized supply chain considering stochastic price-sensitive demand

Ground-Water Contamination

Application of Induction Machine in Wind Power Generation System

HOBAS NC Line. Make things happen.

Assessing Emission Allocation in Europe: An Interactive Simulation Approach

Optimal Policies for Perishable Items when Demand Depends on Freshness of Displayed Stock and Selling Price

TOWARD ESTABLISHING A COMPREHENSIVE PRESSURE-SINKAGE MODEL FOR SMALL DIAMETER WHEELS ON DEFORMABLE TERRAINS

Solar in Wetlands. Photo credit: a k e.org/blog/2012/08/15mw solar field near philadelphia.html

CITY OF ANN ARBOR ENGINEERING RIVERVIEW DRIVE SANITARY SEWER AND WATER MAIN EXTENSION PROJECT WARREN STEIN BARTON NIXON EARHART DHUVARREN TRAIL GREEN

TRAINING NEEDS ANALYSIS and NATIONAL TRAINING STRATEGIES

Nolan et al, United States Geological Survey National Ambient Water Quality Assessment Program Risk of Groundwater Contamination.

Detection of allele-specific methylation through a generalized heterogeneous epigenome model

Springback Simulation with Complex Hardening Material Models

FACTORS INFLUENCING ENERGY CONSUMPTION IN FRUIT AND VEGETABLE PROCESSING PLANTS. Janusz Wojdalski, Bogdan DróŜdŜ, Michał Lubach

E T HIGH PERFORMANCE MULTI-MATERIAL MILLING. The Mastermill VX range: Exceptional performance and reliability. UROPA OOL

The Brazilian ethanol industry

Two-tier Spatial Modeling of Base Stations in Cellular Networks

Improving Software Effort Estimation Using Neuro-Fuzzy Model with SEER-SEM

Combining ability analysis for yield and quality traits in indigenous aromatic rice

Time of Day Tariff Structure

Self-assessment for the SEPA-compliance of infrastructures

Rapid Drawdown with Effective Stress

Environmental Externalities in the Presence of Network Effects: Adoption of Low Emission Technologies in the Automobile Market

ABSTRACT INTRODUCTION

DEW POINT OF THE FLUE GAS OF BOILERS CO-FIRING

Newcastle University, Newcastle upon Tyne, United Kingdom

One-to-one Marketing on the Internet

Transcriptome-based distance measures for grouping of germplasm and prediction of hybrid performance in maize

Social Rewarding in Wiki Systems Motivating the Community

Experimental Evaluation of the Energy Performance of an Air Vortex Tube when the Inlet Parameters are Varied

of the North American Automotive Industry VOLUME 3: MATERIALS June, 1998 Published by

DRAFT Traffic Operations & Safety Evaluation Technical Memorandum

Self-organization approach for THz polaritonic metamaterials

PROGRAMA BIOEN Projeto 2008/ Simulating Land Use and Agriculture Expansion in Brazil: Food, Energy, Agro industrial and Environmental Impacts

Introduction. Keywords: bamboo, dynamic nanoindentation, heat treatment, quasi-static nanoindentation

DETERMINATION OF TOTAL AVAILABLE MOISTURE IN Sol LS*

Transcription:

1 Intoduction Salt Flow Example Total hydaulic head consists o elevation head and pessue head. Pessue head is dependent on the density o the poe luid, which is a unction o both tempeatue and chemical composition. Fo densitydependent goundwate low poblems, the diving oces o low include the hydaulic gadient, as well as a buoyancy oce tem caused by vaiations in density. Consequently, spatial vaiations in salinity geneate a total hydaulic head gadient that govens density-dependent goundwate low. The obective o this detailed example is to veiy, by means o some simple calculations, the hydaulic head and goundwate luxes calculated by CTRAN/W o coupled one-dimensional density-dependent goundwate low poblems. 2 Backgound Only a bie summay o the theoy o density-dependent low is povided hee. A moe compehensive eview can be ound in the CTRAN/W Engineeing book and the liteatue (e.g. Fette, 1998; Find, 1982a, b). As noted in the intoduction, the poe luid density aects the pessue head component o total hydaulic head. Conside the two point measuements o hydaulic head shown in Figue 1. The actual hydaulic pessue at P 1 in the saline-wate aquie is P gh [1] 1 s s whee s = saline poe luid density; g = acceleation due to gavity; and, h s = height o saline wate in the piezomete. Figue 1 Equivalent esh wate head (ate Fette, 1988) Assume that anothe piezomete was completed in the saline-wate aquie at P 2, but that it was illed with esh wate. The hydaulic pessue at P 2 is CTRAN Example File: Salt Flow Example (pd)(gsz)page 1 o 7

P gh [2] 2 whee = eshwate density; and, h = height o esh wate in the piezomete. The piezometes ae completed at the same elevation, so P 1 must equal P 2. Setting Eq. [1] equal to Eq. [2] esults in the ollowing elationship between the esh wate pessue head and saline-wate pessue head: h s hs [3] The equivalent esh wate total head can now be calculated as the esh wate pessue head plus the elevation head z : h s s z [4] Use o the equivalent eshwate total head o density-dependent goundwate low poblems equies the geneal Dacy equation to be ecast as qi Ki n x [5] whee K i = hydaulic conductivity tenso; n 1 indicates the vetical diection and n 0 indicates the hoizontal diection; and, = elative density deined as: s 1 [6] The indices i and ae vaied as i 0, which coesponds to the hoizontal low component (note: the hoizontal low component is unaected by the second tem because n 0 ), and i 1 which coesponds to the vetical low diection. In this om, Dacy s equation contains two dynamic diving oces: the hydaulic gadient calculated om the equivalent eshwate total head and the buoyancy oce ( tem). The buoyancy oce is oten eeed to as the body oce and epesents the additional gadient caused by vaiations in density. The implementation o Eq. [5] equies knowledge o the poe luid density s, o moe speciically the atio o s. The poe luid density is a unction o the concentation o the dissolved solute. Fo CTRAN Example File: Salt Flow Example (pd)(gsz)page 2 o 7

isothemal conditions and a ange o concentations up to that o seawate, thee is essentially a linea elationship between luid density and concentation (Figue 2) that can be witten as (1 ) [7] s c whee c is the concentation nomalized to the maximum concentation (C max ) and anging om 0 to 1.0, and is the contaminant density contast equal to max 1 [8] 1030 1025 Maximum Density 1020 s 1015 1010 1005 1000 0 0.2 0.4 0.6 0.8 1 1.2 c (non-dimensional) Figue 2 Relationship between density and concentation Substituting Eq. [7] into [6] yields the ollowing o elative density ( ): c [9] By substituting Equation [9] into [5], Dacy s Law can be witten as qi Ki cn x [10] In this om, the contaminant density contast ( ) and nomalized concentation (c) ae equied to compute seepage luxes. In SEEP/W, the use is equied to speciy a elative density at a eeence concentation unde the KeyIn Analysis dialogue box. The elative density (not to be conused with Eq. [6]) is simply the atio o / max in Eq. [8] at a maximum concentation (i.e. the eeence concentation). Accodingly, CTRAN can compute the nomalized concentation (c) using the eeence concentation (C/C e ). Fo example, assume that the use input elative density was 1.025 (i.e. seawate) at a eeence concentation o 10,000 g/m 3. I the concentation at a point in the model domain was 5000 g/m 3, the elative concentation is c 0.5 and = 0.025. CTRAN Example File: Salt Flow Example (pd)(gsz)page 3 o 7

Fo density-dependent poblems, the constitutive elationship (i.e. Eq. [5]), and theeoe the goundwate velocity, is a unction o concentation via the luid density ( s ). Similaly, the govening equation o solute tanspot (ee to the CTRAN Engineeing book) is a unction o the goundwate velocity though the advective tanspot tem. The equations ae theeoe coupled though density and velocity. In the CTRAN/W and SEEP/W omulation, SEEP/W computes the velocity and passes this inomation to CTRAN/W. CTRAN/W then computes the concentation and then passes the concentation values back to SEEP/W. The two pogams pass this inomation back and oth until thee is no uthe change in H and C, o in othe wods, until the solution has conveged. 3 Bounday Conditions and Mateial Popeties The Salt Flow gsz ile includes a density-dependent SEEP/W analysis and a density-dependent CTRAN/W analysis. Adding a density-dependent SEEP/W analysis automatically geneates the associated CTRAN/W analysis (o vice vesa). The time step inomation and convegence citeia ae speciied in the CTRAN/W KeyIn Analysis. A sceen captue o the KeyIn Analyses dialogue box is pesented in Figue 3. The elative density was speciied as 1.025 (i.e. seawate) at a eeence concentation c 1.0 g/m 3. Figue 3 Model stuctue o the Salt Flow Example The example ile includes two model domains: a vetical column and a hoizontal column. Each column is 1 m in length and 0.1 m in width with a mesh that consists o 20 elements and 22 nodes. The hydaulic conductivity and poosity o the soil is 1 m/sec and 0.35, espectively. Fo the vetical column, the top bounday is set as a constant head o 1 m (H = 1 m). The let and ight boundaies o the hoizontal column ae set to total hydaulic heads o 0.2 m and 0.1 m, espectively. The soil is assigned a coeicient o diusion (D) o 1 10-5 m 2 /sec. The longitudinal and tansvese dispesivity values wee abitaily set to a low value (1 10-20 m 2 /sec). A unit concentation o 1 g/m 3 is applied to both columns. Accodingly, the concentation thoughout the model domain is equal to the use-deined eeence concentation (i.e. c = 1.0) and the body oce tem will equal 0.025. The initial CTRAN Example File: Salt Flow Example (pd)(gsz)page 4 o 7

Height (m) GEO-SLOPE Intenational Ltd, Calgay, Albeta, Canada www.geo-slope.com poe wate conditions ae speciied using a piezometic line, while the initial concentations ae deined using the activation concentation unde KeyIn Mateials. The analyses wee un o an elapsed time o 100 seconds with one time incement. 4 Results and Discussion 4.1 Vetical Column Figue 4 pesents a poile o the equivalent esh wate head computed by SEEP/W o the vetical column. The esh wate head at the bottom o the column is 1.025 m, which is equal to the hydaulic pessue (10.052 kpa) divided by the unit weight o esh wate (9.81 kpa/m). Although thee is an upwads hydaulic gadient o x1 0.025 in the column, the vetical goundwate velocity is zeo. This occus because the upwad hydaulic gadient is countebalanced by the downwad body oce c 0.025 in Eq. [10]. 1 0.9 0.8 0.7 Fesh Wate Head 0.6 0.5 0.4 0.3 0.2 0.1 0 1 1.005 1.01 1.015 1.02 1.025 Fesh Wate Head (m) Figue 4 Vetical Poile o Fesh Wate Head 4.2 Hoizontal Column Figue 5 pesents the contous o equivalent esh wate head along with values at the ou cones o the hoizontal column. The esh wate hydaulic heads computed at points A, B, C, and D ae consistent with Eq. [3]. Fo example, the salt wate head along the let bounday was set to 0.2 m, so the poe-wate pessue at point A is equal to 1.005525 kpa (i.e. sghs = (1025 kg/m 3 )(9.81 m/s 2 )(0.2 0.1)m). The equivalent eshwate head is calculated as 0.2025 m using Eq. [3]. Thee is an upwad esh wate hydaulic gadient o 0.025 m/m acoss the entie column, as was the case with the vetical column. CTRAN Example File: Salt Flow Example (pd)(gsz)page 5 o 7

Figue 5 Contous o Equivalent Fesh Wate Total Head Results o a Gauss egion in the model domain ae shown in Figue 6. The upwad esh wate hydaulic gadient is countebalanced by the downwad body oce, so the vetical gadient and the liquid y-velocity thoughout the model domain ae zeo. The esh wate hydaulic gadient in the hoizontal diection acoss the column at all elevations is 0.1025. Given a hydaulic conductivity o 1.0 m/s and a column length o 1.0 m, the calculated goundwate lux is 0.1025 m/s. The cumulative lux ove an elapsed time o 100 seconds is 1.025 m 3, as shown on the lux section in Figue 5. Figue 6 Results o a Gauss Region 5 Concluding Remaks This example illustates the esh wate hydaulic heads and luxes calculated by SEEP/W o a coupled density-dependent goundwate low poblem. All hydaulic heads ae conveted to an equivalent esh wate total head based on the density o the poe luid. Poe luid density is a unction o the solute concentation, so the solution is coupled and theeoe SEEP/W must be integated with CTRAN/W. Intepeting the computed hydaulic heads and goundwate luxes equies an undestanding o the undelying theoy o density-dependent goundwate low poblems. This simple example demonstates that SEEP/W and CTRAN/W have been coectly coded o densitydependant low and that the pocedue o passing velocity and concentation between the two pogams is an acceptable pocedue o solving this coupled pocess, even though the two patial dieential equations ae not solved simultaneously. CTRAN Example File: Salt Flow Example (pd)(gsz)page 6 o 7

6 Reeences GEO-SLOPE Intenational Ltd, Calgay, Albeta, Canada www.geo-slope.com Fette, 1994. Applied Hydogeology, 3 d Edition. Pentice Hall, Englewood Clis, NJ. Find, 1982a. Simulation o long-tem tansient density-dependent tanspot in goundwate. Advances in Wate Resouces, Vol. 5, pp. 73-88 Find, 1982b. Seawate instuction in continuous coastal aquie-aquitad systems. Advances in Wate Resouces, Vol. 5, pp89-97. CTRAN Example File: Salt Flow Example (pd)(gsz)page 7 o 7