Derivation of the Dupuit Equation - Unconfined Flow

Slides:



Advertisements
Similar presentations
Flood Profile Modeling with Split Flows and Weirs
Advertisements

Groundwater Hydraulics Daene C. McKinney
Groundwater Flow Equations
Principles of Groundwater Flow
CIV3248 Flow Net Workshop1 CIV3248 Groundwater,seepage and environmental engineering Workshop (4) Flownet sketching Keith H McKenry.
PRINCIPLES OF GROUNDWATER FLOW
TOPIC 2 STEADY STATE FLOW THROUGH SOIL Course: S0705 – Soil Mechanic Year: 2008.
Chapter 6: Bounded Aquifers Stephanie Fulton January 24, 2014.
Philip B. Bedient Civil & Environmental Engineering Rice University
Effects of Boundary Condition on Shape of Flow Nets
Wedge-shaped and sloping aquifers Adam Forsberg January 28, 2013.
Water Movement in Soil and Rocks. Two Principles to Remember:
Midterm Review. Calculus Derivative relationships d(sin x)/dx = cos x d(cos x)/dx = -sin x.
Principles of Groundwater Flow
Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Basic Governing Differential Equations CEE 331 June 12, 2015.
Basic Governing Differential Equations
Theory of Groundwater Flow
Monroe L. Weber-Shirk S chool of Civil and Environmental Engineering Basic Governing Differential Equations CEE 331 July 14, 2015 CEE 331 July 14, 2015.
ESS 454 Hydrogeology Module 3 Principles of Groundwater Flow Point water Head, Validity of Darcy’s Law Diffusion Equation Flow in Unconfined Aquifers &
GRADUALLY VARIED FLOW CVE 341 – Water Resources
8. Permeability (Das, chapter 7)
Ground Water Hydrology Introduction
LINTON UNIVERSITY COLLEGE SCHOOL OF CIVIL ENGINEERING
Stream Function Definitions
Прикладная Гидрогеология Tomsk Polytechnic University Tomsk, Russian Federation Spring Semester 2014 Yoram Eckstein, Ph.D. Fulbright Professor 2013/2014.
Hydrology & Water Resources Engineering
CHAPTER SEVEN Groundwater
Cross Section of Unconfined and Confined Aquifers
9. Seepage (Das, chapter 8) Sections: All except 8.2, 8.6, 8.7, 8.8, 8.9.
Lecture Notes Applied Hydrogeology
Theory of Groundwater Flow
Darcy’s Law and Flow CIVE Darcy allows an estimate of: the velocity or flow rate moving within the aquifer the average time of travel from the head.
Water Supply and Treatment. Average Precipitation.
FLOW NETS Bernoulli's Equation Elevation Head, m Fluid Pressure Head, m Velocity Head, m water travels very slowly through soil as opposed to channel flow.
Groundwater pumping to remediate groundwater pollution March 5, 2002.
Lecture 20 Ground Water (3) Ground water movement
Principles of Groundwater Flow
Basic Hydraulics: Channels Analysis and design – I
Darcy’s Law Philip B. Bedient Civil and Environmental Engineering Rice University.
Final Project I. Calibration Drawdown Prediction Particle Tracking
SI and English Units SI: - Mass = kilogram - Length = meter
CE 3354 Engineering Hydrology
Groundwater Flow Equations Groundwater Hydraulics Daene C. McKinney.
Groundwater Systems D Nagesh Kumar, IISc Water Resources Planning and Management: M8L3 Water Resources System Modeling.
Flow Through A Small Orifice. Velocity can be predicted at the orifice using the Bernoulli equation between points 1 & 2. Notice that u 1 at the surface.
CHAPTER 3 SUB-SURFACE DRAINAGE THEORY
1 Permeability. 2 Soil Permeability- Definition It is a property of soil that allows the flow of fluid through its interconnected void space OR It is.
Chapter1:Static pressure in soil due to water.
Groundwater Flow Equations and Flow Nets
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.
Groundwater Learning objectives
Flow in Aquifers – 1 Confined Aquifer Flow
Darcy’s Law and Richards Equation
Principles of Groundwater Flow
Flow to Wells – 2 Steady flow to a well in an unconfined aquifer
Lecture 20 Ground Water (3) Ground water movement
Aquifers and Groundwater flow
Weir Prevent flooding Measure discharge River navigation River Canal Weir or barrage.
Steady flow in a confined aquifer
Contaminant Transport Equations
Some Quiz Questions Unit: Subsurface Flow.
Finite Difference Method
Groundwater withdrawal and recharge (steady state situation)
Groundwater hydraulics – wells – lectures 7
Groundwater hydraulics – lecture 8
Copyright © 2012, Elsevier Inc. All rights Reserved.
Some Quiz Questions Unit: Subsurface Flow.
Find: hmax [m] L hmax h1 h2 L = 525 [m]
Chapter 2 Equations & Numerical Methods
Chapter Four RUNOFF When a storm occurs, a portion of rainfall infiltrates into the ground and some portion may evaporate. The rest flows as a thin sheet.
Presentation transcript:

Derivation of the Dupuit Equation - Unconfined Flow

Dupuit Assumptions For unconfined ground water flow Dupuit developed a theory that allows for a simple solution based off the following assumptions: 1) The water table or free surface is only slightly inclined 2) Streamlines may be considered horizontal and equipotential lines, vertical 3) Slopes of the free surface and hydraulic gradient are equal

Derivation of the Dupuit Equation Darcy’s law gives one-dimensional flow per unit width as: q = -Kh dh/dx At steady state, the rate of change of q with distance is zero, or d/dx(-Kh dh/dx) = 0 OR (-K/2) d2h2/dx2 = 0 Which implies that, d2h2/dx2 = 0

Dupuit Equation Integration of d2h2/dx2 = 0 yields h2 = ax + b Where a and b are constants. Setting the boundary      condition h = ho at x = 0, we can solve for b b = ho2 Differentiation of h2 = ax + b allows us to solve for a, a = 2h dh/dx And from Darcy’s law, hdh/dx = -q/K

Dupuit Equation So, by substitution h2 = h02 – 2qx/K Setting h = hL2 = h02 – 2qL/K Rearrangement gives q = K/2L (h02- hL2) Dupuit Equation Then the general equation for the shape of the parabola is h2 = h02 – x/L(h02- hL2) Dupuit Parabola However, this example does not consider recharge to the aquifer.

Cross Section of Flow q

Adding Recharge W - Causes a Mound to Form Divide

Dupuit Example Example: 2 rivers 1000 m apart K is 0.5 m/day average rainfall is 15 cm/yr evaporation is 10 cm/yr water elevation in river 1 is 20 m water elevation in river 2 is 18 m Determine the daily discharge per meter width into each River.

Example L = 1000 m Dupuit equation with recharge becomes h2 = h02 + (hL2 - h02) + W(x - L/2) If W = 0, this equation will reduce to the parabolic Equation found in the previous example, and q = K/2L (h02- hL2) + W(x-L/2) Given: L = 1000 m K = 0.5 m/day h0 = 20 m hL= 28 m W = 5 cm/yr = 1.369 x 10-4 m/day

Example For discharge into River 1, set x = 0 m q = K/2L (h02- hL2) + W(0-L/2) = [(0.5 m/day)/(2)(1000 m)] (202 m2 – 18 m2 ) + (1.369 x 10-4 m/day)(-1000 m / 2) q = – 0.05 m2 /day The negative sign indicates that flow is in the opposite direction From the x direction. Therefore, q = 0.05 m2 /day into river 1

Example For discharge into River 2, set x = L = 1000 m: q = K/2L (h02- hL2) + W(L-L/2) = [(0.5 m/day)/(2)(1000 m)] (202 m2 – 18 m2 ) + (1.369 x 10-4 m/day)(1000 m –(1000 m / 2)) q = 0.087 m2/day into River 2 By setting q = 0 at the divide and solving for xd, the water divide is located 361.2 m from the edge of River 1 and is 20.9 m high

Flow Nets - Graphical Flow Tool Q = KmH / n n = # head drops m= # streamtubes K = hyd cond H = total head drop

Flow Net in Isotropic Soil Portion of a flow net is shown below Y Stream tube F Curvilinear Squares

Flow Net Theory Streamlines Y and Equip. lines  are . Streamlines Y are parallel to no flow boundaries. Grids are curvilinear squares, where diagonals cross at right angles. Each stream tube carries the same flow.

Seepage Flow under a Dam