Lecture 9.5 & 10 Storage in confined aquifers Specific storage & storage coefficient.

Slides:



Advertisements
Similar presentations
Yhd Subsurface Hydrology
Advertisements

Groundwater Hydraulics Daene C. McKinney
Groundwater Flow Equations
Principles of Groundwater Flow
Yhd Soil and Groundwater Hydrology
Chapter Four Fluid Dynamic
Chapter 16 Kruseman and Ridder (1970)
Aquifer Tests in Unconfined Aquifers Lauren Cameron Spring 2014.
Conductivity Testing of Unsaturated Soils A Presentation to the Case Western Reserve University May 6, 2004 By Andrew G. Heydinger Department of Civil.
STABILITY ANALYSIS IN PRESENCE OF WATER Pore pressures Rainfall Steady state flow and transient flow.
Unsaturated Flow Governing Equations —Richards’ Equation.
ESS 454 Hydrogeology Module 2 Properties of Materials Basic Physics Darcy’s Law Characteristics of Aquifers Elasticity and Storage Instructor: Michael.
Ground-Water Flow and Solute Transport for the PHAST Simulator Ken Kipp and David Parkhurst.
Continuum Equation and Basic Equation of Water Flow in Soils January 28, 2002.
Subsurface Air Flow Air is a fluid (but not a liquid) that behaves similarly to water We see pressure changes in the subsurface due to barometric pressure.
General governing equation for transient, heterogeneous, and anisotropic conditions Specific Storage S s =  V / (  x  y  z  h)
Lecture 7 & 8 Refraction of q Equivalent K for fractured media.
ME 221Lecture 141 ME 221 Statics Lecture #14 Sections 4.1 – 4.2.
Subsurface Hydrology Unsaturated Zone Hydrology Groundwater Hydrology (Hydrogeology )
Analytical and Numerical Solutions are affected by: Differences in conceptual model (confined vs unconfined) Dimensionality (1D vs 2D) Numerical Solutions.
CE 230-Engineering Fluid Mechanics Lecture # 18 CONTINUITY EQUATION Section 5.3 (p.154) in text.
Review Of Basic Hydrogeology Principles. Types of Terrestrial Water Groundwater SoilMoisture Surface Water.
Lecture 4 Pressure variation in a static fluid N.S. Equations & simple solutions Intro DL.
1 Thermodynamics of Interfaces And you thought this was just for the chemists...
An example moving boundary problem Dry porous media Saturated porous media x = 0 x = s(t) h(0) = L Fixed Head If water head remains at fixed value L at.
Figure from Hornberger et al. (1998) Darcy’s data for two different sands.
Datum h A = total head W.T. )h = h A - h B W.T. Impervious Soil pervious Soil h B = total head Seepage Through Porous Media.
BIOPLUME II Introduction to Solution Methods and Model Mechanics.
GROUNDWATER HYDROLOGY II WMA 302 Dr. A.O. Idowu, Dr. J.A. Awomeso and Dr O.Z. Ojekunle Dept of Water Res. Magt. & Agromet UNAAB. Abeokuta. Ogun State Nigeria.
Chapter II Isentropic Flow
AQUIFERS AND THEIR CHARACTERISTICS
Unit 01 : Advanced Hydrogeology Review of Groundwater Flow Malcolm Reeves Civil and Geological Engineering.
Baseflow Recession Q0.
Cross Section of Unconfined and Confined Aquifers
1 4 Geology and Groundwater Introduction –Geology complexities are reflected in hydrogeology –Geology is the basis for any groundwater investigation Topics.
CE 394K.2 Hydrology Infiltration Reading AH Sec 5.1 to 5.5 Some of the subsequent slides were prepared by Venkatesh Merwade.
Lecture Notes Applied Hydrogeology
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.

Aquifer Storage Properties CVEG 5243 Ground Water Hydrology T. Soerens.
Example (a) What head is supplied to the turbine when Q = 8 ft3/s?
Contaminant Transport CIVE 7332 Lecture 3. Transport Processes Advection The process by which solutes are transported by the bulk of motion of the flowing.
AE 2350 Lecture Notes #6 April 19, 1999 We have studied... Meaning of Incompressible Flow How and why speed of the flow affects compressibility Streamlines.
Lecture 15 Soil Water (2) Soil Water Movement (1) Concept of Hydraulic Head Soil moisture Characteristics Darcy’s Law Infiltration.
Groundwater Jeopardy What is primary porosity? Porosity between grains
CHAPTER SEVEN INTRODUCTORY WELL HYDROLOGY. GROUNDWATER OCCURRENCE.
ATM 301 Lecture #7 (sections ) Soil Water Movements – Darcy’s Law and Richards Equation.
Lecture 20 Ground Water (3) Ground water movement
CE 3354 Engineering Hydrology Lecture 21: Groundwater Hydrology Concepts – Part 1 1.
How does groundwater flow ? February 26, TOC  Definitions  Groundwater flow overview Equipotentials and flowlines  Wells  Laplace  Boundary.
SI and English Units SI: - Mass = kilogram - Length = meter
CE 3354 Engineering Hydrology
Settlement and Consolidation CHAPTER 4. §4 Settlement and Consolidation § 4.1 General § 4.2 Oedometer test § 4.3 Preconsolidation pressure § 4.4 Consolidation.
Groundwater Flow Equations Groundwater Hydraulics Daene C. McKinney.
Groundwater Systems D Nagesh Kumar, IISc Water Resources Planning and Management: M8L3 Water Resources System Modeling.
Water Resources Assessment Main Resources – Surface water – Groundwater – Unconventional Tools – Flood routing/delineation models – Runoff models – GIS.
The First Law of Thermodynamics
CHAPTER 2 MASS BALANCE and APPLICATION
Groundwater Review Aquifers and Groundwater Porosity
Darcy’s Law: Q = KA(–dh/dl)
Flow in Aquifers – 1 Confined Aquifer Flow
Darcy’s Law and Richards Equation
Principles of Groundwater Flow
Example Estimate the average drawdown over an area where 25 million m3 of water has been pumped through a number of uniformly distributed wells.
Contaminant Transport Equations
Transport Modeling in Groundwater
Determine the storage coefficient
Determine the storage coefficient
Chapter 2 Equations & Numerical Methods
Transport Modeling in Groundwater
Presentation transcript:

Lecture 9.5 & 10 Storage in confined aquifers Specific storage & storage coefficient

Storage in confined aquifers & 1-D flow equation

Moisture distribution & water retention curve Water pressure is GT atmospheric Pores remain full Where would the water come from ?

Examine storage changes in a finite element in a confined aquifer Consider the shown element ( size Δx, Δy, Δz ) This element contains a mass of water M = ρ φ Δx Δy Δz Change in water mass dM = d(ρ φ Δx Δy Δz ) = Δx Δy d(ρ φ Δz ) Or dM = Δx Δy [Δz φ d(ρ) + ρ d(φ Δz )]

Change in mass due to water compressibility dM = Δx Δy [Δz φ d(ρ) + ρ d(φ Δz )] Define water compressibility Relate β to dρ ρ= m/Vfor constant mass dρ = -m/V 2 dV Therefore dρ/ρ = -dV/V Use in equation for β to get dρ = ρ β dP

Change in mass due to aquifer compressibility dM = Δx Δy [Δz φ d(ρ) + ρ d(φ Δz ) ] substituting dM = Δx Δy [Δz φ ρ β dP + ρ α p φΔz dP ] Define bulk volume compressibility Relate α to d(φΔz) Vp (pores) = φΔz ΔxΔy d (φΔz) = α p φΔz dP

Storage/ confined aquifer dM = Δx Δy Δz ρ φ [ β + α p ] dP dM / ρ = dV = (Δx Δy Δz) φ [ β + αp ] dP dV/V = φ [ β + αp ] dP = φ [ β + αp ] dh * γ Specific storage or storativity [1/L]

Specific storage & storage coefficient S volume of water released per unit aquifer volume per unit decline in head Can define S c if the aquifer have a constant thickness B = S B S c volume of water released per unit aquifer area per unit decline in head (analogus to S y )

Flow in confined aquifers

Flow equation Darcy law Mass balance (1-d flow) ROMA= net mass flux in notice units Volume/time/volume 3d flow

The governing equation is obtained by using DL in CE

If the confined aquifer has a constant thickness then we can integrate over the vertical neglecting vertical flow (h not h(z)): Define new parameters (i.e. storage coef & transmissivity) The resulting equation w/out source term is:

For homogeneous isotropic aquifer with constant thickness the GPDE is For axisymmetric problems:

Air flow in porous media

Air flow through porous media The applicable form of Darcy law is : Neglecting gravity and considering 1-D flow in x-d : Therefore mass flow rate is:

Example (Bear, 1972 page 192)