03-presentation_basic groundwater hydraulics

Upload: franklinaraya3

Post on 03-Apr-2018

236 views

Category:

Documents


0 download

TRANSCRIPT

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    1/46

    1

    11

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    2/46

    2

    3-2

    this topic we will study the concepts of groundwater flow in aermeable or semi-permeable medium.

    What is an aquiferWhat are aquicludes and aquitards?Definition of hydraulic head.Hydraulic parameters that control saturated groundwater flowSteady state flow and non-steady state (transient) flow.

    The assumptions that are made in (use of) the governingequations.Flownets, equipotentials and groundwater flowlines.

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    3/46

    3

    3-3

    Basic hydraulic parameters and termsBasic hydraulic parameters and terms

    Aquifers, aquicludes and aquitards. Hydraulic head Hydraulic gradient Hydraulic conductivity Permeability

    Transmissivity Porosity Confined and unconfined aquifers Specific yield Sy for Unconfined Aquifers Specific storage Ss and Storativity for Confined Aquifers

    Water table Phreatic surface Confined aquifer - Potentiometric surface Steady and Non-steady State Flow

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    4/46

    4

    3-4

    What is an Aquifer?What is an Aquifer?

    An aquifer is a geological unit that carries water and can be

    exploited economically for water supply or can be drained usingpumping wells. Typically aquifers are areally extensive butpermeable fractured rock systems that we see in somemining environments are normally limited in area and depth.

    There is no clear definition of an aquifer in terms of its hydraulicconductivity it is somewhat arbitrary. However it is clear thatin most cases in mining we are not dealing with aquifers.

    A more formal definition is provided in Freeze and Cherry.

    There an aquifer is defined as a saturated permeable geologicunit that can transmit significant quantities of water underordinary hydraulic gradients.

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    5/46

    5

    3-5

    What is an Aquifer? (2)What is an Aquifer? (2)

    In most (but certainly not all) mining cases we are notdealing with true aquifers but with low permeability media,typically fractured rock which does not act as a true porousmedium for which most groundwater flow theory is developed.

    Some exceptions that can be encountered in a mining contextare alluvium overlying the mine, limestones, highly fractured andextensive hard rock systems, coal beds, gravels (in gravel pits),

    etc.

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    6/46

    6

    3-6

    AquicludesAquicludes andand AquitardsAquitards

    An aquiclude is a saturated geological unit that is incapableof transmitting significant quantities of water under ordinaryhydraulic gradients.

    An aquitard is defined as a low permeability unit within ageologic sequence that may be significant in a regionalsense but does not transmit water on a local scale.

    VERY VAGUE DEFINITIONS!!

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    7/46

    7

    3-7

    Components of Hydraulic HeadComponents of Hydraulic Head

    Hydraulic HeadHydraulic Head

    FigurefromFreeze&Cherry.Groundwater

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    8/46

    8

    3-8

    Illustration of Hydraulic HeadIllustration of Hydraulic Head

    Ground surface

    Water Table elevation = 1800 msnm hydraulic head = 1800m

    elevation head = 1800m

    pressure head = 0

    hydraulic head = 1800m

    Elevation = 1200 msnm elevation head = 1200m

    pressure head = 600m

    Datum = sea level = 0 msnm

    1 kPa = 0.102 m of water

    1m of water = 9.804 kPa

    1psi = 2.3 ft of water = 0.704m of water

    Conversion factors

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    9/46

    9

    3-9

    Hydraulic GradientHydraulic Gradient

    The head difference between two points over a horizontal

    distance. Groundwater flows as a result of this hydraulicgradient.

    Hydraulic gradient = (h1-h2)

    L

    h1 h2

    L

    Confined aquifer

    Note: Definition the same for unconfined aquifer

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    10/46

    10

    3-10

    Permeability & Hydraulic ConductivityPermeability & Hydraulic Conductivity

    (Related to water) a permeable medium is one through which water will

    flow under the influence of a hydraulic gradient. There are two definedparameters - Hydraulic Conductivity and Intrinsic Permeability.

    Intrinsic permeability can be referred to as permeability but HydraulicConductivity should not be referred to a permeability although it often is.

    Intrinsic permeability k is a property of the medium, independent of thefluid.

    Hydraulic conductivity relates k to density and dynamic viscosity ofthe fluid and gravitational constant g.

    K (hydraulic conductivity) = kg/

    Hydraulic conductivity is an integral parameter in Darcys Law andother groundwater flow equations.

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    11/46

    11

    3-11

    Derivation of Hydraulic ConductivityDerivation of Hydraulic Conductivity

    DARCY'S LAW for steady-state flow

    For flow Q in a cross-section of Area = A

    With hydraulic gradient i= Dh/Dx

    Q = KiA

    Where K = Hydraulic Conductivity

    Units SI units

    Q m3/d

    i

    A m2

    so k m/d

    L2

    L3/L

    2T = L/T

    x

    Dimensions

    L3/T

    dimensionless

    This relationship is analagous to those governing heattransfer and flow of electricity. Also note that Hydraulic

    Conductivity K has units of L/T but it IS NOT a velocity.

    Groundwater flow velocity depends upon the porosity ofthe medium in which it flows.

    (v = Ki/where is porosity)

    Qin

    Qout

    h

    Cross-sectional Area = A

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    12/46

    12

    3-12

    Hydraulic Conductivity Values for Different Materials

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    13/46

    13

    3-13

    Controls on Fracturing and Permeability ofControls on Fracturing and Permeability of

    Rock MassRock Mass

    Structure Depth Lithology Alteration Mineralization Secondary effects from Blasting and Unloading

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    14/46

    14

    3-14

    TransmissivityTransmissivity

    AND:Alternate form of Darcy's Law Q = KiA is Q = Tiw

    where i = (h1-h2)/L

    Aquifer with Hydraulic Conductivity K, Width w,

    and thickness b

    TRANSMISSIVITY T = Kb (the product of hydraulicconductivity x aquifer thickness per unit width of

    aquifer.)

    b

    w

    h1 h2

    h

    L

    Groundwater flow

    through element

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    15/46

    15

    3-15

    PorosityPorosity

    Porosity is the percentage of void space within a soil or rock,typically denoted as or n.

    However not all voids are connected and so we talk ofInterconnected Porosity. Of this the majority of the void spacecan be drained under gravity, and this term is called SpecificYield Sy. The part that cannot be drained is called SpecificRetention Sr

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    16/46

    16

    3-16

    Unconfined & Confined AquifersUnconfined & Confined Aquifers

    Flowingwell

    Piezometric surface

    FigurefromJohnsonScreensGroundwater&Wells

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    17/46

    17

    3-17

    Specific Yield (from unconfined aquifer)Specific Yield (from unconfined aquifer)

    Specific Yield Sy of an unconfined aquifer is the volume ofwater released from storage per unit area per unit decline inhead. It is dimensionless.

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    18/46

    18

    3-18

    StorativityStorativity of Confined Aquiferof Confined Aquifer

    The storativity S of a confined aquifer is the volume of waterreleased from storage per unit area per unit decline inpressure head. It is dimensionless.

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    19/46

    19

    3-19

    Specific Storage (Elastic Storage)Specific Storage (Elastic Storage)

    The volume of water released from storage in a unit volume ofconfined aquifer for a unit decline in head. Specific Storage,Ss is related to porosity and compressibility of the systemmatrix and of water by the equation

    Ss= g(+)

    where is the density of water, gis acceleration due to gravity, is the porosity of the rock, is the compressibility of the

    matrix framework and is the compressibility of water.

    Dimensions of Specific Storage are 1/L, typical range is from1 x 10-4 to 5 x 10-7 m-1

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    20/46

    20

    3-20

    Storage andStorage and StorativityStorativity

    FigurefromFreeze&CherryGroundwater

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    21/46

    21

    3-21

    PhreaticPhreatic Surface andSurface and PotentiometricPotentiometric SurfaceSurface

    Direction of groundwater flow

    (piezometric)

    FigurefromFreeze&CherryGroundwater

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    22/46

    22

    3-22

    Groundwater Flow VelocityGroundwater Flow Velocity

    Dimensions of Hydraulic conductivity are L/T (e.g m/d).

    However it is NOT a velocity.

    Darcys Law is stated as Q = KiA

    Dimensions for Hydraulic Conductivity should correctly beshown as L3/T/L2 (e.g) m3/d/m2 .

    In reality A is a unit area (e.g. m2) through which water flows

    only within the pore space . It can be deduced thereforethat flow velocity should be estimated by

    v = Ki////

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    23/46

    23

    3-23

    Groundwater Flow VelocityGroundwater Flow Velocity

    FigurefromFreeze&CherryGroundwater

    Think of Darcys Law, Q moving uniformly, obviously actual velocity is faster toproportion of porosity AND, higher K pathways flow faster.

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    24/46

    24

    3-24

    Hydraulic Conductivity and Groundwater FlowHydraulic Conductivity and Groundwater Flow

    We see how Hydraulic Conductivity is a controlling factor in groundwaterflow, along with hydraulic gradient and flow area. Clearly the flow in asystem is limited by the lowest overall K, i and A.

    Plan view

    EdgeSection

    K1 K2 K3

    Possible pressure surface

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    25/46

    25

    3-25

    Steady and Non SteadySteady and Non Steady--State Groundwater FlowState Groundwater Flow

    Steady-state flow occurs when the magnitude and directionof the flow velocity is constant with time at any point in theflow field.

    Non-Steady State (transient) flow occurs when the magnitudeand direction of the flow velocity changes with time at any pointin the flow field.

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    26/46

    26

    3-26

    Steady and Non SteadySteady and Non Steady--State Groundwater FlowState Groundwater Flow

    Qzout

    Qyout

    Qxin Qxout

    y

    Qyin

    Qzin

    z

    x

    For Steady State Flow:

    /x(Kx

    h/x) + /y(Ky

    h/y) + /z(Kz

    h/z) = 0

    For Transient (non-steady state) Flow

    ((((/x(Kxh/x) + /y(Kyh/y) + /z(Kzh/z) = Ssh/t + Q

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    27/46

    27

    3-27

    r2

    h2 h1

    Then, Q 2T(h2-h1)

    ln(r2/r1)

    r1

    If there are two observation wells at radii R1 and R2, and where

    piezometric heads are h1 and h2 respectively

    THEIM Equation for Steady State Flow to a well

    Usual constraints re aquifer continuity, etc.

    Then by applying Darcy's Law, Q = kiA which is the same as Q

    = k x dh/dr x 2rm

    =2Ts

    ln(r2/r1)

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    28/46

    28

    3-28

    Note that as the volume of water thatis drawn towards a pumping wellremainsconstant it is logical that the cross-section area through which it passesis reduced.

    It therefore follows from Darcys Lawthat the hydraulic gradient must

    increase as the water nears the well.(see following slide).

    Figurefro

    mJohnsonScreensGroundwater&Wells

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    29/46

    29

    3-29

    Methods for Solving NonMethods for Solving Non--Steady FlowSteady Flow

    Equation to find Hydraulic Conductivity andEquation to find Hydraulic Conductivity and

    Confined Storage (Confined Storage (StorativityStorativity))

    There are a number of solutions to solving the non-steadystate equation to determine the aquifer hydraulic parametershydraulic conductivity and storativity.

    Note that there are many assumptions made in using all ofthese types of solutions, such as: (For most methods) that the aquifer is fully confined,

    The aquifer has uniform thickness and is of infinite arealextent, The aquifer is homogeneous (conductivity and storativity

    does not vary with depth or direction).

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    30/46

    30

    3-30

    TheisTheis Equation for Solving NonEquation for Solving Non--Steady FlowSteady Flow

    EquationEquation

    Q r2S

    4T 4Tts = W(u) where u =

    W(u) is an exponential integralW(u) = -.5772 ln u + u + u2/2.2! + u3/3.3! + u4/4.4!

    and T = Kd Transmissivity(hydraulic conductivity x aquifer thickness).Q = flowrate,s = drawdown.t = elapsed time

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    31/46

    31

    3-31

    TheisTheis Equation for NonEquation for Non--Steady Groundwater FlowSteady Groundwater Flow

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    32/46

    32

    3-32

    FunctioningFunctioning TheisTheis SpreadsheetSpreadsheet

    Spreadsheet with THEIS solution to find s (drawdown) for combinations of Q, kD, t, r and S

    Q

    (m3/d)

    kD

    (m2/d)

    Time

    t

    (day)

    Radius

    r (m)S u W(u) s (m)

    200 1000 100 500 0.0001 6.25E-05 9.1025 0.1449

    ONLY CHANGE VALUES IN YELLOW CELLS MAX u!

    9

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    33/46

    33

    3-33

    CooperCooper--Jacob Approximation ofJacob Approximation of TheisTheis EquationEquation

    for Solving Nonfor Solving Non--Steady Flow EquationSteady Flow Equation

    We have seen that the Theis solution is

    or s = Q/4T(-.5772 ln u + u + u2/2.2! + u3/3.3! + u4/4.4! )

    for large values of t or small values of r the value of u becomes negligible

    so that the series can be rewritten as s = Q/4T x (-.5772 ln r2S/4Tt)

    In decimal logarithms this becomes s = (2.3Q/4T)log(2.25Tt/r2S),Then T = 2.3Q/4s

    Plot graph of drawdown against log time (see next slide), determine sand estimate T

    For data from an observation well it is possible to derive storativity S

    S = 2.25 Tt0/r2

    Qr2S

    4T 4Tts = W(u) where u =

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    34/46

    34

    3-34

    Jacob PlotJacob Plot Drawdown per Log CycleDrawdown per Log Cycle

    Decenso in Pozo de Bombeo Z1

    15

    16

    17

    18

    19

    20

    100 1000 10000

    Tiempo (minutos)

    Decenso(m)

    s = drawdown per log cycle = 2.3m

    Time (minutes)

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    35/46

    35

    3-35

    The Effect of Varying Hydraulic Parameters onThe Effect of Varying Hydraulic Parameters on

    Depressurization EffectsDepressurization Effects

    FigurefromFreeze&CherryGroundwater

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    36/46

    36

    3-36

    EquipotentialEquipotential SurfacesSurfaces

    Surface joining points of equal hydraulic head

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    37/46

    37

    3-37

    EquipotentialsEquipotentials and Flow in Uniformand Flow in Uniform

    MediumMedium

    FigurefromFreeze&CherryGroundwater

    equipotential

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    38/46

    38

    3-38

    Groundwater Flow Patterns Close toGroundwater Flow Patterns Close to

    BoundariesBoundaries

    FigurefromFreeze&CherryGroundwater

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    39/46

    39

    3-39

    Steady State andSteady State andTransient FlowTransient Flow

    FigurefromFreeze&CherryGroundwater

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    40/46

    40

    3-40

    SimpleSimple FlownetFlownet ExampleExample

    FigurefromFreeze&CherryGroundwater

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    41/46

    41

    3-41

    Variations in Hydraulic ConductivityVariations in Hydraulic Conductivity

    FigurefromFreeze&CherryGroundwater

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    42/46

    42

    3-42

    Effects of Anisotropy on Hydraulic HeadEffects of Anisotropy on Hydraulic Head

    DistributionDistribution

    FigurefromFreeze&CherryGroundwater

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    43/46

    43

    3-43

    Flow System from Recharge Area toFlow System from Recharge Area to

    Discharge AreaDischarge Area

    FigurefromFreeze&CherryGroundwater

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    44/46

    44

    3-44

    Unconfined AquiferUnconfined Aquifer Flow to a WellFlow to a Well

    FigurefromFreeze&CherryGroundwater

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    45/46

    45

    3-45

    Flow to Well in aFlow to Well in aConfined AquiferConfined Aquifer

    FigurefromFreeze&CherryGroundwater

  • 7/28/2019 03-Presentation_Basic Groundwater Hydraulics

    46/46

    3-46

    Flow Towards an Open PitFlow Towards an Open Pit

    FigurefromFreeze&CherryGroundwater