bfc21103 chapter1

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BFC21103 Hydraulics Chapter 1. Flow in Open Channel Tan Lai Wai, Wan Afnizan & Zarina Md Ali [email protected] Updated: February 2015

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hydraulics : Types of flow in open channel

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  • BFC21103Hydraulics

    Chapter1.FlowinOpenChannel

    TanLaiWai,WanAfnizan&[email protected]

    Updated:February2015

  • LearningOutcomes

    Attheendofthischapter,studentsshouldbeableto:

    i. Defineandexplainontypesandstatesofflowinopenchannels

    ii. Identifytypesofopenchannels

    iii. Defineopenchannelgeometries

    BFC21103HydraulicsTanetal.([email protected])

  • Openchannelflowisflowofaliquidinaconduitwithafreesurfacesubjectedtoatmosphericpressure.

    Examples:flowofwaterinrivers,canals,partiallyfullsewers anddrainsandflowofwateroverland.

    Freesurface

    Flow

    Datum x

    y

    uyA

    B

    T

    Figure.Sketchofopenchannelgeometry

    BFC21103HydraulicsTanetal.([email protected])

  • StormwaterManagementandRoadTunnel(SMART),KualaLumpur,Malaysia

    Tahanriverrapids

    Siberianmeanderingriver

  • Comparisonbetweenpipeflowandopenchannelflow

    Channelbottom

    Watersurface

    Datumline

    1 2

    V1

    V2

    Energyline

    y1

    y2

    z2

    hf

    gV2

    22

    z1

    gV2

    21

    Centerlineofpipe

    Hydraulicgradeline

    Datumline

    1 2

    V1

    V2

    Energyline

    y1

    y2

    z2

    hf

    gV2

    22

    z1

    gV2

    21

  • Practicalapplicationsofopenchannelflowstudies:

    a. flowdepthinrivers,canalsandotherconveyanceconduits,

    b. changesinflowdepthduetochannelcontrolse.g.weirs,spillways,andgates,

    c. changesinriverstageduringfloods,

    d. surfacerunofffromrainfalloverland,

    e. optimalchanneldesign,andothers

    BFC21103HydraulicsTanetal.([email protected])

  • 1.1FlowParametersandGeometricElementsa. Depthofflowy istheverticalmeasureofwaterdepth.

    Normaldepthd ismeasurednormaltothechannelbottom.

    d =y cosFormostapplications,d y when 10%,e.g.cos1 =0.9998.

    Freesurface

    FlowQ

    Datum x

    y d

    So =bottomslope

    Sw =watersurfaceslope

    BFC21103HydraulicsTanetal.([email protected])

  • b. Flow ordischargeQ isthevolumeoffluidpassingacrosssectionperpendiculartothedirectionofflowperunittime.

    MeanvelocityV isthedischargedividedbythecrosssectionalarea

    AQ

    V =

    BFC21103HydraulicsTanetal.([email protected])

  • c.WettedperimeterP isthelengthofchannelperimeterthatiswettedorcoveredbyflowingwater.

    A=crosssectionalareacoveredbyflowingwater

    B=bottomwidth

    T=topwidth

    AP

    y

    BFC21103HydraulicsTanetal.([email protected])

  • BFC21103HydraulicsTanetal.([email protected])

    d. HydraulicradiusR istheratiooftheflowareaA towettedperimeterP.

    B

    T

    AP

    y

    PA

    R =

    e. HydraulicdepthD istheaveragedepthofirregularcrosssection.

    TA

    D ==widthtopareaflow

  • ChannelsectionAreaA

    TopwidthT

    WettedperimeterP

    By B B +2y

    Table.Openchannelgeometries

    y

    B

    T

    Rectangular

    yz

    T

    Triangular

    1 zy2 2zy212 zy +

    By+zy2 B +2zy 212 zyB ++yz

    T

    Trapezoidal

    1

    B

    y

    T

    Circle

    2D( ) sin22

    8

    2

    D DsinD

  • BFC21103HydraulicsTanetal.([email protected])

    Find:

    (a) TopsurfacewidthT,flowareaA,wettedperimeterP,andhydraulicradiusR.

    (b) IfQ =2.4m3/s,determinethestateofflow.

    (c) IflongitudinallengthL =50m,findthecosttoconstructthechannel.Givenexcavationcost=RM3/m3 andliningcost=RM5/m2.

    Activity1.1

    3m

    2m

    1m

    60

  • BFC21103HydraulicsTanetal.([email protected])

    5774.060tan1 == oz

    zyBT 2+=( )( )25774.023+=Tm309.5=T

    212 zyBP ++=( ) 25774.01223 ++=Pm619.7=P

    2zyByA +=( ) ( )225774.023 +=A

    2m309.8=A

    PA

    R =

    619.7309.8=R

    m091.1=R

    (a) TopsurfacewidthT,wettedareaA,wettedperimeterP andhydraulicradiusR.

  • BFC21103HydraulicsTanetal.([email protected])

    (b) IfQ =2.4m3/s,determinethestateofflow.

    m/s2888.0309.84.2 ===

    AQ

    V

    gDV=Fr

    VR=Re

  • (c) IfthelengthofthechannelisL =50m,findthecosttoconstructthechannel.Givenexcavationcost=RM3/m3 andliningcost=RM5/m2.

    Volumeofexcavation LA = channel( ) 5035774.033 2 +=

    3m81.709=

    Costofexcavation = costUnit 81.709m/3RM 3 =42.2129RM=

    BFC21103HydraulicsTanetal.([email protected])

  • Areaoflining LPA = channellining ( ) 505774.01323 2lining ++=A3

    lining m41.496=A

    Costoflining liningcostUnit A= 41.496m/5RM 2 =05.2482RM=

    Totalcost 05.2482RM42.2129RM += 611.474RM=

    BFC21103HydraulicsTanetal.([email protected])

  • BFC21103HydraulicsTanetal.([email protected])

    Find:

    (a) FlowareaA

    (b) WettedperimeterP

    (c) HydraulicradiusR

    Activity1.2

    3m4m2m1m

    2m

    2m

    1m A1

    A2 A3A4

  • BFC21103HydraulicsTanetal.([email protected])

    1.2TypesofOpenChannel

    Prismatic andnonprismatic channelsPrismaticchannel isthechannelwhichcrosssectionalshape,sizeandbottomslopeareconstant.Mostofthemanmade(artificial)channelsareprismaticchannelsoverlongstretches.Examplesofmanmadechannelsareirrigationcanal,flume,drainageditches,roadsidegutters,drop,chute,culvertandtunnel.

    Allnaturalchannels generallyhavevaryingcrosssectionsandthereforearenonprismatic.Examplesofnaturalchannelsaretinyhillsiderivulets,throughbrooks,streams,riversandtidalestuaries.

  • BFC21103HydraulicsTanetal.([email protected])

    Rigid andmobileboundary channelsRigidchannels arechannelswithboundariesthatisnotdeformable.Channelgeometryandroughnessareconstantovertime.Typicalexamplesarelinedcanals,sewersandnonerodibleunlinedcanals.

    Mobileboundarychannels arechannelswithboundariesthatundergodeformationduetothecontinuousprocessoferosionanddepositionduetotheflow.Examplesareunlinedmanmadechannelsandnaturalrivers.

  • BFC21103HydraulicsTanetal.([email protected])

    Canalsisusuallyalongandmildslopedchannelbuiltintheground,whichmaybeunlinedorlinedwithstonedmasonry,concrete,cement,woodorbituminousmaterial.

    GriboyedovCanal,St.Petersburg,Russia

    TerusanWanMuhammadSaman,Kedah

  • BFC21103HydraulicsTanetal.([email protected])

    ThisflumedivertswaterfromWhiteRiver,Washingtontogenerateelectricity BullRunHydroelectricProjectdiversionflume

    Flumesisachannelofwood,metal,concrete,ormasonry,usuallysupportedonorabovethesurfaceofthegroundtocarrywateracrossadepression.

  • BFC21103HydraulicsTanetal.([email protected])

    Openchannelflumeinlaboratory

  • BFC21103HydraulicsTanetal.([email protected])

    Chuteisachannelhavingsteepslopes.

    Naturalchute(falls)ontheleftandmanmadeloggingchuteontherightontheCoulongeRiver,Quebec,Canada

  • BFC21103HydraulicsTanetal.([email protected])

    Dropissimilartoachute,butthechangeinelevationiswithinashortdistance.

    ThespillwayofLeasburgDiversionDamisaverticalhardbasindropstructuredesignedtodissipateenergy

  • BFC21103HydraulicsTanetal.([email protected])

    Stormwatersewerisadrainordrainsystemdesignedtodrainexcessrainfrompavedstreets,parkinglots,sidewalksandroofs.

    Stormdrainreceivingurbanrunoff

    Stormsewer

  • BFC21103HydraulicsTanetal.([email protected])

    1.3TypesandClassificationofOpenChannelFlows

    Openchannelflow

    Steadyflow Unsteadyflow

    Uniformflow Nonuniformflow

    GraduallyvariedflowRapidlyvariedflow

    Varioustypesofopenchannelflow

  • BFC21103HydraulicsTanetal.([email protected])

    Openchannelflowconditionscanbecharacterisedwithrespecttospace (uniformornonuniformflows)andtime (steadyorunsteadyflows).

    Space howdotheflowconditionschangealongthereachofanopenchannelsystem.

    a.Uniformflow depthofflowisthesameateverysectionoftheflowdy/dx =0

    b.Nonuniformflow depthofflowvariesalongtheflowdy/dx 0

  • BFC21103HydraulicsTanetal.([email protected])

    a.Uniformflow

    b.Nonuniformflowy1

    y2 Depthchangesalongthechannel

    y y Constantwaterdepthx

    Depthofflowisthesameateverysectionalongthechannel, 0dd =xy

    Depthofflowvariesatdifferentsectionsalongthechannel, 0dd xy

  • BFC21103HydraulicsTanetal.([email protected])

    Time howdotheflowconditionschangeovertimeataspecificsectioninanopenchannelsystem.

    c.Steadyflow depthofflowdoesnotchange/constantduringthetimeintervalunderconsiderationdy/dt =0

    d.Unsteadyflow depthofflowchangeswithtimedy/dt 0

  • BFC21103HydraulicsTanetal.([email protected])

    c.Steadyflow

    d.Unsteadyflow

    y1

    Time=t1

    y2

    Time=t2

    y1

    t3

    t2t1

    Depthofflowisthesameateverytimeinterval, 0dd =ty

    Depthofflowchangesfromtimetotime, 0dd ty

    y1 =y2

    y1 y2 y3

  • BFC21103HydraulicsTanetal.([email protected])

    Theflowisrapidlyvaried ifthedepthchangesabruptlyoveracomparativelyshortdistance.Examplesofrapidlyvariedflow(RVF)arehydraulicjump,hydraulicdrop,flowoverweirandflowunderasluicegate.

    Theflowisgraduallyvaried ifthedepthchangesslowlyoveracomparativelylongdistance.Examplesofgraduallyvariedflow(GVF)areflowoveramildslopeandthebackingupofflow(backwater).

  • BFC21103HydraulicsTanetal.([email protected])

    RVF RVFGVF RVFGVF RVFGVF

    Sluice

    Hydraulicjump

    Flowoverweir

    Hydraulicdrop

    Contractionbelowthesluice

  • BFC21103HydraulicsTanetal.([email protected])

    1.4StateofFlowThestateorbehaviourofopenchannelflowisgovernedbasicallybytheviscosity andgravityeffects relativetotheinertialforces oftheflow.

    Effectofvisco sity dependingontheeffectofviscosityrelativetoinertialforces,theflowmaybeinlaminar,turbulent,ortransitional state.

    Reynoldsnumber representstheeffectofviscosityrelativetoinertia,

    VR=Re

    whereV isthevelocity,R isthehydraulicradiusofaconduitand isthekinematicviscosity(forwaterat20C, =1.004 106 m2/s,dynamicviscosity =1.002 103 Ns/m2 anddensity =998.2kg/m3).

  • BFC21103HydraulicsTanetal.([email protected])

    Re

  • BFC21103HydraulicsTanetal.([email protected])

    Effectofgravity dependingontheeffectofgravityforcesrelativetoinertialforces,theflowmaybesubcritical,criticalandsupercritical.

    Froudenumber representstheratioofinertialforcestogravityforces,

    gDV=Fr

    whereV isthevelocity,D isthehydraulicdepthofaconduitandg isthegravityacceleration(g =9.81m/s2).

  • BFC21103HydraulicsTanetal.([email protected])

    Fr1 ,theflowisinsupercriticalstate

    gDV

  • BFC21103HydraulicsTanetal.([email protected])

    1.5RegimesofFlow

    Acombinedeffectofviscosityandgravitymayproduceanyoneofthefollowingfourregimesofflowinanopenchannel:

    a. subcritical laminar ,whenFr12500

    d. subcritical turbulent ,whenFr12500

  • BFC21103HydraulicsTanetal.([email protected])

    Assignment#1

    Q1. [FinalExamSemI,Session2010/2011]Justifythedifferencebetween:(a) uniformflowandnonuniformflow(b) stateofflowusingReynoldsnumberReandFroudenumberFr.

    Q2. [FinalExamSemI,Session2008/2009](a) Define

    (i) Wettedperimeter(ii) Graduallyvariedflow(iii) Nonuniformflow(iv) Froudenumber

    (b) Explainthedifferencesbetweencanalandsewer.

  • BFC21103HydraulicsTanetal.([email protected])

    Q3. [FinalExamSemI,Session2006/2007]Define(a) Reynoldsnumber(b) Froudenumber(c) Hydraulicradius(d) Prismaticchannel(e) Uniformflow

    Q4. Adischargeof16.0m3/sflowswithadepthof2.0minarectangularchannelof4.0mwide.Determinethestateofflowbasedon(a) Froudenumber,and(b) Reynoldsnumber.

  • BFC21103HydraulicsTanetal.([email protected])

    Q5. Atriangularchannelofapexangle120 carriesadischargeof1573L/s.Calculatethecriticaldepth.

    EndofQuestion

    1.2m

    1.5m

    32 1.2m

    1.5m

    0.3m

    Q6. FindT,A,P,R,andD forthefollowingcompoundsections.

  • THANKYOU

    BFC21103HydraulicsTanetal.([email protected])