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  • 5/26/2018 BLT1110 Hydraulics Notes

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    Hydraulics BLT1110

    Module Notes

    John Pickering & Rob Eggleton

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    Hydraulics Module Notes

    TABLEOFCONTENTS

    Hydralic!""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""#S$ %nit!"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""'a!! and (eight""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""")*i+en!ion!""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""")Linear, con!tant acceleration""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""")*i+en!ional Ho+ogeneity"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""-.Pre!!re"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""-.Frictional Shear Stre!!"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""-.Pro/ertie! o0 Flid!""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""--Coe00icient o0 *yna+ic 1i!co!ity 2 345 +6""""""""""""""""""""""""""""""""""""""""""""""""""""""""--

    5ine+atic 1i!co!ity345 n6""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""--

    Flid Flo7"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""--$ntrodction to Flid 'echanic!"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""-8

    The La7! o0 Hydro!tatic!"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""-8Pre!!re 'ea!re+ent""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""-9

    Ab!olte and 4age Pre!!re"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""-9Pre!!re Head""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""-9The 'ercry Baro+eter"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""-9The Aneroid Baro+eter""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""-:The *ead7eight Pi!ton 4age""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""-:The Bordon 4age"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""-:Pre!!re Tran!dcer!""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""-:

    The Pie;o+eter Tbe"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""-:The %a+/le! ? Pre!!re 'ea!re+ent""""""""""""""""""""""""""""""""""""""""""""""""""""""-@Ttorial e!tion! ? Pre!!re 'ea!re+ent""""""""""""""""""""""""""""""""""""""""""""""""""""""-)Stability and Boyancy o0 Floating Bodie!"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""8.

    Archi+ede! Princi/le""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""8.*eter+ination o0 'etacentric Height, '4""""""""""""""""""""""""""""""""""""""""""""""""""""""""8-

    (orked E>a+/le! < Boyancy"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""88Ttorial e!tion! < Boyancy"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""89Hydro!tatic Force! on Sb+erged Sr0ace!"""""""""""""""""""""""""""""""""""""""""""""""""""""""8:

    'o+ent o0 a Force, Rotation and Eilibri+"""""""""""""""""""""""""""""""""""""""""""""""""""""8=(orked E>a+/le! ? Hydro!tatic Force!""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""8@Ttorial e!tion! ? Hydro!tatic Force!""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""8)

    Hydrodyna+ic! ? Flid! in 'otion"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""9.Ty/e! o0 Flo7"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""9.*eter+ination o0 La+inarTrblent Flo7 ? Reynold! N+ber, Re""""""""""""""""""""9.Analy!i! o0 Flid Flo7""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""9-(orked E>a+/le! < Continity"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""98Ttorial e!tion! ? Continity """""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""98

    (ork, Energy and E00iciency"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""99

    (ater Energy"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""994raDitational or Potential Energy"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""99Energy Head""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""9:

    Pre/ared Jne 8..# Page 8 o0 .

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    5inetic Energy""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""9:Pre!!re Energy""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""9:Energy Lo!!e!"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""9:

    Frictional Energy Lo!!""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""9:'inor Energy Lo!!e!""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""9=

    The Energy BernolliG Eation""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""9=(orked E>a+/le! ? Energy""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""9@Ttorial e!tion! ? Energy""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""9#Flo7 'ea!re+ent in /i/eline!"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""9'o+ent+ Eation""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""9)

    Jet $+/act on a Stationary Flat Plate"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""9)Jet $+/act on a Stationary CrDed 1ane"""""""""""""""""""""""""""""""""""""""""""""""""""""""""9)Force! on a Pi/e Bend""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""":.Force! on a Pi/e Contraction or No;;le"""""""""""""""""""""""""""""""""""""""""""""""""""""""""":.Thr!t Block!"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""":.

    (orked E>a+/le! ? 'o+ent+"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""":-

    Ttorial e!tion! ? 'o+ent+"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""":8Friction Lo!! in Pi/eline! """""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""":9

    The *arcya+/le! ? %ni0or+ Channel Flo7""""""""""""""""""""""""""""""""""""""""""""""""""""""""@9Ttorial e!tion! ? %ni0or+ Channel Flo7""""""""""""""""""""""""""""""""""""""""""""""""""""""""@@Non

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    Fnction! and Ty/e!""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""#8Po!itiDe *i!/lace+ent P+/!"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""#8Rotodyna+ic P+/!""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""#9Ty/e! o0 Rotodyna+ic P+/!"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""#9

    Centri0gal P+/! lo7 , high HG"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""#9

    A>ial Flo7 P+/! high , lo7 HG""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""#:'i>ed Flo7 P+/!"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""#:'lti!tage P+/!"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""#:

    P+/ Per0or+ance Characteri!tic! CrDe!G""""""""""""""""""""""""""""""""""""""""""""""""""""""#=Centri0gal P+/ CrDe!"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""#=A>ial Flo7 P+/ CrDe!""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""#='i>ed Flo7 P+/ CrDe""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""#=Other Characteri!tic CrDe!"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""#@

    Hydro Po7er Trbine!"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""#@Franci! Trbine"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""#@A>ial Flo7 Trbine""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""##

    Pelton (heel Trbine"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""#Se7age P+/ing Station Layot!"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""#)

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    L$STOFF$4%RES

    Figre - Flid Flo7""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""--Figre 8 Pre!!re 1ariation7ith *e/th""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""-8Figre 9 Pre!!re in Connected Flid!"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""-8Figre : 4age Pre!!re Scale""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""-9Figre = 'ercry Baro+eter""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""-9Figre @ Aneroid Baro+eter""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""-:Figre # *ead7eight Pi!ton 4age"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""-:Figre Bordon 4age"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""-:Figre ) Pre!!re Tran!dcer"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""-:Figre -. aG Pie;o+eter bG 'ano+eter 7ith Secondary 4age Flid""""""""""""""-=Figre -- *i00erential 'ano+eter""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""-=Figre -8 (orked P"'" E>a+/le -""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""-@

    Figre -9 Soltion 0or P"'" E>a+/le -""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""-@Figre -: (orked P"'" E>a+/le 8""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""-#Figre -= (orked P"'" E>a+/le 9""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""-Figre -@ P"'" Ttorial e!tion! Figre!""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""-)Figre -# Boyancy Force""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""8.Figre - Eilibri+ Condition!"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""8-Figre -) Hydro!tatic Force on Sb+erged Sr0ace""""""""""""""""""""""""""""""""""""""""""""8:Figre 8. 'o+ent o0 Force"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""8=Figre 8- (orked E>a+/le H"F" -""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""8@Figre 88 (orked E>a+/le H"F" 8""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""8#Figre 89 (orked E>a+/le H"F" 9""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""8#

    Figre 8: (orked E>a+/le H"F" 9 Soltion""""""""""""""""""""""""""""""""""""""""""""""""""""""""""8Figre 8= (orked E>a+/le H"F" 9 Soltion 'o+ent!G""""""""""""""""""""""""""""""""""""""""8Figre 8@ H"F" Ttorial e!tion! """"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""8)Figre 8# Flo7 Continity""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""9-Figre 8 (orked E>a+/le! Continity""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""98Figre 8) (ork < *irected Force"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""99Figre 9. Pre!!re Energy""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""9:Figre 9- Bernolli Energy *iagra+"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""9=Figre 98 (orked E>a+/le! E" -""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""9@Figre 99 (orked E>a+/le! E" 8""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""9#Figre 9: Jet $+/act on Stationary Flat Plate"""""""""""""""""""""""""""""""""""""""""""""""""""""""9)

    Figre 9= Jet $+/act on a Stationary CrDed 1ane""""""""""""""""""""""""""""""""""""""""""""""9)Figre 9@ Force! on a Pi/e Bend"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""":.Figre 9# Force! on a Pi/e Contraction"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""":.Figre 9 (orked E>a+/le! '" -""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""":-Figre 9) (orked E>a+/le! '" 8""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""":8Figre :. (orked E>a+/le! *"E""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""::Figre :- Pi/eline *e!ign Table""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""":@Figre :8 Table o0 'inor Lo!!e!""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""":Figre :9 Entry to a Pi/e""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""":)Figre :: Sdden $ncrea!e in Pi/e *ia+eter""""""""""""""""""""""""""""""""""""""""""""""""""""""":)Figre := Sdden *ecrea!e in Pi/e *ia+eter""""""""""""""""""""""""""""""""""""""""""""""""""""""=.Figre :@ Bend!, Elbo7!, and Tee Jnction!"""""""""""""""""""""""""""""""""""""""""""""""""""""""=.Figre :# *iDergent Ta/er or *i00!er"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""=-

    Pre/ared Jne 8..# Page = o0 .

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    Figre : Partially Clo!ed 1alDe!""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""=8Figre :) E>it 0ro+ a Pi/e into a re!erDoir""""""""""""""""""""""""""""""""""""""""""""""""""""""""""=8Figre =. E>it 0ro+ a Pi/e to at+o!/here"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""=9Figre =- (orked E>a+/le! '"L" -""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""=:Figre =8 (orked E>a+/le! '"L" 8""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""==

    Figre =9 (orked E>a+/le! '"L" 9""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""=@Figre =: %ni0or+ Flo7"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""=)Figre == Nona+/le! %"C"F" -"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""@9Figre @. (orked E>a+/le! %"C"F" 8"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""@9Figre @- (orked E>a+/le! %"C"F" 9"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""@:Figre @8 (orked E>a+/le! %"C"F" :"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""@=Figre @9 Hydralic J+/""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""@#

    Figre @: J+/ Eation *iagra+""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""@Figre @= Broad Cre!ted (eir Figre @@ Rond Cre!ted (eir""""""""""""""""""""""""""@Figre @= Broad Cre!ted (eir Figre @@ Rond Cre!ted (eir""""""""""""""""""""""""""@Figre @# 1ial Flo7 P+/""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""#:Figre # 'i>ed Flo7 P+/""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""#:Figre #) Centri0gal P+/ Characteri!tic CrDe!"""""""""""""""""""""""""""""""""""""""""""""""#=Figre . A>ial Flo7 P+/ Characteri!tic CrDe!""""""""""""""""""""""""""""""""""""""""""""""""#=Figre - 'i>ed Flo7 P+/ Characteri!tic CrDe""""""""""""""""""""""""""""""""""""""""""""""""#=Figre 8 *e!ign Point CrDe"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""#@Figre 9 Fa+ilie! o0 Characteri!tic CrDe!"""""""""""""""""""""""""""""""""""""""""""""""""""""""""#@Figre : Franci! Trbine"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""#@

    Figre = A>ial Flo7 Trbine"""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""##Figre @ Pelton (heel Trbine""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""""#Figre # Se7age P+/! < A>ial and 'i>ed Flo7""""""""""""""""""""""""""""""""""""""""""""""""#)Figre Se7age P+/! < Centri0gal and Sb+er!ible"""""""""""""""""""""""""""""""""""".

    Pre/ared Jne 8..# Page @ o0 .

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    Hydraulics Module Notes

    Hydraulics

    Hydralic! 30ro+ the 4reek 7ord 0or 7ater6 i! the !tdy o0 the /roble+! o0 the 0lo7

    and !torage o0 7ater, bt i! o0ten a//lied to other liid!"

    Flid +echanic! i! the !ection o0 a//lied +echanic! concerned 7ith the !tatic! anddyna+ic! o0 liid! and ga!e!"

    A 0lid can o00er no re!i!tance to any 0orce ca!ing change o0 !ha/e"

    Change o0 !ha/e i! ca!ed by !hearing 0orce!"

    $0 a 0lid i! at re!t there are no !hear 0orce! acting"

    Flid! +ay be either liid! or ga!e!"

    A liid i! di00iclt to co+/re!! and occ/ie! a 0i>ed Dol+e"

    A ga! i! ea!ily co+/re!!ed and e>/and! to 0ill any De!!el"

    Pre/ared Jne 8..# Page # o0 .

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    Hydraulics Module Notes

    SI Units

    The Sy!te+e $nternational ha! !i> ba!ic nit!

    length metre (m)

    +a!! kilogramme (kg)

    ti+e second (s or sec)

    electric crrent ampere (A)

    ab!olte te+/eratre kelvin (k)

    l+ino! inten!ity candela (cd)

    All other nit! are deriDed 0ro+ the!e 0nda+ental nit!"

    The nit o0 Delocity i! obtained by diDiding the nit o0 di!tance, the +etre, by thenit o0 ti+e, the !econd, and i! th! +etre! /er !econd"

    The relation!hi/ bet7een +a!! and 0orce i! deriDed 0ro+ Ne7ton! !econd la7+aking the con!tant o0 /ro/ortionality eal to oneG"

    FORCE I 'ASS ACCELERAT$ON

    The nit o0 0orce i! a /rodct o0 +a!! and acceleration"

    kg3+!ec86 I Ne7ton

    Other !y!te+! e>i!t

    0ootPre/ared Se/te+ber 8..= Page o0 .

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    Hydraulics Module Notes

    ass and !eig"t

    The 7eight o0 a body i! the 0orce 7ith 7hich it i! attracted to7ard! the earth" $0 abody 0all! 0reely then, neglecting air re!i!tance, it! acceleration i! con!tant" Thi!acceleration i! denoted by Kg and i! called the Kacceleration de to graDity"

    i"e" (eight ( I +g 7here + i! +a!!

    N"B" $0 +a!! +G i! +ea!red in kg and g in +!8, then ( i! +ea!red in NNe7tonG"

    #imensions

    $n +echanic! all antitie! can be e>/re!!ed in ter+! o0 0nda+ental di+en!ion!

    +a!!

    length L

    ti+e T

    th! acceleration $ distance % time&

    there0ore dimensions o' acceleration $ L % T&

    and 'orce $ L % T&

    Linear constant acceleration

    e"g", acceleration de to graDity

    $0 a body 7ith initial Delocity !/eedG K ndergoe! con!tant acceleration Ka 0or ti+eKt to bring it to a 0inal Delocity KD oDer a di!tance K! then

    -G

    Frther, the ( )vuspeedaverage &1 += and tspeedaveragetravelleddistance =

    th! ( )tvus &1 += 8GSb!titting 0or D 0ro+ -G into 8G giDe!

    9G

    Pre/ared Jne 8..# Page ) o0 .

    atuvt

    uv

    timeinc"ange

    speedinc"angea +=

    == or

    ( ) &&

    1

    &

    1 atutstatuus +=++= or

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    =

    Hydraulics Module Notes

    Sb!titting 0or t 0ro+ -G into 8G giDe!

    i"e", &asuvuv&as &&&& +== or :G

    #imensional Homogeneity

    $0 an eation i! to re/re!ent !o+ething real then ter+! on both !ide! +!t haDethe !a+e di+en!ion! !o that like i! co+/ared 7ith like"

    e"g" v $ u at

    di+en!ion! o0 D are LT*1

    di+en!ion! o0 are LT*1

    di+en!ion! o0 at are LT*&+ T $LT*1

    Note that !o+e /ractical 0or+lae do not a//ear to be di+en!ionally correct" Therea!on i! that a coe00icient +ay not be a /re n+ber" E"g", g +ay be 7ritten a!)"- bt ha! the nit! LT*&"

    ,ressure

    The 7eight o0 the block acting on an area KA o0 the !r0ace /rodce! a /re!!re K/on that !r0ace, 7here

    Pre!!re

    i"e", /re!!re i! 0orce nit area

    -rictional S"ear Stress

    Shear 0orce!, !ch a! 0riction, /rodce a !hear !tre!! on the area oDer 7hich

    they act, 7here

    !hear !tre!! 8+N

    A

    F

    area

    0orce!hear==

    Pre/ared Jne 8..# Page -. o0 .

    (

    Area KA

    /

    F

    Area KA

    ( ) ( ) auvvus&

    1 +=

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    Hydraulics Module Notes

    ,roperties o' -luids

    ASS #./SIT 345 rho6 i! +a!! /er nit Dol+e, nit! kg+9

    S,.I-I !.I2HT7 i! the 7eight /er nit Dol+e, nit! N+9

    7eight I +a!! > graDitational accelerationgw =

    S,.I-I 23A4ITor relatiDe den!ity i! the ratio o0 the den!ity o0 a!b!tance to the den!ity o0 7ater"

    N"B" den!ity o0 7ater, w I -... kg+9

    den!ity o0 +ercry, m I -9@.. kg+9

    den!ity o0 dry air, a I -"9 kg+9at NTP

    oe''icient o' #ynamic 4iscosity 5 627 mu8

    The coe00icient o0 dyna+ic Di!co!ity i! de0ined a! the s"ear 'orce % unit areareired to drag one layer o0 0lid 7ith nit Delocity /a!t another layer nit di!tancea7ay 0ro+ it in the 0lid"

    skg%mms/unitsSI & or

    7inematic 4iscosity 627 nu8The kine+atic Di!co!ity i! the ratio o0 dyna+ic Di!co!ity to +a!! den!ity"

    C!ec+nit!8

    =

    1i!co!ity o0 liid! decrea!e! 7ith increa!e in te+/eratre"

    1i!co!ity o0 ga!e! increa!e! 7ith increa!e in te+/eratre"

    -luid -lo9

    A! 0lid! 0lo7 along /i/e! or channel!, the 0lid /article!ne>t to the bondary /i/e 7all or channel bedG are held atre!t by 0riction" Thi! generate! internal !hearing 0rictionG0orce! bet7een the layer! o0 0lid a! they !lide oDer oneanother" The Di!co!ity o0 a 0lid deter+ine! the rate at7hich it! /article! can !lide oDer one another nder a giDen!hear !tre!!"

    -igure 1 : -luid -lo9

    i;e;

    =

    dy

    dv

    Th! a KDelocity gradient e>i!t!, /er/endiclar to the direction o0 0lo7"

    Pre/ared Jne 8..# Page -- o0 .

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    Hydraulics Module Notes

    Introduction to -luid ec"anics

    T"e La9s o' Hydrostatics

    -" *irection o0 Force at a Bondary

    (hen a 0lid i! at re!t, no 0riction !hearG 0orce e>i!t! at it! bondarie!"Hence, any 0orce e>erted by the 0lid on a bondary or i++er!ed obect+!t act in a direction nor+al /er/endiclarG to that bondary and beinde/endent o0 Di!co!ity"

    8" 1ariation o0 Pre!!re $nten!ity 7ith *irection

    The /re!!re inten!ity at a /oint in a 0lid ha! the !a+e +agnitde in alldirection!"

    9" 1ariation o0 Pre!!re $nten!ity 7ith *e/th

    $t i! co++on kno7ledge that the /re!!re in a liidincrea!e! 7ith de/th" Con!ider the Derticaleilibri+ o0 the cylinder o0 0lid !ho7n, i0 the areao0 the end i! A then

    -igure & : ,ressure 4ariation9it" #ept"

    7here atI at+o!/heric /re!!re /!hing do7n on the !r0ace o0 the 7ater

    No7 AhggvolumegmW ===

    hence AatpghApA +=

    i"e", atpghp +=

    th! /re!!re increa!e! linearly 7ith de/th"

    :" Pre!!re in Connected Flid!

    The /re!!re along any hori;ontal line MM 7ill be the !a+e +agnitde in eachar+ o0 the De!!el /roDiding the 0lid i!the !a+e"

    -igure < : ,ressure in onnected -luids

    Pre/ared Jne 8..# Page -8 o0 .

    0== AatpWpAyR

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    Hydraulics Module Notes

    ,ressure easurement

    Absolute and Gauge Pressure

    -igure = : 2auge ,ressure Scale

    N"B" Ab!olte ;ero /re!!re I /er0ect Dac+G

    Ab!olte Pre!!re /ab!I /at gh$n /ractice, /re!!re i! +ea!red relatiDe to at+o!/heric /re!!re, a! gage/re!!re"

    4age Pre!!re / I /ab!? /atI gh

    N"B, NegatiDe gage /re!!re I !b/re!!ed

    in ter+! o0 the height h o0 a col+n o0 0lid den!ity, G reired to /rodce that/re!!re regardle!! o0 ho7 the /re!!re i!, in 0act, /rodcedG"

    The nit o0 +ea!re+ent i! then +etre! +G and the /re!!re i! e>/re!!ed inter+! o0 K+etre! head o0 0lid" E"g", K+etre! head o0 7ater or K+etre! head o0+ercry"

    The Mercury Barometer

    A gla!! tbe abot -+ long i! 0illed 7ith +ercryand then inDerted in a bo7l o0 +ercry" AboDe the+eni!c! +ercry Da/or 0or+! at Da/or /re!!re

    0or +ercry, 7hich i! al+o!t ab!olte ;ero /re!!re"The at+o!/heric /re!!re acting on the !r0ace o0the +ercry in the bo7l !//ort! a col+n o0+ercry in the tbe o0 height h" Pre!!re at A leDel7ith liid !r0aceG I /re!!re on liid !r0ace Iat+o!/heric /re!!re, /at" 1ertical eilibri+ o0the +ercry col+n reire! that

    Pre!!re 0orce acting /7ard! at A I 7eight o0+ercry aboDe A

    -igure > : ercury Barometer

    Pre/ared Jne 8..# Page -9 o0 .

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    Hydraulics Module Notes

    i"e", /at> a I +gah /atI +gh

    7here a I bore o0 tbe +I den!ity o0 +ercry

    At+o!/heric /re!!re Darie! abot a +ean Dale o0 /atI -.-kN+8" E>/re!!ing

    thi! a! a /re!!re head it i! ."#@+ o0 +ercry or -."9=+ o0 7ater"

    The Aneroid Barometer

    The 0le>ible cha+ber i! eDacated, bt/reDented 0ro+ colla/!ing by the !/ring"1ariation! in at+o!/heric /re!!re ca!e thebo> to +oDe in or ot !o that the /ll o0 the!/ring I 0orce de to at+o!/heric /re!!re"The!e +oDe+ent! are a+/li0ied +echanicallyand +oDe a /ointer oDer a calibrated !cale"

    -igure ? : Aneroid Barometer

    The Deadweight Piston Gauge

    The /re!!re at A in the 0lid i! +ea!red by balancing it7ith 7eight! acting on the /i!ton" Thi! a//arat! i! +ainly!ed to calibrate other ty/e! o0 gage!"

    -igure @ : #ead9eig"t ,iston 2auge

    The Bourdon Gauge

    The crDed tbe o0 0lattened cro!! !ection i! held rigidly atone end 7ith the 0ree end connected to a /ointer" (hen

    /re!!re i! ad+itted to the tbe it tend! to !traighten" The+oDe+ent o0 the 0ree end ca!e! the /ointer to rotate oDera gradated !cale"

    -igure : Bourdon 2auge

    Pressure Transducers

    Flid i! ad+itted to the !+all cha+ber on one !ide o0 thedia/hrag+" Change! in /re!!re re!lt in change! in the!tre!! and con!eently the electrical re!i!tance o0 thedia/hrag+" The re!i!tance change i! +ea!red on a digitalDolt+eter and calibrated 7ith the /re!!re change"

    -igure : ,ressure Transducer

    N"B" The dead7eight /i!ton gage, Bordon gage and /re!!re tran!dcer!+ea!re Kgage /re!!re"

    The Piezometer Tube

    The /re!!re / in the /i/eline !//ort! a col+n o0 liid height h in the Derticaltran!/arent tbe" The /re!!re i! th! +ea!red directly in +etre! head

    / I h +etre! o0 liid I gh N+8, 7here I den!ity o0 liid kg+9G

    Pre/ared Jne 8..# Page -: o0 .

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    Hydraulics Module Notes

    -igure 10 : (a) ,ieCometer (D) anometer 9it" Secondary 2auge -luid

    N"B" The /ie;o+eter i! o/en to the at+o!/here and +ea!re! gage /re!!re"Thi! i! tre 0or all +ano+eter!"

    The U-tube Manometer

    Thi! !e! a !econdary gage liid, den!er than the 0lid in the /i/eline" Thi! i!nece!!ary

    iG 7hen the /i/eline 0lid i! a ga! 7hich 7old e!ca/e 0ro+ a /ie;o+eter and7old not 0or+ a +eni!c!G

    iiG 7hen h 7old be too large 7ithot the introdction o0 a +ch den!er gage0lid, e"g" 7ater or alcohol 0or air, and +ercry 0or 7ater in the /i/eline"

    The /re!!re at leDel > i! the !a+e in both tbe!" i"e", />I / Agy I Bgy

    Hence / I Bgh < Agy N+8

    The Differential Manometer

    Thi! allo7! the /re!!re di00erence bet7een t7o/oint! in a /i/eline to be +ea!red"

    N"B" B A" $0 BQ Athen the +ano+eter

    +!t be inDerted" $t i! then kno7n a! an KinDerted%

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    !orked .+amples E ,ressure easurement

    -" For the !itation! !ho7n in Figre -8"

    aG $0 the /i/eline and +ano+eter 0lid den!itie! are [email protected]+9and +I [email protected]+

    9re!/ectiDely, > I .")+and the /re!!re at i! ). kN+8, 0ind the di00erence in+eni!c! leDel!, h"

    bG For the !a+e 0lid den!itie! a! in aG, bt 7ith > I-"9+ and h I -":+, 0ind the /re!!re at "

    -igure 1& : !orked ,;; .+ample 1

    Solution:

    aG *ra7 a dat+ leDel M ? M throgh the lo7er+eni!c!" The /re!!re at leDel M ? M 7ill be the !a+e inboth li+b! o0 the % ? tbe +ano+eter" See Figre -9"

    For the right

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    8" For the !itation !ho7n in Figre -:, i0 the /i/elineand +ano+eter 0lid den!itie! are I --..kg+9brineGand +I [email protected]+

    9re!/ectiDely, > I ."#+ and the/re!!re at i! ? 9. kN+8, 0ind the di00erence in+eni!c! leDel!, h"

    -igure 1= : !orked ,;; .+ample &

    Solution:

    Note that the right

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    9" For the !itation! !ho7n in Figre -=, i0the /i/eline and +ano+eter 0lid den!itie!are I -...kg+9and +I [email protected]+

    9

    re!/ectiDely, the /re!!re di00erencebet7een ' and N i! 9=kN+8, a I -".+ and

    b I ."9+, 7hat i! the di00erence in +eni!c!leDel!, h

    -igure 1> : !orked ,;; .+ample i! Dertical" *en!ity o0

    !ea 7ater I -.8=kg+9

    G"3'4 I < .":8.+W n!table6

    8" A rectanglar /ontoon -8+ long by #"=+ 7ide by 9+ dee/ ha! a +a!! o0 ).+etric ton! and 0loat! in !ea 7ater I -.8=kg+9 G" The centre o0 graDity o0 the/ontoon i! at the geo+etrical centre" Find the +etacentric height" 39"#)9+6

    9" A rectanglar /ontoon -9"=+ > =":+ > 9".+ high 0loat! in 7ater 7ith the 9".+!ide Dertical" The /ontoon 7eigh! :8.kN and it! centre o0 graDity i! -"8+ aboDe

    the ba!e o0 the /ontoon" Calclate the +etacentric height o0 the /ontoon 7hen0loating in

    a" 0re!h 7aterb" !ea 7ater I -.8=kg+9G

    $n 7hich o0 the!e 0lid! doe! the /ontoon haDe greater !tability

    3a" '4 I 9"898+W b" '4 I 9"98+W !ea 7ater6

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    >

    Hydrostatic -orces on SuDmerged Sur'aces

    So 0ar 7e haDe !een that the /re!!re in a 0lid increa!e! linearly 7ith de/thW

    / I gh

    'ore !ally, 7hen de!igning hydralic !trctre! !ch a! da+!, lock gate!, 0la/DalDe! etc" it i! the re!ltant hydro!tatic 0orce F that i! reired"

    Thi! 0orce F i! the !++ation o0 the /re!!re 0orce! acting on the !b+ergedarea" $t act! at right angle! to the !b+erged !r0ace"

    -igure 1 : Hydrostatic -orce on SuDmerged Sur'ace

    Strctre! +ay be /artially or 7holly !b+erged in the 0lid, ho7eDer there i! ageneral 0or+la 7hich can be !ed to deter+ine the 0orce FW

    (here A i! the !b+erged area, i! the Dertical di!tance 0ro+ the 7ater !r0aceto the centroid o0 the !b+erged area"

    $t i! al!o !e0l to kno7 7here the re!ltant 0orce act! in relation to the 7ater!r0ace" The /oint at 7hich the 0orce act! i! kno7n a! the centre o0 /re!!re"

    Thi! di!tance >/i! +ea!red /arallel to the !b+erged !r0ace and can bedeter+ined 0ro+ the general 0or+la

    (here cgi! the !econd +o+ent o0 area abot the centroid o0 the !b+erged area"

    i! the di!tance 0ro+ the 7ater !r0ace to the centroid o0 the !b+erged area+ea!red /arallel to the !b+erged !r0ace"

    (hen the !b+erged !r0ace i! Dertical X I ).Y, hence !in X I - and

    hRgAF=

    h

    >

    >A

    >cg

    / +

    =

    !inX

    h> =

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    oment o' a -orce 3otation and .GuiliDrium

    A 0orce +ay ca!e not only linear +otion, bt al!orotation o0 a body" Thi! /rinci/le i! !ed in the ca!e o0a leDer !y!te+" The /er!on /!he! do7n 7ith 0orce F,

    ca!ing a load ( to ri!e by rotation abot the /iDot P"

    -igure &0 : oment o' -orce

    The +agnitde o0 F reired to ca!e rotation de/end! on ( and on > and y, theK/er/endiclar di!tance! 0ro+ the 0orce! to the /iDot P" Each 0orce i! !aid to/rodce a K+o+ent abot P"

    i"e", the K+o+ent o0 the 0orce F abot P I F > anticlock7i!eGand the K+o+ent o0 the 0orce ( abot P I ( y clock7i!eGFor anticlock7i!e rotation to take /lace, F > ( y"

    For clock7i!e rotation to take /lace, ( y F >"For Kbalance, Keilibri+ or Kno rotation, F > I ( y"

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    @.Y-"8+

    h

    >>

    /

    a

    2

    ,

    -"=+

    9".+

    !orked .+amples E Hydrostatic -orces

    -" A rectanglar /late -"=+ > 9".+ i! !b+erged in 7ater and +ake! an angle [email protected] 7ith the hori;ontal, the -"=+ !ide! being hori;ontal" Calclate the +agnitde o0

    the 0orce on the /late and the location o0 the /oint o0 a//lication o0 the 0orce, 7ithre0erence to the to/ edge o0 the /late, 7hen the to/ edge o0 the /late i! -"8+belo7 the 7ater !r0ace"

    Solution:

    m88625138615160

    21x ....

    sin

    .=+=+

    =

    m499260886260xh .sin.sin ===

    51349928191000Ahg- ... ==

    N92109N1092109- 3 .. ==

    x12

    dx

    x!d

    1

    12

    !dx

    xA

    $xx

    23,

    . +=+=+=

    m146326008862886212

    3

    8862x

    2

    . ..... =+=+=

    Fro+ the to/ edge o0 the /late, m760138611463a ... ==

    -igure &1 : !orked .+ample H;-; 1

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    8" A Dertical blkhead :+ 7ide diDide! a !torage tank" On one !ide o0 theblkhead /etrol S"4" I ."#G i! !tored to a de/th o0 8"-+ and on the other !ide7ater i! !tored to a de/th o0 -"8+" *eter+ine the re!ltant 0orce on the blkheadand the /o!ition 7here it act!"

    Solution:

    !gh!h2

    hgAhg- 2

    21 ===

    N567N412819780- 221

    1 ... ==

    N2528N4218191000- 221

    2 ... ==

    -igure && : !orked .+ample H;-; &

    Hence the re!ltant 0orce

    N25392528567--- 21/ ... ===

    ( ) h6

    h

    2

    h

    2h!h

    1

    12

    !h

    2

    h

    xA

    $xx

    32

    3,

    . =+=+=+=

    Fro+ the diagra+, x = h 2/3h =1/3h

    Hence, x1= 2.1 / 3 = 0.7mand x2= 1.2 / 3 = 0.4m

    Taking +o+ent! abot O, FRZ>RI F-Z>-? F8Z>8

    i"e" 9)"8= >RI @#"= ."# ? 8"8= .": and hence >RI .")-@+

    9" A hinged, circlar gate #=.++ india+eter i! !ed to clo!e the o/eningin a !lo/ing !ide o0 a tank, a! !ho7nin the diagra+ in Figre 89" The gatei! ke/t clo!ed again!t 7ater /re!!re/artly by it! o7n 7eight and /artly bya 7eight on the leDer ar+" Find the+a!! ' reired to allo7 the gate tobegin to o/en 7hen the 7ater leDel i!=..++ aboDe the to/ o0 the gate"The +a!! o0 the gate i! @. kg"Neglect the 7eight o0 the leDer ar+"G

    -igure &< : !orked .+ample H;-; @..++ rectanglar 0lat /late 7ith the @..++ !idehori;ontalG i! !ed to clo!e the o/ening in a !lo/ing !ide o0 a tank, a! !ho7n

    in Figre 8@*iagra+ 8" The gate i! ke/t clo!ed again!t 7ater /re!!re/artly by it! o7n 7eight and /artly by a 7eight on the leDer ar+" Find the+a!! ' reired to allo7 the gate to co++ence to o/en 7hen the 7aterleDel i! :..++ aboDe the to/ o0 the gate" Neglect the 7eight o0 the leDerar+G" 3898 kg6

    -igure &? : H;-; Tutorial Fuestions

    #iagram 1 #iagram &

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    Hydrodynamics E -luids in otion(hil!t hydro!tatic! i! a relatiDely /reci!e !bect, hydrodyna+ic! can only beanaly!ed 7ith a//ro>i+ate accracy" The rea!on 0or thi! i! that the +otion o0 0lid/article! i! o0ten rando+n/redictable 7hich create! inaccracie! in analy!i!"

    The +aor e00ect i! 0riction bet7een the /i/e 7all and the 0lid 7hich create! aDelocity Dariation acro!! the /i/e dia+eter" Ho7eDer to !i+/li0y +atter! in thi! nitall Delocitie! con!idered 7ill be aDerage Delocitie!, i"e" D I A"

    Types o' -lo9

    Steady 'lo9condition! at a /oint in the 0lo7 !y!te+ re+ain con!tant7ith re!/ect to ti+e"

    Unsteady 'lo9 condition! change 7ith re!/ect to ti+e"

    Uni'orm 'lo9 0lo7 condition! re+ain con!tant 7ith re!/ect to di!tance"

    /on*uni'orm 'lo9 condition! change 7ith re!/ect to di!tance"

    Laminar 'lo90lid /article! retain !a+e relatiDe /o!ition! at!cce!!iDe cro!! !ection!"

    TurDulent 'lo9 0lid /article! 0ollo7 rando+, di!organi!ed /ath!"

    /;B; >K o' real li'e 'lo9s are turDulent;

    #etermination o' Laminar%TurDulent -lo9 E 3eynolds/umDer 3e

    Reynold! recogni!ed that Di!co!ity, aDerage Delocity and the dia+eter o0 the /i/edeter+ined the 0lo7 /attern" He deter+ined the Reynold! N+ber to /redict 0lo7ty/e, 7here

    I aDerage Delocity d I /i/e dia+eter

    2 I coe00icient o0 dyna+ic Di!co!ity I 0lid den!ity

    Re :... and 0lo7 i! trblent

    8... Q ReQ :... and 0lo7 i! tran!itional

    ReQ 8... and 0lo7 i! la+inar

    The +aor di00erence bet7een the t7o 0lo7 /attern! i! that greater 0rictional lo!!e!

    occr in trblent 0lo7"

    -

    8

    9

    = vd

    /&

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    Analysis o' -luid -lo9

    The three ba!ic eation! are

    -G Continity Eation

    8G Energy Eation BernolliG9G 'o+ent+ Eation

    -G Continity Eation

    For continity, the 0lo7 rate entering !ection - +!t be eal to the 0lo7 rateleaDing !ection 8" i"e", -I 8I and

    -I Dol+e!ec I length!ec > area i"e", -I 1-A-and 8I 18A8

    th! I 1-A-I 18A8

    -igure &@ : -lo9 ontinuity

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    !orked .+amples * ontinuity

    A 9..++ dia+eter /i/eline diDide! into t7o !+aller /i/eline!, one being -=.++ india+eter and the other being 88=++ in dia+eter" $0 the Delocity in the -=.++ /i/e

    i! ."=+! and that in the 88=++ /i/e i! ."+!, calclate the 0lo7rate in litre!!and the Delocity in +! in the 9..++ /i/e

    Solution:

    *m10848504

    150vA

    332

    150150150=

    == ..

    .

    *m10831804

    2250vA

    332

    225225225=

    == ..

    .

    ( ) *'t&*6440*m10831848 33

    225150300 ... =+=+=

    *m575030

    1064404

    430

    A

    v

    2

    3

    2

    300

    300

    300300 .

    .

    .

    .=

    =

    ==

    -igure & : !orked .+amples ontinuity

    Tutorial Fuestions E ontinuity

    A 8..++ dia+eter /i/eline diDide! into t7o !+aller /i/eline!, one being -..++ india+eter and the other being -=.++ in dia+eter" $0 the Delocity in the -..++ /i/e

    i! ."9+! and that in the -=.++ /i/e i! ."@+!, calclate the 0lo7rate in litre!!and the Delocity in +! in the 8..++ /i/e" 3-9 l!, .":-9+!6

    1>0mm

    &&>mm

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    !ork .nergy and .''iciency(hen the /oint at 7hich the0orce act! +oDe!, the 0orce i!!aid to haDe done 7ork" The+an +oDing the block ha!done 7ork eal to thecon!tantG 0orce a//lied ti+e!the di!tance he ha! +oDed theblock in the direction o0 thea//lied 0orce"

    -igure & : !ork * #irected -orce

    i"e", (ork done I P! I 0orce > di!tance +oDed K(ork done i! a !calar antity"The nit! are N+ or ole! i"e", - N+ I - oleG"

    A body 7hich ha! the ca/acity to 7ork i! !aid to /o!!e!! energy" A! a body doe!7ork it e>/end! energy e"g", the +an +oDing the blockG" Th!, nit! o0 energy arethe !a+e a! tho!e o0 7ork ole!G"

    There are +any 0or+! o0 energyW e"g", electrical energy, che+ical energy, heatenergy, nclear energy, +echanical energy, etc" ObDio!ly, they all haDe the!a+e nit!" A 0nda+ental la7 o0 /hy!ic! !tate! that energy can be neithercreated nor de!troyed bt can change 0ro+ one 0or+ to another"

    The a+ont o0 energy e>/ended by the +an +oDing the block I (ork done energy 7a!ted" The energy 7a!ted i! +ainly heat generated +oDing the block i!

    a lot o0 7ork[G %100')pt)&gytpt%

    ''&)y =

    i"e", the e00iciency o0 the +an! body in +oDing the block i!

    !ater .nergy

    (ater in a re!erDoir /o!!e!!e! energy !ince it can be !ed to do the 7ork o0driDing a trbine !ally to /rodce electrical energyG" (ater energy i! a+echanical energy and +ay be held by the 7aterG in three 0or+!

    4raDitational or /otential energy

    5inetic energyPre!!re energy

    2ravitational or ,otential .nergy

    $0 a body e"g", o0 7aterG o0 +a!! + i! at a height ; aboDe !o+e arbitraryG dat+,e"g", !ea leDel, then it i! !aid to /o!!e! a Potential energy I +g; ole!G relatiDeto the dat+" Thi! i! the 7ork 7hich +!t be done to rai!e a +a!! + o0 0lid by aheight o0 ; +etre!"

    g&)&at&d&)&gyh&at*.

    *

    +

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    .nergy Head

    Since 0lid! +oDe a! a contin+ rather than a! a di!crete +a!! +, it i!conDenient to con!ider their Kenergy /er nit 7eight or Kenergy head"

    i"e", Potential energy head I +g; +gG I ;

    Hence, energy head ha! the di+en!ion o0 length and i! +ea!red in +etre!"

    7inetic .nergy

    A body e"g", o0 7aterG +ay /o!!e!! energy de to it! +otion! a! 7ell a! it!/o!ition" The kinetic energy o0 a body +ay be de0ined a! the a+ont o0 7ork7hich +!t be done by a 0orce in order to bring it to re!t"

    Let a body o0 +a!! + +oDing 7ith !/eed D be broght to re!t 7ith ni0or+retardation di!tance +oDed!ec

    -igure

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    Minor #nergy $osses

    Other energy lo!!e! occr at /articlar /lace! in the /i/e or channel 7hen theni0or+ 0lid 0lo7 i! interr/ted by bend!, DalDe!, change! in /i/e dia+eter or7hen the 7ater 0lo7! into or or o0 a re!erDoir" The!e energy lo!!e!, ca!ed bythe 0lid !7irling abot and generating heat, are +ch !+aller than the 0rictionalenergy lo!!e!" Hence they are called K+inor head lo!!e!, hL"

    T"e .nergy (Bernoulli) .Guation

    The Ktotal energy head H o0 the 0lid i! 0ond by adding the three ty/e! o0+echanical energy /o!!e!!ed by the 0lid at that /oint"

    A! 7ater 0lo7! bet7een t7o /oint!, or !ection! o0 a /i/eline or channel, no energy

    can be created or de!troyed 0nda+ental la7 o0 /hy!ic! concerning con!erDationo0 energyG" Ho7eDer, i0 any +echanical energy i! conDerted into !ay heat energythrogh 0riction then it i! lo!t to the +echanical !y!te+ and the Ktotal energy headH i! redced"

    The energy head! inDolDed are +ea!red in +etre! and can be re/re!ented a!Dertical di!tance! height!G on an energy diagra+"

    Con!idering 0lo7 bet7een 8 /oint! labelled - and 8

    or

    -igure

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    !orked .+amples E .nergy

    -" Oil S"4" I ."=G at a /re!!re o0 -=. 5N+8 0lo7! at a rate o0 9+9+in throgh/i/e A -..++ dia+eterG" A ta/ered !ection, =+ long, connect! /i/e A to /i/e B

    -=.++ dia+eterG !itated at a di!tance h belo7 /i/e A" $0 the /re!!re in /i/e Bi! -. 5N+8 and the energy lo!! de to 0riction throgh the ta/ered !ection i!."-8++ length, deter+ine the di!tance h"

    Solution:

    *m3766010

    34

    410

    603

    4d

    v

    222A

    AA .

    ..=

    =

    =

    =

    *m83260150

    34

    4d

    v

    22+

    +

    +

    ..

    =

    =

    =

    ;+

    2++

    A

    2AA h

    g2

    v

    g

    p

    g2

    v

    g

    p+++

    =++

    -igure

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    8" A =..+ long /i/eline !lo/e! /7ard! at - in =. and change! 0ro+ :=.++ india+eter to 9..++ in dia+eter 9..+ 0ro+ it! lo7er end" $0 the 0rictional headlo!!e! in the /i/e! are -". and #".+k+ length re!/ectiDely and the /re!!re atthe //er end i! -8. 5N+8, 0ind the /re!!re at the lo7er end 7hen the 0lo7 ratein the /i/eline i! -.. l!"

    Solution:

    *m630450

    104

    4450

    10

    4d

    v

    2221

    11 .

    .

    .

    .

    .=

    =

    =

    =

    *m42130

    104

    4d

    v

    22

    2

    22 .

    .

    .=

    =

    =

    -igure

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    -lo9 easurement in pipelines

    There are t7o deDice! 7hich are co++only !ed to +ea!re 0lo7 in /i/e!

    -" The Dentri+eter

    8" The ori0ice +eter

    The Dentri+eter con!i!t! e!!entially o0 a conDergence in a /i/eline 0ollo7ed by a!hort /arallel !ided Kthroat and then a diDergence"

    Continity reire! a greater Delocity at the throat than the inlet, there i!con!eentially a di00erence o0 /re!!re bet7een the inlet and throat and+ea!re+ent o0 thi! /re!!re di00erence allo7! the 0lo7 rate to be calclated"

    The ori0ice +eter 7ork! on a !i+ilar /rinci/al to the Dentri+eter and i! chea/erand !i+/ler to in!tall bt it generate! larger energy lo!!e!" $t con!i!t! o0 a circlardi!c, 7ith an ori0ice +achined in it! centre, 7hich i! ea!ily bolted bet7een /i/e

    length!"

    The 0lo7 rate throgh a 1entri and Ori0ice +eter can be 0ond 0ro+ the eation

    g:2aa

    aa=

    22

    21

    21d

    =

    7here the cro!!

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    omentum .Guation

    (hen a 0orce act! on a 0lid in +otion, there i! a rate o0 change o0 +o+ent+ inthe 0lid in the direction o0 the 0orce, in accordance 7ith Ne7ton! Second La7 o0

    'otion"i"e",

    Thi! eation i! a//lied in Dario! !itation!, inclding the i+/act o0 0lid et! on/late! and Dane! trbine! and /+/!G and the 0orce! occrring on /i/e no;;le!,

    contraction! and bend!"

    %et &mact on a 'tationary "lat Plate

    A//lying the +o+ent+ eation /er/endiclar to

    the /late, F>I D>8?D>-G

    No7, D>8I . ?all 0lo7 a0ter i+/act i! /arallel to the y a>i!"

    D>-I D-co!

    Hence F>I

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    th! ^ I tan

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    !orked .+amples E omentum

    -" A ta/ered !ection in a hori;ontal /i/eline redce! the dia+eter 0ro+ @..++ to:=.++ in the direction o0 0lo7" $0 the 0lo7rate i! #=. l! and the /!trea+ /re!!re

    i! 9.. 5N+8

    , calclateaG the do7n!trea+ /re!!re

    bG the +agnitde and direction o0 the 0orce on the ta/er

    Solution:

    A//lying Ne7ton! 8ndla7 o0 +otion, the re!ltant 0orce on the 7ater in the ta/er,

    ( )122211x vvAp-Ap/ == " F i! the 0orce e>erted by the ta/er on the 7ater"

    Hence, ( )122211 vvApAp- =*m6532

    60

    7504

    4d

    v

    22

    1

    11 .

    .

    .=

    =

    =

    -igure

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    8" A :=.++ dia+eter /i/eline conDeying -". +9! o0 7ater contain! a 88"=Y bendin the hori;ontal /lane" $0 the /re!!re in the bend i! 8=. 5N+8, calclate the+agnitde and direction o0 the 0orce on the bend"

    Solution:

    *m296450

    014

    4d

    v

    22 ..

    .=

    =

    =

    ( )( )+= 5221vpA-x .cos

    ( )N522129601104

    45010250 3

    23

    += .cos...

    ( )( ) ( ) N535221054652212967639 ..cos..cos.. ==+=

    -igure D

    D

    88"=Y

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    gd2

    ;v

    h

    2

    =

    +=

    Re.

    .log

    512

    d73

    2 *

    -riction Loss in ,ipelines

    T"e #arcy*!eisDac" .Guation

    So 0ar 7e haDe e>/re!!ed 0rictional head lo!! in +etre!+etre length 7hen!b!titting in Bernolli! Eation" The 0ollo7ing detail! a +ore reali!tic 7ay o0a!!e!!ing /i/e 0riction lo!!e!"

    TurDulent -lo9s

    Trblent 0lo7 in /i/e! i! highly co+/le> and cannot be !olDed by +ath! alone"For trblent 0lo7! Ne7ton! La7! o0 1i!co!ity do not a//ly" Reynold!e>/eri+ent! and 7ork by *arcy (ei!bach !ho7ed that 0rictional head lo!! 7a!/ro/ortional to the !are o0 the Delocity" The 0ollo7ing eation 7a! deDelo/ed

    (here h0i! the 0riction head lo!!, L i! the /i/e length, i! the 0lo7 Delocity, d i! the

    /i/e dia+eter, i! the *arcy 0riction 0actor" Note i! di+en!ionle!!" The

    eation i! !o+eti+e! 7ritten 7ith :0 re/lacing , thi! i! the A+erican Der!ion"

    N"B" The head lo!! de to 0riction /er nit length o0 /i/e h0LG i! the hydralic

    gradient iG" Th! i I h0L I 88dg" Thi! 7ill be the gradient o0 the TEL and H4L"

    Th!, 0or a giDen 0lo7 rate, h0-d=, i"e" halDing the !i;e o0 /i/e to be !ed 7ill

    increa!e 0rictional head lo!!e! 98 ti+e!" The head lo!! de to 0riction i! a +lti/le

    LdG o0 the kinetic D88gG, i"e" h0I LdGD88gG"

    Originally it 7a! thoght that 7a! con!tant, ho7eDer, e>/eri+ent! !ho7ed that it

    7a! related to Reynold! N+ber and /i/e roghne!!"

    oleDrook*!"ite -ormula 'or

    The 0ollo7ing eation 0or 7a! deriDed by carrying ot laboratory e>/eri+ent! on

    co++ercial /i/e!" The eation i!

    (here k!i! height o0 /i/e !r0ace roghne!!, d i! the /i/e dia+eter and Re i! theReynold! N+ber o0 the 0lo7"

    $n thi! 0or+at it i! di00iclt to 0ind directly, +odi0ication! 7ere +ade by Barr

    +=

    890* 12865

    d73

    2

    1.

    Re

    .

    .log

    2

    22

    d

    4

    dg2

    ;h

    d

    4

    A

    ===

    ?

    @

    ?

    henceandAl!o,

    5

    2

    5

    2

    2d112

    ;h

    d

    ;

    g2

    16h

    .

    @@

    ?=

    =

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    !orked .+amples E #arcy*!eisDac" .Guation

    A /i/eline connecting t7o re!erDoir! haDing a di00erence o0 leDel o0 @+ i! #8.+long, and ri!e! to a height o0 9+ aboDe the //er re!erDoir at a di!tance o0 8:.+0ro+ the entrance be0ore 0alling to the lo7er re!erDoir" $0 the /i/e i! -8+ in

    dia+eter and the 0rictional coe00icient, $ .".:, 7hat 7ill be the di!charge and the/re!!re at the highe!t /oint o0 the /i/eline

    -igure =0 : !orked .+amples #;.;

    Solution:Figre :.!ho7! the layot" Since no in0or+ation i! giDen that e>it or entry to the/i/e i! !har/ no !hock lo!! need be con!idered" A//ly Bernolli! eation to Aand B on the 0ree !r0ace o0 the re!erDoir, 7here the Delocitie! are ;ero and the/re!!re! at+o!/heric" Take B a! dat+ leDel"

    Total energy /er nit 7t at A $ Total energy /er nit 7t at B 0rictional lo!!

    g2

    v

    d

    ;

    g2

    v

    g

    p0

    g2

    v

    g

    p:

    22++

    2AA ++

    +=+

    +

    /AI /BI . and DAI DBI ., !o thatg2

    v

    d

    ;:

    2=

    Ptting H $ @+, $ .".:, L $ #8.+, d$ -"8+

    g2

    v

    21

    7200406

    2

    .

    . = i"e" 924

    720040

    8192216v2 .

    .

    ..=

    = *m222v .=

    *i!charge I area > Delocity I m5122224

    21 2..

    .=

    9! An!7erG

    To 0ind the /re!!re /Cat C a//ly Bernolli! theore+ to A and C, taking dat+leDel at A and DAI ."

    g2

    v

    d

    ;

    g2

    vh

    g

    p

    g

    p 212

    =A +++

    =

    += d

    ;

    1g2

    v

    hg

    p

    g

    p 12

    A=

    Ptting /AI at+o!/heric /re!!re I ., h I 9+, I .".:, L- I 8:.+, 1 I 8"88+,dI -"8+

    Bat&m26521

    2400401

    8192

    22230

    g

    p 2= ..

    .

    .

    .=

    +

    =

    2

    = mN6512658191000p /... == An!7erG

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    Tutorial Fuestions E #arcy*!eisDac" .Guation

    -" *eter+ine the lo!! o0 head de to 0riction in a ca!t iron /i/e :..+ long and-=.++ in dia+eter 7hich carrie! :9 l!" %!e the *arcy eation 7ith I

    .".8" 3-@".)+68" (hat !i;e o0 /i/e !hold be !ed to deliDer 9. l! o0 7ater throgh a

    di!tance o0 -9..+ i0 the dro/ in the hydralic grade line i! not to e>ceed8=+" Take I .".8=" 3-=#++ ? ie" -#=++6

    9" (ater i! di!charged 0ro+ a re!erDoir throgh a /i/e -=..+ long 7hich i!.":+ dia+eter 0or #=.+ and ."8=+ dia+eter 0or the re+aining di!tance"Calclate the 0lo7rate, taking only 0rictional lo!!e! into accont, i0 the otletleDel o0 the /i/e i! 9.+ belo7 the re!erDoir leDel" I .".-@ 0or the .":+/i/e and .".8: 0or the ."8=+ /i/e" 3-9# l!6

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    TaDles 'or t"e Hydraulic #esign o' ,ipes and Se9ers

    .+planation o' TaDle Layout

    The!e 7ere deDelo/ed a! an aid to /i/eline de!ign" They are ba!ed on the *arcya+/le o0 thi! i! a!hort /+/ing +ain 7here +inor lo!!e! +ay accont 0or / to a third o0 the totalenergy lo!!"

    There are t7o +ethod! o0 analy!ing /i/eline! 7hich inclde +inor lo!!e!" The 0ir!ti! to !i+/ly add each +inor lo!! into the Bernolli EationW

    AlternatiDely, they +ay be e>/re!!ed in ter+! o0 an eiDalent length o0 !traight/i/e 7hich 7old giDe the !a+e 0rictional energy lo!!" The length l i! !allye>/re!!ed a! a +lti/le o0 the /i/e dia+eter d !ee tableG" Th!W l I nd" Th!actal LG and eiDalent /i/e length! lG are added together to giDeW

    g2

    Ch

    2;

    ;

    =

    2;1;2

    222

    1

    211 hhh1 : !orked .+amples ;L; 1

    Solution:A//ly Bernolli! theore+ to A and B Figre =-G, a!!+ing Delocity at A i! ;eroand that /A $ /B$ at+o!/heric /re!!re I ." ;BI . and ;AI H"

    Total energy at A $ Total energy at B lo!! at entry 0rictional lo!!"

    g2

    v

    d

    ;

    g2

    v

    2

    1

    g2

    v:

    222 ++=

    Ptting H $ -8+, $ .".:, L $ :=.+, d$ -..++ $ ."-+

    g2v5181

    1045004051

    g2v12

    22

    =

    += .

    ...

    i"e 315181

    819212v2 .

    .

    . == *m141v /.=

    *i!charge I area > Delocity I m1096814110 32

    41 = ... 9! An!7erG

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    8" (ater i! di!charged 0ro+ a re!erDoir into the at+o!/here throgh a /i/e 9)+long" There i! a !har/ entrance to the /i/e and the dia+eter i! =.++ 0or -=+ 0ro+the entrance" The /i/e then enlarge! !ddenly to #=++ in dia+eter 0or there+ainder o0 it! length" Taking into accont the lo!! o0 head at entry and at theenlarge+ent, calclate the di00erence o0 leDel bet7een the !r0ace o0 the re!erDoir

    and the /i/e e>it 7hich 7ill +aintain a 0lo7 o0 8" l!" Take a! .".-)8 0or the=.++ /i/e and .".89- 0or the #=++ /i/e"

    -igure >& : !orked .+amples ;L; &

    Solution:Figre =8!ho7! the arrange+ent" $0 QI di!charge, then

    22

    241

    12

    141 vdvd ==

    4261050

    10824

    d

    4v

    2

    3

    21

    1 ..

    .=

    =

    =

    +! and 63400750

    10824

    d

    4v

    2

    3

    22

    2 ..

    .=

    =

    =

    +!

    A//lying Bernolli! theore+ to A and * at 7hich /AI /*I at+o!/heric /re!!reand DAI .,

    Total energy at A I Total energy at * !hock lo!! at B 0rictional lo!! in BC !hock lo!! at C 0rictional lo!! in C*"

    There i! no !hock lo!! at * a! di!charge i! to at+o!/here"

    ( )

    g2

    v

    d

    ;

    g2

    vv

    g2

    v

    d

    ;

    g2

    v

    2

    1

    g2

    v:

    2

    2

    2

    22

    2

    21

    2

    1

    1

    1121

    22 +

    +

    ++=

    ( )

    g2

    vv

    d

    ;1

    g2

    v

    d

    ;

    2

    1

    g2

    v 2

    21

    1

    1122

    1

    1121 +

    ++

    +=

    ( )

    g2

    7920

    0750

    24023201

    g2

    6340

    050

    1501920

    2

    1

    g2

    4261 222 .

    .

    ..

    .

    ..+

    ++

    +=

    I ."@:# ."-#9 .".98

    *i00erence o0 leDel I HI ."=8+ o0 7ater" An!7erG

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    9" T7o re!erDoir! are connected by a /i/eline 7hich i! -=.++ in dia+eter 0or the0ir!t @+ and 88=++ in dia+eter 0or the re+aining -=+" The entrance and e>it are!har/ and the change o0 !ection i! !dden" The 7ater !r0ace in the //erre!erDoir i! @+ aboDe that in the lo7er" Tablate the lo!!e! o0 head 7hich occrand calclate the rate o0 0lo7 in +9!" Friction coe00icient i! .".: 0or both /i/e!"

    *ra7 al!o the hydralic gradient and the total energy gradient"

    -igure >< : !orked .+amples ;L; ."9## I 9".=:+Enlarge+ent I -"=@ > ."9## I ."=+Friction in /i/e8 I 8"@# > ."9## I -"..#+E>it I -".. > ."9## I ."9##+

    The total head lo!! i!, o0 cor!e, H I @+"

    The total energy at any /oint can be re/re!ented gra/hically, a! !ho7n in Fig"53.At the entry to the /i/eline there 7ill be an entry lo!! ab; ne>t 0ollo7! the 0rictionallo!! in the 0ir!t /i/e, 7hich giDe! the !lo/ing !traight line bc. The lo!! at the!dden enlarge+ent i! !ho7n a! cd. Fro+ d to e the 0rictional lo!! in the larger/i/e ca!e! the total energy to 0all !lo7ly and the !hock lo!! at e>it efbring! thetotal energy gradient to the leDel o0 the !r0ace in the lo7er re!erDoir"

    The hydralic gradient i! obtained by /lotting the !+ o0 the /otential and /re!!re

    energy and 7ill there0ore be a di!tance eal to the Delocity head in the /i/e belo7the total energy gradient" The hydralic gradient !ho7! the leDel to 7hich the liidin the /i/e 7old ri!e i0 a Dertical !tand /i/e 7a! in!erted in the /i/eline at the/oint nder con!ideration"

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    Tutorial Fuestions E inor Losses

    -" (ater 0lo7! 0ro+ a !torage tank along a 8=.++ dia+eter /i/e, =.+ long ata rate o0 ."-+9!" The /i/e inclde! t7o ).Y bend! kLI ."#G, t7o :=Y bend!

    kLI ."8G, a 0lly o/en gate DalDe kLI ."8=G and a /artially !ht DalDe kLI@G" $0 the /i/e entrance i! !har/ and the 0lo7 di!charge! to at+o!/here atthe end o0 the /i/e, calclate the nece!!ary di00erence in leDel bet7een thetank 7ater leDel and the otlet" Take the /i/e 0riction 0actor, I .".:"39"#-9+6

    8" (ater i! di!charged 0ro+ a re!erDoir into the at+o!/here throgh a /i/e=.+ long" There i! a !har/ entrance to the /i/e and the dia+eter i! #=++0or 8.+ 0ro+ the entrance" The /i/e then enlarge! !ddenly to -..++ india+eter 0or the re+ainder o0 it! length" A DalDe in the #=++ /i/e ha! a kLI-"= 7hen 0lly o/en" Taking into accont the lo!! o0 head at entry, at theDalDe and at the enlarge+ent, calclate the di00erence o0 leDel bet7een the!r0ace o0 the re!erDoir and the /i/e e>it 7hich 7ill +aintain a 0lo7 o0 -. l !"Take a! .".8 0or the #=++ /i/e and .".8= 0or the -..++ /i/e" 38"=9#+6

    9" T7o re!erDoir! are connected by a /i/eline 7hich i! 88=++ in dia+eter 0orthe 0ir!t -8+ and -=.++ in dia+eter 0or the re+aining 8+" The entranceand e>it are !har/ and the change o0 !ection i! !dden, 7ith CcI ."@" The7ater !r0ace in the //er re!erDoir i! #"=+ aboDe that in the lo7er"Calclate the rate o0 0lo7 in +9! and tablate the lo!!e! o0 head 7hichoccr" Friction coe00icient i! .".9 0or the 88=++ /i/e and .".: 0or the-=.++ /i/e" 3.".@)+9!6

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    pen "annel -lo9

    Flo7 in an o/en channel or dct in 7hich the liid ha! a 0ree !r0ace di00er! 0ro+

    0lo7 in /i/e! in !o 0ar a! the /re!!re at the 0ree !r0ace i! con!tant nor+allyat+o!/hericG and doe! not Dary 0ro+ /oint to /oint in the direction o0 0lo7, a! the/re!!re can do in a /i/eline" A 0rther di00erence i! that the area o0 cro!! !ectioni! not controlled by 0i>ed bondarie!, !ince de/th can Dary 0ro+ !ection to !ection7ithot re!traint"

    O/en channel 0lo7 i! generally +ore co+/licated than /i/e 0lo7" O/en channel!haDe !ection! Darying 0ro+ !i+/le geo+etric !ha/e! to irreglar !ection! o0 natral!trea+!" The !tate o0 the bondary !r0ace! +ay Dary 7idely 0ro+ !+oothconcrete to neDen bed! o0 riDer!"

    The choice o0 a 0riction 0actor 0or an o/en channel i! th! likely to be +ore

    ncertain that a !i+ilar choice 0or a /i/e"

    Types o' "annel -lo9

    'o!t 0lo7! in channel! are trblent" The 0lo7 i! !aid to be ni0or+ or non= : Uni'orm -lo9

    +on-uniform "low or *aried "low

    -igure >> : /on*uni'orm (or 4aried -lo9)

    1elocity o0 0lo7 i! con!tant along the

    channel ? occr! 7hen a cro!!

    con!tant de/th

    0lid !r0ace i! /arallel 7ithchannel bed

    Flo7 Delocity i! not con!tant alongthe channel

    de/th Darie!

    0lid !r0ace i! not /arallel7ith channel bed

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    'teady "low

    1elocity and hence de/th re+ain con!tant 7ith re!/ect to ti+e"

    Unsteady "low

    1elocity and de/th Dary 7ith re!/ect to ti+e at any !ection o0 the channel"

    For analy!i! /r/o!e!, it i! !al to con!ider the 0lo7 in o/en channel! to be!teady ni0or+ 0lo7, ho7eDer +o!t real li0e 0lo7! are non? : "annel -lo9 #iagram

    Ter+ *e0inition

    y 0lo7 de/th I Dertical di!tance 0ro+ 0ree !r0ace to channel bed

    kinetic or Delocity energy head

    !/eci0ic energy, E

    B channel 7idth I 7idth o0 channel at 0ree !r0ace

    A area o0 0lo7 nor+al to direction o0 0lo7

    P 7etted /eri+eter I length o0 7etted !r0ace +ea!red nor+al todirection o0 0lo7

    R hydralic radi! I AP

    So !lo/e o0 channel

    Fr Frode N+ber Igy

    0lo7 rate /er nit 7idth I B0or rectanglar channel! onlyG

    g2

    v2

    yg2

    v2+

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    .Guations

    Continity, Energy and 'o+ent+ eation! +ay be a//lied in the !a+e 7ay a!/i/e 0lo7

    -igure >@ : -lo9 #iagram 'or .Guations

    Con!ider /oint M, 7here the Delocity i! D, at a de/th h, belo7 the 0ree !r0ace

    Fro+ Bernolli 7e get ( )hyg2

    v

    g

    p:

    2

    +++=D

    / I hydro!tatic /re!!re at de/th h belo7 0ree !r0ace

    hg

    p=

    i"e"g2

    vy:

    2

    ++= I Total Energy Head -G

    'ecific #nergy

    $n channel 0lo7 ho7eDer, it i! !al to re0er to the channel bed, rather than ahori;ontal dat+" Hence, eation -G beco+e!

    g2

    vy

    2

    + I Energy Head I E, !/eci0ic energy

    The hydralic grade line coincide! 7ith the 0ree !r0ace" The total energy line lie!D88g aboDe thi!"

    For a giDen Dale o0 !/eci0ic energy E the 0lo7 can haDe t7o de/th!" The 0ir!t i!7here the 0lo7 i! dee/ and !lo7 +oDing and i! kno7n a! tranil or !bcritical0lo7" The !econd i! 7here the 0lo7 i! !hallo7 and 0a!t +oDing and i! kno7n a!ra/id or !/ercritical 0lo7"

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    (ritical Deth

    -igure > : ritical #ept" 2rap"

    For a giDen Dale o0 S/eci0ic Energy, it can be !een 0ro+ the diagra+ aboDe, therei! one de/th corre!/onding to +a>i++ 0lo7 rate" Thi! i! called the critical de/th,yc"

    Certain 0lo7 +ea!ring deDice! e"g" 7eir! and 0l+e! generate critical de/th 0lo7in their o/eration"

    The eation 0or critical de/th i!g

    E3y

    2

    =

    The Frode N+ber, Fri! !ed to cla!!i0y the 0lo7

    Fr -, 0lo7 i! !/ercritical ra/id, !hallo7G

    FrI -, 0lo7 i! critical

    FrQ -, 0lo7 i! !bcritical !lo7, dee/G

    #uations for 'teady Uniform "low in .en (hannels

    $nitial e>/eri+ental 7ork 7a! done by Che;y, 7hich led to

    7here C I Che;y! coe00icient ? related to channel geo+etry and channel

    roghne!!"

    $t 7a! thoght that Che;y! C 7a! con!tant 0or all channel!, bt it 7a! 0ond to beDariable !ally =. ? #.G" So 'anning deDelo/ed an eation ba!ed on Che;y

    7here n I 'anning! n+ber ? a roghne!! coe00icient"

    21

    F3

    2

    G/)

    1v= 2

    1

    F3

    2

    G/)

    A =or

    'anning! Eation(very 9idely used in practice)

    F/G=v = Che;y! EationF/GA==or

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    Ty/ical Dale! o0 'anning! Kn

    !+ooth concrete .".--rogh concrete .".-9brick7ork .".-:!teel !heet /ile! .".-!+ooth earth .".88rogh rock .".9=

    !orked .+amples E Uni'orm "annel -lo9

    -" Find the gradient nece!!ary 0or a rectanglar 0l+e -"=+ 7ide and ."#=+ dee/to deliDer 9"=+9! o0 7ater 7hen rnning 0ll" Take C I #8"

    Solution:2m125175051!yA ... ===

    m3750251y2! =+=+= ..

    Hence, m37503

    1251

    A/ .

    .===

    -igure > : !orked .+amples U;;-; 1

    52061

    721251

    53

    3750

    1

    A=

    /

    1G/GA=

    22

    00 ..

    .

    .=

    =

    ==

    8" Arectanglar o/en channel ha! a botto+ 7idth o0 8":+ and a !r0aceroghne!! corre!/onding to 'anning n I .".-=" $0 the !lo/e o0 the bed i! ."..-and the de/th o0 0lo7 i! -"8+, 7hat i! the di!charge nder condition! o0 ni0or+!teady 0lo7

    Solution:2

    m8822142!yA ... ===

    m8421242y2! ... =+=+=

    -igure ?0 : !orked .+amples U;;-; &

    Hence, m6084

    882

    .

    A/ .

    .

    .===

    *m3240010600150

    882G/

    )

    A

    30

    21

    32

    21

    32

    ....

    .===

    y I ."#=+

    b I -"=+

    y I -"8+

    b I 8":+

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    9" A channel o0 tra/e;oidal !ection, 7ith !ide !lo/e! at @.Y to the hori;ontal ba!eo0 the channel, conDey! 7ater at a de/th o0 .")+" Find the 7idth o0 the ba!e andthe gradient o0 the bed to di!charge -"#+9! 7ith a +ean Delocity o0 0lo7 o0 ."@+!"Take 'anning n I .".8="

    Solution:

    833260

    71

    v

    AAv .

    .

    . ====

    -igure ?1 : !orked .+amples U;;-;

    t

    b

    y I .")+ @.Y

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    :" A canal ha! a botto+ 7idth o0 :+ and !ide! 7ith a !lo/e o0 - Dertical to -"=hori;ontal" The de/th o0 7ater i! -".+ 7hen the di!charge i! : +9!"

    aG Calclate the !lo/e o0 the channel bed !ing the 'anning 0or+la 7ithn I .".88"

    bG Calclate the di!charge in +9! 7hen the de/th o0 0lo7 i! -"8+"

    Solution:

    aG ( )[ ] 2

    m5501514y512!!2

    01A ....

    .=+=++=

    m672530124511y2!. 22

    .... =+=++=

    m724067

    55

    .

    A/ .

    .

    .===

    -igure ?& : !orked .+amples U;;-; =

    25401

    724055

    40220

    A/

    )GG/

    )

    A

    22

    003

    23

    2

    21

    32

    =

    =

    ==..

    .

    bG ( ) 2m966215142151421A ...... =+=+=

    m32782532124. ... =+=

    m83603278

    966

    .

    A/ .

    .

    .===

    *m5752540

    183600220966G/

    )A 30

    21

    322132 .... ===

    >

    b

    y I -".+ -

    -"=

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    Tutorial Fuestions E Uni'orm "annel -lo9

    -" Find the gradient nece!!ary 0or a rectanglar 0l+e -"8+ 7ide and ."@+dee/ to deliDer 8"8=+9! o0 7ater 7hen rnning 0ll" Take C I #." 3- in -=-6

    8" Arectanglar o/en channel ha! a botto+ 7idth o0 8":+ and a !r0aceroghne!! corre!/onding to 'anning n I .".-=" $0 the !lo/e o0 the bed i!."..- and the de/th o0 0lo7 i! -"8+, 7hat i! the di!charge nder condition!o0 ni0or+ !teady 0lo7 3:"98 +9!6

    9" A channel o0 tra/e;oidal !ection, 7ith !ide !lo/e! at :=Y to the hori;ontalba!e o0 the channel, conDey! 7ater at a de/th o0 ."#=+" Find the 7idth o0the ba!e and the gradient o0 the bed to di!charge -"8#+9! 7ith a +eanDelocity o0 0lo7 o0 ."#+!" Take Che;y C I @@" 3-":8+W -99--6

    :" A canal ha! a botto+ 7idth o0 9+ and !ide! 7ith a !lo/e o0 - Dertical to 8hori;ontal" The de/th o0 7ater i! -"8+ 7hen the di!charge i! 9"=-+9!"

    %!ing the 'anning 0or+la 7ith n I .".88

    a" Calclate the !lo/e o0 the channel bed" 3-=...6

    b" Calclate the di!charge in +9! 7hen the de/th o0 0lo7 i! -"9+"3:"-8+9!6

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    /on*uni'orm pen "annel -lo9

    There are, broadly !/eaking, t7o kind! o0 !teady non

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    The eation o0 the hydralic +/ i!

    -igure ?= : ump .Guation #iagram

    -lo9 easuring #evices in "annels

    There are three +ain ty/e!

    -" Flo7 +ea!ring !trctre!, /er+anent, e>/en!iDe, a00ect! 0lo7 condition!G"

    8" *eter+ination o0 0lo7 rate 0ro+ Delocity, chea/, te+/orary, accrateG"

    9" Che+ical +ean!, !ed 0or !/ecial condition!, !/eciali!ed, accrateG"

    /0 "low Measuring 'tructures

    Ba!ically, an ob!trction i! /laced in the channel to create critical 0lo7 de/th y cG"There are t7o +ain kind! o0 !trctre! 7eir! and 0l+e!"

    !eirs

    -igure ?> : Broad rested !eir -igure ?? : 3ound rested !eir

    b I 7idth o0 channelCd? 0ond 0ro+ BS 9@.

    Broad cre!ted 7eir! are e!!entially lo7 da+! acro!! the entire channel, 7hich to/rodce critical de/th oDer the 7eir, +!t haDe a 7idth in the direction o0 channel0lo7, o0 at lea!t three ti+e! the +a>i++ height o0 7ater aboDe the 7eir" Th!

    they are +a!!iDe and e>/en!iDe !trctre!, 7hich inDariably collect !ilt again!t

    ( )1-812

    yy

    22

    21 +=

    ( )1-812y

    y

    2

    1

    1

    2 +=

    23

    data !:71= .=

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    their /!trea+ 0ace! and reire annal +aintenance" A! +ea!ring !y!te+! theytend to be inaccrate at lo7 rate! o0 0lo7"

    Cr+/ and 0lat

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    -lumes

    -igure ? : -lume ,lan -igure @0 : -lume .levation

    b I 7idth o0 channelCdCD? 0ond 0ro+ BS 9@.

    Fl+e! do not !00er 0ro+ !iltation /roble+!, !ince any !ilt i! 7a!hed throgh the!trctre" Ho7eDer their length and th! co!t o0 con!trction are higher than 0ornor+al 7eir!" To +ini+i!e the!e co!t!, a large n+ber o0 0l+e! haDe beencon!trcted by driDing !heet /ile! into the channel bed and back0illing to theoriginal riDer bank 7ith !itable 0ill +aterial!"

    Another adDantage o0 0l+e! i! the Dery li+ited backing / o0 the /!trea+ 7aterleDel it /rodce!" $n 0lat area! thi! i! a con!iderable adDantage"

    -igure @1 : #ept" easurement

    10 "low 2ate from *elocity

    %!e! I 1A ? i"e" +ea!ring 1 and A" 1elocity +ea!red 7ith crrent +eter ?Dale! recorded at /oint! acro!! the !ection and aDerage Delocity taken"

    -igure @& : 4ariation o' 4elocity

    23

    vdata !:==71 .=

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    -igure @< : Irregular Sections * 3ivers%Streams

    -" Find area o0 each 7idth by !e o0 +ea!ring !ta00 I A

    8" Record aDerage Delocity 0or each 7idth I 1

    9" Flo7 rate 0or each 7idth I 1A I :" Total 0lo7 rate I I - 8 9f" n

    Thi! +ethod i! kno7n a! UDelocity area gagingV" (ith care the accracy 0or the0lo7 rate eal! ="

    30 (hemical Means

    %!ed 0or rogh, highly di!trbed 0lo7, the +ethod inDolDe! the introdction o0 akno7n antity o0 a che+ical at a /re!cribed rate at an /!trea+ location" Thetrblent natre o0 the 0lo7 en!re! thorogh +i>ing o0 the che+ical" Sa+/le! o0the 0lid are taken at a do7n!trea+ location and by che+ical analy!i!, the

    concentration o0 che+ical in the 0lid can be 0ond" Thi! degree o0 concentrationcan be related to 0lo7 rate" The che+ical diltion +ethod giDe! an accracy to="

    So+e +odern deDelo/! inclde electroche+ical +ethod!, la!er !canning andltra!onic deDice!"

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    Hydraulic ac"ines

    -unctions and Types

    Hydralic +achine! are /o7er or energy conDerter!" They conDert bet7een+echanical and hydralic 0or+! o0 /o7er" There are t7o ty/e! /+/! andtrbine!"

    P+/! A +otor conDert! electrical /o7er into +echanical /o7er" The /+/then conDert! the +echanical /o7er into hydralic /o7er"

    Trbine! The trbine conDert! hydralic /o7er into +echanical /o7er" Agenerator then conDert! the +echanical /o7er into electrical /o7er"

    The e00ect on the hydralic !y!te+ +ay be !ho7n on the total energy diagra+"

    -igure @= : Total .nergy #iagram 'or ,ump and TurDine

    - ? $nlet8 ? Otlet

    ? 0lo7 Delocity +SG

    ? /re!!re N+8G

    H ? total head acro!! the +achine +G

    'o!t /+/! and trbine! /roDide a contino! 0lo7 rate throgh a rotodyna+icaction" Ho7eDer, /o!itiDe di!/lace+ent /+/! are !ed in !o+e !itation!"

    ,ositive #isplacement ,umps

    The!e 0nction a! a re!lt o0 Dol+etric change!7ithin the /+/" E"g" the reci/rocating or /i!ton/+/!f"

    The /i!ton di!/lace! a 0i>ed Dol+e o0 0lid ateach !troke" The action re!lt! in an n!teadydi!contino!G 0lo7 rate"

    The!e /+/! are !ed 0or de7ateringe>caDation!, tran!0erring !ldge at !e7agetreat+ent 7ork! and inecting che+ical! into the

    0lo7 at 7ater treat+ent 7ork!"-igure @> : ,ositive #isplacement ,ump

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    3otodynamic ,umps

    The +echanical /o7er i! tran!+itted throgh a rotating !ha0t P'I 8NT 7att!

    7here N I rotational !/eed o0 !ha0t reD!G

    T I tore in the !ha0t N+G$+/eller blade!, attached to the !ha0t, tran!0er /o7er energy to the 0lid" The

    hydralic /o7er PHI gH 7att!

    7here I di!charge 0lo7 rate throgh the /+/ +9!G

    H I increa!e in total energy head acro!! the /+/ +G

    i"e" H i! the ri!e in the T"E"L" in the direction o0 0lo7"

    The e00iciency o0 the /+/ %% 100.

    .100

    pB&')pt

    pB&tpt

    "

    : ==

    Types o' 3otodynamic ,umps

    Fro+ the eation PHI gH it i! eDident that t7o +achine! /rodcing the !a+e

    /o7er +ay deliDer di00erent 0lo7 rate! at di00erent head!" The relatiDe Dale! o0 and H 7ill de/end on the !ha/e o0 the i+/eller, /rodcing di00erent ty/e! o0+achine! 7hich are !ited to di00erent ta!k!"

    (entrifugal Pums 4low 5! high H6

    -igure @? : entri'ugal ,umps

    Flo7 /a!t the i+/eller i! entirely radial" The Dolte ca!ing i! de!igned to 7ith!tandthe high /re!!re! generated" The centri/etal action /rodce! a relatiDely high/re!!re di00erence"

    The!e ty/e! o0 /+/! are !ed to e>tract 7ater 0ro+ borehole!, in 7ater !//ly/i/eline! and !e7age /+/ing throgh long ri!ing +ain!"

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    A7ial "low Pums 4high 5! low H6

    -igure @@ : A+ial -lo9 ,ump

    Flo7 /a!t the i+/eller i! entirely a>ial" The i+/eller, 7hich i! !ha/ed like a !hi/!/ro/eller, allo7! relatiDely high 0lo7!, bt the head di00erence 7hich can be+aintained acro!! it i! lo7" The t7i!t 7hich i! i+/arted to the 7ater i! /artiallyre+oDed !ing gide Dane! do7n!trea+, th! redcing the energy lo!!"

    The!e ty/e! o0 /+/! are !ed in land drainage !che+e!, and to retrn actiDated!ldge in large !e7age 7ork!"

    Mi7ed "low Pums

    -igure @ : i+ed -lo9 ,ump

    Flo7 /a!t the i+/eller i! /artially radial and /artial a>ial" The !ha/e o0 the i+/ellerand ca!ing de/end! on the characteri!tic! reired" So+e +i>ed 0lo7 /+/!

    re!e+ble centri0gal /+/!, bt 7ith a thickened Dolte ca!ingW other! re!e+blea>ial 0lo7 /+/!, bt 7ith a Kblb or Kbo7l ca!ing arond the i+/eller"

    The!e ty/e! o0 /+/! are !ed to /+/ !tor+ 7ater throgh !hort ri!ing +ain!,and in !+all land drainage !che+e!"

    Multistage Pums

    The!e are 0or+ed by bilding a n+ber o0 identical centri0gal i+/eller! onto a!ingle driDing !ha0t in !erie!G" The !a+e 0lo7 rate /a!!e! each i+/eller in trn,the 7ater receiDing an acc+lating head li0t at each !tage"

    The!e /+/! are !ally in!talled 7ith the !ha0t Dertical in borehole! and dee/7ell!"

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    ,ump ,er'ormance "aracteristics (urves)

    'athe+atical eation! relating the Dariable! H, , N, P and are long and

    co+/licated" $t i! +ore conDenient to hold the in0or+ation in the 0or+ o0 gra/h!,!ing data obtained 0ro+ /er0or+ance te!t!"

    P+/! are !ally te!ted at con!tant !/eed N, and the other Dariable! /lottedagain!t di!charge " The te!t! are re/eated 0or di00erent !/eed!, /rodcing a0a+ily o0 characteri!tic crDe!"

    (entrifugal Pum (ur)es

    A K!table characteri!tic !ho7! a head 7hich 0all!contino!ly 7ith 0lo7 rate" High eddy lo!!e! in the/+/ +ay ca!e an Kn!table characteri!tic, allo7ingKhnting bet7een t7o 0lo7 rate! at a giDen head"

    A Knon

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    .ther (haracteristic (ur)es

    -igure & : #esign ,oint urve

    -igure < : -amilies o' "aracteristic urves

    Hydro ,o9er TurDines

    There are +any hydroelectric /o7er in!tallation! throghot the 7orld" TheDario! +odern 7ater trbine de!ign! are ca/able o0 coDering a 7ide range o0o/erating condition!" Hydroelectric !che+e! +ay no7 be 0ond in +ontain!,

    riDer or e!tarine enDiron+ent!"

    For large !cale /o7er generation, three ty/e! o0 trbine! are do+inant"

    -" Radical 0lo7 or Franci! trbine

    8" A>ial 0lo7 trbine

    9" Pelton (heel trbine

    The 0ir!t t7o are kno7n a! reaction trbine!, the third i! called an i+/l!e trbine"

    "rancis Turbine

    The Franci! trbine +ay be regarded a! a centri0gal /+/ o/erating in KreDer!e"

    -igure = : -rancis TurDine

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    The 7ater enter! the oter /art o0 the ca!ing and 0lo7! throgh the gide Dane!7hich direct the 0lo7 radially in7ard! throgh the rotating ele+ent called thernnerG, tran!0erring energy to the rnner" The 7ater then drain! ot o0 the ca!ingthrogh the central otlet /a!!age"

    A7ial "low TurbineThe a>ial 0lo7 trbine +ay be regarded a! an a>ial 0lo7 /+/ o/erating inKreDer!e" The gide Dane! direct the 0lo7 !o that it +eet! the rnner in an a>ialdirection"

    -igure > : A+ial -lo9 TurDine

    There are t7o +aor di00erence! bet7een the trbine and the /+/

    aG $n the trbine, the rotating ele+ent i! !rronded by gide Dane!, !o thatthe Delocity and direction o0 the 7ater can be ad!ted" Thi! /roDide! 0oro/ti++ 0lo7 condition! oDer a 7ide range o0 di!charge and /o7er ot/t"

    N"B" electrical reire+ent! Dary oDer a 8: hor /eriod"GbG The 7ater leaDing the trbine /a!!e! throgh a dra0t tbe, 7hich i! ta/ered

    !o a! to +ini+i!e the lo!! o0 kinetic energy" Thi! en!re! that the+a>i++ energy i! aDailable at the trbine"

    1irtally all +odern nit! incor/orate +echanical +ean! o0 Darying the /ro/ellerblade angle o0 the rnner, !o that high rnner e00iciency +ay be +aintained oDerthe !/eci0ied range o0 di!charge and /o7er ot/t"

    1ariable angle de!ign! are called K5a/lan trbine!" $n recent year!, a n+ber o0/+/ed !torage !che+e! haDe tili;ed a !/ecial ty/e o0 5a/lan nit" Thi! nito/erate! a! a trbine dring /eriod! 7hen the de+and 0or electricity i! high"Ho7eDer, de+and i! lo7 dring the night" The blade i! then reDer!ed and the niti! +otor driDen !o a! to act a! a /+/"

    Both the 5a/lan and Franci! nit! rn 0ll o0 7ater" There i! there0ore acontino! 0lo7 o0 7ater bet7een the re!erDoir and the tail7ater"

    4enerally, trbine! are Dery e00icient, i"e" hydralic and +echanical energy lo!!e!are lo7" They co++only attain e00iciencie! in e>ce!! o0 )."

    5a/lan nit! are generally a//lied 7here there i! a large di!charge at a lo7/re!!re, 7herea! the Franci! nit i! a//ro/riate 0or +oderate di!charge! at+oderate head 8=. ? 9.. +G"

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    Pelton 8heel Turbine

    The Pelton (heel trbine i! a//ro/riate 7here a high /re!!re 7ater !//ly i!aDailable" $n contra!t to the other trbine!, the ca!ing doe! not rn 0ll o0 7ater"

    -igure ? : ,elton !"eel TurDine

    E!!entially, the rnner co+/ri!e! a di!c, 7ith a !erie! o0 0lo7 de0lector! orKbcket! arond it! /eri/hery" The 7ater enter! the ca!ing throgh one or +oreno;;le! a! a high Delocity et" A! the rnner rotate!, the et i+/inge! /on eachbcket in trn" The 7ater i! de0lected by the bcket!, and the change in+o+ent+ tran!0er! a 0orce to the bcket, and hence a tore to the driDe !ha0t"

    The et incor/orate! a !trea+lined control DalDe 7hich i! !ed to reglate thedi!charge, and hence the /o7er ot/t"

    The gro!! head 0or the Pelton (heel i! de only to the height o0 the re!erDoir

    aboDe the no;;le!"

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    Se9age ,umping Station Layouts

    -igure @ : Se9age ,umps * A+ial and i+ed -lo9

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    -igure : Se9age ,umps * entri'ugal and SuDmersiDle