Rcc Lec 07 Bond and Dev Length

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    By 

    Dr. Attaullah Shah

    Swedish College of Engineering and TechnologyWah Cantt.

    Lec-07

    Bond and Development Length

    Reinforced Concrete Design-I

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    − The basic assumption of theRCC design is that the strain

    in concrete and reinforcingsteel is the same. f thereinforcing steel slips at itsends! this is not "alid. #ence

    it must be ensured thatsufficient bond strength isde"eloped at the interface ofsteel and concrete to a"oidslippage of the steel.

    −  

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    Bond Strength and $e"elopment length− Two types of bond failure can

    be e%pected in reinforcing bars&

    − $irect pull out of the steel bars!when ample concrete confinementis pro"ided in the form of largespacing of bars or large concreteco"er

    − Splitting of concrete along the barwhen co"er confinement or barspacing is insufficient

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    '

    b. (ctual $istribution of )le%ural Bond Stress

    − ure !ending case

    − Concrete fails to resist tensilestresses only where the actualcrac* is located. Steel T isma%imum and

    T  max = M / jd .

    − Between crac*s ! concretedoes resist moderate amount oftension introduced by bond.

    − u is proportional to the rate ofchange of bar force! andhighest where the slope of the

    steel force cur"e is greatest.

    − +ery high local bond stressad,acent to the crac*.

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    -

    − Beam under transverse loads"−  (ccording to simple crac*

    sectional theory! T is proportionalto the moment diagram and u isproportional to shear forcediagram.

    − n actual! T is less than the simple

    analysis prediction e"erywheree%cept at the actual crac*s.

    − Similarly! u is eual with simpleanalysis prediction only at thelocation where slopes of the steel

    force diagrams are euals .f theslope is greater than assumed!bond stress is greater/ if the slopeis less bond stress is less.

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    $epar tment

    2

    3T4(TE B56$ STRE67T# (6$$E+E3584E6T 3E67T#

    − #$pes of !ond failure

    − Direct pullout  of bars9small diameter bars areused with sufficientlylarge concrete co"erdistances and barspacing:

    − Splitting of the concrete along the bar 9co"er orbar spacing is

    insufficient to resist thelateral concrete tensionresulting from thewedging effect of bardeformations:

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    ;

    a. ltimate Bond Strength− Direct pull out

    − )or sufficiently confined bar! adhesi"e bond and friction are o"ercome as thetensile force on the bar is increased. Concrete e"entually crushes locally ahead

    of the bar deformation and bar pullout results.− When pull out resistance is o"ercome or when splitting has spread all theway to the end of an unanchored bar! complete bond failure occurs.

    − Splitting− Splitting comes from wedging action when the ribs of the deformed bars bear

    against the concrete.

    − Splitting in "ertical plane− Splitting in hori

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    Consider a bar embedded in a

    mass of concrete

    8 =τ>?3

    b>π>d

    b@

    8 = σ > ?π>dbA@

    τ = 8 ?3b>π>db@ D τma%

    8 D τma% > ?3b>π>db@σ  = 8 ?π>dbA@ D σma%

    8 D σma% > ?π>dbA@

    To force the bar to be the wea* lin*& τma% > ?3b>π>db@ σma% > ?π>dbA@

     3b  9σma%  τma%:> ?db@

    3b

    db

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    $e"elopment 3ength

    − 3d = de"elopment length− the shortest distance o"er which a bar can achie"e itFs full

    capacity− The length that it ta*es a bar to de"elop its full contribution

    to the moment capacity! 4n

    Cc

    Ts

    4n = 9C or T:>9dist:

    4n

    G

    3d

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    Steel 3imit! σma%

    − sing the bilinear assumption of (C H12&

    σma% = I f y

     3b  9f y  τma%:> ?db@

     3b  f y > db  9>τma%:

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    Concrete Bond 3imit! τma%

    − There are lots of things that affect τma%− The strength of the concrete! fFc− Type of concrete 9normal weight or light weight:

    − The amount of concrete below the bar − The surface condition of the rebar − The concrete co"er on the bar 

    − The pro%imity of other bars transferring stress tothe concrete− The presence of trans"erse steel

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    Concrete Strength! fFc

    − Bond strength! τma%! tends to increase with concretestrength.

    − E%periments ha"e shown this relationship to be

    proportional to the suare root of fFc.

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    Type of Concrete

    − 3ight weight concrete tends to ha"e less bondstrength than does normal weight concrete.

    −  (C H12JG2 introduces a lightweight concrete

    reduction factor! λ! on srt9fFc: in some euations.− See (C H12JG2! 2.'.1 for details

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     (mount of Concrete Below Bars

    − The code refers to Ktop barsLas being any bar which has1A inches or more of freshconcrete below the barwhen the member is poured.

    − f concrete 1AL thenconsolidation settlement

    results in lower bondstrength on the bottom sideof the bar 

    − See (C H12JG2! 1A.A.9a:

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    Surface Condition of Rebar 

    −  (ll rebar must meet (ST4 reuirements for deformationsthat increase pullout strength.

    − Bars are often surface coated is inhibit corrosion.− Epo%y Coating The ma,or concernM− 7al"ani

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    8ro%imity to Surface or 5ther Bars

    − The si

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    8resence of Trans"erse Steel

    − The bond transfer tends to cause a splitting plane

    − Trans"erse steel will increase the strength of the splittingplane.

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    b. $e"elopment 3ength

    − $e"elopment length is the length of embedment necessary to de"elop the full tensile strength of bar! controlled byeither pullout or splitting.

    − n )ig.! let− ma%imum 4 at a and

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    $epar tment

    A1

    (C C5$E 8R5+S56 )5R $E+E3584E6T5) TE6S56 RE6)5RCE4E6T

    3imit3imit

    9c I *9c I *tr tr : d: dbb = A.P for= A.P forpullout casepullout case QQfFc are not to befFc are not to be

    greater than 1GG psi.greater than 1GG psi.

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    AA

    %or t&o cases of practical importance" using 9c I *tr : db = 1.P! 

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    AH

    E%ample&

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    $epar tment

    A

    Continue&

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    AP

    Continue&

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    A'

     (6C#5R(7E 5) TE6S56 B(RS B0

    #55Sn the e"ent that the desired tensile stress in a bar can notn the e"ent that the desired tensile stress in a bar can notbe de"eloped by bond alone! it is necessary to pro"idebe de"eloped by bond alone! it is necessary to pro"idespecial anchorage at the end of the bar.special anchorage at the end of the bar.

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    A-

    b $ l t 3 th d 4 difi ti

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    A2

    b. $e"elopment 3ength and 4odification)actors for #oo*ed Bars

  • 8/20/2019 Rcc Lec 07 Bond and Dev Length

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    A;

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    $epar tment

    HG

    '(ample

    (6C#5R(7E RERE4E6TS )5R

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    H1

     (6C#5R(7E RERE4E6TS )5RWEB RE6)5RCE4E6T

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    $epar tment

    HA

    $E+E3584E6T 5) B(RS 6

    C548RESS56− Reinforcement may be

    reuired to de"elop itscompressi"e strength by

    embedment under "ariouscircumstances.

    −  (C basic de"elopment

    length in compression

     

    l db = 0.02d b f y  /√f c 

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    Determining Locations of FlexuralDetermining Locations of FlexuralCutoffsCutoffs

    Given a simply

    supported beam with a

    distributed load.

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    Determining Locations of FlexuralDetermining Locations of FlexuralCutoffsCutoffs

     Note:

    Total bar length =

    Fully effective length+ Development length

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    Determining Locations of FlexuralDetermining Locations of FlexuralCutoffsCutoffs

     ACI 12.10.3

    ll longitudinal tension bars

    must e!tend a min. distance

    = d "effective depth of the

    member# or $% d b "usually

    larger# past the theoretical

    cutoff for fle!ure "&andlesuncertainties in loads' design

    appro!imations'etc..#

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    Determining Locations of FlexuralDetermining Locations of FlexuralCutoffsCutoffs

    Development of fle!ural

    reinforcement in a typical

    continuous beam.

    () *$,-% - $%.$ forfle!ural reinforcement

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    Bar Cutoffs - General ProcedureBar Cutoffs - General Procedure

    Determine theoretical fle!ural cutoff points for

    envelope of bending moment diagram.

    /!tract the bars to satisfy detailing rules "from() 0ection 1.$*' $%.$' $%.$' $%.$$ and $%.$%#

    Design e!tra stirrups for points where bars are

    cutoff in 2one of fle!ural tension "() $%.$.3#

    $.

    %.

    *.

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    Bar Cutoffs - General RulesBar Cutoffs - General Rules

    4ars must e!tend the longer of d or $%d b past

    the fle!ural cutoff points e!cept at supports

    or the ends of cantilevers "() $%.$$.$#

    All Bars

    ,ule $.

     

    ,ule %. 4ars must e!tend at least ld  from the point of

    ma!imum bar stress or from the fle!ural

    cutoff points of ad5acent bars "() $%.$.%

    $%.$.6 and $%.$%.%#

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    Bar Cutoffs - General RulesBar Cutoffs - General Rules

      Structural Integrity

    −  Simple Supports t least one-third of the positivemoment reinforcement must be e!tend 7 in. intothe supports "() $%.$$.$#.

    − Continuous interior beams with closed stirrups.t least one-fourth of the positive moment

    reinforcement must e!tend 7 in. into the support

    "() $%.$$.$ and 1.$*.%.*#

    Positive Moment Bars

    ,ule *.

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    Bar Cutoffs - General RulesBar Cutoffs - General Rules

      Structural Integrity

    − Continuous interior beams without closedstirrups. t least one-fourth of the positivemoment reinforcement must be continuous or

    shall be spliced near the support with a class

    tension splice and at non-continuous supports beterminated with a standard hoo8. "() 1.$*.%.*#.

    Positive Moment Bars

    ,ule *.

    Bar Cutoffs General RulesBar Cutoffs General Rules

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    Bar Cutoffs - General RulesBar Cutoffs - General Rules

      Structural Integrity

    − Continuous perimeter beams. t least one-

    fourth of the positive moment reinforcementre9uired at midspan shall be made continuousaround the perimeter of the building and must beenclosed within closed stirrups or stirrups with

    $*3 degree hoo8s around top bars. The re9uiredcontinuity of reinforcement may be provided bysplicing the bottom reinforcement at or near thesupport with class tension splices "()1.$*.%.%#.

    Positive Moment Bars

    ,ule *.

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    Bar Cutoffs - General RulesBar Cutoffs - General Rules

      Structural Integrity

    −  Beams forming part of a frame that is the primary lateral load resisting system for thebuilding. This reinforcement must be anchored

    to develop the specified yield strength' f y' at the

    face of the support "() $%.$$.%#

    Positive Moment Bars

    ,ule *.

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    Bar Cutoffs - General RulesBar Cutoffs - General Rules

       Stirrups

    − t the positive moment point of inflection andat simple supports' the positive moment

    reinforcement must be satisfy the following

    e9uation for () $%.$$.*. n increase of *

    in value of ;n < u shall be permitted when theends of reinforcement are confined by

    compressive reaction "generally true for simply

    supports#.

    Positive Moment Bars

    ,ule 6.

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    Bar Cutoffs - General RulesBar Cutoffs - General Rules

    Positive Moment Bars

    ,ule 6.

    a

    u

    n

    d

    l  M l    +≤

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    Bar Cutoffs - General RulesBar Cutoffs - General Rules

    −  Negative moment reinforcement must beanchored into or through supporting columns ormembers "() 0ec. $%.$%.$#.

    Negative Moment Bars

    ,ule 3.

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    Bar Cutoffs - General RulesBar Cutoffs - General Rules

      Structural Integrity

    −  Interior beams. t least one-third of the negativemoment reinforcement must be e!tended by thegreatest of d' $% d b or " ln < $7 # past the negative

    moment point of inflection "() 0ec. $%.$%.*#.

    Negative Moment Bars

    ,ule 7.

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    Bar Cutoffs - General RulesBar Cutoffs - General Rules

       Structural Integrity

    −  erimeter beams. )n addition to satisfying rule 7a'one-si!th of the negative reinforcement re9uired atthe support must be made continuous at mid-span.

    This can be achieved by means of a class tension

    splice at mid-span "() 1.$*.%.%#.

    Negative Moment Bars

    ,ule 7.

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    Moment Resistance DiagramsMoment Resistance Diagrams

    ;oment capacity of a beam is a function of its depth'

    d' width' b' and area of steel' s. )t is common

     practice to cut off the steel bars where they are no

    longer needed to resist the fle!ural stresses. s incontinuous beams positive moment steel bars may be

     bent up usually at 63o' to provide tensile

    reinforcement for the negative moments over the

    support.

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    Moment Resistance DiagramsMoment Resistance Diagrams

    The nominal moment capacity of an under-reinforced

    concrete beam is

    To determine the position of the cutoff or bent point

    the moment diagram due to e!ternal loading is drawn.

    s y

    n s y

    c

      where'% .3

     A f  a M A f d a f b

    = − =

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    Moment Resistance DiagramsMoment Resistance Diagrams

    The ultimate moment resistance of one bar' ;nb is

    The intersection of the moment resistance lines with

    the e!ternal bending moment diagram indicates the

    theoretical points where each bar can be terminated.

    nb bs y bs  where' area of bar %

    a

     M A f d A

    = − −

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    Moment Resistance DiagramsMoment Resistance Diagrams

    Given a beam with the 6 > bars and

    f c=* 8si and f y=3 8si and d = % in.

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    Moment Resistance DiagramsMoment Resistance Diagrams

    The moment diagram is

    )oment Diagram

    G

    PGG

    1GGG

    1PGG

    AGGG

    APGG

    HGGG

    G A C ' 2 1G 1A 1C 1' 12 AG

    ft

           *   -

           i     n

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    Moment Resistance DiagramsMoment Resistance Diagrams

    The moment resistance of one bar is

    ( ) ( )( ) ( )

    ( ) ( )( )

    nb sb y

    %

    s y

    c

    %

    nb

    ub nb

    %

    *.$7 in 3 8si3.% in.

    .3 .3 * 8si $% in.

    3.% in.

    .1? in 3 8si % in. 7 8-in.%

    .? 7 8-in. 7% 8-in.

    a M A f d 

     A f  a

     f b

     M 

     M M φ 

    = −

    = = =

    = − = = = =

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    Moment Resistance DiagramsMoment Resistance Diagrams

    The moment diagram and crossings

    )oment Diagram

    G

    PGG

    1GGG

    1PGG

    AGGG

    APGG

    HGGG

    G A ' 2 1G 1A 1 1' 12 AG

    ft

           *   -

           i     n

    'AG *Jin

    1AG *Jin

    12'G *Jin

    A2G *Jin

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    Moment Resistance DiagramsMoment Resistance Diagrams

    The ultimate moment resistance is %6 8-in. The

    moment diagram is drawn to scale on the basis bar

    can be terminated at a' two bars at b and three bars at c.

    These are the theoretical termination of the bars.)oment Diagram

    G

    PGG

    1GGG1PGG

    AGGG

    APGG

    HGGG

    G A ' 2 1G 1A 1 1' 12 AG

    ft

           *   -       i     n

    'AG *Jin

    1AG *Jin

    12'G *Jin

    A2G *Jin

    a!

    c

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    Moment Resistance DiagramsMoment Resistance Diagrams

    (ompute the bar development length is

    ( )

    ( ) ( )

    a b

    y b

    d

    c

    $% or d

    $% $. in. or % in. % in.

    3 $. in.

    % % *

    63.7 in. 67 in.

    l d 

     f d l 

     f  

    αβλ 

    =

    = ⇒

    = =

    = ⇒

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    Moment Resistance DiagramsMoment Resistance Diagrams

    The ultimate momentresistance is %6 8-in.

    The moment diagram

    is drawn to scale on

    the basis bar can be

    terminated at a' two

     bars at b and three bars

    at c. These are thetheoretical termination

    of the bars.

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    Moment Resistance DiagramsMoment Resistance Diagrams

    )t is necessary to develop

     part of the strength of the bar

     by bond. The () (ode

    specifies that every barshould be continued at least

    a distance d' or $%d b ' which

    ever is greater' beyond the

    theoretical points a' b' and c.0ection $%.$$.$ specify that

    $

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    Moment Resistance DiagramsMoment Resistance Diagrams

    Two bars must e!tend

    into the support and

    moment resistance

    diagram ;ub mustenclose the e!ternal

     bending moment

    diagram.

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    Example – Cutoff Example – Cutoff  

    For the simplysupported beam with

     b=$ in. d =$1.3 in.'

    f y

    =6 8si and f c

    =* 8si

    with 6 > bars. 0how

    where the reinforcing

     bars can be terminated.

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    Example – Cutoff Example – Cutoff  

    Determine the moment capacity of the bars.

    ( ) ( )( ) ( )

    ( ) ( )

    %

    s y

    c

    %

    nb

    *.$7 in 6 8si 6.?* in..3 .3 * 8si $ in.

    6.?* in.

    .1? in 6 8si $1.3 in. %

    6%1.1 8-in. *3.76 8-ft.

     A f  a f b

     M 

    = = =

    = − = ⇒

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    ExampleExample  – Cutoff  – Cutoff 

    Determine the location of the bar intersections ofmoments.

    $ bar *3.76 8-ft.

    % bar 1$.* 8-ft.

    =

    =

    ( )   M x M mx= −

    * bar $1 8-ft.

    6 bar $6%.7 8-ft.

    =

    =

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    ExampleExample  – Cutoff  – Cutoff 

    Determine the location of the bar intersections ofmoments.

    $ bar *3.76 8-ft.

    % bar 1$.* 8-ft.

    =

    =

    $*%.3 8-ft. 1.3 8-ft.$1 8-ft. $*%.3 8-ft.

    7 ft.

    *.6 ft. 6. in. or 6$ in.

     x

     x

    −  = − ÷

     = ⇒

    * bar $1 8-ft.

    6 bar $6%.7 8-ft.

    =

    =

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    ExampleExample  – Cutoff  – Cutoff 

    Determine the location of the bar intersections ofmoments.

    $ bar *3.76 8-ft.

    % bar 1$.* 8-ft.

    =

    =

    * bar $1 8-ft.

    6 bar $6%.7 8-ft.

    =

    =

    1.3 8-ft. . 8-ft.1$.* 8-ft. 1.3 8-ft.

    3 ft.

    .?* ft. $$.$ in. or $$ in.

    or $$ in. + 1% in. = * in. from center 

     x

     x

    −  = − ÷

     = ⇒

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    Example – Cutoff Example – Cutoff  

    The minimum distance is

    ( )

    ( ) ( )

    a b

    y b

    d

    c

    $% or d

    $% $. in. or $1.3 in. $ in.

    6 $. in.

    % % *

    *7.7 in. *1 in.

    l d 

     f d l 

     f  

    αβλ 

    =

    = ⇒

    = =

    = ⇒

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    Example – Cutoff Example – Cutoff 

    The minimum amount of bars are s

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    ExampleExample  – Cutoff  – Cutoff 

    The cutoff for the first bar is 6$ in. or * ft 3 in. and $ in

    or $ ft 7 in. total distance is 6$ in.+$ in. = 3? in. or 6 ft

    $$ in.

    Note error it is 4’-11” not 5’-11”

    E lE l C ffC t ff

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    ExampleExample  – Cutoff  – Cutoff 

    The cutoff for the second bar is * in. + $ in. $$ in. or

    ft 3 in. "*1-in+3-in+$-in+6$-in= $$-in.#

    Note error it is 4’-11” not 5’-11”

    E lE l C t ffC t ff

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    ExampleExample  – Cutoff  – Cutoff 

    The moment diagram is the blue line and the red line is

    the envelope which encloses the moment diagram.

    Bar plicesBar plices

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    pp

    @hy do we need bar splicesA -- for long spans

    Types of 0plices

    $. 4utted B@elded

    %. ;echanical (onnectors

    *. Cay 0plices

    ;ust develop $%3of yield strength ()

    $%.$6.*.% and ()

    $%.$6.*.6

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    !ension Lap plices!ension Lap plices

    @hy do we need bar splicesA -- for long spans

    Types of 0plices

    $. (ontact 0plice

    %. Non-(ontact 0plice "distance between the

     bars 7 and $

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    !"pes of plices!"pes of plices

    Class A Splice  "()

    $%.$3.%#@hen over entire splice

    length.

    and $

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    !"pes of plices!"pes of plices

    Class B Splice  "() $%.$3.%#

    ll tension lay splices not meetingre9uirements of (lass 0plices

    ! i L li #$C% &' &)*! i L li #$C% &' &)*

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    !ension Lap plice #$C% &'(&)*!ension Lap plice #$C% &'(&)*

    wheres "re9Ed# = determined for bending

    ld = development length for bars "not

    allowed to use e!cess reinforcementmodification factor#

      ld must be greater than or e9ual to $% in.

    !ension Lap plice #$C% &' &)*!ension Lap plice #$C% &' &)*

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    !ension Lap plice #$C% &'(&)*!ension Lap plice #$C% &'(&)*

    Cap 0plices shall not be used for bars larger than No. $$."() $%.$6.%#

    Cap 0plices should be placed in away from regions of

    high tensile stresses -locate near points of inflection"() $%.$3.$#

     

    C i L li #$C% &' &+*

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    Compression Lap plice #$C% &'(&+*Compression Lap plice #$C% &'(&+*

    Cap' re9Ed = .3f y d b   for f y  7 psi

    Cap' re9Ed = ".?f y -%6# d b  for f y  7

     psi Cap' re9Ed $% in 

    For f c  * psi' re9uired lap splice shall be multiply

     by "6

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    Compression Lap plice #$C% &'(&,('*Compression Lap plice #$C% &'(&,('*

    )n tied column splices with effective tie area throughout

    splice length .$3 hs  factor = .*

     )n spiral column splices' factor = .13

    The final splice length must be $% in.

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    Example – plice !ensionExample – plice !ension

    (alculate the lap-splice length for 7 > tension bottom

     bars in two rows with clear spacing %.3 in. and a clear

    cover' $.3 in.' for the following cases

    @hen * bars are spliced and s"provided# 

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    Example – plice !ensionExample – plice !ension

    For > bars' d b =$. in and α = β = γ  = λ =$.

    ( )

    yd

     b c tr 

     b

    *

    6

    * 7 $.

    6%.6 6* in.$.3 in. 6 3

    $. in.

     f  l 

    d    f     c K 

    αβγλ =

     + ÷  

    = = ⇒+   ÷  

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    Example – plice !ensionExample – plice !ension

    The s"provided# 

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    Example – plice CompressionExample – plice Compression

    a# f y = 7 8si

     b# f y = 8si

    (alculate the lap splice length for a > $ compression

     bar in tied column when f c= 3 8si and

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    Example – plice CompressionExample – plice Compression

    For >$ bars' d b =$.%1 in.

    ( )

    ( )

    ydy

     b c

    d d

    .%.*

    .% 7$7.?1 or $

    3

    $ $.%1 in. %%.7 in. %* in.

     f  l  f  

    d    f  

    l l 

    = ≥

    = =

    = = ⇒ =

    (hec8 ls  .3 d b f y = *.$ in. 0o ls = *? in.

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    Example – plice CompressionExample – plice Compression

    For >$ bars' d b =$.%1 in. The ld = %* in.

    (hec8 ls  ".? f y J%6# d b 

    =".?"#-%6#"$.%1in.# = 7$ in.

    0o use ls = 7$ in.