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Column Interaction Curve (1)

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    Design of COLUMNS with Uniaxial Moment

    Analyse the given section whether it can carry given axial load

    and moment( one axis at a time)

    Design Parameters used as input for design are

    i. Dimensions b and D of the rectangular cross-section,

    ii. rades of concrete (fc!) and steel (fy)

    iii. "ongitudinal steel reinforcing #ars $ %o. of #ars and its

    distri#utionalong #& and D&. (%ot pt'fc! as per P *)iv. +over to longitudinal reinforcement d& (%ot d&'D as per P

    *)

    v. Axial "oad (Pu) for all the design cases

    . ased on the given design input parameters, graph of two non-dimensional parameters , Pu'fc!/#/d (for axial load) v's0u'fc!/#/d1 (for moment) are produced for the given columnsection from stress #loc! parameters.

    . 2or given axial load Pu and thus Pu'fc!/#/d, corresponding valueof 0u'fc!/#/d1 is found out #y interpolation. 2rom this value

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    To nd Stress for Steel(fs) and Concrete(fc)from Strain() al!es

    +3%+4565

    0aximum allowa#le strain in concrete in axial compression is7.771 while compression plus #ending is 7.7789.

    train due to tension in concrete is :ero.(+oncrete neglected intension :one)

    ;dealised tress-strain curve for concrete shows that up to strainof 7.771, stress varies para#olically with the e ==*/? ( $ 197/?)/ fc! for? @ 7.771 (Sim1lied form!la for c!re)

    > 7.==*/fc!for ? 7.771.

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    To nd Stress for Steel(fs) and Concrete(fc)from Strain() al!es

    655"

    o

    2e197 B Stress is linearl. 1ro1ortional to strain !1

    to .ield 1oint(i/e/ /$%f. 2 '3%/& m4a)/

    Therefore for strain !1 to('3%/&5'x3&)2/3$%&6 stress islinear/

    7or strain -e.ond /3$%&6 stress isconstant

    i/e/ fs 2 x 8s for 9/3$%&

    fs 2 /$%f. 2 '3%/& M4a for :

    /3$%&

    o CD ars (2e=9, 2e977, 2e*77)B

    Stress is linearl. 1ro1ortional to strain!1 to stress al!e of (/$ f.d 2 /$ x/$% f.)

    7rom /$f.d to 3/f.d6 stress ariation is

    (7e'&)

    7e=3&67e&67e>

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    To nd Stress for Steel(fs) and Concrete(fc)from Strain() al!es

    e.g. 2or 2e=9, at 7.E9 fydF

    #nelastic strain from gra1h 2 /3

    8lastic strain 2 /$&x/$%x=3& 5 'x3&2 /3&?

    Total strain 2 /3 < /3&? 2 /3>?

    Ta-le 1roided in s1readsheet

    Ta-le is 1roided in the s1readsheet with strains corres1onding tostresses ar.ing from /$f.d to 3/f.d for reference /

    Gith the help of these stress-strain relations for concrete andsteel, for any value of strain (?), corresponding stress in

    concrete (fc) and steel(fs) can #e found out.

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    Limiting Cases de1ending on Ne!tral @xis

    Depth of neutral axis (xu

    ) is varied with respect to total depth (D)

    through !u factor.

    o +ase B Axial "oad with :ero eccentricity (no ending moment)

    The entire cross;section is !nder direct com1ression with max/Strain of /'

    Pu

    0

    ax strain of 7.771 (in red)

    allowed

    +orresponding max. stress

    > 7.==* fc!

    !u 2 ;nHnity (1.9x77

    used in

    D

    Stress AlocB when B!

    2

    So!rce " *Design of +CCStr!ct!res, -. Dr/ Shah

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    Limiting Cases de1ending on Ne!tral @xis

    o +ase 1B %eutral Axis "ying outside the section ( xu I D F !u I )

    The tensile strains from -ending moments are less than the axialcom1ression strains/

    The entire cross;section is !nder com1ression with max/ Strain of/?& allowed for concrete

    Pu J

    0u

    0ax strain of 7.7789 (in red)

    allowed

    +orresponding max. stress

    > 7.==* fc! train at 8D'K (as shown in

    Hg) is always 7.771 when xuI D and therefore used asreference point for

    calculations.

    D

    ?min

    ?max(7.778

    9)

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    Limiting Cases de1ending on Ne!tral @xis

    o +ase 8B %eutral Axis "ying along the 5dge (xu > D)

    The tensile strains from -ending moments are eE!al to the axialcom1ression strains in magnit!de/

    The entire cross;section is !nder com1ression with max/ Strain of/?& and minim!m strain is F8+O

    Pu J

    0u

    0ax strain of 7.7789 (in

    red) allowed

    +orresponding max. stress

    > 7.==* fc!

    !u 2 3

    D

    ?min >

    7

    ?max

    (7.7789)

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    Limiting Cases de1ending on Ne!tral @xis

    o +ase 8B %eutral Axis "ying within the section (xu @ D)

    The tensile strains from -ending moments are more than the axialcom1ression strains in magnit!de/

    The strain ariation across the section is do!-le triang!lar with max/Com1ressie Strain of /?& and tensile strain(negatie strain) at theother edge

    Pu J

    0u

    0ax strain of 7.7789 (in red)allowed

    +orresponding max. stress >

    7.==* fc!

    6ensile strain of concrete

    ignored train and therefore stress in

    steel #ars in tension side areta!en negative (as shown in

    D

    ?max

    (7.7789)

    ? > -ve

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    Limiting Cases de1ending on Ne!tral @xis

    o +ase 8B %eutral Axis "ying within the section (xu @ D)

    ) alanced section point(!u > !u,max) B Aoth tensile andcom1ressie strains reach .ield

    1) Pure Lexure point (Pu>7) and

    8) Pure tensile axial load point (Mu N 7, Pu @ 7 , 0u > 7)

    (f)

    4t/ (c) " 4!re com1ression 1oint (B!2

    )4t/ (d) " Com1ression < Aending (B!23 )

    4t/ (-) " Aalanced Section 1oint4t/ (a) " 4!re 7lex!re 4oint4t(f) " 4!re tension 1ointGence if !

    uis aried from

    to innit.6 all the 1oints of4!;M! #nteraction C!recan -e 1lotted for giencross section

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    4+OC8DU+8 @DO4T8D TO 7#ND MOM8NTC@4@C#TH O7 COLUMN S8CT#ON

    3) @ss!me diIerent al!es of ne!tral axis with res1ect to de1th of section/

    i/e/ !u is aried from /3 (1!re tension 1oint) to '/&e33 2 innit. (1!recom1ression)

    ') De1ending if !u J 3 6 or !u 3 6 two form!las to calc!late strain al!e at

    diIerent leels of steel -ars are !sed/

    ?) Kith the relationshi1s form!lated -etween strains and stresses -efore6 stressesfor concrete in com1ression and for each row or section of steel -ars are calc!lated/

    !uIi2 /' xi5 (x!

    ?D5%)

    !uO i2 /?& xi 5 x!

    Khere i2 strain of steel at ithrow

    xi2 distance of ithrow from ne!tral axis

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    4+OC8DU+8 @DO4T8D TO 7#ND MOM8NT C@4@C#TH O7 COLUMNS8CT#ON

    =) 7or e

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    4+OC8DU+8 @DO4T8D TO 7#ND MOM8NT C@4@C#TH O7 COLUMNS8CT#ON

    Case '" Khen ne!tral axis l.ing o!tside the section !u 3

    4!c 2 @rea of stress

    -locBP-

    2 /==>(3;C?5>)Q

    PfcB PD

    2 C3PfcBPD

    Khere C?form!la is as

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    4+OC8DU+8 @DO4T8D TO 7#ND MOM8NT C@4@C#TH O7 COLUMNS8CT#ON

    Case ' (Contd)" Khen ne!tral axis l.ing o!tside the section !u 3

    7or nding centroid from highl. com1ressed edge

    Centroid from com1ressed

    edge 2 C'PD

    Khere C'form!la is as

    shown in the 1ict!re

    a-oe

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    4+OC8DU+8 @DO4T8D TO 7#ND MOM8NT C@4@C#TH O7 COLUMNS8CT#ON

    =) c

    c

    c2 Moment of resistance oIered -. concrete in com1ression

    2 4!cx leer arm

    De1ending if !uJ 3 6 or !u 3 6 two form!las are !sed to calc!late leer arm/

    !uI

    Leer arm 2 (/&D C'D)

    !uO

    Leer arm 2 (/&D /=3>B!)

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    4+OC8DU+8 @DO4T8D TO 7#ND MOM8NT C@4@C#TH O7 COLUMNS8CT#ON

    =) c

    c

    2 Total axial com1ressie resistance oIered -. steel at diIerent leels in thesection

    (same for -oth cases of !u)

    > PusJ Pus1J RR.. J Pusn

    >Khere

    i 2 serial n!m-er of the row of reinforcement

    n 2 n!m-er of rows of steel -ars

    2 cross;sectional area of steel in the ithrow

    fsi 2 stress in steel in the ithrow ( Calc!lated from stress;strain relation)

    (Com1ressiestress taBen as 1ositieand tensilestress taBen negatie)

    fci 2 Com1ressie stress in concrete at the ithrow of reinforcement

    2 @lge-raic s!m of the moments of resistance oIered -. steel at diIerent leels

    (same for -oth cases of !u)

    > / yi) ( where .i2 distance of the ithrow from the centroid ofthe section)

    OC O O O C C O CO

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    4+OC8DU+8 @DO4T8D TO 7#ND MOM8NT C@4@C#TH O7 COLUMNS8CT#ON

    &) 7or diIerent al!es of !ustarting from /3 ( almost Qero 2 1!re tension case)

    till

    '/&x333

    (innit. 2 1!re com1ression case)6 al!es of 4! and M! are fo!nd o!tfor the gien section/

    >) The interals taBen -etween these two extreme al!es are as follows/

    %) 7iner interals are taBen from /? to /% to get closer to the -alanced section

    1oint which !s!all. lies in this range for an. section/

    $) 7rom 4! 6 we get al!es of 4!5fcBP-PD/

    P P '

    6rial !u

    3 /3

    ' /&

    ? /3

    = /3& /&

    > /3

    % /&

    $ /%&

    6rial ! u

    R /3

    3 /'

    33 /?

    3' /?&

    3? /=

    3= /=&

    3& /&

    3> /&&

    6rial ! u

    3% />

    3$ />&

    3R /%

    ' /%&'3 /$

    '' /R

    '? 3/

    '= 3/3

    6rial ! u

    '& 3/'

    '> 3/??

    '% 3/&

    '$ ''R '/&x3&

    4+OC8DU+8 @DO4T8D TO 7#ND MOM8NT C@4@C#TH O7 COLUMN

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    4+OC8DU+8 @DO4T8D TO 7#ND MOM8NT C@4@C#TH O7 COLUMNS8CT#ON

    3) Aoth these series are 1lotted as a c!re on a gra1h with increasing !u/

    H;axis ;;; 4!5fcBP-PD

    ;axis ;;; M!5fcBP-PD'


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