session 5-bending workshop

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  • 7/29/2019 Session 5-Bending Workshop

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    Thomas Telford Guide to EC2-2 C R Hendy/D A Smith

    12/09/13

    Worked Example (not in notes): Reinforced concrete beam

    Find the ultimate sagging moment resistance of the beam in Figure 1 using the

    simplified rectangular stress block with 7 No. 20 bars (As = 2199 mm2)

    Reinforcement is B500B and C35/45 concrete

    cc = 0.85 (bridges value)

    s = 1.15

    c = 1.5 cu3 = 0.0035

    171688077.doc Page 1 of 5

    cu3

    s

    x

    d

    b

    As

    x

    z

    Fc

    Fs

    fcd

    x

    zfAzFMyds

    s ==

    =

    bdf

    Afdz

    cd

    syd

    21

    cd

    yds

    fb

    fAx

    =

    +

    1

    1

    3cuss

    yk

    E

    fd

    x

    dx>

    Forfck

    = 35 MPa, = 0.8 and = 1.0. d= 1500 50 10 = 1440 mm

    Assuming reinforcement yields:

    =

    =

    bdf

    AfdfAM

    cd

    syd

    yds2

    1

    Check that steel yields:

    ==cd

    yds

    fbfAx

    mm

    =d

    x

    =

    +1

    1

    3cuss

    yk

    E

    f

    so reinforcement yields and resistance moment =kNm.

    kNm

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    Thomas Telford Guide to EC2-2 C R Hendy/D A Smith

    12/09/13

    Figure 1

    171688077.doc Page 2 of 5

    150

    0m

    m

    7 No. 20

    diameter bars

    1000 mm

    50 mm

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    Thomas Telford Guide to EC2-2 C R Hendy/D A Smith

    12/09/13

    Worked Example 6.1-5: Prestressed concrete M beam

    Figure 6.1-10 - Prestressed concrete M beam

    Consider an M3 prestressed concrete beam with 160 mm deep insitu deck slab as

    illustrated in Figure 6.1-10. Calculate the ultimate moment of resistance (i) using a

    prestressing steel stress-strain relationship with a horizontal top branch, assuming the

    following properties:Class C30/37 slab concrete, fck = 30 MPa

    Class C40/50 beam concrete, fck= 40 MPa

    Parabolic concrete stress distribution therefore cu2 = 0.0035 and c2 = 0.0020

    Prestressing strands (using properties from EN 10138-3, Table 4):

    21 No. 15 mm strands of type Y1670S7

    Nominal diameter = 15.2 mm

    Nominal cross sectional area = 139 mm2

    Characteristic tensile strength, fpk = 1670 MPa

    Characteristic value of maximum force 232101670139 3 == kN

    Characteristic value of 0.1% proof force = 204 kN

    14681670879.01670232

    2041.0,

    ===kpf MPa

    Ep = 195 GPa

    s = 1.15

    Stressing and losses:

    Assume initial stressing to 75% fpkAllow 10% losses at transfer and a further 20% long term losses.

    Prestrain = long term strand stress / Eptherefore prestrain =

    171688077.doc Page 3 of 5

    970 mm

    1000 mm

    160 mm

    200 mm

    60 mm

    200 mm

    80 mm

    50 mm

    160 mm

    400 mm

    160 mm

    0 mm

    330 mm

    160 mm110 mm

    60 mm

    20 mm

    300 mm 30 mm

    80 mm

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    Thomas Telford Guide to EC2-2 C R Hendy/D A Smith

    12/09/13

    The values for reinforcement stress-strain curve first need to be defined as:

    5.127615.1

    1468==pdf MPa

    =

    s

    pkf

    MPa

    p

    pd

    E

    f

    (i) Consider horizontal top branch and a neutral axis depth, obtained by trial and error,

    of 335 mm:

    The strain profile is shown in Figure 6.1-11.

    (a) Idealisation (b) Strains (c) Compressive stresses

    Figure 6.1-11: Stress-strain profile for prestressed M beam

    Therefore total strains at ULS in the four layers of strands including prestrain are:

    =

    =

    =

    =+=

    4

    3

    2

    10102.00046.00056.0

    s

    s

    s

    s

    All strains are greater thanp

    pd

    Ef (=0.00655) therefore all stresses can be taken as fpd =

    1276.5 MPa.

    Thus total steel force, =sF kN.

    The neutral axis is in the top flange of the beam therefore split the compression zone

    into the following three sections and take account of the different concrete strengths:

    (1) Rectangular part of stress block in top slab (top 143.6 mm)

    (2) Parabolic part of stress block in top slab (bottom 16.4 mm)

    (3) Parabolic part of stress block in top flange to neutral axis (175mm deep)Using geometry of the parabolic-rectangular stress-strain distribution it can be shown

    171688077.doc Page 4 of 5

    0.0020

    0.0035

    0.0018

    0.0028

    0.00450.0051

    0.0056

    930 mm

    x =

    335 mm

    60 mm 110 mm

    160 mm

    330 mm

    160 mm 1000 mm

    250 mm

    400 mm

    335 mm

    160 mm

    185 mm 950 mm

    fcd,slab

    or fcd,beam

    a1

    a

    2 a3

    Fc1d

    Fc2d

    Fc3d

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    Thomas Telford Guide to EC2-2 C R Hendy/D A Smith

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    that:

    (1) Fc1 = 2440.7 kN with depth to centroid, a1 = 71.8 mm

    (2) Fc2 = 278.6 kN with depth to centroid, a2 = 149.7 mm

    (3) Fc3 = 1008.5 kN with depth to centroid, a3 = 225.6 mm

    Thus =cF kN

    sF therefore section balances and neutral axis is at the correct level. (Note that

    using the rectangular stress block would be much easier here).

    Taking moments about the neutral axis level gives a resistance moment of:

    =M

    kNm.

    Strictly, since the neutral axis is in the web, a new limiting strain diagram should be

    used in compliance with 2-1-1/6.1(6) as discussed in section 6.1.2.2 of this guide.

    This would require a strain limit of3

    21002

    = .c to be maintained at

    49153

    02160

    22.

    .

    ./h cuc == mm from the underside of the deck slab i.e. 68.6 mm

    from the top. The analysis was conservatively repeated using a strain limit of3

    2 1002

    = .c at the top of the deck slab which gave a resistance moment of 2585

    kNm.

    171688077.doc Page 5 of 5