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N.W.F.P. University of Engineering and
        Technology P h
        T h l       Peshawar




    Lecture 13: Plate Girder




       By: Prof Dr. Akhtar Naeem Khan
              chairciv@nwfpuet.edu.pk

                                         1
Plate Girders
       A girder is a flexural member which is required
        to carr hea loads on relati el long spans
           carry heavy           relatively




CE-409: Lecture 13        Prof. Dr Akhtar Naeem Khan     2
Plate Girder




CE-409: Lecture 13       Prof. Dr Akhtar Naeem Khan   3
Plate Girder
         Plate girders are typically used as long-span
                g            yp    y              g p
         floor girders in buildings, as bridge girders, and
         as crane girders in industrial structures.
                   g
         Commonly term girder refers to a flexural x-
         section made up of a number of elements
                                        elements.
         They are generally considerably deeper than the
             y     g        y          y      p
         deepest rolled sections and usually have webs
         thinner than rolled sections.



CE-409: Lecture 13          Prof. Dr Akhtar Naeem Khan        4
Plate Girder
       Modern plate girders are normally fabricated
       by welding together two flanges and a web
       p
       plate.




CE-409: Lecture 13       Prof. Dr Akhtar Naeem Khan   5
Plate Girder
           Plate girders are at their most impressive in
           modern b id construction where main spans of
              d     bridge      t ti      h       i        f
           well over 200m are feasible, with corresponding
           cross-section d th h
                     ti depths, haunched over th
                                        h d      the
           supports, in the range of 5-10m.




CE-409: Lecture 13          Prof. Dr Akhtar Naeem Khan         6
Plate Girder

               Because plate girders are fabricated
               separately, each may be designed
                  p      y,           y         g
               individually to resist the applied
               actions using proportions that ensure
               low self-weight and high load
               resistance.
               resistance




CE-409: Lecture 13          Prof. Dr Akhtar Naeem Khan   7
Plate Girder
         Changes in X-Section

           There is also considerable scope for variation
           of cross-section in the longitudinal direction.
           Ad i
             designer may choose t reduce th fl
                             h       to d      the flange
           thickness (or breadth) in a zone of low
           applied moment
                   moment.
           Equally, in a zone of high shear, the designer
           might choose to thicken the web plate.




CE-409: Lecture 13          Prof. Dr Akhtar Naeem Khan       8
Plate Girder
           Changes in Material


            Alternatively, higher g
                        y g       grade steel might be
                                                  g
            employed for zones of high applied moment
            and shear, while standard grade would be
            used elsewhere. S
                d l     h      So-called "h b id" girders
                                    ll d "hybrid" i d
            with different strength material in the flanges
            and the web offer another possible means of
            more closely matching resistance to
            requirements.
            requirements



CE-409: Lecture 13            Prof. Dr Akhtar Naeem Khan      9
Plate Girder




CE-409: Lecture 13       Prof. Dr Akhtar Naeem Khan   10
Plate Girder




CE-409: Lecture 13       Prof. Dr Akhtar Naeem Khan   11
Plate Girder
             Any cross-section of a plate girder is normally
             subjected to a combination of shear force and
             bending moment.
             The primary function of the top and bottom
             flange plates of the girder is to resist the axial
             compressive and tensile forces arising from
             the applied bending moment.
                                   moment
             The primary function of the web plate is to
             resist the applied shear force.


CE-409: Lecture 13             Prof. Dr Akhtar Naeem Khan         12
Plate Girder
           Plate girders are normally designed to support
           heavy loads over long spans in situations where it
           is necessary to produce an efficient design by
           providing girders of high strength to weight ratio.
           To produce the lowest axial flange force for a
           given bending moment, the web depth (d) must be
           made as large as possible. To reduce the self
           weight, the web thickness (tw) must be reduced to
           a minimum
             minimum.
           As a consequence, in many instances the web
           plate is of slender proportions and i th f
            l t i f l d              ti       d is therefore
           prone to buckling at relatively low values of
           applied shear
                    shear.
CE-409: Lecture 13            Prof. Dr Akhtar Naeem Khan         13
Plate Girder
               For efficient design it is usual to choose a
               relatively deep girder, thus minimizing the
               required area of flanges for a given applied
               moment, Msd.
                       t
               This obviously entails a deep web whose
                             y             p
               area will be minimized by reducing its
               thickness to the minimum required to carry
               the applied shear, Vsd.
                h     li d h
               Such a web may be quite slender (
                                y   q             (i.e. a high
                                                            g
               d/tw ratio) and may be prone to local buckling
               and shear buckling.

CE-409: Lecture 13             Prof. Dr Akhtar Naeem Khan        14
Plate Girder
             Web buckling does not determine the
             ultimate strength of a plate girder.
              lti t t       th f     l t id
             Plate elements do not collapse when they
                                         p           y
             buckle; they can possess a substantial post-
             buckling reserve of resistance.
             For an efficient design, any calculation
             relating to the ultimate limit state should take
                    g
             the post-buckling action into account.




CE-409: Lecture 13            Prof. Dr Akhtar Naeem Khan        15
Design Criteria
       Criteria for design of plate girder may be
        based on
            Elastic bend-buckling strength
            Elastic h
            El ti shear-buckling strength
                        b kli     t    th
            Post-bend-buckling
            Post bend buckling strength
            Post shear buckling(Tension
            Post-shear-buckling(Tension field)strength


CE-409: Lecture 13        Prof. Dr Akhtar Naeem Khan     16
Design Criteria

               The designer has the choice of following four
               combinations
       1. Elastic bend buckling + Elastic shear buckling
                              g                        g
          (conventional flexural behavior)
       2.
       2 Elastic bend buckling + Post shear buckling
       3. Post bend buckling + Elastic shear buckling
                           g                        g
       4. Post bend buckling + Post shear buckling

CE-409: Lecture 13            Prof. Dr Akhtar Naeem Khan       17
Elastic Bend Buckling
                 Strength
            The extreme f  fiber bending stress at which a
            perfectly flat web buckles is given by




CE-409: Lecture 13           Prof. Dr Akhtar Naeem Khan      18
Elastic Bend Buckling
                 Strength
             Using a FOS of 1.25 w.r.t service load bending
             stress fb gives an eqnuation which is AASHTO
             slenderness limit for plat girders webs




                Using AASHTO allowable stress fb=0.55Fy
                     “ h/t=165 f A36 steel “
                       h/t 165 for    t l
CE-409: Lecture 13             Prof. Dr Akhtar Naeem Khan     19
Elastic Bend Buckling
                 Strength
       The bend buckling resistance of beam webs can be
       increased considerably by reinforcing the slender webs
       with Longitudinal stiffeners.
       Means webs thinner than those given by the equation can be
       used.
       used




              A typical longitudinally stiffened girder is shown after failure

CE-409: Lecture 13                        Prof. Dr Akhtar Naeem Khan             20
Web Stiffeners

           They usually consists of rectangular
           bars to welded to web.
           Transverse stiffeners may be in pairs,
           one on each side of web, or they may
           placed on one side of web.
           Longitudinal stiffeners are usually
           placed on one side of web.

CE-409: Lecture 13        Prof. Dr Akhtar Naeem Khan   21
Web Stiffeners




CE-409: Lecture 13        Prof. Dr Akhtar Naeem Khan   22
Web Stiffeners




CE-409: Lecture 13        Prof. Dr Akhtar Naeem Khan   23
Web Stiffeners
         The main function of the longitudinal stiffeners is
         to increase the buckling resistance of the web
         with respect o bot s ea a d be d g loads. An
           t espect of both shear and bending oads
         effective stiffener will remain straight, thereby
         sub-dividing the web p
                     g            panel and limiting the
                                                   g
         buckling to the smaller sub-panels. The resulting
         increase in the ultimate resistance of the girder
                                                       g
         can be significant.




CE-409: Lecture 13          Prof. Dr Akhtar Naeem Khan         24
Web Stiffeners
          Efficiency of stiffener is a function of its location
          in the compression zone
          The optimum location for a longitudinal stiffener
          has been determined to be at least h/5 from
          compression edge.
          In this case k=129. The corresponding allowable web
                       k 129.
          slenderness is h/t=330 as compare to 165




CE-409: Lecture 13             Prof. Dr Akhtar Naeem Khan         25
Web Stiffeners
          Stiffener acts as a beam supported at the ends
          where a vertical stiffener holds the web in line
                                                      line.
          Stiffener acts as a beam column and hence must
          be
          b proportioned i t
                    ti    d in terms of x-sectional area and
                                      f      ti   l        d
          moment of inertia.
          AASHTO specifies Is as




          Stiffener acts as a beam supported at the ends
          where a vertical stiffener holds the web in line.

CE-409: Lecture 13            Prof. Dr Akhtar Naeem Khan       26
Web Stiffeners
             The stiffeners must also be proportioned to
             resist local buckling.
                          buckling
             For plates supported on one longitudinal
                 p        pp                g
             edge AASHTO require b/t<1625/√fb
             Multiple longitudinal stiffeners are used for
             large depth webs.
             As longitudinal stiffener is also acting as a
             column so it must be satisfied for critical
             stress (Fcrs>0.6Fcrf)


CE-409: Lecture 13            Prof. Dr Akhtar Naeem Khan     27
Post buckling bending
               strength

        If bending strain increases after Fcr, the upper
                 g                           ,      pp
        edge of panels shortens and bottom edge
        lengthens.
        If web were to remain flat there will be increase in
        stress.
        Because the web has buckled, the increase in
        stress is non linear
                  non-linear.


CE-409: Lecture 13          Prof. Dr Akhtar Naeem Khan         28
Post buckling bending
               strength
        As
        A variation i post-buckled state i not k
               i ti in    t b kl d t t is t known,
        simplify assumptions are made.
        Non-linear compression is replaced with linear
        distribution acting on effective depth be.




CE-409: Lecture 13         Prof. Dr Akhtar Naeem Khan    29
Post buckling bending
                strength
        Point A gives point that enables a girder to reach its full
        yield moment(925 /√Fy=154).
        If stiffeners at h/5 is provided gives point B
                                                     B.

    Considering the
    post buckling                                    A         B
    strength, the                                                      0.94
                                                                        0.82
                                                                        0 82
    point where             M/My
    reduction in web                                                    0.4
    effectiveness                                                      0.18
                                                                       0 18
    begins s taken to
                                                   154         315   360
    be 980/√Fy=170.
       980/√Fy 170.
                                                         h/t
CE-409: Lecture 13              Prof. Dr Akhtar Naeem Khan                     30
Post buckling bending
                strength
          Equation connecting the revised point A
          with points corresponding t h/t 360 i
           ith i t             di to h/t=360 is




CE-409: Lecture 13       Prof. Dr Akhtar Naeem Khan   31
Post buckling bending
                strength
           LRFD




           Where




CE-409: Lecture 13   Prof. Dr Akhtar Naeem Khan   32
Compression Flange Vertical
        buckling




CE-409: Lecture 13   Prof. Dr Akhtar Naeem Khan   33
Compression Flange Vertical
        buckling
      If plate girder web is too slender the compression
         plate-girder            slender,
      flange may buckle in vertical plane at stress less
      than yield stress
                  stress.
      The compression flange is a beam-column
              p             g
      continuous over vertical stiffener as supports
      Its stability depends on stiffener spacing and
      relative stiffness of the flange and the web. Fcr is




CE-409: Lecture 13         Prof. Dr Akhtar Naeem Khan        34
Compression Flange Vertical
        buckling
   Slenderness of webs with vertical stiffeners is taken conservatively




    AISC ASD/LRFD li it the h/t by the given equation with
                  limits th     b th i           ti    ith
    Aw/Af =0.5




CE-409: Lecture 13             Prof. Dr Akhtar Naeem Khan                 35
Shear buckling of beam webs
             Shear buckling is seldom a determining
             factor i d i
             f t in design of rolled section b t
                              f ll d     ti but
             plate girders have much larger h/t so it
             must be considered.
                  tb       id d




CE-409: Lecture 13         Prof. Dr Akhtar Naeem Khan   36
Shear buckling of beam webs
            Transverse stiffeners are used to
            increase th b kli strength b
            i        the buckling t      th by
            increasing factor k through a reduction
            in aspect ratio a/h.




CE-409: Lecture 13         Prof. Dr Akhtar Naeem Khan   37
Transverse Stiffeners
        Transverse stiffeners play an important role in
        allowing the full ultimate load resistance of a
        plate girder to be achieved.
        In the first place they increase the buckling
        resistance of the web;
        Secondly they must continue to remain effective
        after the web buckles, to provide anchorage for
                                  p              g
        the tension field;
        finally they must prevent any tendency for the
        flanges to move towards one another.


CE-409: Lecture 13         Prof. Dr Akhtar Naeem Khan     38
Transverse Stiffeners
      The satisfactory performance of a
      transverse stiffener can best be illustrated
      by comparing the girders shown, after
                                shown
      testing.




                                                                Figure 2
                                                                  g
                     Figure 1
                     Fi
CE-409: Lecture 13                 Prof. Dr Akhtar Naeem Khan              39
Transverse Stiffeners
        In Figure 1 the stiffeners have remained straight.
             g                                        g
        In Figure 2 the stiffener has failed and has been
        unable to limit the buckling to the adjacent sub-
                                                      sub
        panels of the girder; instead, the buckle has run
        through the stiffener p
              g                 position extending over
                                                 g
        both panels. Consequently, significant reduction
        in the failure load of the girder occurred.
        In Figure 1 One can also see the effect of aspect
        ratio,i.e greater a/ less k a d s a Fcr.
         at o, e g eate a/h ess and small c



CE-409: Lecture 13         Prof. Dr Akhtar Naeem Khan        40
Transverse Stiffeners
           The stiffener must be of adequate
           rigidity in th di ti perpendicular t
            i idit i the direction        di l to
           the plane of the web to prevent web
           buckling. This condition is satisfied
           p
           provided the stiffener has a second
           moment of area Is that satisfies the
           following empirical formulae:




CE-409: Lecture 13       Prof. Dr Akhtar Naeem Khan   41
Transverse Stiffeners


               AISC/LRFD Moment of Inertia of
               stiffener is:
                tiff     i


          where




CE-409: Lecture 13         Prof. Dr Akhtar Naeem Khan   42
Transverse Stiffeners

               Transverse stiffeners spacing can be
               determined from the following




CE-409: Lecture 13          Prof. Dr Akhtar Naeem Khan   43
Tension Field Action
          The resulting shear stresses on an
          element of a web are equivalent t
           l      t f      b        i l t to
          principal stresses, one Tensile and one
          Compressive, at 45 to the shear stress.




CE-409: Lecture 13       Prof. Dr Akhtar Naeem Khan   44
Tension Field Action

         Once a web panel has buckled in shear, it
                       p                          ,
         loses its resistance to carry additional
         compressive stresses.
                        stresses
         On the other hand tensile principal stress
                                    p     p
         continues to increase in strain in the
         diagonal direction.
                  direction
            Such a panel has a considerable p buckling strength,
                    p                          post         g      g ,
            since increase in tension is limited only by yield stress.


CE-409: Lecture 13               Prof. Dr Akhtar Naeem Khan              45
Tension Field Action

        In this post b ckling range a ne load carr ing
                post-buckling range, new load-carrying
        mechanism is developed, whereby any additional
        shear load is carried by an inclined tensile
        membrane stress field. This tension field anchors
        against the top and bottom flanges and against the
        transverse stiffeners on either side of the web
        panel. The load-carrying action of the plate girder
        than becomes similar to that of the N-truss
        In the post-buckling range, the resistance offered by
        the web plates is analogous to that of the diagonal
        tie bars in the truss.


CE-409: Lecture 13          Prof. Dr Akhtar Naeem Khan          46
Tension Field Action
      Phases of behavior up to collapse of a typical panel in shear




      Prior to Buckling        Post Buckling                Collapse




CE-409: Lecture 13             Prof. Dr Akhtar Naeem Khan              47
Tension Field Action

             The load-carrying action of the plate girder
                 load carrying
             than becomes similar to that of the N-truss
             In the post-buckling range, the resistance
             offered by the web plates is analogous to
             that of the diagonal tie bars in the truss.




CE-409: Lecture 13           Prof. Dr Akhtar Naeem Khan     48
Tension Field Action




CE-409: Lecture 13      Prof. Dr Akhtar Naeem Khan   49
Tension Field Action




CE-409: Lecture 13      Prof. Dr Akhtar Naeem Khan   50
Tension Field Action


                                                                   ft            V
                                              V




              Vt=Tsinφ
              Vt = ft ht cosφ sinφ                                      T=ft ht cosφ

              Vt = (1/2)ft ht sin2φ                                          φ

              Vt =(1/2) ft ht    φ=45
              Vty=(1/2) Fy ht………….(1)
CE-409: Lecture 13                    Prof. Dr Akhtar Naeem Khan                       51
Tension Field Action
                     Vty   =(1/2) Fy ht      = Fy

                     Vy         Fvy ht           2Fvy
                     Vty = √3 Vy = 0.87 Vy
                            2




CE-409: Lecture 13                       Prof. Dr Akhtar Naeem Khan   52
Tension Field Action




          The angle φ for which Vt is max




CE-409: Lecture 13              Prof. Dr Akhtar Naeem Khan   53
Tension Field Action




     Where

CE-409: Lecture 13      Prof. Dr Akhtar Naeem Khan   54
Tension Field Action


                                                             (1)

        Taking inelastic and strain hardening range

                                                             (2)

                                                             (3)




CE-409: Lecture 13              Prof. Dr Akhtar Naeem Khan         55
Tension Field Action
               Codal equations are derived from
               eqn;(1),(2),(3)




CE-409: Lecture 13          Prof. Dr Akhtar Naeem Khan   56
Tension Field Action

             AISC/LRFD


                                                      k



                                                          a/h




CE-409: Lecture 13       Prof. Dr Akhtar Naeem Khan             57
Combined Bending & Shear
            of Webs

           Interaction diagram is based on Tension-
           field f
           fi ld of webs
                      b
           If the web is completely yielded in
           shear,any accompanying moment must
           be
           b resisted entirely b fl
                  i t d ti l by flanges.




CE-409: Lecture 13        Prof. Dr Akhtar Naeem Khan   58
Combined Bending & Shear
     Bending & shear Interaction Curve




                 B                 B C          D
       V vyAw)
       V/(F A




                                                    E 1/√3




                                  0.75 0.83   1.0 1.07 1.12   M/My
CE-409: Lecture 13          Prof. Dr Akhtar Naeem Khan               59
Combined Bending & Shear
                     1.0

     Mu/φMn
                     0.8



                     0.6

                           LRFD I t
                                Interaction Curve
                                       ti C
                     0.4




                     0.2




                            0.2   0.4        0.6        0.8     1.0   Vu/φVn
CE-409: Lecture 13                 Prof. Dr Akhtar Naeem Khan                  60
Web Proportioning
           Notations




CE-409: Lecture 13         Prof. Dr Akhtar Naeem Khan   61
Web Proportioning


             Depth of girder is influenced by many
             factors:
                     Headroom
                     Clearance for high water in deck bridges
                     Traffic passing beneath the bridge




CE-409: Lecture 13                 Prof. Dr Akhtar Naeem Khan   62
Web Proportioning

           Depth: Overall girder depth, h, will
           usually be in the range
                     Lo/12 ≤ h ≤ Lo/8
                                   /8,
                     occasionally lighter loads may be
                     accommodated with Lo/20 /20.

           Flange:
               g

                     The breadth, b, will usually be in the range
                     h/5 ≤ b ≤ h/3,

CE-409: Lecture 13                    Prof. Dr Akhtar Naeem Khan    63
Design Procedure
  1. Maximum Moment & Shear for Factored Load
  2. Web D i
  2 W b Design
        1.              p      girder L/12 ≤ h ≤ L/8
               Assume depth of g
        2.     Depth of Web hw=h-2tf
        3.     Web slenderness
              1.     For a/h <5 …………….
              2.     and for a/h > 5 ……………………
              3.
              3      hw/tw= 970/√Fy
              4.     Select optimum tw


CE-409: Lecture 13                    Prof. Dr Akhtar Naeem Khan   64
Design Procedure


        4. Flange Design
              1.     Find Af
              2.     Select suitable tf and bf
              3.
              3      Flange slenderness
                     1.   bf/ 2tf < 65/√Fy …………….Compact




CE-409: Lecture 13                 Prof. Dr Akhtar Naeem Khan   65
Design Procedure
     5.
     5 Check trial girder section
           1.    Web local buckling limit state
                1.   hw/tw< 640/√Fy…………………..Compact
                2.   640/√Fy< hw/tw < 970/√Fy……Non-Compact
                3.   hw/tw > 970/√Fy…………………..Slender
           2.    Flange local buckling limit state
                1.   bf/ 2tf < 65/√Fy …………….Compact
           3.    Lateral Torsional Buckling
                                          g
                1.   Calculate Iy
                2.   A=Af+Aw/6
                3.   ry= √Iy/A
                4.   Find Lb/ry
                5.   λp= 300/√Fy ………….. λ< λp ______Compact
CE-409: Lecture 13                  Prof. Dr Akhtar Naeem Khan   66
Design Procedure
        6. Bending strength
              1.     Calculate
                     C l l t Ix
              2.     Calculate Sxt
              3.     .


              4.     .


              5.     φMn≥ Mu


CE-409: Lecture 13                Prof. Dr Akhtar Naeem Khan   67
Procedure for Design
        6. Bending strength
              1.     Calculate Ix
              2.
              2      Calculate Sxt
              3.     .


              4.     .


              5.
CE-409: Lecture 13
                     φMn≥ Mu        Prof. Dr Akhtar Naeem Khan
52436966 lecture-13-plate-girders
52436966 lecture-13-plate-girders
52436966 lecture-13-plate-girders
52436966 lecture-13-plate-girders
52436966 lecture-13-plate-girders
52436966 lecture-13-plate-girders
52436966 lecture-13-plate-girders
52436966 lecture-13-plate-girders
52436966 lecture-13-plate-girders
52436966 lecture-13-plate-girders
52436966 lecture-13-plate-girders

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52436966 lecture-13-plate-girders

  • 1. N.W.F.P. University of Engineering and Technology P h T h l Peshawar Lecture 13: Plate Girder By: Prof Dr. Akhtar Naeem Khan chairciv@nwfpuet.edu.pk 1
  • 2. Plate Girders A girder is a flexural member which is required to carr hea loads on relati el long spans carry heavy relatively CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 2
  • 3. Plate Girder CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 3
  • 4. Plate Girder Plate girders are typically used as long-span g yp y g p floor girders in buildings, as bridge girders, and as crane girders in industrial structures. g Commonly term girder refers to a flexural x- section made up of a number of elements elements. They are generally considerably deeper than the y g y y p deepest rolled sections and usually have webs thinner than rolled sections. CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 4
  • 5. Plate Girder Modern plate girders are normally fabricated by welding together two flanges and a web p plate. CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 5
  • 6. Plate Girder Plate girders are at their most impressive in modern b id construction where main spans of d bridge t ti h i f well over 200m are feasible, with corresponding cross-section d th h ti depths, haunched over th h d the supports, in the range of 5-10m. CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 6
  • 7. Plate Girder Because plate girders are fabricated separately, each may be designed p y, y g individually to resist the applied actions using proportions that ensure low self-weight and high load resistance. resistance CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 7
  • 8. Plate Girder Changes in X-Section There is also considerable scope for variation of cross-section in the longitudinal direction. Ad i designer may choose t reduce th fl h to d the flange thickness (or breadth) in a zone of low applied moment moment. Equally, in a zone of high shear, the designer might choose to thicken the web plate. CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 8
  • 9. Plate Girder Changes in Material Alternatively, higher g y g grade steel might be g employed for zones of high applied moment and shear, while standard grade would be used elsewhere. S d l h So-called "h b id" girders ll d "hybrid" i d with different strength material in the flanges and the web offer another possible means of more closely matching resistance to requirements. requirements CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 9
  • 10. Plate Girder CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 10
  • 11. Plate Girder CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 11
  • 12. Plate Girder Any cross-section of a plate girder is normally subjected to a combination of shear force and bending moment. The primary function of the top and bottom flange plates of the girder is to resist the axial compressive and tensile forces arising from the applied bending moment. moment The primary function of the web plate is to resist the applied shear force. CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 12
  • 13. Plate Girder Plate girders are normally designed to support heavy loads over long spans in situations where it is necessary to produce an efficient design by providing girders of high strength to weight ratio. To produce the lowest axial flange force for a given bending moment, the web depth (d) must be made as large as possible. To reduce the self weight, the web thickness (tw) must be reduced to a minimum minimum. As a consequence, in many instances the web plate is of slender proportions and i th f l t i f l d ti d is therefore prone to buckling at relatively low values of applied shear shear. CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 13
  • 14. Plate Girder For efficient design it is usual to choose a relatively deep girder, thus minimizing the required area of flanges for a given applied moment, Msd. t This obviously entails a deep web whose y p area will be minimized by reducing its thickness to the minimum required to carry the applied shear, Vsd. h li d h Such a web may be quite slender ( y q (i.e. a high g d/tw ratio) and may be prone to local buckling and shear buckling. CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 14
  • 15. Plate Girder Web buckling does not determine the ultimate strength of a plate girder. lti t t th f l t id Plate elements do not collapse when they p y buckle; they can possess a substantial post- buckling reserve of resistance. For an efficient design, any calculation relating to the ultimate limit state should take g the post-buckling action into account. CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 15
  • 16. Design Criteria Criteria for design of plate girder may be based on Elastic bend-buckling strength Elastic h El ti shear-buckling strength b kli t th Post-bend-buckling Post bend buckling strength Post shear buckling(Tension Post-shear-buckling(Tension field)strength CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 16
  • 17. Design Criteria The designer has the choice of following four combinations 1. Elastic bend buckling + Elastic shear buckling g g (conventional flexural behavior) 2. 2 Elastic bend buckling + Post shear buckling 3. Post bend buckling + Elastic shear buckling g g 4. Post bend buckling + Post shear buckling CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 17
  • 18. Elastic Bend Buckling Strength The extreme f fiber bending stress at which a perfectly flat web buckles is given by CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 18
  • 19. Elastic Bend Buckling Strength Using a FOS of 1.25 w.r.t service load bending stress fb gives an eqnuation which is AASHTO slenderness limit for plat girders webs Using AASHTO allowable stress fb=0.55Fy “ h/t=165 f A36 steel “ h/t 165 for t l CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 19
  • 20. Elastic Bend Buckling Strength The bend buckling resistance of beam webs can be increased considerably by reinforcing the slender webs with Longitudinal stiffeners. Means webs thinner than those given by the equation can be used. used A typical longitudinally stiffened girder is shown after failure CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 20
  • 21. Web Stiffeners They usually consists of rectangular bars to welded to web. Transverse stiffeners may be in pairs, one on each side of web, or they may placed on one side of web. Longitudinal stiffeners are usually placed on one side of web. CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 21
  • 22. Web Stiffeners CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 22
  • 23. Web Stiffeners CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 23
  • 24. Web Stiffeners The main function of the longitudinal stiffeners is to increase the buckling resistance of the web with respect o bot s ea a d be d g loads. An t espect of both shear and bending oads effective stiffener will remain straight, thereby sub-dividing the web p g panel and limiting the g buckling to the smaller sub-panels. The resulting increase in the ultimate resistance of the girder g can be significant. CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 24
  • 25. Web Stiffeners Efficiency of stiffener is a function of its location in the compression zone The optimum location for a longitudinal stiffener has been determined to be at least h/5 from compression edge. In this case k=129. The corresponding allowable web k 129. slenderness is h/t=330 as compare to 165 CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 25
  • 26. Web Stiffeners Stiffener acts as a beam supported at the ends where a vertical stiffener holds the web in line line. Stiffener acts as a beam column and hence must be b proportioned i t ti d in terms of x-sectional area and f ti l d moment of inertia. AASHTO specifies Is as Stiffener acts as a beam supported at the ends where a vertical stiffener holds the web in line. CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 26
  • 27. Web Stiffeners The stiffeners must also be proportioned to resist local buckling. buckling For plates supported on one longitudinal p pp g edge AASHTO require b/t<1625/√fb Multiple longitudinal stiffeners are used for large depth webs. As longitudinal stiffener is also acting as a column so it must be satisfied for critical stress (Fcrs>0.6Fcrf) CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 27
  • 28. Post buckling bending strength If bending strain increases after Fcr, the upper g , pp edge of panels shortens and bottom edge lengthens. If web were to remain flat there will be increase in stress. Because the web has buckled, the increase in stress is non linear non-linear. CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 28
  • 29. Post buckling bending strength As A variation i post-buckled state i not k i ti in t b kl d t t is t known, simplify assumptions are made. Non-linear compression is replaced with linear distribution acting on effective depth be. CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 29
  • 30. Post buckling bending strength Point A gives point that enables a girder to reach its full yield moment(925 /√Fy=154). If stiffeners at h/5 is provided gives point B B. Considering the post buckling A B strength, the 0.94 0.82 0 82 point where M/My reduction in web 0.4 effectiveness 0.18 0 18 begins s taken to 154 315 360 be 980/√Fy=170. 980/√Fy 170. h/t CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 30
  • 31. Post buckling bending strength Equation connecting the revised point A with points corresponding t h/t 360 i ith i t di to h/t=360 is CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 31
  • 32. Post buckling bending strength LRFD Where CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 32
  • 33. Compression Flange Vertical buckling CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 33
  • 34. Compression Flange Vertical buckling If plate girder web is too slender the compression plate-girder slender, flange may buckle in vertical plane at stress less than yield stress stress. The compression flange is a beam-column p g continuous over vertical stiffener as supports Its stability depends on stiffener spacing and relative stiffness of the flange and the web. Fcr is CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 34
  • 35. Compression Flange Vertical buckling Slenderness of webs with vertical stiffeners is taken conservatively AISC ASD/LRFD li it the h/t by the given equation with limits th b th i ti ith Aw/Af =0.5 CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 35
  • 36. Shear buckling of beam webs Shear buckling is seldom a determining factor i d i f t in design of rolled section b t f ll d ti but plate girders have much larger h/t so it must be considered. tb id d CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 36
  • 37. Shear buckling of beam webs Transverse stiffeners are used to increase th b kli strength b i the buckling t th by increasing factor k through a reduction in aspect ratio a/h. CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 37
  • 38. Transverse Stiffeners Transverse stiffeners play an important role in allowing the full ultimate load resistance of a plate girder to be achieved. In the first place they increase the buckling resistance of the web; Secondly they must continue to remain effective after the web buckles, to provide anchorage for p g the tension field; finally they must prevent any tendency for the flanges to move towards one another. CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 38
  • 39. Transverse Stiffeners The satisfactory performance of a transverse stiffener can best be illustrated by comparing the girders shown, after shown testing. Figure 2 g Figure 1 Fi CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 39
  • 40. Transverse Stiffeners In Figure 1 the stiffeners have remained straight. g g In Figure 2 the stiffener has failed and has been unable to limit the buckling to the adjacent sub- sub panels of the girder; instead, the buckle has run through the stiffener p g position extending over g both panels. Consequently, significant reduction in the failure load of the girder occurred. In Figure 1 One can also see the effect of aspect ratio,i.e greater a/ less k a d s a Fcr. at o, e g eate a/h ess and small c CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 40
  • 41. Transverse Stiffeners The stiffener must be of adequate rigidity in th di ti perpendicular t i idit i the direction di l to the plane of the web to prevent web buckling. This condition is satisfied p provided the stiffener has a second moment of area Is that satisfies the following empirical formulae: CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 41
  • 42. Transverse Stiffeners AISC/LRFD Moment of Inertia of stiffener is: tiff i where CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 42
  • 43. Transverse Stiffeners Transverse stiffeners spacing can be determined from the following CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 43
  • 44. Tension Field Action The resulting shear stresses on an element of a web are equivalent t l t f b i l t to principal stresses, one Tensile and one Compressive, at 45 to the shear stress. CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 44
  • 45. Tension Field Action Once a web panel has buckled in shear, it p , loses its resistance to carry additional compressive stresses. stresses On the other hand tensile principal stress p p continues to increase in strain in the diagonal direction. direction Such a panel has a considerable p buckling strength, p post g g , since increase in tension is limited only by yield stress. CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 45
  • 46. Tension Field Action In this post b ckling range a ne load carr ing post-buckling range, new load-carrying mechanism is developed, whereby any additional shear load is carried by an inclined tensile membrane stress field. This tension field anchors against the top and bottom flanges and against the transverse stiffeners on either side of the web panel. The load-carrying action of the plate girder than becomes similar to that of the N-truss In the post-buckling range, the resistance offered by the web plates is analogous to that of the diagonal tie bars in the truss. CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 46
  • 47. Tension Field Action Phases of behavior up to collapse of a typical panel in shear Prior to Buckling Post Buckling Collapse CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 47
  • 48. Tension Field Action The load-carrying action of the plate girder load carrying than becomes similar to that of the N-truss In the post-buckling range, the resistance offered by the web plates is analogous to that of the diagonal tie bars in the truss. CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 48
  • 49. Tension Field Action CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 49
  • 50. Tension Field Action CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 50
  • 51. Tension Field Action ft V V Vt=Tsinφ Vt = ft ht cosφ sinφ T=ft ht cosφ Vt = (1/2)ft ht sin2φ φ Vt =(1/2) ft ht φ=45 Vty=(1/2) Fy ht………….(1) CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 51
  • 52. Tension Field Action Vty =(1/2) Fy ht = Fy Vy Fvy ht 2Fvy Vty = √3 Vy = 0.87 Vy 2 CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 52
  • 53. Tension Field Action The angle φ for which Vt is max CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 53
  • 54. Tension Field Action Where CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 54
  • 55. Tension Field Action (1) Taking inelastic and strain hardening range (2) (3) CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 55
  • 56. Tension Field Action Codal equations are derived from eqn;(1),(2),(3) CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 56
  • 57. Tension Field Action AISC/LRFD k a/h CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 57
  • 58. Combined Bending & Shear of Webs Interaction diagram is based on Tension- field f fi ld of webs b If the web is completely yielded in shear,any accompanying moment must be b resisted entirely b fl i t d ti l by flanges. CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 58
  • 59. Combined Bending & Shear Bending & shear Interaction Curve B B C D V vyAw) V/(F A E 1/√3 0.75 0.83 1.0 1.07 1.12 M/My CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 59
  • 60. Combined Bending & Shear 1.0 Mu/φMn 0.8 0.6 LRFD I t Interaction Curve ti C 0.4 0.2 0.2 0.4 0.6 0.8 1.0 Vu/φVn CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 60
  • 61. Web Proportioning Notations CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 61
  • 62. Web Proportioning Depth of girder is influenced by many factors: Headroom Clearance for high water in deck bridges Traffic passing beneath the bridge CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 62
  • 63. Web Proportioning Depth: Overall girder depth, h, will usually be in the range Lo/12 ≤ h ≤ Lo/8 /8, occasionally lighter loads may be accommodated with Lo/20 /20. Flange: g The breadth, b, will usually be in the range h/5 ≤ b ≤ h/3, CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 63
  • 64. Design Procedure 1. Maximum Moment & Shear for Factored Load 2. Web D i 2 W b Design 1. p girder L/12 ≤ h ≤ L/8 Assume depth of g 2. Depth of Web hw=h-2tf 3. Web slenderness 1. For a/h <5 ……………. 2. and for a/h > 5 …………………… 3. 3 hw/tw= 970/√Fy 4. Select optimum tw CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 64
  • 65. Design Procedure 4. Flange Design 1. Find Af 2. Select suitable tf and bf 3. 3 Flange slenderness 1. bf/ 2tf < 65/√Fy …………….Compact CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 65
  • 66. Design Procedure 5. 5 Check trial girder section 1. Web local buckling limit state 1. hw/tw< 640/√Fy…………………..Compact 2. 640/√Fy< hw/tw < 970/√Fy……Non-Compact 3. hw/tw > 970/√Fy…………………..Slender 2. Flange local buckling limit state 1. bf/ 2tf < 65/√Fy …………….Compact 3. Lateral Torsional Buckling g 1. Calculate Iy 2. A=Af+Aw/6 3. ry= √Iy/A 4. Find Lb/ry 5. λp= 300/√Fy ………….. λ< λp ______Compact CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 66
  • 67. Design Procedure 6. Bending strength 1. Calculate C l l t Ix 2. Calculate Sxt 3. . 4. . 5. φMn≥ Mu CE-409: Lecture 13 Prof. Dr Akhtar Naeem Khan 67
  • 68. Procedure for Design 6. Bending strength 1. Calculate Ix 2. 2 Calculate Sxt 3. . 4. . 5. CE-409: Lecture 13 φMn≥ Mu Prof. Dr Akhtar Naeem Khan