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  • ORIGINAL ARTICLE

    Experimental and finite element analysis research on I-beamunder web crippling

    Yu Chen Xixiang Chen Chaoyang Wang

    Received: 11 August 2014 / Accepted: 19 December 2014

    RILEM 2014

    Abstract To research web crippling property of

    I-beam under concentrated load, 48 I-beam with

    different boundary conditions, loading conditions,

    bearing lengths and section heights were tested. The

    experimental scheme, failure modes, concentrated

    loadgeneral vertical deformation and equivalent strain

    distribution curves were presented in the paper. The

    effects of boundary condition, loading condition,

    bearing length and section height on web crippling

    ultimate capacity and ductility of I-beam were also

    studied. Results of these tests show that as bearing

    length increases, web crippling ultimate capacity of

    I-beam increase significantly. When bearing length was

    50 and 100 mm, web crippling ultimate capacity of

    I-beam with web slenderness = 17.5 reached its peak;

    when the bearing length was 150 mm, web crippling

    ultimate capacity of I-beam with web slender-

    ness = 22.5 reached its peak. The middle web entered

    plasticity and formed plastic hinge zone in the ultimate

    limit state. The web crippling ultimate capacity of

    I-beam with bearing length = 50 mm in interior one

    flange condition, interior two flanges condition, end one

    flange and end two flanges condition decreased

    progressively. Finite element analysis could simulate

    experimental failure mode and web crippling ultimate

    capacity. The simple calculation method of web

    crippling ultimate capacity put forward in the paper

    can accurately predict experimental value.

    Keywords I-beam Web crippling Experimentalresearch Ultimate capacity Finite element analysis Simple calculation method

    List of symbols

    EOF End-one-flange

    IOF Interior-one-flange

    ETF End-two-flange

    ITF Interior-two-flange

    Rw,ul Experimental web crippling ultimate

    capacity

    Rw,ulc Web crippling ultimate capacity obtained

    by using Chinese steel structures design

    code (GB50013-2003)

    Rw,ule Web crippling ultimate capacity obtained

    by using European design of steel

    structures (Eurocode 3)

    Rw,ulFEA Web crippling ultimate capacity obtained

    by using finite element analysis

    Rw,ulre Web crippling ultimate capacity obtained

    by using equations the paper put forward

    Y. Chen

    School of Urban Construction, Yangtze University,

    Jingzhou 434023, China

    Y. Chen C. WangCollege of Civil Engineering, Huaqiao University,

    Xiamen 361021, China

    X. Chen (&)College of Technology & Engineering, Yangtze

    University, Jingzhou 434023, China

    e-mail: [email protected]

    Materials and Structures

    DOI 10.1617/s11527-014-0508-z

  • fy Tensile yield stress

    fu Ultimate tensile stress

    m Poissons ratiod Elongation after fractureE Elastic modulus

    MD Average deviation of yield stress

    r Standard deviation of yield stressh Overall height of I-beam

    b Flange height of I-beam

    ht Web effective height of I-beam

    t Web thickness of I-beams

    r Internal radius of corner

    a Bearing length

    ht/t Web slenderness

    ei Strain intensitye1 First principal straine2 Second principal straine3 Third principal strain

    1 Introduction

    I-beams nowadays are widely used in stadiums,

    towers and bridges due to their high strength, easy

    fabrication and fast construction. The web of I-beam

    may buckle due to high localized bearing force.

    Therefore, web crippling needs to be considered in

    designing I-beams.

    A considerable amount of research has been

    carried out on cold-formed and aluminum tubular

    sections under web crippling over many years by

    numerous researchers, particularly to validate various

    design rules for web crippling, and the majority was

    based on experimental investigations. In order to

    study the stability of the web in structural steel beams

    under a concentrated load, a cooperative investigation

    was undertaken by Lyse and Godfrey [1]. The test

    program included the testing of six rolled beams, four

    of which were cut from the same section and two

    from another section. A series of tests on aluminum

    square and rectangular hollow sections under web

    crippling was presented by Zhou and Young [2, 3].

    The web crippling strength in end-two-flange (ETF)

    loading condition increased faster than those interior-

    two-flange (ITF) loading condition as the bearing

    length increased. The effect of the bearing length on

    the web crippling strength in ETF loading condition

    was more severe than those in ITF loading condition.

    The new web crippling test data presented in this

    paper could be used to develop design rules for

    aluminum square and rectangular hollow sections. An

    experimental study was conducted at the University

    of Missouri-Rolla by Stephens and Laboube [4] to

    establish the web crippling strength of both box and

    I-beam in interior-one-flange (IOF) loading condition.

    Ren et al. [5] accurately predicted the behavior and

    ultimate strengths of cold-formed steel channels

    subjected to pure bending as well as combined

    bending and web crippling using the verified finite

    element models against test results. Carden et al. [6]

    investigated the critical web limit states in H-beams

    experimentally. The web crippling strength was

    greater than that for two independent, single web

    C-sections. Genetic programming (GP) as a new tool

    for the formulation of web crippling strength of cold-

    formed steel decks for various loading cases was

    presented by Cevik [7]. The results of the proposed

    GP formulations were compared with results of

    existing design codes and were found to be more

    accurate for all loading cases. Nine specimens were

    tested to collect data on V-core panels subjected to

    end one-flange (EOF) loading by Okazaki et al. [8].

    The modified equation was found to adequately

    predict the measured web crippling strength of V-core

    panels. Macdonald et al. [9] presented the results of

    an investigation into web crippling behavior of cold-

    formed thin-walled steel lipped channel beams in

    IOF, ITF, EOF and ETF loading conditions as defined

    by the American Iron and Steel Institute. An exper-

    imental program was developed to obtain the load

    deformation characteristics of beam members with

    varying cross-sectional and loading parameters in the

    three web crippling loading conditions. Eighty two

    web crippling tests of cold-formed steel sections, with

    20 tests on channel sections without web openings

    and 62 tests on channel sections with web openings,

    were conducted by Uzzaman et al. [10, 11]. The finite

    element model was shown to be able to closely

    predict the web crippling behavior of the channel

    sections, both with and without circular web hole. It

    was demonstrated that the main factors influencing

    the web crippling strength were the ratio of the hole

    depth to the flat depth of the web, and the ratio of the

    length of bearing plates to the flat depth of the web. A

    combination of experiments and non-linear finite

    element analyses were used to investigate the effect

    of offset web holes on the web crippling strength of

    Materials and Structures

  • cold-formed steel channel sections in the ETF loading

    condition by Uzzaman et al. [12]. Design recommen-

    dations in the form of web crippling strength reduc-

    tion factors are proposed. An experimental

    investigation of web crippling in stainless steel cold

    formed sections was presented by Bock et al. [13]. A

    new equation was proposed to predict the ultimate

    strength of stainless steel cold-formed members under

    web crippling. Natario et al. [14] evaluated the web

    crippling behavior of cold-formed steel beams by

    using quasi-static analyses with explicit integration.

    The failure mechanism emerged considerably more

    clearly when the quasi-static analysis was adopted.

    Wu and Bai [15] investigated the web crippling

    behavior of pultruded GFRP sections under concen-

    trated loading, employing four square hollow sections

    of different sizes. A simple mechanism based design

    equation was proposed to estimate the strength of

    such pultruded GFRP sections subjected to web

    crippling.

    There is little research being carried out on the

    behavior of I-beam under web crippling. Therefore,

    the ultimate capacity, failure modes and ductility of

    I-beam under web crippling need further investigation.

    In this paper, the experimental work was conducted on

    I-beam under web crippling. The effects of bearing

    lengths, web slenderness, boundary and loading

    conditions on the ultimate capacity and initial stiffness

    of I-beam under web crippling were investigated.

    Furthermore, using the calibrated finite element ana-

    lysis, a parametric study was conducted to compre-

    hensively investigate the effects of some important

    geometric parameters on the ultimate capacity of

    I-beam under web crippling. The new design simple

    calculation method is proposed for I-beam under web

    crippling at the end of the paper.

    2 Experimental investigation

    2.1 Specimens design

    To research web crippling property of I-beam, 48

    I-beams with different boundary condition, loading

    condition, section height, and bearing length were

    tested.

    The bearing plates were fabricated with Q235 steel

    whose nominal yield strength was 235 MPa having the

    nominal thickness of 30 mm. All the bearing plates

    were machined to specified dimensions whose the

    length was 300 mm. The bearing plates were designed

    to act across the full flange widths of the specimen

    sections, so as to ensure the overall displacement

    loading.

    The test specimens under web crippling comprised

    four different section sizes, having nominal heights

    ranging from 100 to 160 mm. The measured ratio of

    the height to the thickness (web slenderness) of the

    webs was 15.0, 18.0, 17.5, 22.5, as shown in Fig. 1.

    In the paper, the specimens were tested in four

    loading conditions, namely, EOF, IOF, ETF and ITF.

    In order to remove the influence of the boundary

    condition, the distance from the edge of the bearing

    plate to the end of the member was set to be at least 1.5

    times the overall height of the web. Figure 2 shows

    photos of web crippling tests in four boundary and

    loading conditions.

    In Table 1, the specimens were labeled so that the

    height of sections, the boundary condition, the loading

    condition and the width of the bearing plates, could be

    identified from the label. Rw,ul is experimental value of

    the web crippling ultimate capacity of I-beam spec-

    imen in the test. Rw,ul is defined as the maximum load

    reached during experiments. For example, the label

    I100-ETF-N100 is explained as follows:

    The notation I100 indicates the section height of

    I-beam in mm (100 mm).

    The next three letters indicate that the loading and

    boundary condition ETF was used in the test.

    Fig. 1 Definition of symbols of I-beam

    Materials and Structures

  • N100 represents the width of bearing plate in mm

    (100 mm).

    2.2 Material properties

    The I-beam specimens were fabricated by hot rolling

    using the Chinese Q325 steel. Tensile coupon tests

    were carried out to determine the material properties

    of the I-beam specimens. The tensile coupons were

    taken from the center face of the web plate in the

    longitudinal direction of the untested specimens. The

    nominal coupons were prepared and tested according

    to Chinese metallic materials-tensile testing at ambi-

    ent temperature (GB/T228-2002) [16], the coupons

    were tested in an MTS displacement controlled the

    testing machine using friction grips. The strain gauges

    and a calibrated extensometer were used to measure

    the longitudinal strain. A data acquisition system was

    used to record the load and strain at regular intervals

    during the material property tests. The material

    properties obtained from the tensile coupon tests are

    summarized in Table 2, including the tensile yield

    stress (fy), the ultimate tensile stress (fu), Poissons

    ratio (m), the elongation after fracture (d), the elasticmodulus (E), average deviation of yield stress (MD),

    and standard deviation of yield stress (r).

    2.3 Loading and test program

    In all structural design, an accurate prediction of the

    ultimate capacity of I-beam under web crippling is

    required for an efficient and safe use. The local

    transverse resistance of the web crippling specimens

    was obtained according to European steel structures

    design code [17], which can be used as the estimated

    load.

    The load classification was conducted according to

    estimated ultimate capacities. Before the values of

    preloading reached 10 % of the estimated ultimate

    capacities, slow loading was made on bearing plate by

    hydraulic jack. Before the values of formal load

    reached 20 % of the estimated ultimate capacities,

    continuous load was made, meanwhile monitoring the

    loading process if the rosettes strain gauges enter

    plasticity or displacement gauges increasing rapidly,

    finally continuously slow load was applied until

    Fig. 2 Photos of web crippling tests in four boundary and loading conditions

    Materials and Structures

  • Table 1 Parameters and ultimate capacity of I-beam under web crippling

    Boundary and

    loading conditions

    Specimens a (mm) b (mm) h (mm) L (mm) ht (mm) t (mm) ht/t r (mm) Rw,ul (kN)

    EOF I100-EOF-N50 50 67.42 99.82 400 75.00 5.08 14.76 6.88 122.3

    I100-EOF-N100 100 67.54 99.80 400 75.06 5.00 15.01 6.60 201.6

    I100-EOF-N150 150 67.70 99.80 400 75.10 5.04 14.90 6.64 179.7

    I120-EOF-N50 50 73.10 119.20 400 91.72 5.10 17.98 7.60 141.6

    I120-EOF-N100 100 73.00 119.52 400 91.58 5.20 17.61 7.64 197.8

    I120-EOF-N150 150 72.32 119.40 400 91.60 5.18 17.68 7.64 170.0

    I140-EOF-N50 50 78.60 140.06 400 113.10 6.40 17.67 7.42 156.8

    I140-EOF-N100 100 79.54 140.00 400 113.12 6.54 17.30 7.88 193.5

    I140-EOF-N150 150 78.62 140.02 400 113.08 6.48 17.45 7.60 256.0

    I160-EOF-N50 50 89.10 161.50 400 135.10 5.90 22.90 7.90 113.3

    I160-EOF-N100 100 89.30 162.00 400 135.10 5.98 22.59 7.88 166.8

    I160-EOF-N150 150 89.22 161.36 400 135.06 5.92 22.81 7.72 343.4

    IOF I100-IOF-N50 50 67.50 99.82 600 75.04 5.06 14.83 6.88 188.3

    I100-IOF-N100 100 67.54 99.84 600 75.04 5.04 14.89 6.76 224.7

    I100-IOF-N150 150 67.62 99.80 600 75.12 5.04 14.90 6.66 311.9

    I120-IOF-N50 50 73.12 119.28 600 91.68 5.18 17.70 7.62 214.1

    I120-IOF-N100 100 73.20 119.52 600 91.54 5.20 17.60 7.64 217.3

    I120-IOF-N150 150 72.30 119.82 600 91.62 5.20 17.62 7.70 353.0

    I140-IOF-N50 50 78.60 140.08 400 113.10 6.44 17.56 7.52 300.5

    I140-IOF-N100 100 79.32 140.10 400 113.12 6.52 17.35 7.88 366.5

    I140-IOF-N150 150 78.80 140.04 400 113.20 6.46 17.52 7.60 431.1

    I160-IOF-N50 50 89.14 161.50 400 135.10 5.92 22.82 7.92 242.8

    I160-IOF-N100 100 89.32 161.48 400 135.18 5.98 22.61 7.88 284.6

    I160-IOF-N150 150 89.22 161.36 400 135.06 5.94 22.74 7.78 458.6

    ETF I100-ETF-N50 50 67.62 99.90 400 75.08 5.08 14.78 6.88 76.0

    I100-ETF-N100 100 67.51 99.80 400 75.06 5.02 14.95 6.60 117.6

    I100-ETF-N150 150 67.68 99.82 400 75.14 5.02 14.97 6.66 200.9

    I120-ETF-N50 50 73.00 119.32 600 91.72 5.10 17.98 7.60 127.0

    I120-ETF-N100 100 73.26 119.52 600 91.58 5.16 17.75 7.68 146.5

    I120-ETF-N150 150 72.32 119.40 600 91.68 5.18 17.70 7.64 193.5

    I140-ETF-N50 50 78.60 140.08 400 113.10 6.48 17.45 7.46 137.3

    I140-ETF-N100 100 78.90 140.02 400 113.16 6.54 17.30 7.88 209.2

    I140-ETF-N150 150 78.62 140.02 400 113.08 6.46 17.50 7.60 263.1

    I160-ETF-N50 50 89.12 161.50 400 135.08 5.88 22.97 7.86 81.7

    I160-ETF-N100 100 89.28 162.00 400 135.10 5.94 22.74 7.88 114.9

    I160-ETF-N150 150 89.20 161.80 400 135.06 5.96 22.66 7.78 314.8

    ITF I100-ITF-N50 50 67.48 99.82 400 75.08 5.00 15.02 6.70 168.8

    I100-ITF-N100 100 67.54 99.80 400 75.06 5.00 15.01 6.60 171.7

    I100-ITF-N150 150 67.68 99.80 400 75.12 5.06 14.85 6.64 230.1

    I120-ITF-N50 50 73.10 119.22 600 91.72 5.10 17.98 7.66 157.0

    I120-ITF-N100 100 73.30 119.52 600 91.58 5.12 17.89 7.84 214.5

    I120-ITF-N150 150 72.32 119.86 600 91.64 5.14 17.83 7.64 266.7

    I140-ITF-N50 50 78.60 140.06 400 113.10 6.42 17.62 7.42 270.7

    I140-ITF-N100 100 79.44 140.04 400 113.12 6.50 17.40 7.88 212.0

    Materials and Structures

  • failure. In the actual control, the upper limit of graded

    load is continuously adjusted according to the dis-

    placement gauges feedback. At the appearance of

    obviously large displacement or drop load, the tests

    were stopped.

    Two displacement gauges D1 and D2 were located

    at the surface of the bearing plates on the top flange of

    the I-beam in order to record the vertical displacement

    during the test, as shown in Fig. 3a. Five rosette strain

    gauge (T15), which enabled strain values to be

    measured simultaneously, were distributed at the same

    interval on the web of I-beam, as shown in Fig. 3b.

    3 Test results

    3.1 Failure modes

    All types of failure modes in four loading conditions,

    namely, EOF, IOF, ETF and ITF were observed from

    the tests, as shown in Fig. 4ad, respectively. In both

    EOF and ETF conditions, the compressive top flange

    buckled, the bottom flange did not buckle, web

    crippled into S type out-of-plane, and the corner

    kept right angle. In IOF condition, the top flange

    buckled, the bottom flange did not buckle, and the

    upper part of web under the bearing plate slightly

    buckled. In ITF condition, both the top and bottom

    flange buckled, while the upper part of web right under

    the bearing plate slightly buckled. Generally, com-

    pressive top flange buckled first, then web crippled,

    and finally bottom flange buckled. The effects of

    bearing lengths and section heights on failure modes

    of I-beam under web crippling were little.

    3.2 Comparison of ultimate capacity under web

    crippling with different bearing lengths

    Table 3 shows the ultimate capacity of I-beam under

    web crippling with different bearing lengths. The

    effect of bearing plate length on the ultimate capacity

    Table 1 continued

    Boundary and

    loading conditions

    Specimens a (mm) b (mm) h (mm) L (mm) ht (mm) t (mm) ht/t r (mm) Rw,ul (kN)

    I140-ITF-N150 150 78.62 140.04 400 113.08 6.48 17.45 7.64 337.3

    I160-ITF-N50 50 89.12 161.50 400 135.04 5.94 22.73 7.96 176.1

    I160-ITF-N100 100 89.30 161.38 400 135.10 5.98 22.59 7.88 241.2

    I160-ITF-N150 150 89.28 161.36 400 135.06 5.92 22.81 7.72 414.5

    Table 2 Result of materialcharacteristic test

    Members fy (MPa) fu (MPa) m d (%) E (GPa) MD r

    I100 9 68 9 5.0 275 390 0.31 38 209 14 2

    I120 9 74 9 5.0 284 396 0.29 36 206 13 1

    I140 9 80 9 6.5 293 385 0.28 37 208 17 2

    I160 9 88 9 6.0 285 405 0.30 34 210 11 3

    D1 D2D1 D2

    Displacement transducers

    Hydraulic jackHydraulic jack

    (ETF and ITF) (EOF and IOF)

    (a) Displacement transducers

    Rosette strain gauge

    Hydraulic jackHydraulic jack

    (ETF and ITF) (EOF and IOF)

    (b) Rosette strain gaugesFig. 3 Arrangement of displacement and rosette strain gauges

    Materials and Structures

  • of I-beam under web crippling was different in the

    different loading conditions.

    Increasing bearing length ranged from 50 to 100 and

    150, the ultimate capacity of I-beam under web

    crippling increased by 44 and 83 % in EOF loading

    condition compared with 41 and 148 % in ETF loading

    condition. Meanwhile, increasing bearing length ran-

    ged from 50 to 100 mm, the ultimate capacity of I-beam

    under web crippling increased by about 15 % in both

    IOF and ITF loading conditions; increasing bearing

    length ranged from 50 to 150 mm, the ultimate capacity

    of I-beam under web crippling increased by about 65 %

    Fig. 4 Failure modes in testand FEA

    Materials and Structures

  • in both IOF and ITF loading conditions, respectively. It

    is shown that the effect of the bearing length on the web

    crippling ultimate capacity of I-beam in end-flange

    loading condition was more obvious than those of

    I-beam in interior-flange loading condition.

    3.3 Comparison of ultimate capacity under web

    crippling with different web slenderness

    The comparison of the ultimate capacity of I-beam

    under web crippling with different web slenderness is

    Table 3 Comparison of ultimate capacity of I-beam under web crippling with different bearing lengths

    Boundary and

    loading conditions

    Specimens Rw,ul(N = 50,

    kN)

    Rw,ul(N = 100,

    kN)

    Rw,ul(N = 150,

    kN)

    Rw,ul (N = 100)/

    Rw,ul (N = 50)

    Rw,ul (N = 150)/

    Rw,ul (N = 50)

    EOF I100-EOF-

    N(50,100,150)

    122.30 201.60 179.70 1.65 1.47

    I120-EOF-

    N(50,100,150)

    141.60 197.80 170.00 1.40 1.20

    I140-EOF-

    N(50,100,150)

    156.80 193.50 256.00 1.23 1.63

    I160-EOF-

    N(50,100,150)

    113.30 166.80 343.40 1.47 3.03

    Mean 1.44 1.83

    COV 0.120 0.446

    IOF I100-IOF-

    N(50,100,150)

    188.30 224.70 311.90 1.19 1.66

    I120-IOF-

    N(50,100,150)

    214.10 217.30 353.00 1.01 1.65

    I140-IOF-

    N(50,100,150)

    300.50 366.50 431.10 1.22 1.43

    I160-IOF-

    N(50,100,150)

    242.80 284.60 458.60 1.17 1.89

    Mean 1.15 1.66

    COV 0.080 0.112

    ETF I100-ETF-

    N(50,100,150)

    76.00 117.60 200.90 1.55 2.64

    I120-ETF-

    N(50,100,150)

    127.00 146.50 193.50 1.15 1.52

    I140-ETF-

    N(50,100,150)

    137.30 209.20 263.10 1.52 1.92

    I160-ETF-

    N(50,100,150)

    81.70 114.90 314.80 1.41 3.85

    Mean 1.41 2.48

    COV 0.128 0.412

    ITF I100-ITF-

    N(50,100,150)

    168.80 171.70 230.10 1.02 1.36

    I120-ITF-

    N(50,100,150)

    157.00 214.50 266.70 1.37 1.70

    I140-ITF-

    N(50,100,150)

    270.70 212.00 337.30 0.78 1.25

    I160-ITF-

    N(50,100,150)

    176.10 241.20 414.50 1.37 2.35

    Mean 1.13 1.67

    COV 0.253 0.299

    Materials and Structures

  • shown in Fig. 5. The web slenderness values of I-beam

    ranged from 15.0 to 22.5.

    When the bearing length was 50 and 100 mm,

    ultimate capacity of I-beam with the web slender-

    ness = 17.5 reached its peak; when the bearing

    lengths was 150 mm, the ultimate capacity of

    I-beam with the web slenderness = 22.5 was the

    largest value, the ultimate capacity of I-beam with

    the web slenderness = 17.5 was the second largest

    value.

    100

    150

    200

    250

    300

    350

    15.0(I100) 17.5(I140) 18.0(I120) 22.5(I160)

    R w,ul/k

    Nht /t

    N50 N100 N150

    150

    200

    250

    300

    350

    400

    450

    500

    15.0(I100) 17.5(I140) 18.0(I120) 22.5(I160)

    R w,ul/k

    N

    ht /t

    N50 N100 N150

    (a) EOF (b) IOF

    50

    100

    150

    200

    250

    300

    350

    15.0(I100) 17.5(I140) 18.0(I120) 22.5(I160)

    R w,ul/k

    N

    ht /t

    N50 N100 N150

    100

    150

    200

    250

    300

    350

    400

    450

    15.0(I100) 17.5(I140) 18.0(I120) 22.5(I160)

    R w,ul/k

    N

    ht /t

    N50 N100 N150

    (c) ETF (d) ITF

    Fig. 5 Comparison ofcapacity of I-beam under

    web crippling with different

    web slenderness

    0

    50

    100

    150

    200

    250

    300

    350

    400

    0 1 2 3 4 5

    N/k

    N

    /mm

    I100-EOF-N150(15.0)I140-EOF-N150(17.5)I120-EOF-N150(18.0)I160-EOF-N150(22.5)

    Top flange buckle

    Web cripple

    050

    100150200250300350400450500

    0 1 2 3 4 5

    N/k

    N

    /mm

    I100-IOF-N150(15.0)I140-IOF-N150(17.5)I120-IOF-N150(18.0)I160-IOF-N150(22.5)

    Top flange buckle

    Upper part of web cripple

    (a) EOF (b) IOF

    0

    50

    100

    150

    200

    250

    300

    350

    0 1 2 3 4 5 6 7 8

    N/k

    N

    /mm

    I100-ETF-N150(15.0)I140-ETF-N150(17.5)I120-ETF-N150(18.0)I160-ETF-N150(22.5)

    Top flange buckle

    Web cripple

    050

    100150200250300350400450

    0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 4.0

    N/k

    N

    /mm

    I100-ITF-N150(15.0)I140-ITF-N150(17.5)I120-ITF-N150(18.0)I160-ITF-N150(22.5)Top flange buckle

    Upper part of web cripple

    Bottom flange buckle

    (c) ETF (d) ITF

    Fig. 6 Loaddisplacementof I-beam under web

    crippling with different web

    slenderness

    Materials and Structures

  • The loaddisplacement of I-beam under web crip-

    pling with different web slenderness is shown in

    Fig. 6. X-axis represents the global vertical displace-

    ment of specimens (d), Y-axis represents the verticalload at loading end (N). The global vertical displace-

    ment of specimens was calculated as average of D1

    and D2 displacement values. The important points on

    the loaddisplacement curves corresponding to the

    attainment of specific phenomena including top flange

    buckled, bottom flange buckled and web crippled were

    marked in Fig. 6. The measured web slenderness

    values of the specimens ranged from 15.0 to 22.5.

    Ductility ratio (du/dy) is defined as ratio of displace-ment at ultimate load (du) to displacement at yield load(dy) of all specimens based on the design criteriarecommended by Kurobane et al. [18]. The greater

    ductility ratio (du/dy), the better ductility of specimens.The greater web slenderness, the smaller initial

    stiffness and the better ductility. Rw,ul can be defined

    as the peak load of loaddisplacement curve.

    3.4 Comparison of ultimate capacity under web

    crippling in different boundary and loading

    conditions

    The comparison of the ultimate capacity of I-beam

    under web crippling in different boundary and loading

    conditions is shown in Fig. 7. When the bearing length

    was 50 mm, the values of the web crippling ultimate

    capacity in interior-flange loading condition were

    larger than those in end-flange loading condition. The

    values of the web crippling ultimate capacity of

    I-beam with bearing length = 50 mm in one flange

    loading condition were larger than those in two flange

    loading conditions. As the bearing length increased,

    the trend got unobvious.

    When the web slenderness was 22.5, the values of

    the web crippling ultimate capacity of I-beam in

    interior-flange loading condition were larger than

    those in end-flange loading condition. Similarly, the

    values of the web crippling ultimate capacity of

    I-beam with the web slenderness = 22.5 in one flange

    loading condition were larger than those in two flange

    loading conditions. As the web slenderness decreased,

    the trend got unobvious.

    Loaddisplacement of I-beam under web crippling

    in different loading conditions is shown in Fig. 8.

    Value of X-axis is the average of D1 and D2

    displacement values. It is shown that the specimens

    in the interior-flange loading conditions had high

    ultimate capacity and good ductility. The initial

    stiffness of the specimens labeled I160 in interior

    loading condition was higher than those of I160 in end

    loading condition. The initial stiffness of the other

    specimens in interior and end loading conditions was

    basically the same.

    3.5 Loadequivalent strain on web curves

    Equivalent strain distribution in the web region was

    derived from the readings of three-element rosettes

    strain gauges. The failure mechanism of the joints

    were studied from equivalent strain distribution. The

    equivalent strain at the measuring points of rosettes

    strain gauges corresponding to different load levels

    covering the elastic and plastic range of typical

    specimens are plotted in Fig. 9, in which the horizon-

    tal axis represents the measuring points of strain

    gauges (as shown in Fig. 3b), the vertical axis

    represents the equivalent strain (ei), and the dash linerepresents the boundary equivalent strain correspond-

    ing to the yield strength.

    50

    100

    150

    200

    250

    300

    350

    15.0(I100) 17.5(I140) 18.0(I120) 22.5(I160)

    N/kN

    ht/t

    EOF IOFETF ITF

    100

    150

    200

    250

    300

    350

    400

    15.0(I100) 17.5(I140) 18.0(I120) 22.5(I160)

    N/kN

    ht/t

    EOF IOFETF ITF

    150

    200

    250

    300

    350

    400

    450

    500

    15.0(I100) 17.5(I140) 18.0(I120) 22.5(I160)

    N/kN

    ht/t

    EOF IOFETF ITF

    (a) N50 (b) N100 (c) N150Fig. 7 Comparison of capacity of I-beam under web crippling in different boundary and loading conditions

    Materials and Structures

  • 050

    100

    150

    200

    250

    300

    350

    0 1 2 3 4 5N/kN

    /mm

    I100-EOF-N150I100-ETF-N150I100-IOF-N150I100-ITF-N150

    0

    50

    100

    150

    200

    250

    300

    350

    400

    0 1 2 3 4 5

    N/kN

    /mm

    I120-EOF-N150I120-ETF-N150I120-IOF-N150I120-ITF-N150

    (a) I100-N150 (b) I120-N150

    050

    100150200250300350400450500

    0 1 2 3 4 5

    N/kN

    /mm

    I140-EOF-N150I140-ETF-N150I140-IOF-N150I140-ITF-N150

    050

    100150200250300350400450500

    0 1 2 3 4 5

    N/kN

    /mm

    I160-EOF-N150I160-ETF-N150I160-IOF-N150I160-ITF-N150

    (c) I140-N150 (d) I160-N150

    Fig. 8 Loaddisplacementof I-beam under web

    crippling in different

    loading conditions

    y=13570

    1000

    2000

    3000

    4000

    5000

    6000

    7000

    8000

    T1 T2 T3 T4 T5

    i/

    Ti

    100kN 200kN250kN 300kN343kN

    y=1357

    0

    1000

    2000

    3000

    4000

    5000

    6000

    7000

    T1 T2 T3 T4 T5

    i/

    Ti

    200kN 300kN350kN 400kN458kN

    (a) I160-EOF-N150 (b) I160-IOF-N150

    y=1357

    0

    2000

    4000

    6000

    8000

    10000

    12000

    14000

    16000

    T1 T2 T3 T4 T5

    i/

    Ti

    200kN 250kN285kN 300kN314kN

    y=13570

    100020003000400050006000700080009000

    T1 T2 T3 T4 T5

    i/

    Ti

    200kN 300kN350kN 400kN414kN

    (c) I160-ETF-N150 (d) I160-ITF-N150

    Fig. 9 Equivalent straindistribution curves

    Materials and Structures

  • ei 12

    p 1m

    e1e2 2 e2e3 2 e3e1 2q

    12

    p 1m

    exey 2 eyez

    2 ezex 232

    c2xyc2yzc2zx

    r

    :

    1In elastic range volume is supposed fixed,

    cyz 0; czx 0; v 0:5: 2The equivalent strain (ei) could be calculated as

    follows [19, 20]:

    ei

    2p

    3

    e1 e2 2 e2 e3 2 e3 e1 2q

    ; 3

    where e1, e2 and e3 are the first, second and thirdprincipal strains, respectively, which were obtained

    from three-element rosettes strain gauges along the

    joint intersection region.

    Measuring points first entered plasticity were

    determined by different loading conditions. All mea-

    suring points on web of I-beam enter plasticity in the

    ultimate limit state. Strain intensity of T3 located at

    the centerline of web was the minimum of equivalent

    strain.

    4 Comparison of web crippling ultimate capacity

    The experimental web crippling ultimate capacity and

    the calculated value of specification in EOF, IOF, ETF

    and ITF loading condition are given in Table 4,

    respectively. The specification values are calculated

    using the measured I-beam geometry size and the

    measured yield strength. Rw,ulc and Rw,ule are the web

    crippling ultimate capacity of I-beam obtained by

    using Chinese steel structures design code (GB50017-

    2003) [21] and European design of steel structures

    (Eurocode 3) [17], respectively. Rw,ulre is the web

    crippling ultimate capacity of I-beam obtained by

    using the following design equation the paper put

    forward. Up to the authors knowledge, the European

    standard is applied to cold formed steel elements or

    profiled sheet. There is no design rule for the hot rolled

    specimens under web crippling. A comparison

    between calculation value obtained by using Eurocode

    3 and experimental result was made to check whether

    design equation of Eurocode 3 is applicable for hot

    rolled specimens or not.

    The design strengths of web crippling ultimate

    capacity of cross-sections with a single unstiffened

    web can be calculated using the design equations as

    follows:

    Rw;ule k1k2 5:92 ht=t132

    1 0:01 at

    h i

    t2fy

    EOF Eurocode 3 17;4

    Rw;ule k4k5 14:7 ht=t49:5

    1 0:0007 at

    h i

    t2fy

    IOF Eurocode 3 17;5

    Rw;ule k1k2 6:66 ht=t64

    1 0:01 at

    h i

    t2fy

    ETF Eurocode 3 17;6

    Rw;ule k4k5 21:0 ht=t16:3

    1 0:0013 at

    h i

    t2fy

    ITF Eurocode 3 17;7

    Rw;ulc t a 5hy

    fy Chinese code 21; 8

    hy h ht =2; 9where fy is the yield stress of I-beam, t is the web

    thickness, a is the bearing length, ht is web height, k1and k4 are the same parameters that account for the

    influence of yield stress, and k2 and k5 are the influence

    function for internal radius of the corners and web

    thickness.

    The mean values of Rw,ulc/Rw,ul ratio are 1.46, 0.90,

    1.74 and 1.14 with the corresponding COV of 0.188,

    0.128, 0.227 and 0.171 in EOF, IOF, ETF and ITF

    loading and boundary conditions, respectively. The

    calculated result obtained by using Chinese steel

    structures design code (Rw,ulc) was far larger than the

    experimental web crippling ultimate capacity (Rw,ul),

    because that the ultimate capacity reduction caused by

    out-of-plane buckling of the thin web and effects of

    loading and boundary conditions on web crippling

    ultimate capacity were not considered in Chinese steel

    structures design code. The mean values of Rw,ule/Rw,ulratio are 0.28, 0.46, 0.37 and 0.73 with the correspond-

    ing COV of 0.275, 0.176, 0.370 and 0.253 for EOF,

    IOF, ETF and ITF loading and boundary conditions,

    respectively. The calculated result obtained by using

    Materials and Structures

  • Table 4 Comparison of capacity of I-beam under web crippling between test, equation and code

    Boundary and

    loading conditions

    Specimens Rw,ul (kN) Rw,ulc (kN) Rw,ulc/

    Rw,ul

    Rw,ule (kN) Rw,ule/

    Rw,ul

    Rw,ulre (kN) Rw,ulre/

    Rw,ul

    EOF I100-EOF-N50 122.3 156.53 1.28 35.87 0.29 82.00 0.67

    I100-EOF-N100 201.6 222.54 1.10 37.95 0.19 123.80 0.61

    I100-EOF-N150 179.7 293.49 1.63 41.70 0.23 169.15 0.94

    I120-EOF-N50 141.6 171.93 1.21 36.64 0.26 84.82 0.60min

    I120-EOF-N100 197.8 250.83 1.27 41.39 0.21 134.07 0.68

    I120-EOF-N150 170.0 322.91 1.90max 44.41 0.26 179.97 1.06max

    I140-EOF-N50 156.8 220.15 1.40 57.65 0.37 122.72 0.78

    I140-EOF-N100 193.5 320.39 1.66 64.41 0.33 187.59 0.97

    I140-EOF-N150 256.0 412.67 1.61 67.53 0.26 245.37 0.96

    I160-EOF-N50 113.3 195.05 1.72 48.23 0.43max 104.88 0.93

    I160-EOF-N100 166.8 285.04 1.71 53.33 0.32 160.68 0.96

    I160-EOF-N150 343.4 364.01 1.06min 56.11 0.16min 211.56 0.62

    Mean 1.46 0.28 0.81

    COV 0.188 0.275 0.210

    IOF I100-IOF-N50 188.3 155.78 0.83 97.28 0.52 148.29 0.79

    I100-IOF-N100 224.7 224.53 1.00 102.80 0.46 212.58 0.95

    I100-IOF-N150 311.9 293.42 0.94 109.06 0.35 277.78 0.89

    I120-IOF-N50 214.1 175.06 0.82 103.75 0.48 158.23 0.74min

    I120-IOF-N100 217.3 250.98 1.16max 111.14 0.51 228.44 1.05max

    I120-IOF-N150 353.0 325.63 0.92 117.73 0.33min 297.65 0.84

    I140-IOF-N50 300.5 221.62 0.74min 161.93 0.54 230.86 0.77

    I140-IOF-N100 366.5 319.89 0.87 174.38 0.48 325.16 0.89

    I140-IOF-N150 431.1 410.92 0.95 179.67 0.42 409.49 0.95

    I160-IOF-N50 242.8 195.72 0.81 133.81 0.55max 194.73 0.80

    I160-IOF-N100 284.6 282.49 0.99 144.04 0.51 277.29 0.97

    I160-IOF-N150 458.6 365.24 0.80 149.69 0.33min 353.40 0.77

    Mean 0.90 0.46 0.87

    COV 0.128 0.176 0.113

    ETF I100-ETF-N50 76.0 156.53 2.06 39.70 0.52 67.49 0.89

    I100-ETF-N100 117.6 223.43 1.90 42.31 0.36 96.60 0.82

    I100-ETF-N150 200.9 292.25 1.45 45.82 0.23 126.96 0.63

    I120-ETF-N50 127.0 172.36 1.36 40.42 0.32 69.48 0.55

    I120-ETF-N100 146.5 248.90 1.70 45.00 0.31 102.77 0.70

    I120-ETF-N150 193.5 322.62 1.67 49.00 0.25 135.43 0.70

    I140-ETF-N50 137.3 223.00 1.62 65.18 0.47 104.68 0.76

    I140-ETF-N100 209.2 320.30 1.53 71.09 0.34 148.15 0.71

    I140-ETF-N150 263.1 411.40 1.56 74.10 0.28 186.80 0.71

    I160-ETF-N50 81.7 194.48 2.38 52.54 0.64max 85.82 1.05

    I160-ETF-N100 114.9 283.14 2.46max 57.77 0.50 123.67 1.08max

    I160-ETF-N150 314.8 368.34 1.17min 62.32 0.20min 160.81 0.51min

    Mean 1.74 0.37 0.76

    COV 0.227 0.370 0.232

    Materials and Structures

  • European steel structures design code was very con-

    servative. The experimental web crippling ultimate

    capacity was relatively close to calculated result in ITF

    condition. The mean values and COV of Rw,ule/Rw,ul in

    ITF condition were 0.73 and 0.251, respectively.

    5 Finite element analysis

    5.1 General

    The finite element program ABAQUS version 6.11

    [22] was used to simulate I-beam under web crippling.

    Three main components have been carefully consid-

    ered in the FEM. These components are the bearing

    plates, I-beam, and the interfaces between the bearing

    plates and I-beam. In the FEM, the measured cross-

    section dimensions and material properties obtained

    from the tests were used. The model was based on the

    centerline dimensions of the cross-sections. Both

    material and geometric nonlinearities have been taken

    into account in the finite element models. The bilinear

    material model based on the elastic modulus and post-

    yield tangential modulus of steel obtained from the

    tensile coupon tests was developed for the material

    modelling, while the Von-Mises yield criterion was

    applied. Arc-length method was adopted as the

    incremental and iterative solution method in the finite

    element analysis.

    5.2 Element type and mesh

    The bearing plates were modeled using analytical rigid

    plates and the I-beams were modeled using the C3D8I

    solid elements. The C3D8I element is an eight-node

    doubly curved thin or thick shell element with reduced

    integration, hourglass control, and finite membrane

    strains. It is mentioned in the ABAQUS manual that the

    element is suitable for complex buckling behavior. The

    C3D8I element has six degrees of freedom per node and

    provides accurate solutions to most applications. The

    finite element mesh used in the model was investigated by

    varying the size of the elements in the cross-section to

    provide both accurate results and less computational time.

    The finite element mesh sizes ranging from 3 9 3 mm

    (length by width) to 8 9 8 mm were used for the flanges

    and webs depending on the size of the sections.

    5.3 Boundary conditions and interfaces

    Following the test procedures, the top bearing plate

    was restrained against all degrees of freedom, except

    for the translational degree of freedom in the loading

    direction. The interfaces between the bearing plates

    and the I-beam were modeled using the contact pair.

    The steel bearing plates were the master elements,

    while the I-beam specimen was the slave element of

    the interface elements in the FEM. The contact pair

    allowed the surfaces to separate under the influence of

    Table 4 continued

    Boundary and

    loading conditions

    Specimens Rw,ul (kN) Rw,ulc (kN) Rw,ulc/

    Rw,ul

    Rw,ule (kN) Rw,ule/

    Rw,ul

    Rw,ulre (kN) Rw,ulre/

    Rw,ul

    ITF I100-ITF-N50 168.8 153.79 0.91 125.48 0.74 120.56 0.71

    I100-ITF-N100 171.7 222.54 1.30 127.10 0.74 136.29 0.79

    I100-ITF-N150 230.1 294.58 1.28 131.82 0.57 155.20 0.67

    I120-ITF-N50 157.0 172.00 1.10 132.36 0.84 127.95 0.81

    I120-ITF-N100 214.5 246.98 1.15 135.10 0.63 145.41 0.68

    I120-ITF-N150 266.7 321.95 1.21 137.85 0.52 162.98 0.61

    I140-ITF-N50 270.7 220.84 0.82min 214.08 0.79 203.91 0.75

    I140-ITF-N100 212.0 318.62 1.50max 221.75 1.05max 230.52 1.09max

    I140-ITF-N150 337.3 412.76 1.22 222.53 0.66 250.74 0.74

    I160-ITF-N50 176.1 196.63 1.12 177.04 1.01 168.34 0.96

    I160-ITF-N100 241.2 282.40 1.17 181.43 0.75 189.57 0.79

    I160-ITF-N150 414.5 364.01 0.88 179.64 0.43min 204.83 0.49min

    Mean 1.14 0.73 0.76

    COV 0.171 0.251 0.202

    Materials and Structures

  • a tensile force. However, the two contact surfaces are

    not allowed to penetrate each other.

    5.4 Method of loading

    The loading method used in the FEA was identical to

    that used in the tests. The displacement control method

    was used for the analysis of the I-beam section under

    web crippling. Transverse compressive load was

    applied to the specimen by specifying a displacement

    to the reference point of the analytical rigid plate that

    modeled the bearing plate. Generally, a displacement

    of 5 mm was specified in the elastic stage. As the

    loading increased, displacement may be reduced to

    increase the convergence of the solution.

    5.5 Material modeling

    The measured stressstrain curves of the tensile

    specimens were used in the FEA. The material

    behavior provided by ABAQUS allows the multi-

    linear stressstrain curve to be used. The first part of

    the multi-linear curve represents the elastic part up to

    the proportional limit stress with measured Youngs

    modulus as well as Poissons ratio of 0.30. Since the

    analysis of post-buckling involves large in-elastic

    strains, the nominal (engineering) static stressstrain

    curve was converted to a true stress and logarithmic

    plastic strain curve. The equations for true stress and

    plastic true strain were specified in ABAQUS.

    5.6 Verification of FEM

    In the verification of the FEM, a total of 48 I-beam

    specimens under web crippling were analyzed. A

    comparison between the experimental results and the

    finite element results was carried out. The main

    objective of this comparison is to verify and check the

    accuracy of the FEM. The comparison of the ultimate

    capacities of all specimens obtained from the test

    results (Rw,ul) and finite element analysis results

    (Rw,ulFEA) is shown in Table 5. The mean values of

    the Rw,ulFEA/Rw,ul ratio were 0.91 with the correspond-

    ing COV of 0.052. The minimum error was -9 %, the

    maximum error was 9 %. The failure modes, load

    displacement curves and equivalent strain-point of

    measurement curves obtained from the test and finite

    element analysis were also compared in Figs. 4 and 10

    for typical specimens, respectively. It is shown from

    the comparison that the finite element analysis results

    generally agreed well with the test results.

    6 Proposed design equations

    Based on material strength failure of compressive

    local web, the calculated results obtained by using

    Chinese steel structures design code were larger than

    the experimental value. Because the small effect of

    bearing length on the web crippling strength in

    European steel structures design code, the calculated

    obtained by using European steel structures design

    code were generally quite conservative.

    The calculation equations of web crippling ultimate

    capacity in four boundary and loading condition

    according to European steel structures design code

    were very complicated and very conservative com-

    paring with experimental results, so the effect of the

    bearing length was improved in accurate calculation

    Eqs. 1013 of I-beam web crippling ultimate capacity

    this paper put forward by using curve fitting method.

    The design values can be reduced appropriately

    according to importance of structure. The design

    ultimate capacity (Rw,ulre) of the I-beam under web

    crippling calculated using Eqs. 1013, respectively,

    were compared with the ultimate capacity obtained

    from the test, as shown in Table 5. The calculation

    equation could accurately predict experimental value.

    The mean values of ratio between the calculation

    values obtain by using Eqs. 1013 (Rw,ulre) and

    experimental values (Rw,ul) were 0.81, 0.87, 0.76 and

    0.76 with the corresponding COV of 0.210, 0.113,

    0.232 and 0.202 for EOF, IOF, ETF and ITF in

    Table 4, respectively.

    The web crippling ultimate capacity of I-beam in

    four boundary and loading condition are calculated

    using Eqs. 1013 as follows:

    Table 5 Comparison of design strengths of equations andFEA results with test results

    A total of 48 specimens Comparison

    Rw,ulFEA/Rw,ul Rw,ulre/Rw,ul

    Max 1.09 1.09

    Min 0.81 0.49

    Mean 0.91 0.80

    COV 0.052 0.189

    Materials and Structures

  • Rw;ulre 0:9 6 ht=t130

    1 0:12 at

    h i

    t2fy EOF;

    10

    Rw;ulre 0:8 15 ht=t50

    1 0:08 at

    h i

    t2fy IOF;

    11

    Rw;ulre 0:9 6 ht=t60

    1 0:085 at

    h i

    t2fy ETF;

    12

    Rw;ulre 0:8 20 ht=t16

    1 0:015 at

    h i

    t2fy ITF;

    13where fy is the yield stress of I-beam, t is the web

    thickness, a is the bearing length, and ht is web height.

    7 Conclusions

    An experimental investigation was conducted in this

    study on the behavior of I-beam under web crippling.

    The ultimate capacity, failure modes, local deforma-

    tions and strain distributions of all specimens were

    reported. In addition, the corresponding finite element

    analysis was also performed and the validated FE

    model was used for the parametric study to evaluate

    the effects of main geometric parameters on the

    behavior of I-beam under web crippling Based on the

    experimental and numerical investigations, the fol-

    lowing conclusions can be drawn:

    (1) The ultimate capacity and initial stiffness of all

    specimens under web crippling significantly

    increased with the increase of bearing lengths.

    (2) The greater web slenderness of I-beam, the

    smaller initial stiffness and the better ductility.

    (3) The web crippling ultimate capacity of I-beam

    with web slenderness = 22.5 in interior-flange

    loading condition were larger than those in end-

    flange loading condition. Similarly, the web

    crippling ultimate capacity in one flange load-

    ing condition were larger than those in two

    flange loading condition.

    (4) A FEA that incorporated the geometric and

    material non-linear has been developed and

    verified against the experimental results. The

    FEM accurately predicted the behavior of

    I-beam under web crippling.

    (5) The proposed simple calculation method of web

    crippling ultimate capacity was verified to be

    accurate and reliable for I-beam under web

    crippling.

    Acknowledgments This research work was supported by theNational Natural Science Foundation of China (Nos. 51278209

    and 51478047) and the Research Grant for Young and Middle-

    aged Academic Staff of Huaqiao University (No. ZQN-PY110).

    The authors are also thankful to Fuan Steel Structure Engineering

    Co., Ltd., for the fabrication of test specimens. The tests were

    conducted in Fujian Key Laboratory on Structural Engineering

    and Disaster Reduction at Huaqiao University. The support

    provided by the laboratory staff is gratefully acknowledged.

    References

    1. Lyse I, Godfrey HJ (1933) Web crippling of steel beams.

    Fritz Laboratory Reports, p 1148

    2. Zhou F, Young B (2008) Aluminum tubular sections sub-

    jected to web cripplingPart I: tests and finite element

    analysis. Thin-Walled Struct 46:339351

    3. Zhou F, Young B (2008) Aluminum tubular sections sub-

    jected to web cripplingPart II: proposed design equations.

    Thin-Walled Struct 46:352361

    0

    50

    100

    150

    200

    250

    300

    350

    0 1 2 3 4 5N

    /kN

    /mm

    I100 -EOF-N150(Test)I100 -ETF-N150(Test)I100 -IOF-N150(Test)I100 -ITF-N150(Test)I100 -EOF-N150(FEA)I100 -ETF-N150(FEA)I100 -IOF-N150(FEA)I100 -ITF-N150(FEA)

    0100020003000400050006000700080009000

    T1 T2 T3 T4 T5

    i/

    Ti

    200kN(Test)200kN(FEA)400kN(Test)400kN(FEA)

    (a) load-displacement curves (b) equivalent strain-point of measurement curves (I160-ITF-N150)

    Fig. 10 Comparisonbetween FEA and test

    results for typical specimens

    Materials and Structures

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    Materials and Structures

    Experimental and finite element analysis research on I-beam under web cripplingAbstractIntroductionExperimental investigationSpecimens designMaterial propertiesLoading and test program

    Test resultsFailure modesComparison of ultimate capacity under web crippling with different bearing lengthsComparison of ultimate capacity under web crippling with different web slendernessComparison of ultimate capacity under web crippling in different boundary and loading conditionsLoad--equivalent strain on web curves

    Comparison of web crippling ultimate capacityFinite element analysisGeneralElement type and meshBoundary conditions and interfacesMethod of loadingMaterial modelingVerification of FEM

    Proposed design equationsConclusionsAcknowledgmentsReferences