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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.
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0
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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)
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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