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IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
__________________________________________________________________________________________
IC-RICE Conference Issue | Nov-2013, Available @ http://www.ijret.org 132
ULTIMATE STRENGTH OF COMPOSITE BEAM WITH WEB OPENINGS
SUBJECTED TO COMBINED NEGATIVE BENDING AND AXIAL
COMPRESSION
MA.Bavan1
, Shahrizan Bin Baharom2
, Siti Aminah Osman3
1, 2, 3
Department of Civil and Structural Engineering, National University of Malaysia, Bandar BaruBangi, Selangor,
Malaysia, mmbavan@yahoo.com
Abstract
Ultimate strength of composite beam subjected to combined interaction of negative bending and axial compression containing
openings in the web of steel beam are reported with various opening parameters such as shapes, diameter in circle openings, width in
square openings and distances between openings. A nonlinear three dimensional finite element model (FEM) was developed for
composite beam subjected to combined negative bending and axial compression. The model was validated with available experimental
data and it was predicted that the axial load, moment and failure mode at ultimate limit state were with an acceptable agreement
between FEM and experiment. A study on the web opening parameters was then carried out with validated finite element model.
Finally, it is shown that the ultimate load carrying capacity is reduced with openings in different quotients in the composite beam
subjected to combined interaction of negative bending and axial compression.
Keywords: composite beam with web openings, combined interaction of negative bending and axial compression, 3D non-
linear FEM models, ultimate limit state, failure mode
---------------------------------------------------------------------***---------------------------------------------------------------------
1. INTRODUCTION
The axial compression, applicable in the high rise buildings
due to the wind load where the composite beams are located in
the windward side, induces unfavorable phenomenon of
failure in the negative bending regions of composite beam
near internal supports. A wide range of previous research
studies are concentrated in the composite beam with web
openings subjected to either positive or negative bending in
past 30 years. The behavior and design of composite beams
subjected to negative bending and compression was reported
by Vasdravellis et al. [2012]. The composite beam with web
openings subjected to combined negative bending and axial
compression is not covered in literature. Thus, this paper
investigates the local buckling and ultimate strength of
composite beam with openings on web of structural steel
member subjected to combined negative bending and axial
compression.
2. EXPERIMENTAL PROGRAMS REVIEWS
A composite beam was included in this study, which was
experimentally carried out by Vasdravellis et al. [2012] and
the composite beam was labeled as CB3. The composite beam
dimension and test arrangements are shown in Figure 1. Both
vertical and axial loads were applied simultaneously until the
failure occurs, vertical load was applied to the steel beam on
the middle segment and the axial load was applied on the edge
surface of steel beam. The failure state was determined
through the failure in material components, and the axial load
and moment were presented at failure state as ultimate limit
state in results.
Fig1 Details of test set-up of composite beam subjected to negative bending and axial compression
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
__________________________________________________________________________________________
IC-RICE Conference Issue | Nov-2013, Available @ http://www.ijret.org 133
3. FEM MODEL AND VALIDATION
The FE model was developed in the software named
ABAQUS and global finite element analyses were conducted.
Three dimensional geometric components were developed to
concrete slab, steel beam and shear studs and the element
C3D8R was applied to all three dimensional material
components except steel beam. The element C3D8I was used
to apply to steel beam due to the high concentrated forces
applied on steel beam and the type of element T3D2 was
applied to reinforcing bars. A uniform slow nodal-
displacement control was maintained in the application of
loads and the vertical and axial loads were on the bottom
flange of steel beam and on the surface end of steel beam,
respectively. The support conditions were made with
considering the experimental work and the nodes in the
relevant area were protected in the vertical and axial
directions. The quasi-static solution in Abaqus explicit
dynamic solver was predicted by uniform slow load
application and smooth amplitude step. Due to the developed
half geometries, the symmetry boundary condition was made
along the direction of composite beam. The developed FE
model and boundary conditions are shown in Figure 2.
Surface-to-surface contact algorithm was used to determine
the contact surfaces. The stiffer body with application of
coarser mesh was selected as master surface. The contact
property was determined in each surface by tangential and
normal behaviours. Penalty friction formulation was selected
to its tangential behavior with the coefficient of 0.5 and the
hard pressure over closure was selected to its normal behavior
with allowing separation behavior. An embedded technique
was used to define the bond of wire mesh and concrete slab.
All the material components were developed with non-linear
behaviors by using the ultimate strength values from the rests
carried-out by Vasdravellis et al. [2012]. The concrete
material model was developed by plasticity damage models
with evaluation of yield surface hardening variables proposed
by Lubliner et al [1989] available in Abaqus. The biaxial
material property of concrete was used with the parameters for
strength hypothesis of concrete recommended by Kmiecik and
Kaminski [2011]. The uniaxial stress and strain responses in
compression and tension were developed by using the
equations proposed by Desay & Krishnan [1964] and
Eurocode [1994], respectively. Structural steel beam
characteristics was considered in the behavior of Von Mises
yield criterion with isotropic hardening law for preferring
large strain analysis proposed by Gattesco [1999]. The
material properties of shear stud and reinforcing bars were
developed by simplified stress and strain characteristics
responses. The convergence study was made with numbers of
meshes as course, medium and fine meshes in each material
component. In order the developed FE model to be used for
parametric studies, the results were compared with
experimental work. The FE model was matched in the failure
mode at ultimate limit state and the combination of axial
compression and moment were with an acceptable agreement.
The responses of axial load- vertical load and the comparison
of moment-axial load at ultimate limit state between
experiment and FE model are shown in Figure 3(a) and 3(b).
Fig. 2 Finite element model and boundary conditions
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
__________________________________________________________________________________________
IC-RICE Conference Issue | Nov-2013, Available @ http://www.ijret.org 134
Fig. 3 (a) Responses of axial load- vertical load (b) Comparison of moment-axial load at ultimate limit state
4. PARAMETRIC FEM STUDY
The validated FE model was then carried out for a range of
parameters. The ultimate strength of composite beam
significantly changes due to the influence of axial
compression (Vasdravellis et al., 2012). Table I shows the
conducted opening parameters in the web of steel beam and a
composite beam with openings is shown in the Figure 4. It
was observed that the early buckling was occurred in the web
and flange of steel beam where the openings were presented in
the steel beam. The numbers of openings was influenced on
both axial and vertical loads and the strength of composite was
reduced highly when high numbers of openings was applied.
Meanwhile, the strength of composite beam was slightly
reduced or no changes on the applications of low numbers of
openings in web. The diameter of circle openings and width of
square openings with raises were accelerated the failure state
in the compression zone of composite beam and in the narrow
areas due to the openings. The possible failure modes such as
concrete crushing and cracking failure, buckling in the web
and flange of steel beam, shear connection failure and
fractures of reinforcing bars were thoroughly alaysed in every
model. All parametric FEM of composite beam were failed by
local buckling because of the large portion of compressive
stresses were in the web of steel beam due to the shifted
plastic neutral axial to steel beam from concrete slab.
The moment was calculated in each model by considering
axial and vertical load with plastic neutral axis. The moment
and axial load are presented in results as ultimate limit state of
composite beam where the failure was occurred in the material
components. The deviations in axial load, vertical load and
moment by means of FEM with openings and without
openings are clearly expressed in the Table 1. The FEM
labeled as GE1 was weak in vertical load and the failure state
was occurred when the axial compressive load was higher than
the FEM without openings. It was observed that the middle of
steel beam was reached the maximum stresses by local
buckling even the stresses developed in the shear studs due to
the excess axial compression and the axial load was started to
drop down at the point of failure. The responses of axial load
and axial displacement of developed FEM are shown in Figure
5(a) to (d). The moment and axial load at ultimate limit state
of model are shown with validated model without openings in
the Figure 6(a) to (d). The Figure 7(a) and (b) show the typical
failure mode of FEM in the development of web buckling
where the circle and square openings applied. It could be
recommended the placing of longitudinal and transverse
stiffeners to be improved the web plate bending and axial
compression due to the development of longitudinal and
transverse stresses.
4.1 Final Sections
The FE models of the composite beam were used to study the
ultimate limit state behavior of the composite beam with web
openings subjected to combined axial compression and
negative bending. The commercial package Abaqus/Explicit
solver was used and the applicability of FE models was
confirmed with available experimental results in open
literature. Early failure state was occurred with the failure
modes of local buckling in the web and flanges of steel beam
of the composite beam with web openings. It could have been
possible to draw a certain conclusions in the behavior of
composite beam with web openings subjected to combined
interaction of axial compression and negative bending. The
axial compression was reduced the strength of composite
beam, and the openings in web additionally influence in the
combined action of axial compression and vertical load. The
investigated parameters such as shapes of openings, distances
between openings, diameters of circle openings and widths of
square openings gave significant changes in the ultimate limit
state of composite beam and major parameters affecting the
buckling of steel beam behavior. The axial compressive load
has an important role when the composite beam with openings
is subjected to combined loadings and thus, the authors
strongly feel that the ultimate limit state of composite beam
should be implemented with combined actions.
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
__________________________________________________________________________________________
IC-RICE Conference Issue | Nov-2013, Available @ http://www.ijret.org 135
REFERENCES
[1] Vasdravellis G, Uy B, Tan EL, Kirkland B, Behavior
and design of composite beams subjected to negative
bending and compression. J Constr Steel Res 79 (2012)
34-47.
[2] Tsavdaridis KD, Mello CD, Web buckling study of the
behaviour and strength of perforated steel beams with
different novel web openings shapes. J Constr Steel Res
67 (2011) 1605-1620.
[3] Lawson RM, Lim JBP, Ola SOP, Pull-out forces in
shear connectors in composite beams with large web
openings. J Constr Steel Res 87 (2013) 48-59.
[4] Lubliner J, Oliver J, Oller S, Onate E. A plastic-damage
model for concrete. International Journal of Solids and
Structures, Vol.25, 1989, pp. 299-329.
[5] Kmiecik P, Kaminski M., Modelling of reinforced
concrete structures and composite structures with
concrete strength degradation taken into consideration.
Proceedings of conference Archives of Civil and
Mechanical Engineering VI, Wroclaw, Poland 2011.
P.623-636.
[6] Desayi P, Krishnan S, Equation for the stress-strain
curve of concrete. ACIJ Proceed 1964;61(22):345-350.
[7] Gattesco N, Analytical modelling of nonlinear behavior
of composite beams with deformable connection. J
Constr Steel Res 52 (1999) 195-218.
[8] ABAQUS user's manual, version 6.11, Dassault
Systèmes Simulia Corp., Providence, RI, USA.
[9] BS EN 1994-1-1, Euro code 4; Design of composite
steel and concrete structure; Part 1.1; general rules and
rules for buildings, London (UK); British Standards
Institution; 2004.
Fig. 4 Composite beam with openings
Table 1 Variation of ultimate limit state in parametric studies
Group Type
Nos. of
opening
Distance
between
opening
(mm)
Diameter
of Circle
opening
(mm)
Width
of
square
opening
(mm)
Ultimate Limit state
UVFE
/UV
UAFE
/UA
MFE
/M
Vertical
Load
(kN)
Axial
Load
(kN)
Moment
(kNm)
Experiment - - - - - 718.00 166.00 0.91 0.95
Validated
FEM - - - - -
113.41 651.54 158.01 1.00 1.00 1.00
GA-1 Circle 10 400 150 - 97.41 592.58 133.12 1.16 1.10 1.19
GA-2 Circle 10 400 100 - 106.13 603.33 144.08 1.07 1.08 1.10
GA-3 Circle 10 400 50 - 111.44 628.20 152.24 1.02 1.04 1.04
GC-1 Circle 4 800 150 - 110.65 598.23 145.81 1.02 1.09 1.08
GC-2 Circle 4 800 100 - 114.67 625.99 154.38 0.99 1.04 1.02
GC-3 Circle 4 800 50 - 114.72 643.45 158.64 0.99 1.01 1.00
GE-1 Square 10 400 - 150 70.22 691.51 100.85 1.62 0.94 1.57
GE-2 Square 10 400 - 100 102.44 613.20 140.78 1.11 1.06 1.12
GE-3 Square 10 400 - 50 109.87 631.72 150.92 1.03 1.03 1.05
GG-1 Square 4 800 - 150 103.45 632.35 139.83 1.10 1.03 1.13
GG-2 Square 4 800 - 100 113.39 630.22 153.78 1.00 1.03 1.03
GG-3 Square 4 800 - 50 113.95 648.57 158.54 1.00 1.00 1.00
UVFE, UAFE and MFE denote ultimate vertical load, ultimate axial load and moment of FEM model without opening. UV, UA and
M denote ultimate vertical load, ultimate axial load and moment of FEM model in parametric studies.
IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308
__________________________________________________________________________________________
IC-RICE Conference Issue | Nov-2013, Available @ http://www.ijret.org 136
Fig. 5 (a)-(d) Responses of axial load and displacement of parametric FE models
Fig. 6 Responses of axial load and moment of parametric FE models
Fig. 7 Stress contour of FE models (a) GA1 (b) GE1

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Ultimate strength of composite beam with web openings subjected to combined negative bending and axial compression

  • 1. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ IC-RICE Conference Issue | Nov-2013, Available @ http://www.ijret.org 132 ULTIMATE STRENGTH OF COMPOSITE BEAM WITH WEB OPENINGS SUBJECTED TO COMBINED NEGATIVE BENDING AND AXIAL COMPRESSION MA.Bavan1 , Shahrizan Bin Baharom2 , Siti Aminah Osman3 1, 2, 3 Department of Civil and Structural Engineering, National University of Malaysia, Bandar BaruBangi, Selangor, Malaysia, mmbavan@yahoo.com Abstract Ultimate strength of composite beam subjected to combined interaction of negative bending and axial compression containing openings in the web of steel beam are reported with various opening parameters such as shapes, diameter in circle openings, width in square openings and distances between openings. A nonlinear three dimensional finite element model (FEM) was developed for composite beam subjected to combined negative bending and axial compression. The model was validated with available experimental data and it was predicted that the axial load, moment and failure mode at ultimate limit state were with an acceptable agreement between FEM and experiment. A study on the web opening parameters was then carried out with validated finite element model. Finally, it is shown that the ultimate load carrying capacity is reduced with openings in different quotients in the composite beam subjected to combined interaction of negative bending and axial compression. Keywords: composite beam with web openings, combined interaction of negative bending and axial compression, 3D non- linear FEM models, ultimate limit state, failure mode ---------------------------------------------------------------------***--------------------------------------------------------------------- 1. INTRODUCTION The axial compression, applicable in the high rise buildings due to the wind load where the composite beams are located in the windward side, induces unfavorable phenomenon of failure in the negative bending regions of composite beam near internal supports. A wide range of previous research studies are concentrated in the composite beam with web openings subjected to either positive or negative bending in past 30 years. The behavior and design of composite beams subjected to negative bending and compression was reported by Vasdravellis et al. [2012]. The composite beam with web openings subjected to combined negative bending and axial compression is not covered in literature. Thus, this paper investigates the local buckling and ultimate strength of composite beam with openings on web of structural steel member subjected to combined negative bending and axial compression. 2. EXPERIMENTAL PROGRAMS REVIEWS A composite beam was included in this study, which was experimentally carried out by Vasdravellis et al. [2012] and the composite beam was labeled as CB3. The composite beam dimension and test arrangements are shown in Figure 1. Both vertical and axial loads were applied simultaneously until the failure occurs, vertical load was applied to the steel beam on the middle segment and the axial load was applied on the edge surface of steel beam. The failure state was determined through the failure in material components, and the axial load and moment were presented at failure state as ultimate limit state in results. Fig1 Details of test set-up of composite beam subjected to negative bending and axial compression
  • 2. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ IC-RICE Conference Issue | Nov-2013, Available @ http://www.ijret.org 133 3. FEM MODEL AND VALIDATION The FE model was developed in the software named ABAQUS and global finite element analyses were conducted. Three dimensional geometric components were developed to concrete slab, steel beam and shear studs and the element C3D8R was applied to all three dimensional material components except steel beam. The element C3D8I was used to apply to steel beam due to the high concentrated forces applied on steel beam and the type of element T3D2 was applied to reinforcing bars. A uniform slow nodal- displacement control was maintained in the application of loads and the vertical and axial loads were on the bottom flange of steel beam and on the surface end of steel beam, respectively. The support conditions were made with considering the experimental work and the nodes in the relevant area were protected in the vertical and axial directions. The quasi-static solution in Abaqus explicit dynamic solver was predicted by uniform slow load application and smooth amplitude step. Due to the developed half geometries, the symmetry boundary condition was made along the direction of composite beam. The developed FE model and boundary conditions are shown in Figure 2. Surface-to-surface contact algorithm was used to determine the contact surfaces. The stiffer body with application of coarser mesh was selected as master surface. The contact property was determined in each surface by tangential and normal behaviours. Penalty friction formulation was selected to its tangential behavior with the coefficient of 0.5 and the hard pressure over closure was selected to its normal behavior with allowing separation behavior. An embedded technique was used to define the bond of wire mesh and concrete slab. All the material components were developed with non-linear behaviors by using the ultimate strength values from the rests carried-out by Vasdravellis et al. [2012]. The concrete material model was developed by plasticity damage models with evaluation of yield surface hardening variables proposed by Lubliner et al [1989] available in Abaqus. The biaxial material property of concrete was used with the parameters for strength hypothesis of concrete recommended by Kmiecik and Kaminski [2011]. The uniaxial stress and strain responses in compression and tension were developed by using the equations proposed by Desay & Krishnan [1964] and Eurocode [1994], respectively. Structural steel beam characteristics was considered in the behavior of Von Mises yield criterion with isotropic hardening law for preferring large strain analysis proposed by Gattesco [1999]. The material properties of shear stud and reinforcing bars were developed by simplified stress and strain characteristics responses. The convergence study was made with numbers of meshes as course, medium and fine meshes in each material component. In order the developed FE model to be used for parametric studies, the results were compared with experimental work. The FE model was matched in the failure mode at ultimate limit state and the combination of axial compression and moment were with an acceptable agreement. The responses of axial load- vertical load and the comparison of moment-axial load at ultimate limit state between experiment and FE model are shown in Figure 3(a) and 3(b). Fig. 2 Finite element model and boundary conditions
  • 3. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ IC-RICE Conference Issue | Nov-2013, Available @ http://www.ijret.org 134 Fig. 3 (a) Responses of axial load- vertical load (b) Comparison of moment-axial load at ultimate limit state 4. PARAMETRIC FEM STUDY The validated FE model was then carried out for a range of parameters. The ultimate strength of composite beam significantly changes due to the influence of axial compression (Vasdravellis et al., 2012). Table I shows the conducted opening parameters in the web of steel beam and a composite beam with openings is shown in the Figure 4. It was observed that the early buckling was occurred in the web and flange of steel beam where the openings were presented in the steel beam. The numbers of openings was influenced on both axial and vertical loads and the strength of composite was reduced highly when high numbers of openings was applied. Meanwhile, the strength of composite beam was slightly reduced or no changes on the applications of low numbers of openings in web. The diameter of circle openings and width of square openings with raises were accelerated the failure state in the compression zone of composite beam and in the narrow areas due to the openings. The possible failure modes such as concrete crushing and cracking failure, buckling in the web and flange of steel beam, shear connection failure and fractures of reinforcing bars were thoroughly alaysed in every model. All parametric FEM of composite beam were failed by local buckling because of the large portion of compressive stresses were in the web of steel beam due to the shifted plastic neutral axial to steel beam from concrete slab. The moment was calculated in each model by considering axial and vertical load with plastic neutral axis. The moment and axial load are presented in results as ultimate limit state of composite beam where the failure was occurred in the material components. The deviations in axial load, vertical load and moment by means of FEM with openings and without openings are clearly expressed in the Table 1. The FEM labeled as GE1 was weak in vertical load and the failure state was occurred when the axial compressive load was higher than the FEM without openings. It was observed that the middle of steel beam was reached the maximum stresses by local buckling even the stresses developed in the shear studs due to the excess axial compression and the axial load was started to drop down at the point of failure. The responses of axial load and axial displacement of developed FEM are shown in Figure 5(a) to (d). The moment and axial load at ultimate limit state of model are shown with validated model without openings in the Figure 6(a) to (d). The Figure 7(a) and (b) show the typical failure mode of FEM in the development of web buckling where the circle and square openings applied. It could be recommended the placing of longitudinal and transverse stiffeners to be improved the web plate bending and axial compression due to the development of longitudinal and transverse stresses. 4.1 Final Sections The FE models of the composite beam were used to study the ultimate limit state behavior of the composite beam with web openings subjected to combined axial compression and negative bending. The commercial package Abaqus/Explicit solver was used and the applicability of FE models was confirmed with available experimental results in open literature. Early failure state was occurred with the failure modes of local buckling in the web and flanges of steel beam of the composite beam with web openings. It could have been possible to draw a certain conclusions in the behavior of composite beam with web openings subjected to combined interaction of axial compression and negative bending. The axial compression was reduced the strength of composite beam, and the openings in web additionally influence in the combined action of axial compression and vertical load. The investigated parameters such as shapes of openings, distances between openings, diameters of circle openings and widths of square openings gave significant changes in the ultimate limit state of composite beam and major parameters affecting the buckling of steel beam behavior. The axial compressive load has an important role when the composite beam with openings is subjected to combined loadings and thus, the authors strongly feel that the ultimate limit state of composite beam should be implemented with combined actions.
  • 4. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ IC-RICE Conference Issue | Nov-2013, Available @ http://www.ijret.org 135 REFERENCES [1] Vasdravellis G, Uy B, Tan EL, Kirkland B, Behavior and design of composite beams subjected to negative bending and compression. J Constr Steel Res 79 (2012) 34-47. [2] Tsavdaridis KD, Mello CD, Web buckling study of the behaviour and strength of perforated steel beams with different novel web openings shapes. J Constr Steel Res 67 (2011) 1605-1620. [3] Lawson RM, Lim JBP, Ola SOP, Pull-out forces in shear connectors in composite beams with large web openings. J Constr Steel Res 87 (2013) 48-59. [4] Lubliner J, Oliver J, Oller S, Onate E. A plastic-damage model for concrete. International Journal of Solids and Structures, Vol.25, 1989, pp. 299-329. [5] Kmiecik P, Kaminski M., Modelling of reinforced concrete structures and composite structures with concrete strength degradation taken into consideration. Proceedings of conference Archives of Civil and Mechanical Engineering VI, Wroclaw, Poland 2011. P.623-636. [6] Desayi P, Krishnan S, Equation for the stress-strain curve of concrete. ACIJ Proceed 1964;61(22):345-350. [7] Gattesco N, Analytical modelling of nonlinear behavior of composite beams with deformable connection. J Constr Steel Res 52 (1999) 195-218. [8] ABAQUS user's manual, version 6.11, Dassault Systèmes Simulia Corp., Providence, RI, USA. [9] BS EN 1994-1-1, Euro code 4; Design of composite steel and concrete structure; Part 1.1; general rules and rules for buildings, London (UK); British Standards Institution; 2004. Fig. 4 Composite beam with openings Table 1 Variation of ultimate limit state in parametric studies Group Type Nos. of opening Distance between opening (mm) Diameter of Circle opening (mm) Width of square opening (mm) Ultimate Limit state UVFE /UV UAFE /UA MFE /M Vertical Load (kN) Axial Load (kN) Moment (kNm) Experiment - - - - - 718.00 166.00 0.91 0.95 Validated FEM - - - - - 113.41 651.54 158.01 1.00 1.00 1.00 GA-1 Circle 10 400 150 - 97.41 592.58 133.12 1.16 1.10 1.19 GA-2 Circle 10 400 100 - 106.13 603.33 144.08 1.07 1.08 1.10 GA-3 Circle 10 400 50 - 111.44 628.20 152.24 1.02 1.04 1.04 GC-1 Circle 4 800 150 - 110.65 598.23 145.81 1.02 1.09 1.08 GC-2 Circle 4 800 100 - 114.67 625.99 154.38 0.99 1.04 1.02 GC-3 Circle 4 800 50 - 114.72 643.45 158.64 0.99 1.01 1.00 GE-1 Square 10 400 - 150 70.22 691.51 100.85 1.62 0.94 1.57 GE-2 Square 10 400 - 100 102.44 613.20 140.78 1.11 1.06 1.12 GE-3 Square 10 400 - 50 109.87 631.72 150.92 1.03 1.03 1.05 GG-1 Square 4 800 - 150 103.45 632.35 139.83 1.10 1.03 1.13 GG-2 Square 4 800 - 100 113.39 630.22 153.78 1.00 1.03 1.03 GG-3 Square 4 800 - 50 113.95 648.57 158.54 1.00 1.00 1.00 UVFE, UAFE and MFE denote ultimate vertical load, ultimate axial load and moment of FEM model without opening. UV, UA and M denote ultimate vertical load, ultimate axial load and moment of FEM model in parametric studies.
  • 5. IJRET: International Journal of Research in Engineering and Technology eISSN: 2319-1163 | pISSN: 2321-7308 __________________________________________________________________________________________ IC-RICE Conference Issue | Nov-2013, Available @ http://www.ijret.org 136 Fig. 5 (a)-(d) Responses of axial load and displacement of parametric FE models Fig. 6 Responses of axial load and moment of parametric FE models Fig. 7 Stress contour of FE models (a) GA1 (b) GE1