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Proceedings of the International Conference on Emerging Trends in Engineering and Management (ICETEM14)
30 – 31, December 2014, Ernakulam, India
56
EFFECT OF CONNECTION ECCENTRICITY IN THE
BEHAVIOUR OF STEEL TENSION MEMBERS
Geethu C V1
, Unni Kartha G2
, Usha S3
1
M.Tech, Computer Aided Structural Engineering, Sree Narayana Gurukulam College of Engineering, Kadayiruppu,
Eranakulam, Kerala, India
2
Head of the Department, Dept of Civil Engineering, Federal Institute of Science and Technology, Ankamaly,
Eranakulam, Kerala, India
3
Professor, Sree Narayana Gurukulam College of Engineering, Kadayiruppu, Eranakulam, Kerala, India
ABSTRACT
Concrete and steel are often used in civil engineering structures. An integral part of some buildings are lateral
bracing and truss members, which are frequently subjected to tension loads. Lateral bracing is generally designed using
single angles, double angles or T sections connected with high strength bolts. When angles are used as tension members,
the most widely used arrangements are as single angles or as a pair of angles symmetrically placed about a gusset plate
that passes between them. However, often the location of the bolt gauge line will not coincide with the centroidal axis of
the member. Since the axial force in the main portion of the member (assumed to act through the centre of gravity of the
cross section) is eccentric, with respect to the connected ends, bending can also be present. But this bending effect due to
connection eccentricity is not considered in current design specifications for statically loaded tension members. The
present study has focused on examining the effects of connection eccentricity on bolted angle tension member capacities.
It is shown that connection eccentricity induced bending effects have the potential to significantly reduce the failure
capacity of a section. Also aims at developing robust finite element model to accurately predict the effect of connection
eccentricity on the failure capacities of the experimental specimens.
Keywords: Bending Moment, Connection Eccentricity, Failure Load, Stress Contour, Strain Contour, Yield Point.
1. INTRODUCTION
An integral part of some buildings are lateral bracing and truss members, which are frequently subjected to
tension loads. Lateral bracing is generally designed using single angles, double angles or T sections connected with high
strength bolts. When angles are used as tension members, the most widely used arrangements are as single angles or as a
pair of angles symmetrically placed about a gusset plate that passes between them. For practical reasons it is unusual to
be able to connect both legs of an angle and the influence of the connection of only one of the two legs on the tensile
capacity is referred to as shear lag. Shear lag is referred as the non-uniform stress distribution that occurs in a tension
member in which all the elements of the cross section are not directly connected. The shear lag reduces the effectiveness
of the component plates of a tension member that are not connected directly to a gusset plate because the entire section is
not fully effective at critical section location. Ideally, in these situations placement of the connectors (or centroid of the
connectors if multiple gauge lines are used) should be along the centroidal axis of the member. However, often the
location of the bolt gauge line does not lie along the centroidal axis of the member. The difference between the centroid
INTERNATIONAL JOURNAL OF CIVIL ENGINEERING AND
TECHNOLOGY (IJCIET)
ISSN 0976 – 6308 (Print)
ISSN 0976 – 6316(Online)
Volume 5, Issue 12, December (2014), pp. 56-65
© IAEME: www.iaeme.com/Ijciet.asp
Journal Impact Factor (2014): 7.9290 (Calculated by GISI)
www.jifactor.com
IJCIET
©IAEME
Proceedings of the International Conference on Emerging Trends in Engineering and Management (ICETEM14)
30 – 31, December 2014, Ernakulam, India
57
of the bolt group and the neutral axis of the member is the eccentricity of the connection. Because the axial force in the
main portion of the member (assumed to act through the centre of gravity of the cross section) is eccentric, with respect
to the connected ends, bending can also be present. So, the main focus of the work is on the detrimental effects of
connection eccentricities on the behaviour of steel tension members.
Present design considerations for statically loaded tension members do not consider the bending effects due to
connection eccentricity. Recent investigations on tension members have shown that connection eccentricity induced
bending effects have the potential to significantly reduce the failure capacity of a section. This paper aims at developing
robust finite element model for accurately predicting the effect of connection eccentricity on the failure capacities of the
experimental specimens. Finite element studies are useful when used in conjunction with an experimental testing
program. In this study, the finite element analysis of the ISA section is carried out using ANSYS SOLID185 element
capable of rep- resenting large deformation geometric and material nonlinearities. The connecting bolts are assumed to
be rigid. An elasto-plastic von Mises yield criterion combined with a tri- linear type constitutive model is used to
represent the material nonlinear effects. The work was focused on examining the effects of connection eccentricity on
load carrying capacity of bolted angle tension members. In this study, experimental as well as finite element analysis of
ISA 50 x 50 x 6, ISA 65 x 65 x 6 and ISA 75 x 75 x 6 using ANSYS was done. The connecting bolts are assumed to be
rigid and a surface-to-surface contact is used to fully transfer the load from the gusset plate to the web. Results of the
finite element analyses are compared with experimental results.
The organization of the paper is as follows. Section 2 describes the present design methodology adopted for
tension members with bolted end connections. Section 3 describes a literature review of the block shear and net section
rupture failure modes of tension members with bolted end connections. The experimental methodology adopted for
testing the specimens is presented in Section 4. In Section 5, a brief description of the experimental behaviour of the ISA
section specimens is given. The effect of connection eccentricity in the behaviour of steel tension members is presented
in section 6. A finite element modeling of the ISA sections that includes both geometric as well as material large
deformation effects is described in Section 7. Section 8, describes the conclusions of the present work. Lastly, Section 9,
presents the scope for future work.
2. PRESENT DESIGN CONSIDERATION
For the design of tension members the designer has to make calculation checks to determine the capacity of a
tension member: yielding of the gross cross sectional area, net section rupture of the critical cross-sectional area and
block shear. The lower of these controls the allowable load capacity of a specified member.
2.1. Gross section yielding
Steel members can sustain loads up to the ultimate load without failure. However, the members will elongate
considerably at this load, and hence make the structure unserviceable. The design strength Tdg is limited to the yielding of
gross cross section which is given by:
Tdg= fyAg / γm0 (1)
where,
fy = yield strength of the material in MPa
Ag = gross area of cross section in mm2
γm0= 1.10 = partial safety factor for failure at yielding
2.2. Net section rupture
This occurs when the tension member is connected to the main or other members by bolts. The holes made in
members for bolts will reduce the cross section, and hence net area will govern the failure in this case. Holes in members
cause stress concentration at service loads. From the theory of elasticity, the tensile stress adjacent to a hole will be about
two to three times the average stress on the net area. This depends on the ratio of the diameter of the hole to the width of
the plate normal to the direction of the stress. When the tension member with a hole is loaded statically, the point
adjacent to the hole reaches the yield stress fy first. On further loading, the stress in other fibres away from the hole
progressively reaches the yield stress fy. Deformations of the member continue with increasing load until final rupture of
the member occurs when the entire net cross section of the member reaches the ultimate stress fu. The rupture strength of
an angle connected through one leg is affected by shear lag. The design strength, Tdn, as governed by rupture at net
section is given by:
Tdn= 0.9 fuAnc / γm1 + β Agofy / γm0 (2)
Proceedings of the International Conference on Emerging Trends in Engineering and Management (ICETEM14)
30 – 31, December 2014, Ernakulam, India
58
where,
β = 1.4 – 0.076 (w/t) (fy / fu) (bs / Lc) ≤ fu γm0 / fy γm1
≥ 0.7
where,
w = outstand leg width
bs = shear lag width
Lc = Length of the end connection, i.e., distance between the outermost bolts in the end joint measured along the load
direction or length of the weld along the load direction.
2.3. Block shear failure
Block shear failure is considered as a potential failure mode at the ends of an axially loaded tension member. In
this failure mode, the failure of the member occurs along a path involving tension on one plane and shear on a
perpendicular plane along the fasteners. The block shear strength, Tdb , of connection shall be taken as the smaller of :
Tdb = (Avgfy /( √3 γm0) + fuAtn / γm1) (3)
Or
Tdb = (Avnfu / (√3 γm1) + fyAtg / γm0) (4)
where,
Avg, Avn = minimum gross and net area in shear along a line of transmitted force, respectively
Atg, Atn = minimum gross and net area in tension from the bolt hole to the toe of the angle, end bolt line, perpendicular to
the line of force
fu, fy = ultimate and yield stress of the material respectively
3. LITERATURE REVIEW
A detailed literature review was conducted. From that it was clear that connection eccentricity induced bending
moments have a potential to significantly reduce the failure load capacities of tension members. So, the main focus of the
work is on the detrimental effects of connection eccentricities on the behaviour of steel tension members. All the
previous tests were conducted on WT sections which are not available in the market here. In this study, experimental as
well as finite element analysis of ISA 50 X 50 X 6, ISA 65 X 65 X 6 and ISA 75 X 75 X 6 to get the effect of connection
eccentricity on the ultimate load capacity. The finite element analysis is to be done using the software, thus developing a
robust finite element model for predicting the effect of connection eccentricity on the failure capacities of the
experimental specimens.
4. EXPERIMENTAL METHODOLOGY
The purpose of present work is to investigate the effect of connection eccentricity on the failure capacities of
bolted angle tension members. In this work, connection eccentricity is varied, while keeping the pitch and end distance as
constant.
4.1. Experimental Specimen
The literature review showed studies that examined shear lag effects on the net section rupture capacities of
tension members. However, the present study has particular focus placed upon the effects of connection eccentricities
with regards to induced bending moments. The experimental program consists of one set of ISA 50 X 50 X 6, ISA 65 X
65 X 6 and ISA 75 X 75 X 6 that are 600 mm in length and fastened at both ends with a single row of high strength
friction grip (HSFG) bolts through one of the leg. The main focus of the experimental program has been on the effects of
connection eccentricity on the failure capacities as determined by the net section rupture and blocks shear failure modes.
In the experimental specimens, the connection eccentricity is varied. Pitch and end distances are held constant in all
specimens as 40mm and 30mm respectively. As per IS 800, the minimum edge distance to be provided for 12 mm
diameter bolt is 18mm. So in ISA 75 x 75 x 6 eccentricity can be varied by 13mm. ie. Bolts are provided at 31mm,
44mm and 55 mm in specimen 1, 2 and 3 respectively. In ISA 65 x 65 x 6 eccentricity can be varied by 8mm. ie. Bolts
are provided at 31mm, 39 mm and 47 mm in specimen 1, 2 and 3 respectively. In ISA 50 x 50 x 6 eccentricity can be
varied by 5 mm. ie. Bolts are provided at 26 mm, 31 mm and 36 mm in specimen 1, 2 and 3 respectively.
All specimens are fitted with a pair of bar-stock grips, which simulates gusset plate effects. They are used to
transfer the load from 1000 KN capacity universal testing machine (UTM) to the specimen. They are fabricated from 40
mm by 10 mm plate and have 12 mm diameter holes drilled at the appropriate pitch for ISA 50 X 50 X 6 and for ISA 65
Proceedings of the International Conference on Emerging Trends in Engineering and Management (ICETEM14)
30 – 31, December 2014, Ernakulam, India
59
X 65 X 6 and ISA 75 X 75 X 6 the plates are fabricated from 40 mm by 10 mm plate and have 14 mm diameter holes
drilled at the appropriate pitch. To prevent bending of the grip ends and, thus, enabling the UTM wedge-grips to have a
truer contact surface with the bar stock grips, spacer plates of the same thickness as a specimen thickness are to be placed
between the ends of the grips. Also, specimens of ISA 50 X 50 X 5 were fitted with 10 mm diameter bolts and others
were fitted with 12mm diameter bolts, tightened to the snug-tight condition, in standard holes located in the one leg.
Snug tight condition is defined as the tightness that exists when all plies in a joint are in firm contact. Once bolted, the
specimen-grip assembly is to be secured in a 1000-kN capacity universal testing machine with wedge grips. Each
specimen is to be then loaded pseudo statically to failure.
4.2. Specimen Fabrication
ISA 50 x 50 x 6, ISA 65 x 65 x 6 and ISA 75 x 75 x 6 each of length 1800 mm, 50 x 10 mm plate of 9120 mm
length and 40 x 10 mm plates of 4320mm length were bought. In addition high strength bolts of 10mm diameter (12
numbers) and 12mm diameter (20 numbers) were bought. ISA 50 x 50 x 6 are to be fitted with 10mm diameter bolts and
others with 12mm diameter bolts. The pitch and end distance are held constant as 40mm and 30mm respectively. In order
to prevent slipping of the specimen the surface of the plate is made rough by welding. Firstly the angle section and the
plates were cut to exact lengths. Appropriate positions were holed have to be drilled is then marked and bolt holes are
drilled in both sides of the angle specimen and at one side of the plate which is to be attached to the angle. Then the
specimen is assembles so that 4 plates are attached to each of the angle. (ie. 2 at top and bottom). Then the bolts are
tightened by wrenches.
4.3. Testing Procedure
After the appropriate grips were fastened to a ISA section the specimen-grip assembly is to be then placed and
centered in the UTM and then secured fast with the wedge-grips in the UTM crossheads. Each specimen is to be tested to
failure (at which point the load applied by the UTM would drop off considerably) by steadily increasing the applied load.
Fig. 1 shows a typical ISA specimen held in UTM.
Fig 1: ISA specimen clamped in UTM jaws
5. EXPERIMENTAL RESULTS
Four modes of failure were observed among the tests. The first mode, exhibited by most specimens with non-
zero connection eccentricities, involved necking down and subsequent rupture of the net section from the lead bolt hole
to the edge of the web. The second failure mode observed was a block shear failure evidenced by rupture of the net
tension area and either partial or full rupture of the gross shear area. The third failure mode consisted of full net section
rupture, with near-simultaneous rupture of both the web and flange areas and the forth one was the bolt failure. These
modes are described as partial rupture of the net section, block shear rupture, and full rupture of the net section
respectively. Table I shows the specimen dimensions as well as the failure loads obtained during the experimental test.
Proceedings of the International Conference on Emerging Trends in Engineering and Management (ICETEM14)
30 – 31, December 2014, Ernakulam, India
60
TABLE I: SPECIMEN DIMENSIONS AND FAILURE LOADS
Spec. no ISA
section
Length of
specimen
No of
bolts
Bolt
diameter
Gauge
distance
Failure
load
Spec. failure
type
1 50 x 50 x 6 600 2 10 26 108 BF
2 50 x 50 x 6 600 2 10 31 94 PNS
3 50 x 50 x 6 600 2 10 36 77 PNS
4 65 x 65 x 6 600 3 12 31 167 BS
5 65 x 65 x 6 600 3 12 39 130 PNS
6 65 x 65 x 6 600 3 12 47 94 PNS
7 75 x 75 x 6 600 3 12 31 253 FNS
8 75 x 75 x 6 600 3 12 44 194 PNS
9 75 x 75 x 6 600 3 12 57 139 PNS
a. All capacities are in shown in KN.
b. All dimensions are in mm.
c. PNS = Partial net section rupture, FNS = Full net section rupture, BS = Block shear, BF = Bolt failure.
5.1. Partial Rupture of the Net Section
The typical specimen failure (specimens: 2, 3, 5, 6, 8, 9) consisted of a partial rupturing of the net section
followed by the tearing of the web. The peak load was reached before fracturing of the full net section, but after rupture
of the partial net section. Fracturing of a specimen’s web initiated at the lead bolt hole and propagated to the web’s
outside edge. Necking down of the tension plane area preceded fracture. Specimens with small eccentricities exhibited a
significant amount of bolt hole deformation. However, it was observed that the amount of deformation decreased with
increasing eccentricity. Those specimens with the largest eccentricities demonstrated very minor hole deformation.
Fig. 2 shows a typical partial net section failure.
Fig 2: Partial Net Section Rupture Followed by the Tearing of Leg (Specimen 5)
Specimens also exhibited in-plane bending. Specimens with larger eccentricities had larger degrees of in-
plane bending. Fig. 3 shows in-plane bending of a specimen. After partial net section rupture had occurred, the
specimens experience significantly more in-plane bending compared with bending prior to fracture. This is due to a
plastic hinge being formed in the web opposite the fracture. Rotation of a connection is easily visible in the bolt hole
deformation patterns shown in the lead and last bolt holes in a connection. As a result of in-plane eccentricity, moments
produced in a specimen were resisted by the specimen’s connections and thus the deformation patterns observed. The
resisting moment of the connection was centered about the connection length’s centre. The evidence of this connection
rotation, as given bolt hole deformation patterns, decreased with decreased eccentricity.
Fig 3: In-plane Bending of the Specimen
Proceedings of the International Conference on Emerging Trends in Engineering and Management (ICETEM14)
30 – 31, December 2014, Ernakulam, India
61
5.2. Full Rupture of the Net Section
Full rupture of the net section occurred in specimens 7 which had a near zero eccentricity. There occurred a
rupturing of the leg on either side of the lead bolt hole, which propagated thorough the rest of both the leg areas
simultaneously. Fig. 4 shows specimen 7 failed in full net section rupture.
Fig 4: Full Net Section Rupture (Specimen 7)
5.3. Block Shear
Block shear failure occurred in specimens 4 which had a near zero eccentricity. The specimen failed in block
shear by a partial rupturing of the net shear area. Fig. 5 shows a typical block shear failure mode.
Fig 5: Block Shear Failure (Specimen 4)
Table II shows the variation of deflection under loading. In each specimen, as the eccentricity is increased the
deflection is increasing. Fig. 6 shows the Graph between load and deflection for typical partial net section, full net
section and block shear failure modes.
TABLE II: DEFLECTION OF SPECIMEN UNDER LOADING (FROM EXPERIMENT)
Load
(kN)
Deflection (mm)
Spec 1 Spec 2 Spec 3 Spec 4 Spec 5 Spec 6 Spec 7 Spec 8 Spec 9
0 0 0 0 0 0 0 0 0 0
5 2 4.9 7 3.9 5.8 3 3.6 6 6
10 3.1 6.6 8.75 6.1 8.4 4.6 5.35 7.8 8
15 3.9 7.98 9.75 7.45 9.4 6 6.8 9 9.6
20 4.2 8.66 10.8 8.4 10.35 7.7 8 9.9 10.6
25 5 10.55 11.8 9.3 11.05 8.9 8.9 10.4 11.4
30 6.4 11 12.58 9.9 11.6 9.7 9.5 10.9 12.1
35 6.8 11.6 13.1 10.5 12.3 10.3 11.5 12.65
40 7.5 12.4 13.98 11.1 12.8 10.8 11.8 13
45 8.1 13.2 14.7 11.4 13.4 11.5 12.3 13.65
50 8.4 13.9 15.15 12.1 14 12.5 12.6 14
55 9.1 14.82 16.3 12.55 14.4 13.2 14.5
60 9.8 13.95 14.95 14.4 15.2
65 10.3
Proceedings of the International Conference on Emerging Trends in Engineering and Management (ICETEM14)
30 – 31, December 2014, Ernakulam, India
62
Fig 6: Graph between load and deflection for typical partial net section, full net section and block shear failure modes
6. EFFECTS OF CONNECTION ECCENTRICITY
Eccentricity is readily observed to have a direct impact on a connection’s net section efficiency. From the
experimental study it is clear that as the eccentricity increases there is a reduction in the load carrying capacity of the
members. This is because of the induced bending moments due to the eccentricity in connection. The effects of an axial
load will be increased because of an eccentricity induced flexural load. This will have the greatest effect on the leg,
causing a premature rupture of the partial net section area. Therefore, the eccentricities should properly be accounted for
in the design equations, but are not. Current design practices do not include the bending effects due to connection
eccentricity. So provisions need to be considered that account for connection eccentricity effects. Presently, eccentricity
induced bending effects are disregarded in design, but as shown in this study the effects of eccentricity reducing the net
section efficiency of bolted connections needs to be considered.
7. FINITE ELEMENT MODELLING
In this section, finite element modelling of the experimental ISA specimens is described. FEA as applied
in engineering is a computational tool for performing engineering analysis. The FEA is performed using 3D structural
solid elements that are capable of representing large deformation geometric and material non-linearities. In the current
study, each of the ISA specimens, shown in Table 1, is analyzed. SOLID185 is used for the 3-D modeling of solid
structures. It is defined by eight nodes having three degrees of freedom at each node: translations in the nodal x, y, and z
directions. The element has plasticity, hyperelasticity, stress stiffening, creep, large deflection, and large strain
capabilities. It also has mixed formulation capability for simulating deformations of nearly incompressible elastoplastic
materials, and fully incompressible hyperelastic materials. An elasto-plastic von Mises yield criterion is adopted to
represent the material non- linear effects. The finite element model included both geometric as well as material nonlinear
effects. The leading edge of the gusset plate is constrained in all the directions except for the longitudinal direction. A
longitudinal displacement boundary condition is applied at the leading edge of the gusset plate. Figure shows the stress
contours, strain contours and deformation at failure. The maximum stress and strain is obtained around the bolt hole. The
results of the work are tabulated in table III. Table IV shows the variation of deflection under loading as obtained from
finite element analysis. In each specimen, as the eccentricity is increased the deflection is increasing.
Fig 7: Finite Element Model (Specimen 8)
Proceedings of the International Conference on Emerging Trends in Engineering and Management (ICETEM14)
30 – 31, December 2014, Ernakulam, India
63
Fig 8: Stress contour at failure (specimen 8) Fig 9: Strain contour at failure (specimen 8)
Fig 10: Deformation diagram (specimen 8)
TABLE III: RESULTS OF THE WORK
Specimen Yield point Failure load Stress at failure Strain at failure Deformation
SP-1 77 108 350.172 0.001691 0.485554
SP-2 66 94 372.901 0.001805 0.444047
SP-3 62 77 314.099 0.001511 0.379868
SP-4 75 167 550.932 0.002695 0.764691
SP-5 60 130 553.399 0.002707 0.634167
SP-6 57 94 418.202 0.002031 0.490776
SP-7 110 253 648.127 0.003181 0.944891
SP-8 98 194 432.192 0.002111 0.571577
SP-9 65 139 539.541 0.002638 0.609589
Proceedings of the International Conference on Emerging Trends in Engineering and Management (ICETEM14)
30 – 31, December 2014, Ernakulam, India
64
TABLE IV: DEFLECTION OF SPECIMEN UNDER LOADING (FROM FEA)
Load Deflection (mm)
(kN) Spec 1 Spec 2 Spec 3 Spec 4 Spec 5 Spec 6 Spec 7 Spec 8 Spec 9
0 0 0 0 0 0 0 0 0 0
5 1.13 1.46 1.66 1.25 1.41 1.49 1.36 1.85 1.44
10 2.27 2.92 3.32 2.51 2.82 2.99 2.73 2.76 2.88
15 3.41 4.38 4.98 3.77 4.23 4.49 4.1 4.15 4.32
20 4.55 5.84 6.64 5.03 5.64 5.98 5.47 5.53 5.76
25 5.69 7.3 8.3 6.28 7.05 7.48 6.83 6.92 7.2
30 6.83 8.76 9.96 7.54 8.47 8.98 8.2 8.3 8.64
35 7.96 10.22 11.62 8.8 9.88 10.47 9.57 9.69 10.08
40 9.1 11.68 13.28 10.06 11.29 11.97 10.94 11.07 11.52
45 10.24 13.14 14.94 11.31 12.7 13.47 12.3 12.75 12.96
50 11.38 14.6 16.6 12.57 14.11 14.96 13.67 13.84 14.4
55 12.52 16.07 18.27 13.83 15.52 16.46 15.04 15.23 15.84
60 13.66 17.53 19.93 15.09 16.94 17.96 16.41 16.61 17.28
65 14.8 18.99 21.59 16.39 18.35 19.45 17.77 17.99 18.72
8. CONCLUSION
Single angles or symmetrically placed double angles with gusset plate in between are often used in civil
engineering structures. In such cases the centroidal axis of the member will not coincide with the bolt gage line. Since the
axial force in the main portion of the member is eccentric, with respect to the connected ends, bending can also be
present. But this bending effect due to connection eccentricity is not considered in current design specifications for
statically loaded tension members. The present work was focused on examining the effects of connection eccentricity on
bolted angle tension member capacities. Here the connection eccentricity is varied while keeping the pitch and end
distance as constant and the failure load was obtained from the test for each experimental specimen. All the three modes
of failure were observed during the test viz, partial net section failure, full net section failure and block shear failure.
Stress and strain contours at failure as well as the yield point were obtained from finite element analysis. Eccentricity is
readily observed to have a direct impact on a connection’s net section efficiency. From the experimental study it is clear
that as the eccentricity increases there is a reduction in the load carrying capacity of the members. This is because of the
induced bending moments due to the eccentricity in connection. Presently, eccentricity induced bending effects are
disregarded in design. Provisions need to be considered that account for connection eccentricity effects. A more
extensive review of specimens needs to be made to see if the present findings are applicable to other specimen
configurations and connection geometries.
9. SCOPE FOR FUTURE WORK
The present work was focused on examining the effects of connection eccentricity on bolted angle steel tension
member capacities. Here the connection eccentricity is varied while keeping the pitch and end distance as constant and
the failure load was obtained from the test for each experimental specimen. The above work can be extended for different
metals. Also the work can be extended by varying connection length and by using punched holes instead of drilled holes
as in present work. Higher order elements can be used to get more precise results.
REFERENCES
[1] Lip H Teh and Veysel Yasici, Effects of Shear Lag on the Bolted Cold Formed Steel Sections, Engineering
Structures, Vol 52, 2013, 536-544.
[2] Cem Topkaya, A Finite Element Parametric Study on Block Shear Failure of Steel Tension Members, Journal of
Constructional Steel Research, Vol 60, 2004, 1615-1635.
Proceedings of the International Conference on Emerging Trends in Engineering and Management (ICETEM14)
30 – 31, December 2014, Ernakulam, India
65
[3] K. E. Barth, J. G. Orbison and R. Nukala, Behavior of Steel Tension Members Subjected to Uniaxial Loading,
Journal of Constructional Steel Research, Vol 58, 2002, 1103-1120.
[4] James G Orbisson, Karl E Barth, Peter A Bartels, Net Section Rupture in Tension Members with Connection
Eccentricity, Journal of Structural Engineering, Vol 128, 2002, 976-985.
[5] James G Orbison, Mark E Wagner and William P Fritz, Tension Plane Behaviour in Single Row Bolted
Connections Subject to Block Shear, Journal of Constructional Steel Research, Vol 49, 1999, 225-239.
[6] Murthy, K. S. Madugula, S. Mohan, Angles in Eccentric Tension, Journal of Structural Engineering, Vol 114,
1998, 2387-2396.
[7] Geoffrey L Kulak, Eric Yue Wu, Shear Lag in Bolted Angle Tension Members, Journal of Structural
Engineering, Vol 123, 1997, 1144-1152.
[8] W Samuel Easterling, Lisa Gonzalez Giroux, Shear Lag Effects in Steel Tension Members, American Institute
of Steel Construction, 1993, 77-89.
[9] Reidar Bjorhovde, S. K. Chakrabarti, Tests of Full Size Gusset Plate Connections, Journal of Structural
Engineering, Vol 111, 1985, 667-684.
[10] James M Ricles, Joseph A Yura, Full-scale Testing of Coped and Uncoped Double-row Bolted-web
Connections, Journal of Structural Engineering, Vol 109, 1983, 126-142.
[11] Wani Ahmad and Javed Ahmad Bhat, “Pre-Tensioned Precast Elements as a Replacement to Wooden Bracings
in the Armature Cross Wall System: An Abstract Attempt to Revive the Forgotten Heritage”, International
Journal of Civil Engineering & Technology (IJCIET), Volume 3, Issue 2, 2012, pp. 181 - 187, ISSN Print:
0976 – 6308, ISSN Online: 0976 – 6316.

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Effect of connection eccentricity in the behaviour of steel tension members

  • 1. Proceedings of the International Conference on Emerging Trends in Engineering and Management (ICETEM14) 30 – 31, December 2014, Ernakulam, India 56 EFFECT OF CONNECTION ECCENTRICITY IN THE BEHAVIOUR OF STEEL TENSION MEMBERS Geethu C V1 , Unni Kartha G2 , Usha S3 1 M.Tech, Computer Aided Structural Engineering, Sree Narayana Gurukulam College of Engineering, Kadayiruppu, Eranakulam, Kerala, India 2 Head of the Department, Dept of Civil Engineering, Federal Institute of Science and Technology, Ankamaly, Eranakulam, Kerala, India 3 Professor, Sree Narayana Gurukulam College of Engineering, Kadayiruppu, Eranakulam, Kerala, India ABSTRACT Concrete and steel are often used in civil engineering structures. An integral part of some buildings are lateral bracing and truss members, which are frequently subjected to tension loads. Lateral bracing is generally designed using single angles, double angles or T sections connected with high strength bolts. When angles are used as tension members, the most widely used arrangements are as single angles or as a pair of angles symmetrically placed about a gusset plate that passes between them. However, often the location of the bolt gauge line will not coincide with the centroidal axis of the member. Since the axial force in the main portion of the member (assumed to act through the centre of gravity of the cross section) is eccentric, with respect to the connected ends, bending can also be present. But this bending effect due to connection eccentricity is not considered in current design specifications for statically loaded tension members. The present study has focused on examining the effects of connection eccentricity on bolted angle tension member capacities. It is shown that connection eccentricity induced bending effects have the potential to significantly reduce the failure capacity of a section. Also aims at developing robust finite element model to accurately predict the effect of connection eccentricity on the failure capacities of the experimental specimens. Keywords: Bending Moment, Connection Eccentricity, Failure Load, Stress Contour, Strain Contour, Yield Point. 1. INTRODUCTION An integral part of some buildings are lateral bracing and truss members, which are frequently subjected to tension loads. Lateral bracing is generally designed using single angles, double angles or T sections connected with high strength bolts. When angles are used as tension members, the most widely used arrangements are as single angles or as a pair of angles symmetrically placed about a gusset plate that passes between them. For practical reasons it is unusual to be able to connect both legs of an angle and the influence of the connection of only one of the two legs on the tensile capacity is referred to as shear lag. Shear lag is referred as the non-uniform stress distribution that occurs in a tension member in which all the elements of the cross section are not directly connected. The shear lag reduces the effectiveness of the component plates of a tension member that are not connected directly to a gusset plate because the entire section is not fully effective at critical section location. Ideally, in these situations placement of the connectors (or centroid of the connectors if multiple gauge lines are used) should be along the centroidal axis of the member. However, often the location of the bolt gauge line does not lie along the centroidal axis of the member. The difference between the centroid INTERNATIONAL JOURNAL OF CIVIL ENGINEERING AND TECHNOLOGY (IJCIET) ISSN 0976 – 6308 (Print) ISSN 0976 – 6316(Online) Volume 5, Issue 12, December (2014), pp. 56-65 © IAEME: www.iaeme.com/Ijciet.asp Journal Impact Factor (2014): 7.9290 (Calculated by GISI) www.jifactor.com IJCIET ©IAEME
  • 2. Proceedings of the International Conference on Emerging Trends in Engineering and Management (ICETEM14) 30 – 31, December 2014, Ernakulam, India 57 of the bolt group and the neutral axis of the member is the eccentricity of the connection. Because the axial force in the main portion of the member (assumed to act through the centre of gravity of the cross section) is eccentric, with respect to the connected ends, bending can also be present. So, the main focus of the work is on the detrimental effects of connection eccentricities on the behaviour of steel tension members. Present design considerations for statically loaded tension members do not consider the bending effects due to connection eccentricity. Recent investigations on tension members have shown that connection eccentricity induced bending effects have the potential to significantly reduce the failure capacity of a section. This paper aims at developing robust finite element model for accurately predicting the effect of connection eccentricity on the failure capacities of the experimental specimens. Finite element studies are useful when used in conjunction with an experimental testing program. In this study, the finite element analysis of the ISA section is carried out using ANSYS SOLID185 element capable of rep- resenting large deformation geometric and material nonlinearities. The connecting bolts are assumed to be rigid. An elasto-plastic von Mises yield criterion combined with a tri- linear type constitutive model is used to represent the material nonlinear effects. The work was focused on examining the effects of connection eccentricity on load carrying capacity of bolted angle tension members. In this study, experimental as well as finite element analysis of ISA 50 x 50 x 6, ISA 65 x 65 x 6 and ISA 75 x 75 x 6 using ANSYS was done. The connecting bolts are assumed to be rigid and a surface-to-surface contact is used to fully transfer the load from the gusset plate to the web. Results of the finite element analyses are compared with experimental results. The organization of the paper is as follows. Section 2 describes the present design methodology adopted for tension members with bolted end connections. Section 3 describes a literature review of the block shear and net section rupture failure modes of tension members with bolted end connections. The experimental methodology adopted for testing the specimens is presented in Section 4. In Section 5, a brief description of the experimental behaviour of the ISA section specimens is given. The effect of connection eccentricity in the behaviour of steel tension members is presented in section 6. A finite element modeling of the ISA sections that includes both geometric as well as material large deformation effects is described in Section 7. Section 8, describes the conclusions of the present work. Lastly, Section 9, presents the scope for future work. 2. PRESENT DESIGN CONSIDERATION For the design of tension members the designer has to make calculation checks to determine the capacity of a tension member: yielding of the gross cross sectional area, net section rupture of the critical cross-sectional area and block shear. The lower of these controls the allowable load capacity of a specified member. 2.1. Gross section yielding Steel members can sustain loads up to the ultimate load without failure. However, the members will elongate considerably at this load, and hence make the structure unserviceable. The design strength Tdg is limited to the yielding of gross cross section which is given by: Tdg= fyAg / γm0 (1) where, fy = yield strength of the material in MPa Ag = gross area of cross section in mm2 γm0= 1.10 = partial safety factor for failure at yielding 2.2. Net section rupture This occurs when the tension member is connected to the main or other members by bolts. The holes made in members for bolts will reduce the cross section, and hence net area will govern the failure in this case. Holes in members cause stress concentration at service loads. From the theory of elasticity, the tensile stress adjacent to a hole will be about two to three times the average stress on the net area. This depends on the ratio of the diameter of the hole to the width of the plate normal to the direction of the stress. When the tension member with a hole is loaded statically, the point adjacent to the hole reaches the yield stress fy first. On further loading, the stress in other fibres away from the hole progressively reaches the yield stress fy. Deformations of the member continue with increasing load until final rupture of the member occurs when the entire net cross section of the member reaches the ultimate stress fu. The rupture strength of an angle connected through one leg is affected by shear lag. The design strength, Tdn, as governed by rupture at net section is given by: Tdn= 0.9 fuAnc / γm1 + β Agofy / γm0 (2)
  • 3. Proceedings of the International Conference on Emerging Trends in Engineering and Management (ICETEM14) 30 – 31, December 2014, Ernakulam, India 58 where, β = 1.4 – 0.076 (w/t) (fy / fu) (bs / Lc) ≤ fu γm0 / fy γm1 ≥ 0.7 where, w = outstand leg width bs = shear lag width Lc = Length of the end connection, i.e., distance between the outermost bolts in the end joint measured along the load direction or length of the weld along the load direction. 2.3. Block shear failure Block shear failure is considered as a potential failure mode at the ends of an axially loaded tension member. In this failure mode, the failure of the member occurs along a path involving tension on one plane and shear on a perpendicular plane along the fasteners. The block shear strength, Tdb , of connection shall be taken as the smaller of : Tdb = (Avgfy /( √3 γm0) + fuAtn / γm1) (3) Or Tdb = (Avnfu / (√3 γm1) + fyAtg / γm0) (4) where, Avg, Avn = minimum gross and net area in shear along a line of transmitted force, respectively Atg, Atn = minimum gross and net area in tension from the bolt hole to the toe of the angle, end bolt line, perpendicular to the line of force fu, fy = ultimate and yield stress of the material respectively 3. LITERATURE REVIEW A detailed literature review was conducted. From that it was clear that connection eccentricity induced bending moments have a potential to significantly reduce the failure load capacities of tension members. So, the main focus of the work is on the detrimental effects of connection eccentricities on the behaviour of steel tension members. All the previous tests were conducted on WT sections which are not available in the market here. In this study, experimental as well as finite element analysis of ISA 50 X 50 X 6, ISA 65 X 65 X 6 and ISA 75 X 75 X 6 to get the effect of connection eccentricity on the ultimate load capacity. The finite element analysis is to be done using the software, thus developing a robust finite element model for predicting the effect of connection eccentricity on the failure capacities of the experimental specimens. 4. EXPERIMENTAL METHODOLOGY The purpose of present work is to investigate the effect of connection eccentricity on the failure capacities of bolted angle tension members. In this work, connection eccentricity is varied, while keeping the pitch and end distance as constant. 4.1. Experimental Specimen The literature review showed studies that examined shear lag effects on the net section rupture capacities of tension members. However, the present study has particular focus placed upon the effects of connection eccentricities with regards to induced bending moments. The experimental program consists of one set of ISA 50 X 50 X 6, ISA 65 X 65 X 6 and ISA 75 X 75 X 6 that are 600 mm in length and fastened at both ends with a single row of high strength friction grip (HSFG) bolts through one of the leg. The main focus of the experimental program has been on the effects of connection eccentricity on the failure capacities as determined by the net section rupture and blocks shear failure modes. In the experimental specimens, the connection eccentricity is varied. Pitch and end distances are held constant in all specimens as 40mm and 30mm respectively. As per IS 800, the minimum edge distance to be provided for 12 mm diameter bolt is 18mm. So in ISA 75 x 75 x 6 eccentricity can be varied by 13mm. ie. Bolts are provided at 31mm, 44mm and 55 mm in specimen 1, 2 and 3 respectively. In ISA 65 x 65 x 6 eccentricity can be varied by 8mm. ie. Bolts are provided at 31mm, 39 mm and 47 mm in specimen 1, 2 and 3 respectively. In ISA 50 x 50 x 6 eccentricity can be varied by 5 mm. ie. Bolts are provided at 26 mm, 31 mm and 36 mm in specimen 1, 2 and 3 respectively. All specimens are fitted with a pair of bar-stock grips, which simulates gusset plate effects. They are used to transfer the load from 1000 KN capacity universal testing machine (UTM) to the specimen. They are fabricated from 40 mm by 10 mm plate and have 12 mm diameter holes drilled at the appropriate pitch for ISA 50 X 50 X 6 and for ISA 65
  • 4. Proceedings of the International Conference on Emerging Trends in Engineering and Management (ICETEM14) 30 – 31, December 2014, Ernakulam, India 59 X 65 X 6 and ISA 75 X 75 X 6 the plates are fabricated from 40 mm by 10 mm plate and have 14 mm diameter holes drilled at the appropriate pitch. To prevent bending of the grip ends and, thus, enabling the UTM wedge-grips to have a truer contact surface with the bar stock grips, spacer plates of the same thickness as a specimen thickness are to be placed between the ends of the grips. Also, specimens of ISA 50 X 50 X 5 were fitted with 10 mm diameter bolts and others were fitted with 12mm diameter bolts, tightened to the snug-tight condition, in standard holes located in the one leg. Snug tight condition is defined as the tightness that exists when all plies in a joint are in firm contact. Once bolted, the specimen-grip assembly is to be secured in a 1000-kN capacity universal testing machine with wedge grips. Each specimen is to be then loaded pseudo statically to failure. 4.2. Specimen Fabrication ISA 50 x 50 x 6, ISA 65 x 65 x 6 and ISA 75 x 75 x 6 each of length 1800 mm, 50 x 10 mm plate of 9120 mm length and 40 x 10 mm plates of 4320mm length were bought. In addition high strength bolts of 10mm diameter (12 numbers) and 12mm diameter (20 numbers) were bought. ISA 50 x 50 x 6 are to be fitted with 10mm diameter bolts and others with 12mm diameter bolts. The pitch and end distance are held constant as 40mm and 30mm respectively. In order to prevent slipping of the specimen the surface of the plate is made rough by welding. Firstly the angle section and the plates were cut to exact lengths. Appropriate positions were holed have to be drilled is then marked and bolt holes are drilled in both sides of the angle specimen and at one side of the plate which is to be attached to the angle. Then the specimen is assembles so that 4 plates are attached to each of the angle. (ie. 2 at top and bottom). Then the bolts are tightened by wrenches. 4.3. Testing Procedure After the appropriate grips were fastened to a ISA section the specimen-grip assembly is to be then placed and centered in the UTM and then secured fast with the wedge-grips in the UTM crossheads. Each specimen is to be tested to failure (at which point the load applied by the UTM would drop off considerably) by steadily increasing the applied load. Fig. 1 shows a typical ISA specimen held in UTM. Fig 1: ISA specimen clamped in UTM jaws 5. EXPERIMENTAL RESULTS Four modes of failure were observed among the tests. The first mode, exhibited by most specimens with non- zero connection eccentricities, involved necking down and subsequent rupture of the net section from the lead bolt hole to the edge of the web. The second failure mode observed was a block shear failure evidenced by rupture of the net tension area and either partial or full rupture of the gross shear area. The third failure mode consisted of full net section rupture, with near-simultaneous rupture of both the web and flange areas and the forth one was the bolt failure. These modes are described as partial rupture of the net section, block shear rupture, and full rupture of the net section respectively. Table I shows the specimen dimensions as well as the failure loads obtained during the experimental test.
  • 5. Proceedings of the International Conference on Emerging Trends in Engineering and Management (ICETEM14) 30 – 31, December 2014, Ernakulam, India 60 TABLE I: SPECIMEN DIMENSIONS AND FAILURE LOADS Spec. no ISA section Length of specimen No of bolts Bolt diameter Gauge distance Failure load Spec. failure type 1 50 x 50 x 6 600 2 10 26 108 BF 2 50 x 50 x 6 600 2 10 31 94 PNS 3 50 x 50 x 6 600 2 10 36 77 PNS 4 65 x 65 x 6 600 3 12 31 167 BS 5 65 x 65 x 6 600 3 12 39 130 PNS 6 65 x 65 x 6 600 3 12 47 94 PNS 7 75 x 75 x 6 600 3 12 31 253 FNS 8 75 x 75 x 6 600 3 12 44 194 PNS 9 75 x 75 x 6 600 3 12 57 139 PNS a. All capacities are in shown in KN. b. All dimensions are in mm. c. PNS = Partial net section rupture, FNS = Full net section rupture, BS = Block shear, BF = Bolt failure. 5.1. Partial Rupture of the Net Section The typical specimen failure (specimens: 2, 3, 5, 6, 8, 9) consisted of a partial rupturing of the net section followed by the tearing of the web. The peak load was reached before fracturing of the full net section, but after rupture of the partial net section. Fracturing of a specimen’s web initiated at the lead bolt hole and propagated to the web’s outside edge. Necking down of the tension plane area preceded fracture. Specimens with small eccentricities exhibited a significant amount of bolt hole deformation. However, it was observed that the amount of deformation decreased with increasing eccentricity. Those specimens with the largest eccentricities demonstrated very minor hole deformation. Fig. 2 shows a typical partial net section failure. Fig 2: Partial Net Section Rupture Followed by the Tearing of Leg (Specimen 5) Specimens also exhibited in-plane bending. Specimens with larger eccentricities had larger degrees of in- plane bending. Fig. 3 shows in-plane bending of a specimen. After partial net section rupture had occurred, the specimens experience significantly more in-plane bending compared with bending prior to fracture. This is due to a plastic hinge being formed in the web opposite the fracture. Rotation of a connection is easily visible in the bolt hole deformation patterns shown in the lead and last bolt holes in a connection. As a result of in-plane eccentricity, moments produced in a specimen were resisted by the specimen’s connections and thus the deformation patterns observed. The resisting moment of the connection was centered about the connection length’s centre. The evidence of this connection rotation, as given bolt hole deformation patterns, decreased with decreased eccentricity. Fig 3: In-plane Bending of the Specimen
  • 6. Proceedings of the International Conference on Emerging Trends in Engineering and Management (ICETEM14) 30 – 31, December 2014, Ernakulam, India 61 5.2. Full Rupture of the Net Section Full rupture of the net section occurred in specimens 7 which had a near zero eccentricity. There occurred a rupturing of the leg on either side of the lead bolt hole, which propagated thorough the rest of both the leg areas simultaneously. Fig. 4 shows specimen 7 failed in full net section rupture. Fig 4: Full Net Section Rupture (Specimen 7) 5.3. Block Shear Block shear failure occurred in specimens 4 which had a near zero eccentricity. The specimen failed in block shear by a partial rupturing of the net shear area. Fig. 5 shows a typical block shear failure mode. Fig 5: Block Shear Failure (Specimen 4) Table II shows the variation of deflection under loading. In each specimen, as the eccentricity is increased the deflection is increasing. Fig. 6 shows the Graph between load and deflection for typical partial net section, full net section and block shear failure modes. TABLE II: DEFLECTION OF SPECIMEN UNDER LOADING (FROM EXPERIMENT) Load (kN) Deflection (mm) Spec 1 Spec 2 Spec 3 Spec 4 Spec 5 Spec 6 Spec 7 Spec 8 Spec 9 0 0 0 0 0 0 0 0 0 0 5 2 4.9 7 3.9 5.8 3 3.6 6 6 10 3.1 6.6 8.75 6.1 8.4 4.6 5.35 7.8 8 15 3.9 7.98 9.75 7.45 9.4 6 6.8 9 9.6 20 4.2 8.66 10.8 8.4 10.35 7.7 8 9.9 10.6 25 5 10.55 11.8 9.3 11.05 8.9 8.9 10.4 11.4 30 6.4 11 12.58 9.9 11.6 9.7 9.5 10.9 12.1 35 6.8 11.6 13.1 10.5 12.3 10.3 11.5 12.65 40 7.5 12.4 13.98 11.1 12.8 10.8 11.8 13 45 8.1 13.2 14.7 11.4 13.4 11.5 12.3 13.65 50 8.4 13.9 15.15 12.1 14 12.5 12.6 14 55 9.1 14.82 16.3 12.55 14.4 13.2 14.5 60 9.8 13.95 14.95 14.4 15.2 65 10.3
  • 7. Proceedings of the International Conference on Emerging Trends in Engineering and Management (ICETEM14) 30 – 31, December 2014, Ernakulam, India 62 Fig 6: Graph between load and deflection for typical partial net section, full net section and block shear failure modes 6. EFFECTS OF CONNECTION ECCENTRICITY Eccentricity is readily observed to have a direct impact on a connection’s net section efficiency. From the experimental study it is clear that as the eccentricity increases there is a reduction in the load carrying capacity of the members. This is because of the induced bending moments due to the eccentricity in connection. The effects of an axial load will be increased because of an eccentricity induced flexural load. This will have the greatest effect on the leg, causing a premature rupture of the partial net section area. Therefore, the eccentricities should properly be accounted for in the design equations, but are not. Current design practices do not include the bending effects due to connection eccentricity. So provisions need to be considered that account for connection eccentricity effects. Presently, eccentricity induced bending effects are disregarded in design, but as shown in this study the effects of eccentricity reducing the net section efficiency of bolted connections needs to be considered. 7. FINITE ELEMENT MODELLING In this section, finite element modelling of the experimental ISA specimens is described. FEA as applied in engineering is a computational tool for performing engineering analysis. The FEA is performed using 3D structural solid elements that are capable of representing large deformation geometric and material non-linearities. In the current study, each of the ISA specimens, shown in Table 1, is analyzed. SOLID185 is used for the 3-D modeling of solid structures. It is defined by eight nodes having three degrees of freedom at each node: translations in the nodal x, y, and z directions. The element has plasticity, hyperelasticity, stress stiffening, creep, large deflection, and large strain capabilities. It also has mixed formulation capability for simulating deformations of nearly incompressible elastoplastic materials, and fully incompressible hyperelastic materials. An elasto-plastic von Mises yield criterion is adopted to represent the material non- linear effects. The finite element model included both geometric as well as material nonlinear effects. The leading edge of the gusset plate is constrained in all the directions except for the longitudinal direction. A longitudinal displacement boundary condition is applied at the leading edge of the gusset plate. Figure shows the stress contours, strain contours and deformation at failure. The maximum stress and strain is obtained around the bolt hole. The results of the work are tabulated in table III. Table IV shows the variation of deflection under loading as obtained from finite element analysis. In each specimen, as the eccentricity is increased the deflection is increasing. Fig 7: Finite Element Model (Specimen 8)
  • 8. Proceedings of the International Conference on Emerging Trends in Engineering and Management (ICETEM14) 30 – 31, December 2014, Ernakulam, India 63 Fig 8: Stress contour at failure (specimen 8) Fig 9: Strain contour at failure (specimen 8) Fig 10: Deformation diagram (specimen 8) TABLE III: RESULTS OF THE WORK Specimen Yield point Failure load Stress at failure Strain at failure Deformation SP-1 77 108 350.172 0.001691 0.485554 SP-2 66 94 372.901 0.001805 0.444047 SP-3 62 77 314.099 0.001511 0.379868 SP-4 75 167 550.932 0.002695 0.764691 SP-5 60 130 553.399 0.002707 0.634167 SP-6 57 94 418.202 0.002031 0.490776 SP-7 110 253 648.127 0.003181 0.944891 SP-8 98 194 432.192 0.002111 0.571577 SP-9 65 139 539.541 0.002638 0.609589
  • 9. Proceedings of the International Conference on Emerging Trends in Engineering and Management (ICETEM14) 30 – 31, December 2014, Ernakulam, India 64 TABLE IV: DEFLECTION OF SPECIMEN UNDER LOADING (FROM FEA) Load Deflection (mm) (kN) Spec 1 Spec 2 Spec 3 Spec 4 Spec 5 Spec 6 Spec 7 Spec 8 Spec 9 0 0 0 0 0 0 0 0 0 0 5 1.13 1.46 1.66 1.25 1.41 1.49 1.36 1.85 1.44 10 2.27 2.92 3.32 2.51 2.82 2.99 2.73 2.76 2.88 15 3.41 4.38 4.98 3.77 4.23 4.49 4.1 4.15 4.32 20 4.55 5.84 6.64 5.03 5.64 5.98 5.47 5.53 5.76 25 5.69 7.3 8.3 6.28 7.05 7.48 6.83 6.92 7.2 30 6.83 8.76 9.96 7.54 8.47 8.98 8.2 8.3 8.64 35 7.96 10.22 11.62 8.8 9.88 10.47 9.57 9.69 10.08 40 9.1 11.68 13.28 10.06 11.29 11.97 10.94 11.07 11.52 45 10.24 13.14 14.94 11.31 12.7 13.47 12.3 12.75 12.96 50 11.38 14.6 16.6 12.57 14.11 14.96 13.67 13.84 14.4 55 12.52 16.07 18.27 13.83 15.52 16.46 15.04 15.23 15.84 60 13.66 17.53 19.93 15.09 16.94 17.96 16.41 16.61 17.28 65 14.8 18.99 21.59 16.39 18.35 19.45 17.77 17.99 18.72 8. CONCLUSION Single angles or symmetrically placed double angles with gusset plate in between are often used in civil engineering structures. In such cases the centroidal axis of the member will not coincide with the bolt gage line. Since the axial force in the main portion of the member is eccentric, with respect to the connected ends, bending can also be present. But this bending effect due to connection eccentricity is not considered in current design specifications for statically loaded tension members. The present work was focused on examining the effects of connection eccentricity on bolted angle tension member capacities. Here the connection eccentricity is varied while keeping the pitch and end distance as constant and the failure load was obtained from the test for each experimental specimen. All the three modes of failure were observed during the test viz, partial net section failure, full net section failure and block shear failure. Stress and strain contours at failure as well as the yield point were obtained from finite element analysis. Eccentricity is readily observed to have a direct impact on a connection’s net section efficiency. From the experimental study it is clear that as the eccentricity increases there is a reduction in the load carrying capacity of the members. This is because of the induced bending moments due to the eccentricity in connection. Presently, eccentricity induced bending effects are disregarded in design. Provisions need to be considered that account for connection eccentricity effects. A more extensive review of specimens needs to be made to see if the present findings are applicable to other specimen configurations and connection geometries. 9. SCOPE FOR FUTURE WORK The present work was focused on examining the effects of connection eccentricity on bolted angle steel tension member capacities. Here the connection eccentricity is varied while keeping the pitch and end distance as constant and the failure load was obtained from the test for each experimental specimen. The above work can be extended for different metals. Also the work can be extended by varying connection length and by using punched holes instead of drilled holes as in present work. Higher order elements can be used to get more precise results. REFERENCES [1] Lip H Teh and Veysel Yasici, Effects of Shear Lag on the Bolted Cold Formed Steel Sections, Engineering Structures, Vol 52, 2013, 536-544. [2] Cem Topkaya, A Finite Element Parametric Study on Block Shear Failure of Steel Tension Members, Journal of Constructional Steel Research, Vol 60, 2004, 1615-1635.
  • 10. Proceedings of the International Conference on Emerging Trends in Engineering and Management (ICETEM14) 30 – 31, December 2014, Ernakulam, India 65 [3] K. E. Barth, J. G. Orbison and R. Nukala, Behavior of Steel Tension Members Subjected to Uniaxial Loading, Journal of Constructional Steel Research, Vol 58, 2002, 1103-1120. [4] James G Orbisson, Karl E Barth, Peter A Bartels, Net Section Rupture in Tension Members with Connection Eccentricity, Journal of Structural Engineering, Vol 128, 2002, 976-985. [5] James G Orbison, Mark E Wagner and William P Fritz, Tension Plane Behaviour in Single Row Bolted Connections Subject to Block Shear, Journal of Constructional Steel Research, Vol 49, 1999, 225-239. [6] Murthy, K. S. Madugula, S. Mohan, Angles in Eccentric Tension, Journal of Structural Engineering, Vol 114, 1998, 2387-2396. [7] Geoffrey L Kulak, Eric Yue Wu, Shear Lag in Bolted Angle Tension Members, Journal of Structural Engineering, Vol 123, 1997, 1144-1152. [8] W Samuel Easterling, Lisa Gonzalez Giroux, Shear Lag Effects in Steel Tension Members, American Institute of Steel Construction, 1993, 77-89. [9] Reidar Bjorhovde, S. K. Chakrabarti, Tests of Full Size Gusset Plate Connections, Journal of Structural Engineering, Vol 111, 1985, 667-684. [10] James M Ricles, Joseph A Yura, Full-scale Testing of Coped and Uncoped Double-row Bolted-web Connections, Journal of Structural Engineering, Vol 109, 1983, 126-142. [11] Wani Ahmad and Javed Ahmad Bhat, “Pre-Tensioned Precast Elements as a Replacement to Wooden Bracings in the Armature Cross Wall System: An Abstract Attempt to Revive the Forgotten Heritage”, International Journal of Civil Engineering & Technology (IJCIET), Volume 3, Issue 2, 2012, pp. 181 - 187, ISSN Print: 0976 – 6308, ISSN Online: 0976 – 6316.