CHAPTER 5 CODAL COMPARISON -...
Transcript of CHAPTER 5 CODAL COMPARISON -...
117
CHAPTER 5
CODAL COMPARISON
5.1 GENERAL
Singly symmetric angle sections may fail either by buckling about
the plane of symmetry or by a combination of twisting and bending. For open
sections like plain angles, lipped angles, channels, lipped channels the
torsional flexural buckling load can be significantly lower than the Euler load.
5.2 BUCKLING OF MONO SYMMETRIC SECTIONS
A singly symmetric section, centrally loaded tends to bend in
one of the principle planes containing the centroidal axis. If this plane also
contains the shear centre axis, bending can take place without simultaneously
inducing twist. However, if this plane of bending does not contain the shear
centre axis as in the case of a member in a panel with panelling eccentricity,
the bending is accompanied by twisting. This torsional flexural buckling
deformation is shown in Figure 5.1. The section has only one axis of
symmetry, the x-axis and the shear centre axis lies on that axis and yo = 0.
Then the torsional-flexural buckling equation is given by (Timoshenko and
Gere, 1985)
0]r
xPP)P)(PP)[(P(P
20
20
2
xy =−−−− ϕ (5.1)
This relation is satisfied either if
2
y2
yl
EIπPP == (5.2)
118
or if
0r
xPP)P)(P(P
2
0
2
0
2
x =−−− ϕ (5.3)
where P - Critical load
E - Modulus of elasticity of steel
Iy - Moment of inertia about Y – axis
l - Unbraced length of column
x
y
u
C.G
x o
Shear
Centre
Shear
Centre
y
x
i
xo
C.G
v
Figure 5.1 Torsional-flexural buckling deformation
119
2
x
2
xl
EIπP = (Euler load for Ix) (5.4)
where Ix - Moment of inertia about x-axis
)l
ECπ(GJ
r
1P
2
w
2
2
0
+=ϕ (5.5)
where ro - The polar radius of gyration
G - Shearing modulus of elasticity
J - St. Venant torsional constant
Cw - Warping constant
xo - Distance from shear centre to centroid along the x-axis
yo - Distance from shear centre to centroid along the y-axis
u - x-axis translation
v - y-axis translation
I - rotation about shear centre w.r.t x-axis
In general the mode of buckling for the mono symmetric sections
depends on the unsupported length of the column. When the slenderness ratio
is in the Euler column range or more than 120 the column will fail in flexural
buckling. When the columns are short columns with slenderness ratio less
than 50, then the column will fail by local buckling or by yielding depending
on the flat width to thickness ratio of the element. When the columns are in
the intermediate range with slenderness ratio 50 to 120 the column may fail
by interaction of torsional, torsional-flexural, flexural and local buckling.
Most of the members in latticed masts are designed as intermediate columns.
Moreover the leg members of transmission line towers are mostly designed in
the inelastic range of stresses and compact sections are usually preferred.
When a mono symmetric section buckles in the torsional mode the
120
mid-section bifurcates by rotating about the shear centre. However sectional
failure will be initiated by local buckling of the plate elements. For compact
sections, the local buckling strength is always more than or equal to the
torsional buckling strength, the effect of torsional-flexural buckling must be
considered.
In general, torsional flexural buckling may be the critical mode of
failure for short columns with slender outstands. Transmission line towers
normally consist of two types of members. Leg members which are the main
load carrying members are connected on both flanges as shown in
Figure 5.2(a) and hence they are concentrically loaded. However bracing
members which add stability to the leg members are connected on one flange
only and are eccentrically loaded as shown in Figure 5.2(b).
Bra
cing
ShearCentre
Eccentricity
x
y
C.G C.G
y
Bracing
Leg
x x
y
y
(a) Leg member (b) Bracing member
Figure 5.2 Connection details
121
When mono symmetric sections are subjected to eccentric loading,
the flexural buckling load about weak axis is lower than the torsional flexural
buckling load. On the other hand if the torsional flexural buckling load is
lower than the flexural buckling load the member tends to twist and fail by
torsional flexural. The load at which the members start twisting depends on
the restraint coefficients, eccentricity and sectional parameters.
5.3 STUDIES ON EQUIVALENT RADIUS OF GYRATION
The effect of equivalent radius of gyration on hot rolled angles
sections is studied. Variation of radius of gyration about minor axis,
equivalent radius of gyration with respect to length is compared in
Figure 5.3(a) and 5.3(b).
Based on the studies on the behaviour of radius of gyration versus
effective length behaviour shown in Figure 5.3, a non dimensional curve is
developed to determine the relation between width to thickness ratio and the
slenderness ratio upto which the equivalent radius of gyration is critical as
shown in Figure 5.4. The equivalent radius of gyration (rtf) is not critical for
the angle sections with width to thickness ratio upto 15. For sections with
width to thickness ratio in between 15 to17 the equivalent radius of gyration
is critical upto a slenderness ratio below 45 as shown in Figure 5.4.
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10
14
18
22
26
30
34
38
42
46
50
0 250 500 750 1000 1250 1500 1750 2000 2250 2500 2750 3000
LENGTH IN mm
RA
DIU
S O
F G
YR
AT
ION
IN
mm
rvvrtf
100x100x6 :b/t =16.67
ISA 200x200x12 rtf
150x150x10 rtf
ISA 130x130x8 rtf
ISA 100x100x6 & 100x100x7
rvv
ISA 100*100*6 rtf130x130x8 : b/t =16.25
150x150x10 rvv : b/t =15
200x200x12 rvv : b/t =16.67
b/t >14.25
100*100*7 rtf
100x100x7 :b/t =14.28
(a)
0
5
10
15
20
25
30
35
40
45
50
0 250 500 750 1000 1250 1500 1750 2000 2250 2500 2750 3000
LENGTH IN mm
RA
DIU
S O
F G
YR
AT
ION
IN
mm
150*150*12 b/t <14
80*80*6 rtf
80*80*6 rvv
150*150*12 rtf
150*150*12 rvv
80*80*6 b/t <14
b/t <14
rtf rvv
(b)
Figure 5.3 Radius of gyration vs. Effective length behaviour
123
0
10
20
30
40
50
60
70
80
12 12.5 13 13.5 14 14.5 15 15.5 16 16.5 17 17.5 18 18.5 19 19.5 20
WIDTH TO THICKNESS RATIO
SL
EN
DE
RN
ES
S R
AT
IO G
OV
ER
NE
D B
Y E
QU
IVA
LE
NT
RA
DIU
S O
F
GY
RA
TIO
N (
rtf)
Figure 5.4 Slenderness ratio (governed by equivalent radius of
gyration) vs. Effective width behaviour
Generally in transmission line towers the slenderness ratio of leg
members varies from 40 to 60 and in this range the compression capacity of
the angle section is equal to the tension capacity. Mostly the leg members are
concentrically loaded and with insignificant bending. Hence leg members are
not subjected to torsional flexural buckling. The bracing members are
eccentrically loaded and subjected to bending along with axial forces may be
subjected to torsional flexural buckling. But the slenderness ratio of the
bracing members is generally greater than 60 and hence the equivalent radius
of gyration is not critical for their design.
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5.4 LIMITATING WIDTH TO THICKNESS RATIO
5.4.1 IS -802: (Part 1 /Sec 2):1992
For effective width calculations, the distance between the edges of
fillet to free end is considered in the Indian standards. The limiting width to
thickness ratio is given by
ylim
F)210(t
b=
(5.6)
where, yF is minimum guaranteed yield stress of the material in MPa. The
maximum permissible width to thickness ratio (b/t) for any type of steel shall
not exceed 25.
5.4.2 ASCE 10-97:2000
For effective width calculations, the distance between the edges of
fillet to free end is considered in the American Standards. The limiting width
to thickness ratio is given by
ylim
F)80(t
bΨ=
(5.7)
where, Ψ = 2.62 for yF in MPa.
For sections supported on only one longitudinal edge the flat width
to thickness ratio shall not exceed 25.
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5.4.3 British Standard (BS 8100-3:1999)
The effective width of angle is considered as the distance between
toe to toe of angles in British Standard. The limiting effective width to
thickness ratio is given by
σ=
ylim
E567.0
t
b (5.8)
where yσ is specified minimum yield stress of the material in MPa.
5.5 DESIGN OF COMPRESSION MEMBERS
Compression members are broadly classified as concentrically
loaded members subjected to flexural buckling and columns subjected to
torsional or torsional-flexural buckling. The allowable stress equations
recommended by various standards are discussed in the following sections:
5.5.1 ASCE 10-97:2000
Members with singly symmetric open cross-section shall be
checked for flexural buckling in the plane of symmetry and for torsional-
flexural buckling. The design torsional-flexural buckling stress is calculated
with the radius of gyration ry replaced by rtf computed on the gross cross
section.
The design compressive stress Fa on the gross cross-sectional area
of axially loaded compression member shall be:
y
2
ca F
C
rKL
2
11F
−= cC
r
KL≤ (5.9)
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2
2
a
r
KL
EF
π= cC
r
KL> (5.10)
y
cF
E2C π= (5.11)
where Fy - Minimum guaranteed yield stress;
E - Modulus of Elasticity;
L - Unbraced length;
r - Radius of gyration; and
K - Effective length coefficient.
If the width to thickness ratio (w/t) exceeds (w/t)lim given by
Ψ=
ylim F
80
t
w
( ) y
limcr F
tw
tw677.0677.1F
−= (5.12)
ylim F
144
t
w
t
w Ψ≤
≤
( )2
2
crtw
E0332.0F
π=
yF
144
t
w Ψ> (5.13)
where Ψ = 2.62 for Fy in MPa
The ratio (w/t) of flat width to thickness shall not exceed 25 for
elements supported on only one longitudinal edge.
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The common design practice is to design the redundant members
for 1 to 2.5% of the load in the supported member.
5.5.2 IS: 802 (Part 1 /Sec 2):1992
The allowable unit stress aF , in MPa on the gross cross sectional
area of the axially loaded compression members shall be:
2
a y
C
1 KL rF 1 F
2 C
= −
(5.14)
when C
KL r C≤
and ( )
2
a 2
EF
KL r
π= (5.15)
when CKL r C>
where C yC 2E F= π (5.16)
Fy = minimum guaranteed yield stress of the material, MPa.
E = modulus of elasticity of steel (2×105 MPa)
rKL = largest effective slenderness ratio of any unbraced
segment of the member,
L = unbraced length of the compression member in cm, and
r = appropriate radius of gyration in cm.
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The formulae given above is applicable provided the largest width
thickness ratio b/t is not more than the limiting value given by
( ) ymin F/210tb = (5.17)
where b = distance from edge of fillet to the extreme fibre in mm,
and t = thickness of flange in mm.
where the width to thickness ratio exceeds the limits.
Then formulae given below shall be used substituting for Fy
the value crF given by
( )
( )cr y
lim
0.677 b tF 1.677 F
b t
= −
(5.18)
when lim y(b t) 378 F≤
and ( )tb
65550Fcr = when yF378tb ≥ (5.19)
The redundant members shall be checked individually for
2.5 percent of axial load carried by the member to which it is providing
support. For the design of the compression member six curves are given based
on the type of end fixity and eccentricity similar to the American Standard.
5.5.3 BS 8100-3 :1999
The design buckling resistance, N, of a compression member
should be taken as:
r mN jxA /= σ γ (5.20)
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where j - 0.8 for single angle members connected by one bolt at each
end, 0.9 for single angle members connected by one bolt at
one end and continuous at the other end and 1.0 in all other
cases;
A - the cross-sectional area of the member;
χ - the reduction factor for the relevant buckling mode, given
in reduction factor.
rσ - reference stress given in calculation of reference stress.
mγ - the partial factor on strength, as given in BS 8100-1 and -4,
appropriate to the quality class of the structure, subject to
the following:
• For untested structures
mγ is 1.1 for Class A structures;
mγ is 1.2 for Class B structures;
mγ varies from about 1.3 to 1.45 for Class C structures
depending on the performance requirements.
• For angle section towers which have successfully been
subjected to full scale tests under the equivalent factored
loading or where similar configurations have been type tested:
mγ is 1.0 for Class A structures;
mγ is 1.1 for Class B structures;
mγ varies from about 1.2 to 1.35 for Class C structures
depending on the performance requirements.
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For hot rolled steel members with the types of cross-section
commonly used for compression members, the relevant buckling mode is
general “flexural” buckling. In some cases the “torsional” or “flexural-
torsional” modes may govern.
Reduction factor χ
For constant axial compression in members of constant cross-
section, the value of χ for the appropriate effective slenderness effA should
be determined from:
0.5
2 2
eff
1x
A=
φ + φ −
(5.21)
where ϕ = ( )[ ] 5.02effeff A2.0A15.0 +−α+
α is an imperfection factor;
Λeff = KΛ (5.22)
Λ= λ/λ1 (5.23)
λ1 = slenderness ratio
[ ] 5.0/2758.85 rσλ = (5.24)
rσ = reference stress
and where χ ≤ 1.
The imperfection factor corresponding to the appropriate
buckling curve is given. Values of the reduction factor χ for the appropriate
effective slenderness Λeff are also given.
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The reference stress ‘ rσ ’ required to derive the ultimate stress of a
member depends on the slenderness of the section. Most hot rolled sections
are at least semi-compact. Values of µ and the limiting t/B and t/D ratios
are given below, together with formulae for the reference stress rσ which is
used in place of the yield stress yσ for the design of slender sections.
For hot rolled angle sections
yr σ=σ if µ≤tB / (5.25)
)/2( tByr µσσ −= if
µµ 33.1/ << tB
(5.26)
22 )/1.5/( tBEr
πσ = if µ≥tB /
(5.27)
where yσ is the specified minimum yield stress of material,
‘B’ is the leg length of the angle. For unequal angles and compound
angles, ‘B’ is the longer length, except for single angles connected
by bolts or welding through one leg only at both ends of the
element under consideration for which ‘B’ should be taken as the
length of the connected leg;
‘t’ is the thickness of angle leg;
y0.567 E µ = σ (5.28)
‘E’ is the modulus of elasticity.
Effective slenderness factor ‘K’ for leg members is specified as 0.9
in the British Standard. For bracing members the effective slenderness factor
‘K’ varies based on end condition whether continuous or discontinuous and
the same for single bolted and double bolted connections.
132
5.5.3.1 Compound Members
For compound members built up with two angles as cruciform
section and intermittently connected and used as leg members, the possible
additional deformations due to shear should be taken into account by
modifying the slenderness ratio, ‘λ ’ in accordance with the following:
2 2 2
0 1λ = λ + λ (5.29)
where 0λ - is the slenderness ratio of the full member;
1λ - is the slenderness ratio of one component angle ( )vvrC
It is good practice to have 10 λ≥λ and 501 ≤λ
Compound members consisting of a pair of identical angles back
to back as ‘T’ section separated by a small distance and connected at intervals
by spacers and stitch bolts, may be used for bracing. They should be checked
for buckling about both rectangular axes.
• For buckling about the xx axis the two angles should be
assumed to act compositely for the purpose of calculating
stiffness and radius of gyration.
• For buckling about the yy axis the additional deformation due
to shear should be taken into account by modifying the
slenderness ratio, λ in accordance with the following:
21
20
2 λ+λ=λ taking a maximum value of 01 75.0 λ=λ
where 0λ is the slenderness ratio of the full compound member;
1λ is the slenderness ratio of one component angle ( )vvrC
C is the length of individual angle between stitch bolts
133
In order to keep the effect of this interaction to a minimum, the
spacing between stitch bolts should be limited to give a maximum value 1λ of
90. When only stitch bolts and packs are used, composite section properties
should be based on either;
• The actual space between the individual angle members, or
• A space taken as 1.5 times the thickness of one of the angle
members, whichever is smaller. If batten plates are used,
composite section properties may always be used based on the
actual space between the individual angle members.
5.6 REVIEW ON THE CODAL PROVISIONS
Design provisions given in Indian, American and British standards,
on width to thickness ratio, effective slenderness ratio and permissible
compressive stresses are compared. The Indian Standard IS:802 - Use of
Structural Steel in overhead Transmission line towers – Part 1 gives six
buckling curves for computing the buckling stress of hot rolled angles similar
to ASCE 10-97 standard based on slenderness ratio and end conditions. The
permissible stress curves are based on Euler formula in the elastic range and
Structural Stability Research Council (SSRC) formula in the inelastic range
for concentrically loaded columns. Test experience on tower members is
limited in the slenderness range of 0 to 50, but indications are that the SSRC
formula applies equally well in this range if concentric framing details are
used. The ASCE standard is suitable for steels with yield points up to 448MPa
and for width to thickness values of 25. The recommendations are intended
for both hot-rolled and cold formed members. The influence of end fixity is
assumed to have negligible effect. Using the curves, the strength of angle strut
is checked for buckling. Local buckling is accounted for by considering the
width to thickness ratio of angle sections and appropriately reducing the yield
134
stress if the ratio exceeds the prescribed limit. The strengths given in BS
8100-3:1999 are based on 95% probability values. The design strengths are
obtained by dividing the characteristic strengths by the appropriate partial
factor. The recommendations given in BS standard is valid for tubular or solid
round sections, angle sections either hot rolled or cold formed.
• The Indian and American Standards suggest six different
formulae for the design of the compression member based on
the type of loading and end restraint.
• The Indian and American Standards consider the width after
deducting the thickness and root radius of the fillet in the
angle section in effective width to thickness ratio calculations.
• The Indian Standard specifically mentions that the redundant
member shall be designed for 2.5% of the axial force in the
main member. This is a useful assumption. Tower failures
have indicated that the leg members and main bracing
members have failed due to insufficient strength of redundant
members.
• The British Standard considers an effective length factor of
0.9 for the leg members. The effective length factor for
bracing members varies depending upon the continuous or
discontinuous ends and is the same for both single bolted and
double bolted members.
• The British Standard considers the effect of shear deformation
in the compound members made from two angles in the form
of ‘T’ and star sections by modifying the slenderness ratio.
• The British Standard specifies a separate procedure for
calculating the forces in the secondary members.
135
5.7 COMPARISON OF LEG AND BRACING MEMBER
CAPACITIES
The results predicted from the experimental and analytical studies
conducted on transmission line towers are compared with the codal
predictions and given in Tables 5.1 and 5.2. The 400 kV (0-20) tangent double
circuit tower and 275 kV ‘H’ type large angle deviation tower that have failed
below 75% of their respective design loads are compared separately in
Table 5.3.
Figures 5.5 and 5.6 show the comparison of failure loads for leg
and bracing members calculated based on different standards, Finite Element
analysis and also based on experiments. It shows that the member capacity
predicted by American standard is always higher than the experimental values
for all the slenderness ratios of the members. Nonlinear FE analysis results
are 10 to 12% more than the test results.
In Figures 5.7 and 5.8 there is a wide discrepancy between code
prediction and experimental values since the premature failures in some of the
towers studied are mainly due to non triangulated hip bracing pattern and
inadequate member sizes and non compliance of codes and over estimation of
member forces.
13
6
Table 5.1 Bracing members
Tower
type
Member details Failure load in
percentage
Non Linear analysis
force in kN Member capacity
Remarks
Size L/r Fy Test
FE
Nonlinear
analysis
At test
failure
Load
At FE
failure
Load
ASCE 10-97/
IS:802
in kN
BS
in kN
(1) 220kV
D/C ‘DE' 90O
Dev
ISA
90×90×8 89 290
100 103
186 189 240 193 X- brace
top Half
ISA
90×90×8 96 290 191 196 228 183
Bottom
half
(2) 400kV D/C
‘DB'
ISA
100×100×8 133 255 95 102 148 160 185 146
K- brace
In second panel
(3)
400kV
D/C ‘DD'
ISA
130×130×10 79 350 93 106 399 450 493 426
K- brace
below
middle
Cross arm
(4)
400kV
S/C
ISA
130×130×10 89 350
99 106
404 429 454 397 X- brace
Top half
ISA
120×120×10 60 350 425 449 521 447
X- brace
Bot half
13
7
Table 5.1 (Continued)
Tower
type
Member details Failure load in
percentage
Non Linear analysis
force in kN Member capacity
Remarks
Size L/r Fy Test
FE
Nonlinear
analysis
At test
failure
Load
At FE
failure
Load
ASCE 10-97/
IS:802
in kN
BS
in kN
(5)
400kV
D/C ‘DC'
┘└
80×80×6 105 350 100 106 267 284 291 253
K brace in
second
panel
(8)
400kV
D/C ‘DE'
ISA
110×110×8 100 350 90 104 205 237 276 247
Brace in
portal
(10)
400kV D/C
(0-2o)
with ‘V’
insulator strings
ISA
70×70×5 200 255
100 105
36 37 45 39 Bracing in
2nd panel
ISA
75×75×6 163 255 65 69 79 66
Bracing in 4th panel
ISA
80×80×6 114 255 91 94 126 96
Bracing in
5th panel
(13)
220kV M/C
ISA
100×100×8 193 255
100 107
98 103 112 95 X brace in
3rd panel
ISA
100×100×8 177 255 117 124 126 107
X brace in
4th panel
13
8
Table 5.2 Leg members
Tower
type
Member details Failure load in
percentage
Non Linear analysis
force in kN Member capacity
Remarks
Size L/r Fy Test
FE
Nonlinear
analysis
At test
failure
Load
At FE
failure
Load
ASCE 10-
97/ IS:802
in kN
BS
in kN
(4)
400kV
S/C
ISA
200×200×20 45 350 99 106 1953 2056 2428 2497 Leg
(5)
400kV
D/C ‘DC'
ISA
200×200×20 50 350 100 106 1962 2091 2378 2465
Leg in second
panel from
ground
(6) 220kV
D/C ‘D9DT'
Cruciform with
two ISA
200×200×18
23 350 90 105 3466 4027 4659 4401
Leg in second
panel from ground
(7) 800kV
S/C
ISA
150×150×20 63 255 100 109 1138 1221 1249 1305
Girder Top
chord member
(10)
400kV D/C
(0-2o) with
‘V’ insulator
strings
ISA
130×130×10 50 450
100 105
872 927 896 950 Leg in third
Panel
ISA
130×130×10 60 450 798 848 826 904
Leg in fourth
panel
13
9
Table 5.2 (Continued)
Tower
type
Member details Failure load in
percentage
Non Linear analysis
force in kN Member capacity
Remarks
Size L/r Fy Test
FE
Nonlinear
analysis
At test
failure
Load
At FE
failure
Load
ASCE 10-
97/ IS:802
in kN
BS
in kN
(12)
275kV D/C
Medium dev.
ISA
150×150×18 52 410
100 101
1464 1481 1795 1883 Leg in first
panel
ISA
150×150×18 52 410 1399 1410 1795 1883
Leg in second
panel
ISA
150×150×18 62 410 1334 1361 1663 1786
Leg in third
panel
(13)
220kV M/C
(0-15O)
Cruciform with
two ISA
150×150×12
26 255 100 107 1502 1592 1726 1628
Leg in fourth
panel from ground
14
0
Table 5.3 LEG and bracing members (Failed due to instability)
Tower
type
Member details Failure load in
percentage
Non Linear analysis
force in kN Member capacity
Remarks
Size L/r Fy Test
FE
Nonlinear
analysis
At test
failure
Load
At FE
failure
Load
ASCE 10-
97/ IS:802
in kN
BS
in kN
(9)
400kV D/C (0-2o)
ISA
150×150×12 61 255
75 97
520 669 774 807 Leg in first
panel
ISA
150×150×12 58 255 505 648 785 813
Leg in second
panel
ISA
80×80×6 182 255 35 44 65 62
Bracing in
first panel
(11)
275kV D/C
‘H’ type
Large
deviation
ISA
150×150×18 36 410
62.3 94.4
1011 1504 1943 1980 Leg in first
panel
ISA
150×150×18 43 410 970 1450 1882 1939
Leg in second
panel
ISA
120×120×8 150 275 62 94 192 170
Bracing in first
panel
ISA
90×90×6 128 275 50 77 133 108
Bracing in
second panel
141
LEG MEMBERS
0
300
600
900
1200
1500
1800
2100
2400
2700
3000
3300
3600
3900
4200
4500
4800
5100
CA
PA
CIT
Y (
kN
)FEM
TEST
ASCE and IS
BS
T TOWER NUMBER
T4 T13T12T12T12T10T10T7T6T5
Figure 5.5 Comparison of capacity of leg members
BRACING MEMBERS
0
50
100
150
200
250
300
350
400
450
500
550
CA
PA
CIT
Y (
kN
)
FEM
TEST
ASCE and IS
BS
T TOWER NUMBER
T1 T10T8T5T4T4T3T2 T10 T10 T13T13
Figure 5.6 Comparison of capacity of bracing members
142
LEG MEMBERS
0
200
400
600
800
1000
1200
1400
1600
1800
2000
2200
CA
PA
CIT
Y (
kN
)
FEM
TEST
ASCE and IS
BS
T TOWER NUMBER
T9 T11T11T9
Figure 5.7 Comparison of capacity of leg members
BRACING MEMBERS
0
20
40
60
80
100
120
140
160
180
200
220
CA
PA
CIT
Y (
kN
)
FEM
TEST
ASCE and IS
BS
T 9
T TOWER NUMBER
T 11 T 11
Figure 5.8 Comparison of capacity of bracing members