Thin-Walled Structures 42 (2004) 1329–1355 www.elsevier.com/locate/tws Concrete-filled double skin (SHS outer and CHS inner) steel tubular beam-columns Lin-Hai Han a,, Zhong Tao a , Hong Huang a , Xiao-Ling Zhao b a College of Civil Engineering and Architecture, Fuzhou University, Gongye Road 523, Fuzhou, Fujian Province 350002, People’s Republic of China b Department of Civil Engineering, Monash University, Clayton, Vic. 3168, Australia Received 26 June 2003; received in revised form 13 February 2004; accepted 13 February 2004 Abstract A series of tests on concrete-filled double skin steel tubular (CFDST) stub columns (14), beams (four) and beam-columns (12) were carried out. The specimens had square hollow section (SHS) as outer skin and circular hollow section (CHS) as inner skin. A mechanics model is developed in this paper for the CFDST stub columns, columns and beam-columns. A unified theory is described where a confinement factor (n) is introduced to describe the composite action between the steel tubes and the sandwiched concrete. The load versus axial strain relationship for CFDST stub columns is predicted. Simplified model is derived for sec- tion capacities of CFDST. The predicted beam-column strength is compared with that obtained in beam and beam-column tests. The load versus mid-span deflection relationship for CFDST beams and beam-columns is predicted. A simplified model is developed for cal- culating the member capacity of the CFDST beams. Simplified interaction curves are derived for CFDST beam-columns. # 2004 Elsevier Ltd. All rights reserved. Keywords: Concrete-filled; Beams; Columns; Beam-columns; Design; Hollow sections; Double-skin; Mechanics model 1. Introduction 1.1. Background ‘‘Double skin’’ composite construction was originally used in submerged tube tunnels for pressure vessels [1–5], which consisted of an inner and outer steel skin Corresponding author. Tel.: +86-591-789-2459; fax: +86-591-373-7442. E-mail address: [email protected] (L.-H. Han). 0263-8231/$ - see front matter # 2004 Elsevier Ltd. All rights reserved. doi:10.1016/j.tws.2004.03.017
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Lin-Hai Han a,�, Zhong Tao a, Hong Huang a, Xiao-Ling Zhao b
a College of Civil Engineering and Architecture, Fuzhou University, Gongye Road 523, Fuzhou,
Fujian Province 350002, People’s Republic of Chinab Department of Civil Engineering, Monash University, Clayton, Vic. 3168, Australia
Received 26 June 2003; received in revised form 13 February 2004; accepted 13 February 2004
Abstract
A series of tests on concrete-filled double skin steel tubular (CFDST) stub columns (14),beams (four) and beam-columns (12) were carried out. The specimens had square hollowsection (SHS) as outer skin and circular hollow section (CHS) as inner skin. A mechanicsmodel is developed in this paper for the CFDST stub columns, columns and beam-columns.A unified theory is described where a confinement factor (n) is introduced to describe thecomposite action between the steel tubes and the sandwiched concrete. The load versus axialstrain relationship for CFDST stub columns is predicted. Simplified model is derived for sec-tion capacities of CFDST. The predicted beam-column strength is compared with thatobtained in beam and beam-column tests. The load versus mid-span deflection relationshipfor CFDST beams and beam-columns is predicted. A simplified model is developed for cal-culating the member capacity of the CFDST beams. Simplified interaction curves are derivedfor CFDST beam-columns.# 2004 Elsevier Ltd. All rights reserved.
‘‘Double skin’’ composite construction was originally used in submerged tube
tunnels for pressure vessels [1–5], which consisted of an inner and outer steel skin
Nomenclature
Ac concrete cross-sectional areaAc,nominal nominal cross-sectional area of concrete, given by B2 � Aso
Asc cross-sectional area of the composite section, given by Aso þ Ac þ Asi
Asco cross-sectional area of the outer steel tube and the sandwichedconcrete, given by Aso þ Ac
Asi cross-sectional area of the inner steel tubeAso cross-sectional area of the outer steel tubeB outer width of square tubeCFDST concrete-filled double skin steel tubeCFST concrete-filled steel tubeD outer diameter of the inner circular tubee load eccentricitye=r load eccentricity ratios, r can be given by B=2Ec concrete modulus of elasticityEs steel modulus of elasticityfsyo yield strength of the outer steel tubefsyi yield strength of the inner steel tubefcu characteristic 28-day concrete cube strengthfck characteristic concrete strength (fck ¼ 0:67fcu for normal strength
pIsc moment of inertia for CFDST cross-sectionL effective buckling length of column in the plane of bendingMu ultimate strength of CFDST beamsMuc,mm predicted moment capacity using mechanics modelMuc,sm predicted moment capacity using simplified modelMue maximum test momentMi,u moment capacity of the inner tubeMosu,u moment capacity of the outer steel tube filled with concreteNu ultimate strength of the composite columnsNuc,mm predicted ultimate strength using mechanics modelNuc,sm predicted ultimate strength using simplified modelNi,u compressive capacity of the inner tubeNosu,u compressive capacity of the outer steel tube filled with concreteNue experimental ultimate strengthtso wall thickness of the outer steel tubetsi wall thickness of the inner steel tubeWscm section modulus of the outer steel tube and the sandwiched concrete,
given by B3=6� pD4=ð32BÞWsi plastic section modulus of the inner tubev hollow ratio, given by D=B
L.-H. Han et al. / Thin-Walled Structures 42 (2004) 1329–13551330
r stresse strain/ curvaturek slenderness ratios, given by L=in confinement factor (¼ ðAso � fsyoÞ=ðAc;nominal � fckÞ)
1331L.-H. Han et al. / Thin-Walled Structures 42 (2004) 1329–1355
with the annulus between the skins filled with concrete. This type of sandwich
cross-section was shown to have high bending stiffness that avoids instability under
external pressure.In recent years, a similar concept called concrete-filled double skin tubes
(CFDST) was developed, and reported by Wei et al. [6,7], Nakanishi et al. [8],
Yagishita et al. [9], Lin and Tsai [10], Elchalakani et al. [11], Zhao and Grzebieta
[12], and Zhao et al. [13–15]. Similar to fully concrete-filled steel tubes (CFST),
advantages of CFDST include: increased section modulus; enhanced global stab-
ility; lighter weight; utilization of the space in the inner tube if necessary, good
damping characteristics and good cyclic performance. CFDST columns may have
reasonable fire resistance period because that the inner tubes are protected by the
sandwiched concrete under a fire. Recently, CFDST have been used as high-rise
bridge piers in Japan [9] to reduce the structure self-weight, while maintaining a
large energy absorption capacity against earthquake loading. There may be a
potential for CFDST to be used in building structures, as observed for concrete-
filled steel tubes (CFST) in the past few decades [16]. Therefore, there is a need
to study the behavior of CFDST stub columns, columns and beam-columns.The research conducted so far on CFDST is summarized in Table 1 where refer-
ences are listed. It can be seen that there are four combinations of square hollow
section (SHS) and circular hollow section (CHS) as outer and inner tubes. This
paper focuses on CFDST with SHS as outer skin and CHS as inner skin. Only
Table 1
Summary of research Conducted on CFDST
Combinations M
ember types
Stub columns
Beams C olumns B eam-columns
CHS outer and CHS
inner
W
L
ei et al. [6,7],
in and Tsai [10]
Lin and Tsai [10] –
Y agishita et al. [9]
SHS outer and SHS
inner
Z
[
hao and Grzebieta
12], Zhao et al. [13,14]
Zhao and
Grzebieta [12]
–
–
CHS outer and SHS
inner
E
lchalakani et al. [11] – – –
SHS outer and CHS
inner
Z
p
hao et al. [13], this
aper
This paper T
his paper T his paper
L.-H. Han et al. / Thin-Walled Structures 42 (2004) 1329–13551332
some stub column tests were reported on this combination in the past [15] wherecold-formed SHS and CHS were used. The contribution of this paper can be sum-marized as follows:
1. More realistic sizes of SHS and CHS are used. The tube sizes used in the currentstudy are up to about three times that used by Zhao et al. [15].
2. The ratio of the inner tube diameter (D) to the outer tube width (B) varies from0 to 0.75 compared with that ranging from 0.49 to 0.60 by Zhao et al. [15].
3. Beams, columns and beam-columns are tested in the current study.4. Mechanics models and simplified models are developed for stub columns,
beams, columns and beam-columns.
1.2. This paper
Tests on 14 CFDST stub columns, four CFDST beams and 12 CFDST beam-columns were carried out. The main parameters varied in the testing program are:(1) hollow section ratio (v ¼ D=B) from 0 to 0.75, where D is the inner tube diam-eter and B is the outer tube width; (2) outer tube width to thickness ratio from 40to 100; (3) column slenderness (k), from 29 to 58; and (4) load eccentricity (e), from15 to 80 mm, for beam-columns.Mechanics models were developed to predict the behavior of CFDST stub
columns, beams, columns and beam-columns. The unified theory [17] was adoptedin the derivation, where a confinement factor (n) was introduced to describe thecomposite action between the steel tube and the sandwiched concrete. The loadversus axial strain relationship is established for concrete-filled SHS stub columns.The load versus mid-span deflection relationship is established for CFDST beamsand beam-columns. Simplified models were developed to estimate the strength ofCFDST stub columns, beams, columns and beam-columns. All predictions werecompared with test results with reasonable agreement achieved.
2. Experimental investigations
2.1. Materials and specimen preparation
A series of tests on concrete-filled double skin steel tubular (CFDST) stub col-umns, beams and beam-columns were carried out. The experimental study was notonly to determine the maximum load capacity of the specimens, but also to investi-gate the failure modes up to and beyond the ultimate load.A schematic view of the cross-section is shown in Fig. 1 where the outer skin is a
square box and the inner skin is a CHS. The tubes were all manufactured frommild steel sheet. Four sheet plates were cut, tack welded into a square shape andthen welded with a single bevel butt weld along the corners to form the outer tube.One sheet plate was cut, rolled to a circular shape and then welded with a singlebevel butt weld. A 25 mm thick plate was welded to one end of each specimen.
1333L.-H. Han et al. / Thin-Walled Structures 42 (2004) 1329–1355
Standard tensile coupon tests were conducted to measure material properties ofthe steel sheet. Three coupons were taken from each steel sheet used for manufac-turing specimens. The average yield stress of the outer tube (fsyo), and that of theinner tube (fsyi) for each specimen is listed in Tables 2–4. The modulus of elasticityof the outer and the inner tubes were found to be approximately 200,000 MPa.One type of concrete, with a nominal compressive cube strength (fcu) at 28 days
of 40 MPa, was designed. The mix proportions of the concrete were as follows:
– C
ement: 528 kg/m3
– W
ater: 201 kg/m3
– S
and: 585 kg/m3
– C
oarse aggregate: 1086 kg/m3.
For each batch of concrete mixed, three 150 mm cubes were also cast and curedin conditions similar to the related specimens. The average cube strength at thetime of testing was 46.8 MPa. The modulus of elasticity (Ec) of concrete was foundto be 33,300 MPa.The concrete was filled in the annulus between the outer and inner skins. The
specimens were vibrated by poker vibrator. They were placed upright to air-dryuntil testing. During curing, a very small amount of longitudinal shrinkage of0.6–0.8 mm or so occurred at the top of the columns. A high-strength epoxy wasused to fill this longitudinal gap so that the concrete surface was flush with thesteel tube at the top. Prior to testing, this surface was ground smooth and flat
Fig. 1. Column specimen details and dimensions (schematic view).
Table2
Specim
enlabels,materialproperties
andsectioncapacities
(stubcolumns)
No.
Specim
en
label
Outertube
dim
ension
B�t so(m
m)
Inner
tube
dim
ension
D�t si(m
m)
vL (m
m)
f syo
(MPa)
f syi
(MPa)
Nue
(kN)
Nuc,mm
(kN)
Nuc;mm=N
ue
1scc1-1
&-120�3
–0
360
275.9
–982
882
0.898
2scc1-2
&-120�3
–0
360
275.9
–990
882
0.891
3scc2-1
&-120�3
U32�3
0.27
360
275.9
422.3
1054
967
0.917
4scc2-2
&-120�3
U32�3
0.27
360
275.9
422.3
1060
967
0.912
5scc3-1
&-120�3
U58�3
0.48
360
275.9
374.5
990
976
0.986
6scc3-2
&-120�3
U58�3
0.48
360
275.9
374.5
1000
976
0.976
7scc4-1
&-120�3
U88�3
0.75
360
275.9
370.2
870
947
1.089
8scc4-2
&-120�3
U88�3
0.75
360
275.9
370.2
996
947
0.951
9scc5-1
&-180�3
U88�3
0.49
540
275.9
370.2
1725
1785
1.035
10
scc5-2
&-180�3
U88�3
0.49
540
275.9
370.2
1710
1785
1.044
11
scc6-1
&-240�3
U114�3
0.48
720
275.9
294.5
2580
2756
1.068
12
scc6-2
&-240�3
U114�3
0.48
720
275.9
294.5
2460
2756
1.120
13
scc7-1
&-300�3
U165�3
0.50
900
275.9
320.5
3240
3855
1.190
14
scc7-2
&-300�3
U165�3
0.50
900
275.9
320.5
3430
3855
1.124
15
Empty
tube
&-120�3
––
360
275.9
–376
––
Mean
1.014
COV
0.009
L.-H. Han et al. / Thin-Walled Structures 42 (2004) 1329–13551334
Table3
Specim
enlabels,materialproperties
andsectioncapacities
(beams)
No.
Specim
en
label
Outertube
dim
ension
B�t so(m
m)
Inner
tube
dim
ension
D�t si(m
m)
vL (m
m)
f syo
(MPa)
f syi
(MPa)
Mue
(kN)
Muc,mm
(kN)
Muc;mm=M
ue
1scb1
&-120�3
–0
1400
275.9
–24.37
19.79
0.812
2scb2
&-120�3
U32�3
0.27
1400
275.9
422.3
25.87
22.46
0.868
3scb3
&-120�3
U58�3
0.48
1400
275.9
374.5
26.90
25.87
0.962
4scb4
&-120�3
U88�3
0.73
1400
275.9
370.2
28.98
33.49
1.156
5Empty
tube
&-120�3
––
1400
275.9
–17.44
––
Mean
0.950
COV
0.023
1335L.-H. Han et al. / Thin-Walled Structures 42 (2004) 1329–1355
Table4
Specim
enlabels,materialproperties
andmem
ber
capacities
(columnsandbeam-columns)
No.
Specim
en
label
Outertube
dim
ension
B�t so(m
m)
Inner
tube
dim
ension
D�t si(m
m)
vL (m
m)
kf syo
(MPa)
f syi
(MPa)
e (mm)
Nue
(kN)
Nuc,mm
(kN)
Nuc;mm=N
ue
1scbc1-1
&-120�3
U58�3
0.48
1070
29
275.9
374.5
4856
912.
1.065
2scbc1-2
&-120�3
U58�3
0.48
1070
29
275.9
374.5
4872
912
1.046
3scbc2-1
&-120�3
U58�3
0.48
1070
29
275.9
374.5
14
667
755
1.132
4scbc2-2
&-120�3
U58�3
0.48
1070
29
275.9
374.5
14
750
755
1.007
5scbc3-1
&-120�3
U58�3
0.48
1070
29
275.9
374.5
45
480
483
1.006
6scbc3-2
&-120�3
U58�3
0.48
1070
29
275.9
374.5
45
486
483
0.994
7scbc4-1
&-120�3
U58�3
0.48
2136
58
275.9
374.5
0920
860
0.935
8scbc4-2
&-120�3
U58�3
0.48
2136
58
275.9
374.5
0868
860
0.991
9scbc5-1
&-120�3
U58�3
0.48
2136
58
275.9
374.5
15.5
596
602
1.010
10
scbc5-2
&-120�3
U58�3
0.48
2136
58
275.9
374.5
15.5
570
602
1.056
11
scbc6-1
&-120�3
U58�3
0.48
2136
58
275.9
374.5
45
380
389
1.024
12
scbc6-2
&-120�3
U58�3
0.48
2136
58
275.9
374.5
45
379
389
1.026
Mean
1.024
COV
0.002
L.-H. Han et al. / Thin-Walled Structures 42 (2004) 1329–13551336
1337L.-H. Han et al. / Thin-Walled Structures 42 (2004) 1329–1355
using a grinding wheel with diamond cutters. This was to ensure that the load
was applied evenly across the cross-section and simultaneously to the steel and
concrete.
2.2. Stub column tests
A total of 12 stub columns were tested. A summary of the specimens is presented
in Table 2, where the section sizes, material properties and hollow ratio (v) are
given. The length of stub columns (L) was chosen to be three times the width of
outer SHS sections to avoid the effects of overall buckling and end conditions [17].All the tests were performed on a 5000 kN capacity testing machine. The speci-
mens were sitting on the machine base plate. The load was applied through a load-
ing ram. Eight strain gauges were mounted on each specimen to measure strains at
the middle height, two on each flat face of the outer tube. Four strain gauges were
placed along the direction of loading while the other four were placed perpendicu-
lar to the loading direction. Two displacement transducers were used to measure
the axial deformation. A load interval of less than one-tenth of the estimated load
capacity was used. Each load interval level was maintained for about 2 min.Typical failure mode of the outer tube was local (outward folding) failure mech-
anism. This is the same as that observed by Zhao et al. [15] for CFDST with SHS
outer and CHS inner. This failure mode is also similar to that observed for con-
crete-filled steel tubes (CFST) by many other researchers, such as Ge and Usami
[18], Han et al. [17], O’Shea and Bridge [19], and Song and Kwon [20], just to list a
few. The typical failure mode is shown in Fig. 2(a). The failure mode of the inner
CHS behaves differently from that for empty CHS in compression where an
‘‘elephant foot’’ occurs. The failure mode shown in Fig. 2(b) is very much the same
as that observed for the inner CHS tube of CFDST [13,14]. One test on empty
outer tube was also carried out for comparison purpose. The details are listed in
Table 2.Load versus axial strain curves are shown in Fig. 3. The maximum loads (Nue)
obtained in the test are summarized in Table 2. It can be found from Fig. 3(d) that
the ultimate strength and the ductility of CFDST stub columns are much larger
than those of the empty stub columns.
2.3. Beam tests
Four CFDST beam specimens with different hollow ratio (v) were tested in the
same machine that was used for the stub column tests. The specimens were labeled
as shown in Table 3.A four-point bending rig was used to apply the moment similar to that described
by Zhao and Grzebieta [12]. The mid-span deflection was measured using a dis-
placement transducer. The strains in the outer tube were measured at mid-span of
the beam by strain gauges on both top and bottom surfaces.Failure modes of the current tested beams were very similar to those described
by Zhao and Grzebieta [12] for CFDST (SHS outer and SHS inner) beams. No
L.-H. Han et al. / Thin-Walled Structures 42 (2004) 1329–13551338
tensile fracture was observed on the tension flange. The failure modes of inner con-
crete and inner tubes are shown in Fig. 4(a) and (b), respectively.One empty beam with the same tube dimension as the outer tube was also car-
ried out for comparison purposes. The details of the specimen were listed in
Table 3.The bending moment is plotted in Fig. 5 against the compressive and tensile
strains of the extreme fiber at mid-span. The bending moment versus mid-span
deflection curves are given in Fig. 6. The maximum experimental moment (Mue) is
listed in Table 3. It can be found from Table 3 and Fig. 6(a) that both the ultimate
strength and the ductility of CFDST beams are much larger than those of the
empty tube beam.
2.4. Beam-column tests
Fourteen tests on composite columns and beam-columns were carried out. A
summary of the specimens is presented in Table 4 where the section sizes, slender-
ness ratios (k), load eccentricities (e), and sectional hollow ratio (v) are given. The
load eccentricity (e) ranges are from 0 to 45 mm. The slenderness ratio (k) ranges
Typical failure mode of the of CFDST stub columns. (a) Specimen after testing and (b)
Fig. 2. inner
tube.
1339L.-H. Han et al. / Thin-Walled Structures 42 (2004) 1329–1355
Fig. 3. Load versus axial strain curves.
L.-H. Han et al. / Thin-Walled Structures 42 (2004) 1329–13551340
are from 29 to 58. The value of slenderness ratio (k) is defined as
k ¼ L
i; ð1Þ
where L is the effective length of a column, which is the same as the physical length
of the column (L) with pin-ended supports. i ¼ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiIsc=Asco
p, is the section radius of
gyration, Isc and Asco are the moment of inertia and area of CFDST composite
cross-section, respectively.The desired eccentricity was achieved by accurately machining grooves that are
6 mm deep into the stiff endplate that was welded to the steel tubes. For the con-
centrically loaded column, the groove was in the middle of the plate. The endplate
was considered very stiff with a thickness of 30 mm. The axial load was applied
through a very stiff top platen with an offset triangle hinge, which also allowedspecimen rotation to simulate pin-ended supports. Both the endplate and the top
platen were made of very hard and very high-strength steel. Eight strain gauges
were used for each specimen to measure the longitudinal and transverse strains at
the middle height. Two displacement transducers were used to measure the axial
deformation. Five transducers were used to measure the lateral deflection. Fig. 7
gives a general view of the test arrangement.A load interval of less than one-tenth of the estimated load capacity was used.
Each load interval was maintained for about 2 min. At each load increment, the
Typical failure modes of the of CFDST beams. (a) Sandwiched concrete and (b) inner
Fig. 4. tube.
1341L.-H. Han et al. / Thin-Walled Structures 42 (2004) 1329–1355
Fig. 5. Moment versus extreme fibre strains at mid-span of beam specimens.
Fig. 6. Load versus mid-span deflection of beam specimens (a) scb1; (b) scb2; (c) scb3; (d) scb4.
L.-H. Han et al. / Thin-Walled Structures 42 (2004) 1329–13551342
strain readings and the deflection measurements were recorded. All specimens wereloaded to failure. Each test took approximately 30 min to reach the maximum loadand 1.5 h to complete. All the test specimens behaved in a relatively ductile mannerand testing proceeded in a smooth and controlled way.Typical failure mode was overall buckling failure. When the load was small, the
lateral deflection at middle height is small and approximately proportional to theapplied load. When the load reached about 60–70% of the maximum load, thelateral deflection at middle height started to increase significantly. Specimenno. scbc5-1 is selected to illustrate the lateral deflection in the middle-span of thecomposite beam-column with different axial loads (N), as shown in Fig. 8, wherethe ratio of n is given by N=Nue.The axial load (N) versus extreme fiber strain curves are shown in Fig. 9. The
load (N) versus mid-height deflection (um) curves for the composite columns arepresented in Fig. 10. The maximum loads (Nue) obtained in the test are summar-ized in Table 4.
3. Mechanics models
3.1. Mechanics model for stub columns
Mechanics models were developed by Han et al. [17] for concrete-filled SHSs.Stress versus strain relations were given in Han et al. [17] for steel tubes and con-
Fig. 7. A general view of beam-column test.
1343L.-H. Han et al. / Thin-Walled Structures 42 (2004) 1329–1355
fined concrete. In this paper, the same stress–strain relations were adopted for steeltubes and concrete in the analysis.A typical stress–strain curve for steel consists of five stages as shown in Fig. 11.
Detailed expressions were given in Han et al. [17].It is assumed that the inner tube can restrict the inner indentation of the con-
crete core, so the sandwiched concrete in the annulus was confined in the same wayas that in a fully in-filled steel tube. A typical stress–strain curve for the confinedconcrete with fck ¼ 41 MPa is shown in Fig. 12, where the confinement factor (n) isdefined as
n ¼ Aso � fsyoAc;nominal � fck
; ð2Þ
in which Aso is the cross-section area of the outer steel tube, Ac,nominal is the nom-
inal cross-section area of concrete, given by B2 � Aso, fsyo is the yield stress of theouter steel tube, and fck is the compression strength of concrete. The value of fckfor normal strength concrete is determined using 67% of the compression strengthof cubic blocks. Detailed expressions are given in Han et al. [17].It can be seen from Fig. 12 that the higher the confinement factor (n) is, the
higher the compression strength of confined concrete is. It can also be seen fromFig. 12 that the higher is n, the more ductile is the confined concrete. The confine-ment factor (n), to some extent, represents the ‘‘composite action’’ between steeltubes and concrete.The fabrication of concrete-filled steel SHS columns involves welding which
introduces residual stresses in the specimens. Fig. 13 shows a typical residual stress
lateral deflection along the column at different loa
Fig. 8. Mid-span d level (scbc5-1).
L.-H. Han et al. / Thin-Walled Structures 42 (2004) 1329–13551344
distribution for a steel plate in a column that has been fabricated with four steel
plates and a longitudinal fillet weld [21]. The residual stresses in steel plates for
concrete-filled steel SHS columns were found to be 0:15fsy � 0:25fsy in compression
and about fsy in tension [21]. The average value of 0.2fsy in compression is adopted
in this paper as shown in Fig. 13.The load versus axial strain relations can be established based on the following
assumptions:
Fig. 9. Axial load versus extreme fibre strains at mid-height of test specimens.
1345L.-H. Han et al. / Thin-Walled Structures 42 (2004) 1329–1355
1. There is no slip between the steel and concrete.2. Longitudinal stress–strain models of steel and concrete given in Han et al. [17]
are adopted in the analysis.3. Residual stress distribution for a steel plate of a column shown as in Fig. 13 is
used in the analysis.
Fig. 10. Load (N) versus mid-height lateral deflection (um) curves.
L.-H. Han et al. / Thin-Walled Structures 42 (2004) 1329–13551346
. Typical stress–strain curves for steel (schematic
Fig. 11 view).
Fig. 12. r versus e relations of concrete core.
sidual stress distribution across plate of steel bo
Fig. 13. Re x column.
1347L.-H. Han et al. / Thin-Walled Structures 42 (2004) 1329–1355
4. Force equilibrium and deformation consistencies are considered along the longi-tudinal direction, i.e.
N ¼ Nsi þNc þNso; ð3Þesil ¼ ecl ¼ esol; ð4Þ
in which Nsi, Nc and Nso are longitudinal forces carried by the inner steel tube,the sandwiched concrete, and the outer steel tube, respectively; esil, ecl and esolare longitudinal strains in the inner steel tube, the sandwiched concrete, and theouter steel tube, respectively.
The procedures to calculate load versus axial strain are expressed as follows.For a given (ith) increment in axial strain deli ! ith axial strain e1;iþ1 ¼
eli þ deli ! ith axial stress rsil;iþ1; rcl;iþ1 and rsoil;iþ1 ! ith forces Nsi;i; Nc;i and
Nso;i ! ith force Ni.The predicted curves of load versus axial strain are compared in Fig. 3 with
experimental curves. Good agreement is obtained between the predicted and testedcurves. The predicted section capacities using mechanics model (Nuc,mm) are com-pared in Table 2 with those obtained in the current tests (Nue). A mean ratio(Nuc=Nue) of 1.014 is obtained with a coefficient of variation (COV) of 0.009.
3.2. Mechanics model for the composite beam-columns
A member subjected to compression is shown in Fig. 14, where N is the com-pression force, e is the load eccentricity and um is the mid-span deflection. Whenthe load eccentricity (e) equals zero, the member under compression is called a col-umn. Otherwise, the member is called a beam-column, i.e. it is under combinedbending and compression.The load versus mid-span deflection relations can be established based on the
following assumptions:
1. The stress–strain relationship for steel given in Han et al. [17] is adopted forboth tension and compression. The stress–strain relationship for concrete givenin Han et al. [17] is adopted for compression only. The contribution of concretein tension is neglected.
2. Original plane cross-sections remain plane.3. The effect of shear force on deflection of members is omitted.
Fig. 14. A schematic view of a beam-column.
L.-H. Han et al. / Thin-Walled Structures 42 (2004) 1329–13551348
4. The deflection curve of the member is assumed as a sine wave.5. Residual stress distribution for a steel plate of a column shown as in Fig. 13 is
used in the analysis.
According to the assumption no. 4, the deflection (u) of the member can be
expressed as:
u ¼ um � sin pL� z
� �; ð5Þ
where um is the mid-span deflection, L is the length of the member and z is the
horizontal distance from the left support as defined in Fig. 14.The curvature (/) at the mid-span can be calculated as:
/ ¼ p2
L2� um: ð6Þ
The strain distribution is shown in Fig. 15, where eo is the strain along the
geometrical centre line of the section. The term ei is the strain at the location yi as
defined in Fig. 15. Along the line with y ¼ yi, the section can be divided into three
kinds of elements (dAso,i and dAsi,i for outer and inner steel tubes, respectively, and
dAci for concrete) with unit depth. The strain at the centre of each element can be
expressed as:
ei ¼ eo þ / � yi: ð7Þ
The stress at the centre of each element (rso,i and rsi,i for outer and inner steel
tubes, respectively, or rc,i for concrete) can be determined using the stress–strain
relationship given in Han et al. [17]. The internal moment (Min) and axial force
Fig. 15. Distribution of strains.
1349L.-H. Han et al. / Thin-Walled Structures 42 (2004) 1329–1355
From the above equations, the load versus mid-span deflection relations can beestablished for a certain eccentricity (e). The geometrical imperfection is taken asL=1000 [17].The predicted curves of load versus lateral deflection are compared in Figs. 6
and 11 with those obtained in the current beam and beam-column tests. A reason-able good agreement is achieved between the predicted and tested curves.The predicted ultimate capacities for beams and beam-columns are compared
with the experimental values in Tables 3 and 4, where a mean of 1.072 and 0.95,and COV of 0.023 and 0.020 are obtained for the CFDST beams and beam-col-umns, respectively.Fig. 16 illustrates a typical calculated interaction relationship between compress-
ive strength ratio (N=Nu) and bending strength ratio (M=Mu) of a CFDST beam-column with different column slenderness ratio (k). Nu and Mu are the sectioncapacity in compression and bending moment capacity of CFDST, respectively. Itcan be found that the member capacities of the composite beam-columns decreasewith the increasing of member slenderness ratio (k). A careful examination of thepredicted results also revealed an interesting phenomenon, i.e. the N=Nu �M=Mu
dicted axial load (N=Nu) versus moment (M=Mu) interaction
Fig. 16. Pre curves (tube:
&-600� 600� 14 mm, v ¼ 0:5, fsy ¼ 345 MPa, fck ¼ 26:8 MPa).
L.-H. Han et al. / Thin-Walled Structures 42 (2004) 1329–13551350
relationships of the CFDST beam-columns are very similar to those of the CFST
members [17].
4. Simplified models
4.1. Section capacity
It is assumed that the total capacity (Nu,sm) of CFDST is a sum of the inner tube
capacity (Ni,u) and a capacity (Nosu,u) which contributed by the outer tube togetherwith the concrete, i.e.
Nu;sm ¼ Nosc;u þNi;u; ð12Þ
in which Ni;u ¼ Asi � fsyi and Nosu,u is determined similarly to that of fully concrete-filled steel tubular sections [17] with the relevant concrete section area for CFDST.Nosu,u can be expressed by:
Nosc;u ¼ fscy � Asco; ð13Þ
in which Asco ¼ Aso þ Ac;
fscy¼ 1:212þ 0:138� fsyo235
þ0:7646
� ��nþ �0:0727� fck
20þ0:0216
� ��n2
� �fck; ð14Þ
where the units for fscy and fck are N/mm2.The section capacities predicted using the simplified model are compared in
Fig. 17(a) with those obtained in stub column tests by Zhao et al. [15] and in the
current study. Good agreements are obtained.
4.2. Bending moment capacity
Similar to the approach used for stub columns, the bending moment capacity ofCFDST (Mu,sm) can be expressed as:
Mu;sm ¼ Mosc;u þMi;u ð15Þ
in which Mi;u ¼ Wsi � fsyi is moment capacity of the inner tube, Mosc,u is determinedsimilarly to that of fully concrete-filled steel tubular sections [17] with the relevant
concrete section area for CFDST. Mosu,u is given by:
Mosc;u ¼ cm �Wscm � fscy ð16Þ
in which cm ¼ �0:2428n þ 1:4103ffiffiffin
p; Wscm ¼ ðB3=6Þ � ðp �D4=32BÞ, fscy is given
by Eq. (14).The flexural capacities predicted using the simplified model are compared in
Fig. 17(b) with those obtained in current tests. Results in this figure clearly show
that the predicted values are slightly lower than experimental ones.
1351L.-H. Han et al. / Thin-Walled Structures 42 (2004) 1329–1355
alculated capacity between simplified model and tes
Fig. 17. Comparison of c ts. (a) Stub columns, (b)
beams and (c) beam-columns.
L.-H. Han et al. / Thin-Walled Structures 42 (2004) 1329–13551352
4.3. Interaction curves
The interaction equation suggested by Han et al. [17] for concrete-filled beam-columns are used in this paper to predict the CFDST beam-columns with relevantcapacities for CFDST defined in Eqs. (12) and (15). The interaction curves wererewritten here as
11� 0:25N=NE
¼ 1� g=u1� 2g0o=u
for g � 2g0o; ð17aÞ
11� 0:25N=NE
¼ a � gu
� �2
þb � gu
� �þ 1 for g < 2g0o; ð17bÞ
in which
g ¼ N
Nu;sm; 1 ¼ M
Mu;sm;
Nu,sm, Mu,sm are the sectional capacity and bending moment capacity of CFDSTsection given by Eqs. (12) and (15), respectively;
NE ¼ p2 � Eelasticsc � Asco
k2;
Asco ¼ Aso þ Ac;
Eelasticsc is the section modulus of concrete-filled steel SHS in elastic stage [17]; u is
the stability reduction factor for the composite slender columns [17].
a ¼ ð1� 10oÞ=g0o2;
b ¼ �2g00ð1� f0oÞðu � g0oÞ;
g00 ¼ u3go;
f0o ¼ 1þ u5ðfo � 1Þ;
go ¼ 0:2 � fck20
� �0:65
� 235
fsyo
� �0:38
� 0:1
a
� �0:45
;
fo ¼ 1þ 0:11fck20
� �1:46
� 235
fsyo
� �1:65
� 0:1
a
� �1:4
;
where the units for fsyo and fck are N/mm2.The member capacities predicted using the simplified model are compared with
the experimental results in Fig. 17(c). Fig. 18 shows the axial load (N) versusmoment (M) interaction curves for the current specimens with dimensions of theouter and the inner tubes are &-120� 3 and U58� 3, respectively. It can be foundfrom the above comparisons that the accuracy with which the formula predictedthe experimental strength is reasonable, and in general, the predictions are some-what conservative.
1353L.-H. Han et al. / Thin-Walled Structures 42 (2004) 1329–1355
5. Conclusions
A series of tests, including 14 stub columns, four beams and 12 beam-columnson CFDST (SHS outer and CHS inner) sections have been performed. Mechanicsmodels have been established for CFDST stub columns, beams and beam-columns.A confinement factor has been used to describe the ‘‘composite action’’ betweensteel tubes and the sandwiched concrete. The following observations and conclu-sions can be drawn based on the limited research reported in the paper:
1. Enhanced strength and ductility have been observed for CFDST (CHS innerand SHS outer) stub columns, beams and bean-columns due to the ‘‘compositeaction’’ between the steel tubes and the sandwiched concrete.
2. Mechanics models have been developed to predict the behavior of CFDST stubcolumns, beams, columns and beam-columns.
ersus moment (M) interaction curves for the tested spec
Fig. 18. Axial load (N) v imens. (a) scb3, scbc1-1,
L.-H. Han et al. / Thin-Walled Structures 42 (2004) 1329–13551354
3. The load versus axial strain relationship has been established for concrete-filledSHS stub columns. The load versus mid-span deflection relationship has beenestablished for CFDST beams and beam-columns. Simplified models have beendeveloped to estimate the strength of CFDST stub columns, beams, columnsand beam-columns. All predictions were compared with test results with reason-able agreement achieved.
Acknowledgements
The research work reported herein was made possible by the Fujian ProvinceScience and Technology Project, the financial support is highly appreciated. Theauthors also express special thanks to Mr. Zheng Yong-Qian, Mr. Liu Cheng-Chao,Miss Zheng Huai-Ying, and Mr. Zhuo Qiu-Lin for their assistance in the experi-ments.
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