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PHYSICAL TESTS AND ANALYSES OF COMPOSITE STEEL-CONCRETE BEAM-COLUMNS By S. Ali Mirza,! Fellow, ASCE, Ville Hyttinen,:Z and Esko Hyttinen 3 ABSTRACT: The composite steel-concrete beam-columns in which steel shapes are encased in concrete and second-order effects are significant were studied from 16 specimens loaded to failure. Loading included com- binations of axial and transverse forces producing a wide range of different external eccentricities. Observations from the physical tests indicate that, for static loads, the bonding condition at the interface of steel rib connectors and the surrounding concrete has a small effect on ultimate strength. The tests also show that the ACI 318 assumption of maximum usable strain of 0.003 at concrete extreme compression fibers near ultimate load is valid for such beam-columns. Analyses based on ACI 318, Eurocode 4, and finite-element modeling procedures were compared to test results that provided further insight into understanding the structural behavior of such beam-columns. umn tests. Steel rib connectors with three different bonding conditions were used for the beam-column specimens reported on in this study (Fig. 2). The objective of the study was four- fold: (1) to investigate the behavior and ultimate strength of composite steel-concrete beam-columns in which steel shapes L = 4000 9 .J,.V u Itllt tllllll til" 1500 I 1000 I 1500 a "I a <a) INTRODUCTION During the past few decades, several composite steel-con- crete structural systems have been used in the construction of tall buildings. One such system employs composite columns that consist of steel shapes encased in concrete and composite girders that use metal deck between the steel section and con- crete slab. This system combines the rigidity and formability of reinforced concrete with the strength and speed of construc- tion associated with structural steel to produce an economic structure (Griffis 1986). The concrete used for encasing a structural steel section not only increases its strength and stiff- ness, but also protects it from fire damage. As a result, the use of such columns is gaining popularity in building construction in addition to applications in marine structures. The lateral loads acting on a completed structure are resisted by stiff shear walls, frame action, or both. Regardless of how the lateral loads are resisted, most columns are subjected to the combined effects of axial force and bending moment and are classified as beam-columns. Past studies on composite beam-columns have mostly concentrated on specimens in which eccentric axial loads are applied at member ends. Con- sequently, the physical tests on composite beam-columns with steel shapes encased in concrete and subjected to axial and transverse loads seem to be rare in the literature reviewed (Morino et al. 1986; Ricles and Paboojian 1994; Zang and Yamada 1992). This is particularly valid for slender beam- columns. This paper describes experimental and analytical studies in which slender composite steel-concrete beam-col- umns were subjected to the combined effect of proportionally applied static axial and transverse loads, as indicated by the test setup shown in Fig. l(a). Several studies have reported physical tests conducted on composite girders and push-out specimens in which intercon- nection between the steel section and concrete slab was suc- cessfully achieved by welding the steel ribs with holes (per- fobond strips) to the flanges of the steel sections (Leonhardt et al. 1987; Oguejiofor and Hosain 1992, 1994). However, such interconnection has rarely been investigated in beam-col- 'Prof., Dept. of Civ. Engrg., Lakehead Univ., Thunder Bay, Ontario, Canada. 2Acad. of Finland Res. Assoc., Struct. Engrg. Res. Lab., Univ. ofOulu, Oulu, Finland. 'Prof., Dept. of Civ. Engrg., Univ. of Oulu, Oulu, Finland. Note. Associate Editor: W. Samuel Easterling. Discussion open until April I, 1997. To extend the closing date one month, a written request must be filed with the ASCE Manager of Journals. The manuscript for this paper was submitted for review and possible publication on April 4, 1995. This paper is part of the ]ourlUll of Structural Engineering, Vol. 122, No. 11, November, 1996. ©ASCE, ISSN 0733-9445/96/0011- 1317-1326/$4.00 + $.50 per page. Paper No. 10455. (b) <c) FIG. 1. Loading Arrangement: (a) Test Setup; (b) Schematic Loading Diagram; (c) Schematic Bending Moment Diagram (DI- mensions are In mm) JOURNAL OF STRUCTURAL ENGINEERING / NOVEMBER 1996/1317 J. Struct. Eng. 1996.122:1317-1326. Downloaded from ascelibrary.org by Saskatchewan University on 10/13/12. Copyright ASCE. For personal use only; all rights reserved.
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Page 1: Physical Tests and Analyses of Composite Steel-Concrete Beam-Columns

PHYSICAL TESTS AND ANALYSES OF COMPOSITE STEEL-CONCRETE

BEAM-COLUMNS

By S. Ali Mirza,! Fellow, ASCE, Ville Hyttinen,:Z and Esko Hyttinen3

ABSTRACT: The composite steel-concrete beam-columns in which steel shapes are encased in concrete andsecond-order effects are significant were studied from 16 specimens loaded to failure. Loading included com­binations of axial and transverse forces producing a wide range of different external eccentricities. Observationsfrom the physical tests indicate that, for static loads, the bonding condition at the interface of steel rib connectorsand the surrounding concrete has a small effect on ultimate strength. The tests also show that the ACI 318assumption of maximum usable strain of 0.003 at concrete extreme compression fibers near ultimate load isvalid for such beam-columns. Analyses based on ACI 318, Eurocode 4, and finite-element modeling procedureswere compared to test results that provided further insight into understanding the structural behavior of suchbeam-columns.

umn tests. Steel rib connectors with three different bondingconditions were used for the beam-column specimens reportedon in this study (Fig. 2). The objective of the study was four­fold: (1) to investigate the behavior and ultimate strength ofcomposite steel-concrete beam-columns in which steel shapes

L = 4000

9 V~ .J,.Vu

~ Itllt tllllll til"~

~"'~---~----~~m

1500 I 1000 I 1500

a"Ia

<a)

INTRODUCTION

During the past few decades, several composite steel-con­crete structural systems have been used in the construction oftall buildings. One such system employs composite columnsthat consist of steel shapes encased in concrete and compositegirders that use metal deck between the steel section and con­crete slab. This system combines the rigidity and formabilityof reinforced concrete with the strength and speed of construc­tion associated with structural steel to produce an economicstructure (Griffis 1986). The concrete used for encasing astructural steel section not only increases its strength and stiff­ness, but also protects it from fire damage. As a result, the useof such columns is gaining popularity in building constructionin addition to applications in marine structures.

The lateral loads acting on a completed structure are resistedby stiff shear walls, frame action, or both. Regardless of howthe lateral loads are resisted, most columns are subjected tothe combined effects of axial force and bending moment andare classified as beam-columns. Past studies on compositebeam-columns have mostly concentrated on specimens inwhich eccentric axial loads are applied at member ends. Con­sequently, the physical tests on composite beam-columns withsteel shapes encased in concrete and subjected to axial andtransverse loads seem to be rare in the literature reviewed(Morino et al. 1986; Ricles and Paboojian 1994; Zang andYamada 1992). This is particularly valid for slender beam­columns. This paper describes experimental and analyticalstudies in which slender composite steel-concrete beam-col­umns were subjected to the combined effect of proportionallyapplied static axial and transverse loads, as indicated by thetest setup shown in Fig. l(a).

Several studies have reported physical tests conducted oncomposite girders and push-out specimens in which intercon­nection between the steel section and concrete slab was suc­cessfully achieved by welding the steel ribs with holes (per­fobond strips) to the flanges of the steel sections (Leonhardtet al. 1987; Oguejiofor and Hosain 1992, 1994). However,such interconnection has rarely been investigated in beam-col-

'Prof., Dept. of Civ. Engrg., Lakehead Univ., Thunder Bay, Ontario,Canada.

2Acad. of Finland Res. Assoc., Struct. Engrg. Res. Lab., Univ. ofOulu,Oulu, Finland.

'Prof., Dept. of Civ. Engrg., Univ. of Oulu, Oulu, Finland.Note. Associate Editor: W. Samuel Easterling. Discussion open until

April I, 1997. To extend the closing date one month, a written requestmust be filed with the ASCE Manager of Journals. The manuscript forthis paper was submitted for review and possible publication on April 4,1995. This paper is part of the ]ourlUll of Structural Engineering,Vol. 122, No. 11, November, 1996. ©ASCE, ISSN 0733-9445/96/0011­1317-1326/$4.00 + $.50 per page. Paper No. 10455.

(b)

Nu~m,

M"L~]M~<c)

FIG. 1. Loading Arrangement: (a) Test Setup; (b) SchematicLoading Diagram; (c) Schematic Bending Moment Diagram (DI­mensions are In mm)

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Page 2: Physical Tests and Analyses of Composite Steel-Concrete Beam-Columns

6-mmdla.

AxIs ofBending

10- mm dla

I. 240

Xpc =72 (series RHB)

xpc. 92 (8eries RHNB and RNHB)

27-mm dla. holes

Xpc

240

- ___ Xpc tr-~

.1(SerIes RNHB)

HE100A E3E:=aosection

T a.6

~FIG. 2. Cross-8ectlon Details of Test Specimens (Dimensions are In mm)

TABLE 1. Mechanical Properties of Concrete and Steel

External Concrete Structural Steel Reinforcing Steel

Specimen eccentricity strength '~ubo 'y '. 'y '.designation ratio elh (MPa) (MPa) (MPa) Em (MPa) (MPa) Em(1 ) (2) (3) (4) (5) (6) (7) (8) (9)

(a) Series RHB: ribs (with holes) bonded to concrete

RHB-I 0.165 33.6 293.4 424.0 0.21 565.0 640.3 0.14RHB-2 0.274 33.6 293.4 424.0 0.21 565.0 640.3 0.14RHB-3 0.440 34.2 293.4 424.0 0.21 565.0 640.3 0.14RHB-4 0.834 31.9 311.2 428.6 " 634.0 747.7 0.18RHB-4A 1.545 31.0 293.4 424.0 0.21 565.0 640.3 0.14RHB-5 2.640 35.3 293.4 424.0 0.21 565.0 640.3 0.14

(b) Series RNHB' ribs (without holes) bonded to concrete

RNHB-l 0.205 34.0 311.2 428.6 " 634.0 747.7 0.18RNHB-2 0.240 34.0 311.2 428.6 - " 634.0 747.7 0.18RNHB-3 0.441 33.0 293.4 424.0 0.21 565.0 640.3 0.14RNHB-4 0.871 33.6 293.4 424.0 0.21 565.0 640.3 0.14RNHB-5 2.624 34.7 293.4 424.0 0.21 565.0 640.3 0.14

(c) Series RHNB: ribs (with covered holes) not bonded to concrete

RHNB-l 0.174 34.0 311.2 428.6 " 634.0 747.7 0.18RHNB-2 0.247 34.0 311.2 428.6 " 634.0 747.7 0.18RHNB-3 0.410 31.9 311.2 428.6 " 634.0 747.7 0.18RHNB-4 0.858 31.9 311.2 428.6 " 634.0 747.7 0.18RHNB-5 2.584 31.9 311.2 428.6 " 634.0 747.7 0.18

"The maximum (fracture) strain Em was not measured for these tests.

are encased in concrete and second-order effects are significantover almost the entire range of the interaction diagram; (2) tostudy the effect of different bonding conditions at the interfaceof steel ribs and surrounding concrete; (3) to examine the ap­plicability of ACI 318 (Building 1995), Eurocode 4 (Design1992), and nonlinear finite-element modeling procedures tosuch beam-columns; and (4) to compare the results from threecomputational procedures with each other and with those ob­tained from physical tests.

PHYSICAL TESTS

The behavior of slender tied composite beam-columns wasobserved from 16 specimens tested to failure. The failure loadsconsisted of concentric axial load N. and a pair of transverseloads V. acting simultaneously on pin-ended specimens, asshown in Fig. 1. Since the specimens were cast and tested

1318/ JOURNAL OF STRUCTURAL ENGINEERING / NOVEMBER 1996

horizontally, they were also subjected to uniformly distributedtransverse load g due to the self-weight of the specimen.

The externally applied (first-order) bending moment at thefailure section (midlength) of a specimen is given by M.e =V.a + gL2/8, where a = shear span and L = length of thespecimen, and the external eccentricity at the same location iscomputed from e =M.e/N•. This eccentricity was nondimen­sionalized by dividing it by the overall depth h of the com­posite cross section in the plane of bending. The resulting ec­centricity ratio e/h, ranging approximately from 0.17 to 2.6(Table 1), were used to investigate the beam-column behaviorover almost the entire practical range of the axial load-bendingmoment interaction diagram.

Axial and transverse loads were applied through load-con­trolled methods and monitored by readings from the load cells.The distribution of forces within the specimens could be traced

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Page 3: Physical Tests and Analyses of Composite Steel-Concrete Beam-Columns

by means of electric strain gauges that were attached to thecompression face of the concrete cross section at rnidlengthand to the outside faces of the structural steel flange over­hangs. The transverse deflections of the specimens were alsomeasured. The loading procedure involved monitoring of re­sponse to service load forces before loads were increasedenough to create a failure condition. The testing time rangedfrom 19 to 69 min. The ratio of transverse to axial loads waskept constant at all stages of loading for a given specimen butvaried from specimen to specimen. The loads produced singlecurvature bending in all beam-column specimens with bendingmoments acting about the major axis of the steel cross section.

All specimens had the same structural steel shape and over­all dimensions of the concrete cross section which was squareand symmetrical about both axes. Specific cross-section detailsare given in Fig. 2. The ratio of the cross-sectional area ofstructural steel to the area of overall concrete cross sectionwas 4.2%. To avoid local buckling of component plates, astocky steel shape was used with width-to-thickness ratio ofthe flange overhangs of 5.8 and that of the web of 15.5.

Nominal amounts of longitudinal and transverse reinforcingsteel were provided for all specimens. Four corner bars havinga cross-sectional area of about 0.55% of the gross cross sectionwere used in the longitudinal direction, whereas closed rectan­gular ties having a volumetric ratio of approximately 0.25%were placed at 150 mm on centers over almost the entirelength of the specimens. Near the specimen ends, the volu­metric ratio of the ties was increased to approximately 2.65%and the tie spacing was decreased to 50 mm. This was doneto control the bursting effect in end regions due to the highbearing stresses caused by applied axial loads.

Ribs were welded to both sides of the steel section (Fig. 2)to enhance interconnection between the steel section and con­crete for some specimens. Based on the type of steel ribs used,specimens were grouped into three series as indicated by Table1: (1) RHB refers to six specimens that contain ribs with holesbonded to concrete; (2) RNHB' stands for five specimens hav­ing ribs without holes bonded to concrete; and (3) RHNB rep­resents five specimens consisting of ribs with covered holesthat are not bonded to concrete. The last mentioned involveda series of specimens (series RHNB) in which rib holes werefilled with wooden disks and then covered with smooth plastic

tape that was coated with a layer of oil to break the bondbetween the steel ribs and surrounding concrete. For speci­mens of the RHB series, reinforcing steel ties passed throughevery third rib hole, acting as mechanical connectors betweensteel and concrete. This mechanical interconnection was notavailable for the specimens of the other two series, becausethe ties passed over the ribs for those specimens. As a result,for specimens of series RHB, the resistance to horizontal shearforce at the interface of ribs and concrete was provided bylateral ties acting as mechanical connectors plus the bearingand shearing of concrete inside the rib holes in addition to thebond due to adhesion and friction at the interface of ribs andsurrounding concrete. The bond due to adhesion and frictionalone resisted the horizontal shear force at the interface of ribsand concrete for specimens of series RNHB. As observed ear­lier, the bond was broken at the interface of ribs and concretefor series RHNB specimens. Bond due to adhesion and frictionexisted at the interface of the steel section and surroundingconcrete for specimens of all three series.

The concrete strengths were measured on standard (150 X150 X 150 mm) cubes. The strengths shown in Table 1 arethe averages of three cube tests. For equivalent cylinderstrengths, a conversion factor of 0.81 was used for strengthanalyses presented in the later part of this paper. This value isthe average conversion factor for the 16 cube strengths listedin Table I and was computed from the equation given byL'Hermite (1955)

I;yllnder =[0.76 + 0.2 loglO(f;UbeI19.6)lf;ube (1)

in which I~Ube = measured compressive strength of standardcubes; and I~Ylinder = equivalent compressive strength of stan­dard cylinders.

The modulus of elasticity of steel sections, ribs, and rein­forcing bars was 200,000 MPa whereas the yield strength ofsteel ribs was 293.4 MPa. The yield strengths IY, tensilestrengths !u' and maximum (fracture) strains Em of structuralsteel given in Table 1 are averages of five to 11 tests conductedon coupons approximately 211 X 25 X 5 mm in size thatwere machined from flanges of the steel sections. Similarly,j;"f", and Em values of reinforcing steel in Table 1 are averagesof three tests conducted on lO-mm diameter (cross-sectionalarea = 79 mm2

) bars 241 mm in length.

TABLE 2. Test Results at Failure

Lateral Test Strengths MomentExternal deflection magnification

Specimen eccentricity at midheight Ilm Nu Vu Mu• Mum factordesignation ratio e1h (mm) (kN) (kN) (kN ·m) (kN'm) 0= Mum/Mu•

(1 ) (2) (3) (4) (5) (6) (7) (8)

(a) Series RHB' ribs (with holes) bonded to concrete

RHB-I 0.165 27.8 950.0 23.0 37.7 64.1 1.70RHB-2 0.274 49.1 550.0 22.0 36.2 63.2 1.75RHB-3 0.440 31.5 570.0 38.0 60.2 78.2 1.30RHB-4 0.834 59.3 307.5 38.9 6\.5 79.8 1.30RHB-4A \.545 56.8 154.3 36.0 57.2 66.0 1.15RHB-5 2.640 56.4 95.0 38.0 60.2 65.6 1.09

(b) Series RNHB' ribs (without holes) bonded to concrete

RNHB-I 0.205 39.8 925.0 28.1 45.4 82.2 1.81RNHB-2 0.240 40.5 775.0 27.6 44.6 76.0 1.70RNHB-3 0.441 46.5 540.0 36.0 57.2 82.3 1.44RNHB-4 0.871 56.9 352.5 47.0 73.7 93.8 \.27RNHB-5 2.624 53.7 107.5 43.0 67.7 73.5 1.09

(c) Senes RHNB' nbs (With covered holes) not bonded to concrete

RHNB-l 0.174 35.9 927.0 23.7 38.7 72.0 1.86RHNB-2 0.247 37.9 720.0 26.3 42.7 69.9 1.64RHNB-3 0.410 55.3 540.0 33.3 53.1 83.0 1.56RHNB-4 0.858 64.1 296.0 38.5 6 \.0 79.9 1.31RHNB-5 2.584 67.2 100.0 39.2 62.0 68.7 1.11

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Page 4: Physical Tests and Analyses of Composite Steel-Concrete Beam-Columns

TEST RESULTS

Ultimate Strengths

Table 2 contains a summary of test results at failure con­dition. The table displays for each specimen the ultimate axialand transverse loads that could be resisted by the specimenand the corresponding lateral deflection am recorded at mid­length of the specimen. The externally applied (first-order)bending moment Mu• and the magnified bending moment Mum,both acting at the failure section (midlength) of the specimens,were computed from the following:

M u• =aVu + Mg = l.5Vu + 3.2 (kN'm) (2)

Mum =M u• + Nuti.m (3)

in which Mg = bending moment caused by the self-weight ofthe specimen = gL2/8. The term Nuti.m in (3) represents thesecond-order bending moment caused by the transverse de­flection of the specimen at the failure section. The momentmagnification factor for a beam-column was defined as theratio of the magnified bending moment to the externally ap­plied bending moment, both acting at the failure section (& =Mum/Mu.). The computed values of Mue> Mum, and l) are listedin Table 2.

The moment magnification factors shown in Table 2 arequite high, especially for test specimens with eccentricity ra­tios (e/h) lower than 0.9. This is because the specimens had ahigh slenderness with L/h = 16.7. This corresponded to theL/r ratios of 71.6 (series RNHB) or 72.9 (series RHB andRHNB), where r = radius of gyration of the composite crosssection in the plane of bending computed according to ACI318 (Building 1995). A comparison of moment magnificationfactors for specimens from the three series shows small dif­ferences in their values (Table 2), indicating insignificant effectof the bonding condition at the interface of rib connectors andconcrete.

The effect of the bonding condition at the interface of ribsand concrete was further investigated by comparing the non­dimensionalized axial load ratios Nu/No for the tests from threeseries. No is the pure axial force capacity of the compositecross section and was computed from

sum of cross-sectional areas of structural and reinforcingsteels; and L/yAs = sum of compressive yield forces resistedby structural and reinforcing steels. Again, the plotted valuesof Nu/No shown in Fig. 3 indicate the small effect of the bond­ing condition at the interface of ribs and concrete. This impliesthat the bond due to adhesion and friction at the interface ofthe steel section and surrounding concrete provides sufficientinterconnection and additional interconnection through shearconnectors may not be necessary for beam-columns, especiallywhen they are subjected to low eccentricities. However, thisobservation may not be applicable to beam-columns subjectedto seismic forces or fatigue effects, since the specimens in­vestigated here dealt with static loads alone. In this regard, theACI 318 provisions (Building 1995) require shear connectorsfor the transfer of forces between steel and concrete at all axialload levels, whereas the American Institute of Steel Construc­tion (AISC) load and resistance factor design (LRFD) provi­sions (Load 1993) require shear connectors to develop the fullplastic moment resistance of beam-columns at low axial loads.

Structural Steel Stresses

The variation of stresses in flanges of the steel section be­tween applied transverse loads (in the central part of the spec­imen) is shown in Fig. 4. These stresses were measured fromthe strain gauges attached to the outside faces of the top andbottom flanges. Twelve strain gauges were used for each spec­imen and were located at midlength and 500 mm each sidefrom the midlength along the axis of the specimen.

Three different load levels are used for plotting these steelstresses: (1) 33% of the failure load; (2) 66% of the failureload; and (3) failure load. If the service live load and service

II-Eltl !!!!! 1)1111!!I~fj--

-400 .----..,...----..----.,-----,

-e/l1-0.410 --- e/h-0.858 - -e/l1-2.584

in which Ag = gross area of the concrete cross section; LAs =

0.5 ~--....----r----r----r----r-----'

CompMllon YIelding of Top Flange

-------

A10.33-{FaUuN ._. _Lead .....~ ..._~

l:At O.ell Failure L.oed~ - •--..- _----:.. .-- --------

---- --- -.·-s;;J;.~~:~d~--~~-----_ ... - At033......_-- ...&1•••••• }-FailUnI---- --- Load

0~-------------==---1

-100

-300

+100

+200

Tenelon YIelding 01 BollDm Flange

+300 ~-.,......_l..AtliFi~liiiure~l.oiedN~:;; ~---=1

(4)

.......... seriesRHB

A---A series RNHB

...... series RHNB

0.1

0.4

'0

~E:. 0.3

J~.::l 0.2

)

3.0

+400 L-..__....L. ...L- ..L-__-.J

500 0 500

Distance from Mid-length (mm)

FIG. 4. Variation of Stress in Flanges of Structural Steel Sec­tion

0.0 1...-__...L-__-.1.-__---l. l...-__...L-__-J

0.0 1.0 2.0External Eccentricity Ratio (e/h)

FIG. 3. Effect on Strength of Bonding Condition at InterfaceofSteel Ribs and Surrounding Concrete

1320 I JOURNAL OF STRUCTURAL ENGINEERING I NOVEMBER 1996

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Page 5: Physical Tests and Analyses of Composite Steel-Concrete Beam-Columns

FIG. 6. Typical Failure Mode

of the failure load) are well within elastic limits (Fig. 4). Atfailure load, the bottom flange of all three specimens yieldedin tension although yielding did not occur over the full lengthof the central region in the specimen with elh = 0.410, asindicated by Fig. 4. However, the stresses in the top (com­pression) flange were lower than the yield stress for specimenswith elh = 0.410 and 0.858 and much lower than the yieldstress for the specimen with elh = 2.584. This is expectedbecause high eccentricity ratios involve low axial forces, re­sulting in decreased stresses due to axial compression.

To avoid congestion of Fig. 4, the structural steel stressesfor specimens with elh = 0.247 and 0.174 are not plotted. Thestresses in the top flange of these specimens at all three load

...

At Failure Load

ACI Alaumpllon for Ultimate Strength

( At 0.88 Failure Load

•-_I L At 0.33 Failure Load

.~.._......~------ .....

0.005 ,....--""'T""--...---""'T""--...---...,...----:t

L~'6.~U3 0.003 I----,I----L-----------t

.~

i 0.002

~~ 0.001

.~:::E o '--_....L.._--L__..I.-_........__"--_~

o 1.0 2.0 3.0

External Eccentricity Ratio (e/h)

FIG. 5. Variation of Strain In Extreme Compression Fibers ofConcrete

dead load are assumed to be equal in magnitude, the 66% ofthe failure load approximately represents the total service deadand live load, whereas the 33% of the failure load approxi­mately equals the service dead load alone. The steel stressesin Fig. 4 are plotted from data from specimens RHNB-3,RHNB-4, and RHNB-5, having external eccentricity ratios ofelh =0.410, 0.858, and 2.584, respectively. According to ACI318 (Building 1995), these eccentricity ratios would producecompression, balance, and tension failure condition, respec­tively, at the fai'ure section of the beam-column specimens.

As expected, the structural steel stresses at service dead load(33% of the failure load) and service dead plus live load (66%

TABLE 3. Comparison of Code Strengths with Test Strengths

CODE STRENGTHSRatios of Test to Code Strengths

External ACI318 Eurocode 4 (Nu or M"" Ratios)

Specimen eccentricity Nu M"" Nu Mu•

designation ratio e1h (kN) (kN'm) (kN) (kN·m) ACI318 Eurocode 4(1 ) (2) (3) (4) (5) (6) (7) (8)

(a) Series RHB: ribs (with holes) bonded to concrete-

RHB-l 0.165 742.9 29.4 967.9 38.0 1.28 0.99RHB-2 0.274 578.5 38.0 711.3 45.8 0.95 0.78RHB-3 0.440 438.7 46.1 494.7 52.6 1.30 1.15RHB-4 0.834 263.0 52.5 277.0 55.8 1.17 1.11RHB-4A 1.545 146.8 54.4 140.9 52.5 1.05 1.09RHB-5 2.640 91.0 57.6 82.2 52.5 1.04 1.15

(b) Series RNHB: ribs (without holes) bonded to concreteb

RNHB-l 0.205 741.7 36.3 947.3 46.7 1.25 0.97RNHB-2 0.240 685.9 39.5 880.8 49.8 1.13 0.89RNHB-3 0.441 475.4 50.3 512.6 54.5 1.14 1.05RNHB-4 0.871 288.2 60.1 283.1 59.8 1.22 1.24RNHB-5 2.624 101.9 64.0 95.1 60.2 1.05 1.13

(c) Series RHNB: Ribs (with covered holes) not bonded to concrete"

RHNB-l 0.174 753.0 31.4 1,007.1 41.4 1.23 0.93RHNB-2 0.247 638.3 37.9 837.8 49.2 1.13 0.86RHNB-3 0.410 464.6 45.6 535.5 52.9 1.16 1.01RHNB-4 0.858 275.7 56.6 288.0 59.3 1.07 1.03RHNB-5 2.584 99.5 61.6 95.5 59.3 1.01 1.05

Note: Overall average value for columns 7 and 8 =1.14 and 1.03, respectively; and overall coefficient of variation for columns 7 and 8 =8.9 and11.8%, respectively.

'Average value for columns 7 and 8 =1.13 and 1.05, respectively; and coefficient of variation for columns 7 and 8 =12.5 and 13.6%, respectively.bAverage value for columns 7 and 8 = 1.16 and 1.06, respectively; and coefficient of variation for columns 7 and 8 = 6.8 and 12.9%, respectively."Average value for columns 7 and 8 = 1.12 and 0.98, respectively; and coefficient of variation for columns 7 and 8 =7.5 and 8.1%, respectively.

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levels were similar to, although somewhat lower than, thosefor the specimen with e/h = 0.410. For the bottom flange,however, the stresses in specimens with e/h = 0.247 and 0.174were significantly lower than the stresses in the specimen withe/h = 0.410, regardless of the load level considered. Fig. 4shows the data for series RHNB specimens. The structuralsteel stresses in specimens of the other two series (RHB andRNHB) were similar to those plotted in Fig. 4.

Concrete Strains

The variation of maximum compressive strain of concreteis plotted in Fig. 5. These strains were measured from thestrain gauges mounted on the top (compression) face at mid­length of each specimen. Fig. 5 indicates that the maximumcompressive strain of concrete at failure load varied from ap­proximately 0.0028 to 0.0044. This means that the ACI 318(Building 1995) assumption of maximum usable strain of0.003 at concrete extreme compression fiber near ultimatestrength is also valid for the type of composite beam-columnstested. For the other two load levels, representing dead loadalone and dead plus live load (33 and 66% of the failure load),the concrete strains are much lower than those at the failureload, as indicated by Fig. 5. Again, the data for series RHNBspecimens are shown; the data for specimens of the other twoseries were similar to those plotted in Fig. 5, especially thoseat failure load. The maximum compressive strain of concreteat failure load varied approximately from 0.0025 to 0.0044 for

specimens of series RHB and from 0.0035 to 0.0043 for spec­imens of series RNHB.

Failure Mode

All specimens failed in a similar mode. As the load wasincreased close to the failure condition, wide cracks appearedon the bottom (tension) face of the specimen. These crackswere accompanied by tension yielding of the bottom longitu­dinal reinforcing bars and, if e/h was greater than 0.4, by ten­sion yielding of the bottom flange of the structural steel sectionas well. Just prior to failure, concrete strain in the extreme top(compression) fibers near the midlength of the specimenreached around 0.0025 -0.0044, depending on the externale/h ratio. Finally, the failure took place by the crushing ofconcrete in these fibers, as indicated in Fig. 6.

COMPARISON WITH ACI AND EUROCODESTRENGTHS

The ultimate strengths of beam-column specimens werecomputed using the ACI 318 (Building 1995) and Eurocode 4(Design 1992) methods and compared to the test strengths. Allcomputations for both methods were carried out as given inthese codes except that the understrength factors for ACI 318and the so-called partial safety factors (material resistance fac­tors) for Eurocode 4 were taken equal to 1.0. The computedstrengths, therefore, represent the unfactored code strengths.

Segments

Nodes

1

I[I] 0 [II[£]0 0 [2] 01

1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 1.7

I: 8x250

2000

Segment m

15•

16•250

(a)

17•

.1

••

m+-----X----m

ConcreteIntegration points 15 x 15

RelnfcrcementlsteellIntegration points1 polnt/bar

Steel memberIntegration points5+9+5

Steel ribsIntegration points5+5

(b)

FIG. 7. Finite-Element Model of Composite Beam-Columns: (a) Side View of Element Model; (b) Cross Sections of Ele­ments

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FIG. 8. Schematic Stress-5train Curves Used for FEM Method

The Eurocode 4 method is somewhat different from the ACIcode in the sense that it adopts the European buckling curvesfor steel columns as the basic design curves for compositecolumns. It also uses a simplified axial force-bending momentinteraction curve for the composite cross sections. The equiv­alent compressive strengths of standard cylinders computedfrom (1) were used for both design methods. The modulus ofelasticity of concrete was taken as 4,750Vf~Ylinder for the ACIcode and as 30,500 MPa for Eurocode 4.

Table 3 shows the values of Nu and M ue computed from theACI code and Eurocode 4 methods for all beam-column spec­imens. Also given in this table are the ratios of test to codestrengths (strength ratios) for the two methods. An examina­tion of these strength ratios indicates that both methods predictthe composite beam-column strength with reasonable accu­racy, with the exception of specimen RHB-2 in Table 3 wherethe Eurocode 4 method somewhat overestimates the teststrength. Table 3 also shows that the ACI 318 procedure pro­duces somewhat more conservative and less variable resultsthan the Eurocode 4 method. This can be seen by comparingthe average strength ratios and related coefficients of variationobtained from the two methods (footnotes of Table 3) for thebeam-column tests of individual series and all three seriescombined. This is not surprising because ACI 318 uses thestrain-compatibility solution for the cross-section strength,whereas Eurocode 4 uses a modified plastic strength analysisin which the cross section is assumed to have been yieldedpartly in compression and partly in tension.

The strength comparisons given in Table 3 are based on theassumption that the cylinder strength is equal to 0.81 timesthe cube strength. When this conversion factor was increasedto 0.85 and 0.9, the average ratios of test to code strengths inTable 3 decreased by 2.5 and 4.5%, respectively, for ACI 318and by 1 and 2%, respectively, for Eurocode 4. The coeffi­cients of variation remained unaffected in both cases. Thisindicated the nearly insignificant effect of the concrete strengthconversion factor within the range studied (0.81-0.9), whichwas expected because the cross-sectional area of longitudinal

E

-0

E

(a) Stress-Strain Relationship for Concrete

E

(b) Stress-Strain Relationship forStructural and Reinforcing Steel

-E

TABLE 4. Comparison of FEM Strengths with Test Strengths

External FEM Strengths Ratios of Test to FEM Strengths

Specimen eccentricity Nu Vu Mu• Mum N.. V.. ordesignation ratio elh (kN) (kN) (kN'm) (kN·m) Mu• ratios Mum ratios

(1 ) (2) (3) (4) (5) (6) (7) (8)

(a) Series RHB: ribs (with holes) bonded to concrete'

RHB-I 0.165 940.2 22.7 37.3 61.4 1.01 1.04RHB-2 0.274 695.2 27.8 45.5 70.8 0.79 0.89RHB-3 0.440 493.1 32.9 52.1 74.4 1.16 1.05RHB-4 0.834 275.8 34.9 55.5 69.5 1.11 1.15RHB-4A 1.545 149.5 34.9 55.5 62.2 1.03 1.06RHB-5 2.640 91.2 36.5 57.9 62.2 1.04 1.05

(b) Series RNHB: ribs (without holes) bonded to concreteb

RNHB-I 0.205 916.9 27.9 45.0 75.4 1.01 1.09RNHB-2 0.240 831.0 29.6 47.7 77.4 0.93 0.98RNHB-3 0.441 551.4 36.8 58.3 83.1 0.98 0.99RNHB-4 0.871 299.6 39.9 62.7 76.2 1.18 1.23RNHB-5 2.624 102.4 41.0 64.6 70.0 1.05 1.05

(c) Senes RHNB' ribs (with covered holes) not bonded to concrete<

RHNB-I 0.174 980.6 25.1 40.8 68.8 0.95 1.05RHNB-2 0.247 782.7 28.6 46.2 75.8 0.92 0.92RHNB-3 0.410 548.1 33.8 53.9 79.7 0.99 1.04RHNB-4 0.858 295.2 38.4 60.8 74.3 1.00 1.08RHNB-5 2.584 100.7 39.5 62.4 67.7 0.99 1.02

Note: Overall average value for columns 7 and 8 = 1.01 and 1.04, respectively; and overall coefficient of variation = 9.3 and 7.6%, respectively.'Average value for columns 7 and 8 = 1.02 and 1.04, respectively; and coefficient of variation for columns 7 and 8 = 12.4 and 7.9%, respectively.bAverage value for columns 7 and 8 = 1.03 and 1.07, respectively; and coefficient of variation for columns 7 and 8 = 9.0 and 9.4%, respectively.<Average value for columns 7 and 8 = 0.97 and 1.02, respectively; and coefficient of variation for columns 7 and 8 = 3.6 and 5.8%, respectively.

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200

20 40 60 80External Bending Moment, Mue (kN-m)

1000-r------tt--""/----,

20 40 60 80External Bending Moment, Mue (kN-m)

800

200

20 40 60 80External Bending Moment, Mue (kN-m)

" Test Results

+ ACI318

x Eurocode4

o FEM

FIG. 9. Comparison of FEM, AC1318, Eurocode 4, and Test Strengths: (a) Series RHBj (b) Series RNHBj (c) Series RHNB

(structural and reinforcing) steel was 4.75% of the area of theoverall concrete cross section.

FINITE-ELEMENT MODELING

The finite-element modeling (FEM) of beam-column spec­imens was carried out by using a nonlinear FEM software(ABAQUS I 989a,b). The objective was to model the ultimatestrength and load-deflection response of these specimens. Thespecimens were modeled with three-node, three-dimensionalbeam elements as shown in Fig. 7. I-beam elements were usedto model the structural steel section whereas eccentric rectan­gular elements were employed for steel ribs. Ribs in seriesRHB and RHNB beam-column specimens had holes spacedalong the rib length as indicated in Fig. 2. Parts of these ribswere modeled with narrower rectangular elements having thesame cross-sectional area as the ribs at the hole location. Theelements for concrete, reinforcing bars, structural steel section,and steel ribs had common nodal points. The integration pointsof the element cross sections used for taking into account theproperties of different materials are shown in Fig. 7.

The schematic stress-strain relationships for concrete andsteel are given in Fig. 8. As shown in this figure, the elastic­plastic stress-strain curves were used for reinforcing and struc­tural steels. The stress-strain relationship for concrete in uni­axial compression was represented by the following expression(Saenz 1964):

1324/ JOURNAL OF STRUCTURAL ENGINEERING / NOVEMBER 1996

(5)

in which I; = compressive strength; Eo = strain correspondingto compressive strength = 0.002; and Ec = modulus of elastic­ity of concrete. The stress-strain curve for concrete in uniaxialtension was taken from BaZant and Dh (1984):

CT = EcE for E S E,p (6a)

CT =1: - E,(E - E,p) for E,p < E < Elf (6b)

CT =0 for E ~ Elf (6c)

in which I: = tensile strength; E, = tension softening modulus= 0.48E/(0.39 + I:); E,p = strain corresponding to tensilestrength = 1:IEc ; and Elf = final strain when tensile stress re­duces to zero = E,p + (/:IE,).

The compressive strength, tensile strength, and modulus ofelasticity of concrete used in (5) and (6) included the rate ofloading effect on beam-column specimens and were calculatedfrom

I; =I~Yllnder[0.87 + 0.07 loglO(l45/;Ylinder1t)] (7)

/: =0.33v:t;; Ec =5,OOOv:t; (8, 9)

in which/;ylinder = equivalent compressive strength of standardcylinders computed from (1); and t = time (in seconds) taken

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Page 9: Physical Tests and Analyses of Composite Steel-Concrete Beam-Columns

F-~E.STl~EMJ

10 20 30 40 50 60 70

f> [mm]

10 20 30 40 50 60 70

f> [mm]

Specimen RHNB-2

Specimen RHNB-4

50

40

~3020

>10(b) 0 L...__- _

10 20 30 40 50 60 70 0

f> [mm]

50

40

~ 3020

>10

(d) O¥----------10 20 30 40 50 60 70 0

f> [mm]

Spe.lmen RHNB·l

Specimen RHNB-3

50

40

~3O> 20

10(a) 0 L- _

o

50 Specimen RHNB.540 _._-__..-

~30> 20

10

(e) 0¥---------­o 10 20 30 40 50 eo 70

f> (mm]

FIG. 12. Load-Deflection Curves for Series RHNB Specimens

Load-Deflection Behavior

In Figs. 10, 11, and 12, the transverse loads (V) are plottedagainst the transverse midlength deflections (a) for seriesRHB, series RNHB, and series RHNB tests, respectively. Inthese figures, the load-deflection response measured from thephysical tests is compared to that obtained from the FEM pro­cedure. These plots indicate an excellent predictability of theload-deflection behavior by the FEM analysis in almost allcases. Again, the only exception is specimen RHB-2 in Fig.10, where the actual response is somewhat "softer" than thatcomputed by FEM analysis.

strengths with reasonable accuracy for almost all specimens.The only exception is specimen RHB-2 in Table 4 where theFEM procedure somewhat overestimates the test strength.However, the average ratios of test to FEM strengths are closeto 1.0 and the related coefficients of variation are small (foot­notes of Table 4), indicating the predication acceptability ofthe FEM procedure used.

The strength comparisons given in Table 4 are based onf:yllnder = 0.81f:ube· When this conversion factor was increasedto 0.85 and 0.9, the average ratios of test to FEM strengths inTable 4 decreased by 1-3% and 3-5%, respectively, whilethe coefficients of variation remained unaffected, indicatingagain the near insignificance of the concrete strength conver­sion factor within the range studied for these specimens.

Fig. 9 compares the Nu-Mut strength interaction diagramscomputed from the FEM method (Table 4), from the ACI 318and Eurocode 4 procedures (Table 3), and from test results(Table 2). Three sets of plots are shown in the figure. Eachset represents a different series of tests and, hence, a differentbonding condition at the interface of the steel ribs and sur­rounding concrete. Fig. 9 shows that although there are somedifferences in strengths obtained from the three computationalmethods, particularly at e/h ratios less than 0.9, all three meth­ods predict the beam-column specimen test strengths withinreasonable accuracy over the entire range of e/h ratios tested.This seems valid regardless of the bonding condition at theinterface of steel ribs and surrounding concrete.

SUMMARY AND CONCLUSIONS

The structural behavior and ultimate strength of slendercomposite steel-concrete beam-columns was observed from 16

.... --

I TEST I-- FEM

10 20 30 40 50 60 70

f> [mm]

10 20 30 40 50 60 70

f> [mm]

Spe.lmen RNHB-2

Specimen RNHB-4 ~ _

10 20 30 40 50 60

f> [mm]

Specimen RNHB-J

Spe.lmen RNHB.5:....-==--_

50 5040 Specimen RNHB-l 40

~3O ~3O> 20 > 20

10 7 10(a) 0---- (b) 0 l:- _

o 10 20 30 40 50 60 70 0

f> (mm)

50 50

40Specimen RHB·l 40 Spe.lmen RHB·2

~3O ~3O ----- .....> 20 > 20

10 10

(a) 00 (b) 010 20 30 40 50 60 70 0 10 20 30 40 50 60 70

f> [mm) f> [mm]

50 50 Spe.lmen RHB-4

40Speelmen RHB-J 40

~30 ~30

> 20 > 20 iI' "iI'

10 10 ,..

(.) 0 00 10 20 30 40 50 60 70 (eI) 0 10 20 30 40 50 60 70

f> (mm) f> [mmj

50 Specimen RHB-4A 50 Specimen RHB-540 40

~3O ~30> 20 > 20

10 10

(e) 0 (I) 00 10 20 30 40 50 60 70 0 10 20 30 40 50 60 70

f> (mm] f> [mm)

I TEST I-- FEM

FIG. 10. Load-Deflection Curves for Series RHB Specimens

10 20 30 40 50 60 70

f> [mm)

FIG. 11. Load-Deflection Curves for Series RNHB Specimens

by a beam-column specimen to reach its failure load. The termshown inside the square brackets in (7) represents the effectof rate of loading on the strength of in-situ concrete and isdocumented in a study by Mirza et al. (1979). This term variedfrom 0.87 to 0.91 for the 16 beam-column specimens reportedhere.

The possible effects of concrete confinement due to lateralties, of slip between longitudinal steel and surrounding con­crete, and of the presence of shear forces on resistance in com­bined axial compression and bending were neglected for FEM.

Ultimate Strengths

The values of Nu, Vu, Mu.. and Mum computed from the FEMprocedure are given in Table 4 for all beam-column specimens.Also given in this table are the ratios of test to FEM strengths.Table 4 indicates that the FEM procedure predicts the test

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specimens loaded to failure under the combined effect of axialand transverse forces. The external eccentricity covered theentire practical range of the axial force-bending moment in­teraction diagram. Three bonding conditions at the interfaceof steel rib connectors and surrounding concrete were inves­tigated. The structural steel stresses and concrete strains weremeasured and the typical failure mechanism was identified.

Observations from the physical tests indicate that, for staticloads, the bonding condition at the interface of steel ribs andsurrounding concrete had a small effect on the ultimatestrength. The tests also show that the present ACI 318 andEurocode 4 procedures adequately estimate the ultimatestrength of composite beam-columns, and that the ACI 318assumption of maximum usable strain of 0.003 at concreteextreme compression fibers near ultimate load is valid for suchbeam-columns. Predictions from a nonlinear finite-elementmodeling procedure provide good comparisons to the ultimatestrength and load-deflection response obtained from the phys­ical tests.

APPENDIX I. REFERENCES

ABAQUS version 4.8 theory manual. (1989a). Hibbit, Karlsson, and Sor­ensen Inc., Pawtucket, R.I.

ABAQUS version 4.8 users' manual and example problems. (1989b). Hib­bit, Karlsson, and Sorensen, Inc., Pawtucket, R.I.

Bafant, Z. P., and Oh, B. H. (1984). "Deformation of progressively crack­ing reinforced concrete beams." ACI J., 81(3), 268-278.

Building code requirements for structural concrete (ACI 318-95) andCommentary (ACI 3I8R-95). (1995). Am. Concrete Inst. (ACI), De­troit, Mich.

Design of composite steel and concrete structures-part I-I: general rulesand rules for buildings (Eurocode 4). (1992). Euro. Committee forStandardization, Brussels, Belgium.

Griffis, L. G. (1986). "Some design considerations for composite-framestructures." AlSC Engrg. J., 23(2), 59-64.

Leonhardt, F., Andrii, w., Andrii, H.-P., and Harre, W. (1987). "Neues,vorteilhaftes Verbundrnittel fUr Stahlverbund-Tragwerke mit hoherDauerfestigkeit." Beton- und Stahlbetonbau, Berlin, Germany, 12,325-331.

L'Herrnite, R. (1955). Idees actuelles sur la technologie du beton. Col­lection de L'lnstitut Technique du Batiment et des Travaux Publics,Paris, France.

Load and resistance factor design specification for structural steel build­ings. (1993). Am. Inst. of Steel Constr. (AISC), Chicago, Ill.

Mirza, S. A., Hatzinikolas, M., and MacGregor, J. G. (1979). "Statisticaldescriptions of strength of concrete." J. Struct. Div.. , ASCE, 105(6),1021-1037.

Morino, S., Matsui, C., and Yoshikai, S. (1986). "Local buckling of steelelements in concrete encased columns." Proc., Pacific Struct. SteelConf, New Zealand Heavy Engrg. Res. Assn., Auckland, New Zealand,Vol. 2, 319-335.

Oguejiofor, E. C., and Hosain, M. U. (1992). "Perfobond rib connectors

1326/ JOURNAL OF STRUCTURAL ENGINEERING / NOVEMBER 1996

for composite beams." Proc.• Compos. Constr. in Steel and ConcreteII, ASCE. New York, N.Y., 883-898.

Oguejiofor, E. C., and Hosain, M. U. (1994). "A parametric study ofperfobond rib shear connector." Can. J. of Civ. Engrg., Ottawa, Can­ada, 21(4), 614-625.

Ric1es,1. M., and Paboojian, S. D. (1994). "Seismic performance of steel­encased composite columns." J. Struct. Engrg., ASCE, 120(8),2474­2494.

Saenz, L. P. (1964). "Discussion of 'Equation for the stress-strain curveof concrete,' by Prakash Desayi and S. Krishnan." ACI J., 61(9),1229-1235.

Zhang, F., and Yamada, M. (1992). "Composite columns subjected tobending and shear." Proc., Compos. Constr. in Steel and Concrete II,ASCE, New York, N.Y., 483-498.

APPENDIX II. NOTATIONThe following symbols are used in this paper:

a shear span;Ec = modulus of elasticity of concrete (E, =tension softening

modulus);e = external eccentricity acting at the failure section =

MuJNu;f; = compressive strength of concrete used for finite-element

modeling;f~ = measured compressive strength of standard concrete

cubes;f~YUnder = equivalent compressive strength of standard concrete

cylinders;f: = tensile strength of concrete used for finite-element mod-

eling;fu = ultimate tensile strength of steel;h = yield strength of steel;g = transverse load due to self-weight of the specimen;h = overall depth of composite cross section in plane of

bending;L length of specimen;

M u• external (first-order) bending moment acting at failuresection;

Mum = magnified bending moment acting at failure section;No = pure axial force capacity of the composite cross section;Nu applied concentric axial load at failure;

t = time (in seconds) taken to reach the failure load in abeam-column test;

V = applied transverse load (at failure = Vu);

d = transverse deflection at rnidlength (at failure =d m);

8 = moment magnification factor = Mum/Mu.;E = strain;

Em = maximum (fracture) strain of steel;Eo = strain corresponding to f;;Elf = final strain when tensile stress in concrete reduces to

zero;E,p = strain corresponding to f:; and

(J' stress.

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