1. INTRODUCTION
In recent years, earthquake design philosophy has shifted
from a traditional force-based approach toward a
displacement-based ideology. The assumed initial
stiffness of reinforced concrete (RC) columns could affect
the estimation of the displacement and displacement
ductility, which are crucial in displacement-based design.
In addition, the assumed initial stiffness properties of
columns also affect the estimation of the fundamental
period and distribution of internal forces of structures.
Therefore, an accurate evaluation of the initial stiffness of
columns becomes an inevitable requirement.
Literature reviews show that there is a considerable
amount of uncertainty regarding the estimation of the
initial stiffness of columns when subjected to seismic
loads. Current design codes often employ a stiffness
reduction factor to deal with this uncertainty. In an
attempt to address these uncertainties, the study
presented within this paper is devoted to developing a
rational method to determine the initial stiffness of RC
columns when subjected to seismic loads. A
comprehensive parametric study based on the proposed
Advances in Structural Engineering Vol. 15 No. 2 2012 265
Initial Stiffness of Reinforced Concrete Columns with
Moderate Aspect Ratios
Cao Thanh Ngoc Tran1 and Bing Li2,*
1Department of Civil Engineering, International University, Vietnam National University, Ho Chi Minh City, Vietnam
2School of Civil and Environment Engineering, Nanyang Technological University, Singapore 639798
(Received: 1 December 2010; Received revised form: 17 May 2011; Accepted: 4 June 2011)
Abstract: The estimation of the initial stiffness of columns subjected to seismic
loadings has long been a matter of considerable uncertainty. This paper reports a study
that is devoted to addressing this uncertainty by developing a rational method to
determine the initial stiffness of RC columns when subjected to seismic loads. A
comprehensive parametric study based on a proposed method is initially carried out to
investigate the influences of several critical parameters. A simple equation is then
proposed to estimate the initial stiffness of RC columns. The applicability and
accuracy of the proposed method and equation are then verified with the experimental
data obtained from literature studies.
Key words: reinforced concrete, column initial stiffness, stiffness ratio.
method was carried out to investigate the influences of
several critical parameters. A simple equation to estimate
the initial stiffness of RC columns is also proposed
within this paper. The applicability and accuracy of the
proposed method and equation are then verified with the
experimental data obtained from the literature.
2. DEFINING INITIAL STIFFNESS OF RC
COLUMNS
There are two methods as illustrated in Figure 1(a) that are
commonly utilized to determine the initial stiffness of RC
columns (Ki). In the first method, the initial stiffness of RC
columns are estimated by using the secant of the shear
force versus lateral displacement relationship passing
through the point at which the applied force reaches 75%
of the flexural strength (0.75 Vu). In the second method,
the column is loaded until either the first yield occurs in
the longitudinal reinforcement or the maximum
compressive strain of concrete reaches 0.002 at a critical
section of the column. This corresponds to point A in
Figure 1(a). Generally, the two approaches give similar
values. In this study, the later approach was adopted.
*Corresponding author. Email address: cbli@ntu.edu.sg; Tel: +65-6790-5292.
Associate Editor: J.G. Dai.
However, the above mentioned definition cannot be
used for columns whose shear strengths do not
substantially exceed its theoretical yield force. For these
columns, defined as those whose maximum measured
shear force was less than 107% of the theoretical yield
force, the effective stiffness was defined based on a
point on the measured force-displacement envelope
with a shear force equal to 0.8 Vmax as illustrated in
Figure 1(b) (Elwood et al. 2009).
Assuming the column is fixed against rotation at both
ends and has a linear variation in curvature over the
height of the column, the measured effective moment of
inertia can be determined as:
(1)I L K
Ee
i
c
=
3
12
The stiffness ratio (κ) is defined as follows:
(2)
where Ig is the moment of inertia of the gross section; Ki
is the initial stiffness of columns and L is the height of
columns and Ec is the elastic modulus of concrete.
3. REVIEW OF EXISTING INITIAL
STIFFNESS MODELS
3.1. ACI 318-08 (2008)
ACI 318-08 (2008) recommends the following options
for estimating member stiffness for the determination of
lateral deflection of building systems subjected to
factored lateral loads: (a) 0.35 EIg for members with an
axial load ratio of less than 0.10 and 0.70 EIg for
members with an axial load ratio of more than or equal
to 0.10; or (b) 0.50 EIg for all members.
3.2. FEMA 356 (2000)
FEMA 356 (2000) suggests the variation of effective
stiffness values with the applied axial load ratio. The
effective stiffness is taken as 0.50 EIg for members with an
axial load ratio of less than 0.30, while a value of 0.7 EIg
is adopted for members with an axial load ratio of more
than 0.50. This value varies linearly for intermediate axial
load ratios as illustrated in Figure 2.
3.3. ASCE 41 (2007)
As shown in Figure 2, ASCE 41 (2007) recommends that
the effective stiffness is taken as 0.30 EIg for members
κ = ×I
I
e
g
100%
266 Advances in Structural Engineering Vol. 15 No. 2 2012
Initial Stiffness of Reinforced Concrete Columns with Moderate Aspect Ratios
(a)
A' A
Initial stiffness
Sh
ea
r f
or
ce 0.75
Vu
Vu
Vy
Lateral displacement
(b) (Elwood et al. 2009)
Initial stiffness
A
Vu
Sh
ea
r f
or
ce
0.80
Vmax
Vy
Lateral displacement
Figure 1. Methods to determine initial stiffness
0
− 0.1 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7
0.2
0.4
0.6
0.8
1
Axial load ratio f 'c Ag
St
iff
ne
ss
ra
tio
k
(%
)
ACI 318-0.8 (a)
ACI 318-0.8 (b)
FEMA 356
ASCE 41
PP92
EE09
Figure 2. Relationships between stiffness ratio and axial load ratio
of existing models
with an axial load ratio of less than 0.10, as 0.7 EIg for
members with an axial load ratio of more than 0.50 and
varies linearly for intermediate axial load ratios.
3.4. Paulay and Priestley (1992)
According to Paulay and Priestley’s recommendation
(1992), the effective stiffness is taken as 0.40 EIg for
members with an axial load ratio of less than −0.05, as
0.8 EIg for members with an axial load ratio of more
than 0.50 and varies linearly for intermediate axial load
ratios as illustrated in Figure 2.
3.5. Elwood and Eberhard (2009)
Elwood and Eberhard (2009) recommend the following
equation for estimating the initial stiffness of reinforced
concrete columns subjected to seismic loading:
(3)
where db is the diameter of longitudinal reinforcing
bars; a is the shear span and h is the column depth; Ag is
the gross sectional area of columns and f′c is the
compressive strength of concrete.
Figure 2 illustrates the variation of stiffness ratio
based on Elwood and Eberhard’s model (2009) versus
k
P A f
d
h
h
a
g c
b
=
+ ′
+
≤ ≥
0 45 2 5
1 110
1 0
. . /
.and 22
the axial load ratio for specimens with db and a equal to
25 mm and 850 mm respectively.
4. EXPERIMENTAL INVESTIGATION ON
INITIAL STIFFNESS OF RC COLUMNS
In this section, the experimental results obtained from
testing of six RC columns conducted by Tran et al. (2009)
are briefly discussed with respect to the initial stiffness of
the test specimens. Four column axial loads of 0.05, 0.20,
0.35, 0.50 f′c Ag and two aspect ratios of 1.71 and 2.43
were investigated in this experimental program. Table 1
summarizes all the details of the test specimens. It is to be
noted that only a brief summary of important test features
that are relevant to this study are presented within this
paper. Detailed information has been documented in
another publication (Tran et al. 2009).
The relationships between initial stiffness and the
column axial load ratio obtained from all the test
specimens are tabulated in Table 2. The initial stiffness of
SC-1.7 Series specimens enhanced by around 9.8%,
17.6%, and 40.4% as the column axial load was increased
from 0.05 to 0.20, 0.35, and 0.50 f′cAg, respectively. An
analogous trend was observed in the specimens of RC-1.7
Series, whose initial stiffness experienced an
enhancement of around 33.9%, 64.3% and 86.1% with an
increase in the column axial load from 0.05 to 0.20, 0.35
and 0.50 f′cAg, respectively. As compared to Specimen
SC-2.4-0.20, Specimen SC-2.4-0.50 experienced an
Advances in Structural Engineering Vol. 15 No. 2 2012 267
Cao Thanh Ngoc Tran and Bing Li
P
f Ac g'
Table 1. Summary of test specimens (Tran et al. 2009)
Longitudinal Transverse L
Specimen reinforcement reinforcement (MPa) (mm × mm) (mm)
SC-2.4-0.20 0.20
SC-2.4-0.50 1700 0.50
SC-1.7-0.05 8-T20 2-R6 @ 125 0.05
SC-1.7-0.20 ρl = 2.05% ρv = 0.13% 25.0 350 × 350 0.20
SC-1.7-0.35 1200 0.35
SC-1.7-0.50 0.50
′fc
b h××
Table 2. Experimental verification of the proposed method
Specimen (kN/mm)
SC-2.4-0.20 12.9 0.782 0.254 0.355 0.355 0.444 0.305 0.793
SC-2.4-0.50 15.5 0.572 0.301 0.421 0.301 0.301 0.263 0.525
SC-1.7-0.05 24.5 0.918 0.319 0.223 0.223 0.372 0.236 0.560
SC-1.7-0.20 26.9 0.865 0.169 0.236 0.236 0.295 0.203 0.590
SC-1.7-0.35 28.8 0.653 0.188 0.263 0.239 0.239 0.190 0.553
SC-1.7-0.50 34.4 0.620 0.220 0.308 0.220 0.220 0.193 0.507
Mean 0.735 0.242 0.301 0.262 0.312 0.232 0.588
Coefficient of Variation 0.141 0.060 0.076 0.054 0.084 0.046 0.104
K
K
i
i EE
−−
−−
expK
K
i
i PP
−−
−−
expK
K
i
i ASCE
−−
−−
expK
K
i
i FEMA
−−exp
−
K
K
i
i ACI b
−−
−−
exp
( )
K
K
i
i ACI a
−−
−−
exp
( )
K
K
i
p
−−
−−
exp
iKi−−exp
increase in the initial stiffness of 20.2%. The
aforementioned discussion clearly indicated that column
axial load was beneficial to the initial stiffness of test
specimens.
The initial stiffness of Specimens SC-2.4-0.20, SC-1.7-
0.20, SC-2.4-0.50 and SC-1.7-0.50 obtained from the tests
were 12.9 kN/mm, 26.9 kN/mm, 15.5 kN/mm and 34.4
kN/mm respectively. The increase in the initial stiffness
when comparing between Specimens SC-1.7-0.20 and
SC-2.4-0.20 was 108.5%. Similarly, an enhancement in
the initial stiffenss of 121.9% was observed in Specimen
SC-1.7-0.50 as compared to Specimen SC-2.4-0.50.
The initial stiffness of test columns calculated based
on ACI 318-2008 (2008), FEMA 356 (2000), ASCE 41
(2007), Paulay and Priestley (1992), and Elwood and
Eberhard (2009) are also all tabulated in Table 2. All
these models tend to overestimate the initial stiffness of
the test columns. Amongst all of these existing models,
Elwood and Eberhard (2009) provides the best mean
ratio of the experimental to predicted initial stiffness.
However none of these models are accurate.
5. PROPOSED METHOD
5.1. Yield Force (Vy)
The initial stiffness of columns is determined by
applying the second method as described in the previous
section. The yield force (Vy) corresponding to point A in
Figure 1(a) is obtained from the yield moment (My)
when the reinforcing bar closest to the tension edge of
columns has reached its yield strain. Moment-curvature
analysis is adopted to determine this moment.
5.2. Displacement at Yield Force (∆′y)
The displacement of a column at yield force (Vy) can be
considered as the sum of the displacement due to
flexure, bar slip and shear.
(4)
where ∆′y is the displacement of a column at yield force;
∆′flex is the displacement due to flexure and bar slip at
yield force; and ∆′shear is the displacement due to shear
at yield force
5.2.1. Flexure deformations (∆′flex)
In this proposed method, the simplified concept of an
effective length of the member suggested by Priestley et
al. (1996) was used to account for the displacement due
to bar slip in flexure deformations. Assuming a linear
variation in curvature over the height of the column, the
contribution of flexural deformations and bar slips to the
displacement at the yield force for RC columns with a
fixed condition at both ends can be estimated as follows:
′ = ′ + ′∆ ∆ ∆y flex shear
(5)
where φ′y is the curvature at the yield force determined
by using moment-curvature analysis and L is the clear
height of columns.
The strain penetration length (Lsp) is given by:
(6)
where fyl is the yield strength of longitudinal reinforcing
bars; and db is the diameter of longitudinal reinforcing
bars.
5.2.2. Shear deformations (∆′shear)
The idea of utilizing the truss analogy to model cracked
RC elements has been around for many years. The truss
analogy is a discrete modeling of actual stress fields
within RC members. The complex stress fields within
structural components resulting from applied external
forces are simplified into discrete compressive and
tensile load paths. The analogy utilizes the general idea
of concrete in compression and steel reinforcement in
tension. The longitudinal reinforcement in a beam or
column represents the tensile chord of a truss while the
concrete in the flexural compression zone is considered
as part of the longitudinal compressive chord. The
transverse reinforcement serves as ties holding
the longitudinal chords together. The diagonal concrete
compression struts, which discretely simulate the
concrete compressive stress field, are connected to
the ties and longitudinal chords at rigid nodes to attain
static equilibrium within the truss. The truss analogy is
a very promising way to treat shear because it provides a
visible representation of how forces are transferred in a
RC members under an applied shear force.
Park and Paulay (1975) derived a method to
determine the shear stiffness by applying the truss
analogy for short or deep rectangular beams of unit
length. The shear stiffness is the magnitude of the shear
force, when applied to a beam of unit length that will
cause unit shear displacement at one end of the beam
relative to the other. This model is reliable in estimating
shear deformations of short or deep beams in which the
influences of flexure are negligible. The behaviors of
RC columns under seismic loading are much more
complex because of the interaction between shear and
flexure. The influences of axial strain due to flexure in
estimating shear deformations of RC columns should be
considered to accurately predict the initial stiffness of
RC columns. By applying a method that is similar to
Park and Paulay’s analogous truss model (1975), the
L f dsp yl b= 0 022.
′ =
′ +( )
∆ flex
y spL Lφ 2
6
2
268 Advances in Structural Engineering Vol. 15 No. 2 2012
Initial Stiffness of Reinforced Concrete Columns with Moderate Aspect Ratios
shear stiffness of RC columns is derived in this part of
the paper. The effects of flexure in shear deformations
are incorporated in the proposed model through the axial
strains at the center of columns (εy,CL).
Assuming that transverse reinforcing bars start
resisting the applied shear force when the shear cracking
starts occurring, the stress in transverse reinforcing bars
at the yield force is calculated as:
(7)
where d is the distance from the extreme compression
fiber to centroid of tension reinforcement; s is the
spacing of transverse reinforcement; Ast is the total
transverse steel area within spacing s; and θ is the angle
of diagonal compression strut. Hence the strain in
transverse reinforcing bars is:
(8)
where εyt is the yield strain of transverse reinforcing
bars; Es is the elastic modulus of steel.
Similar to Park and Paulay’s model (1975), the
concrete compression stress at the yield force is given as:
(9)
where b is the width of columns; Lcs = d sinθ is the
effective depth of the diagonal strut as shown in Figure 3.
Hence the strain in the concrete compression strut is
given as:
f V
bL
y
cs
2 =
cosθ
ε εx
sy
s
yt
f
E
= ≤
f V V s
A dsy
y cr
st
=
−( )
tanθ
(10)
where Ec is the elastic modulus of concrete given as:
(11)
Based on Vecchio and Collins’s model (1986), the
effective compressive strength of concrete is calculated
as follows:
(12)
By applying Mohr’s circle transformation for the
mean strains at the center of Section C-C as shown in
Figure 4, it gives:
(13)
(14)
(15)
For the axial mean strains, compatibility requires that
the plain sections remain plane. Hence the mean strain
at the center of section C-C is given as:
(16)
where εy, top, εy, bot are the axial strains at the extreme
tension and compression fibers, respectively as shown
in Figure 4(b).
There are six variables, namely εx , εy,CL, γxy, ε1, ε2
and θ; and six independent Eqns 8, 10, 13, 14, 15 and
16. By solving these six independent equations, the
shear strain (γxy) at the center of section C-C could be
determined.
The column is divided into several segments along its
height of the column to determine the total shear
deformation at the top of the column. The mean axial
strain at the center of the section is determined based on
ε
ε ε
y CL
y top y bot
,
, ,=
+
2
tan
,
2θ
γ
ε ε
=
−
xy
x y CL
ε
ε ε ε ε γ
2
2 2
2 2 2
=
+
−
−
+
x y CL x y CL xy, ,
ε
ε ε ε ε γ
1
2 2
2 2 2
=
+
+
−
+
x y CL x y CL xy, ,
f f fce c c= + ≤
'
'
.0 8 170 1ε
E fc c= 5000
ε2 2=
f
Ec
Advances in Structural Engineering Vol. 15 No. 2 2012 269
Cao Thanh Ngoc Tran and Bing Li
Diagonal strut
LCS
d
θθ
Figure 3. Diagonal strut of RC columns (Park and Paulay1975)
the moment-curvature analysis. The shear strains at the
lower and upper section of the segment are calculated
using the above equations. Hence, the total shear
displacement caused by the yield force can be calculated
as follows:
(17)
where γ ixy and γ xyi+1 are the shear strains at the lower and
upper section of the segment i; hi is the height of
segment i and n is the number of segments.
5.3. Initial Stiffness
Once the flexural and shear deformations at the top of
columns under yield force are obtained, the initial
stiffness of columns can be determined as:
(18)
6. VALIDATION OF THE PROPOSED
METHOD
The proposed method is validated by comparing its
results to the initial stiffness of six columns obtained
from the experimental study previously conducted by
Tran et al. (2009).
It was found that the average ratio of experimental
to predicted initial stiffness by the proposed method
was 0.735 as tabulated in Table 2. It shows a relatively
good correlation between the analytical and
K
V
i
y
flex shear
=
′ + ′∆ ∆
′ =
+
+
=
∑∆shear xy
i
xy
i
i
i
n
h
γ γ 1
1 2
experimental results. The initial stiffness of the tested
columns calculated based on ACI 318-2008 (2008),
FEMA 356 (2000), ASCE 41 (2007), Paulay and
Priestley (1992), and Elwood and Eberhard (2009) are
also tabulated in Table 2. The mean ratio of the
experimental to predicted initial stiffness and its
coefficient of variation were 0.242 and 0.060, 0.301
and 0.076, 0.262 and 0.054, 0.312 and 0.084, 0.232
and 0.046, and 0.588 and 0.104 for ACI 318-2008
(2008a), ACI 318-2008 (2008b), FEMA 356 (2000),
ASCE 41 (2007), Paulay and Priestley (1992), and
Elwood and Eberhard (2009) respectively. Comparison
of available models with experimental data indicated
that the proposed method produced a better mean ratio
of the experimental to predicted initial stiffness than
other models. The proposed method may be suitable as
an assessment tool to calculate the initial stiffness of
RC columns.
7. PARAMETRIC STUDIES
A parametric study conducted to improve the
understanding of the effects of various parameters on
the initial stiffness of RC columns is presented within
this section. The parameters investigated are transverse
reinforcement ratios (ρv), longitudinal reinforcement
ratios (ρl), yield strength of longitudinal reinforcing
bars (fyl), concrete compressive strength (f′c), aspect
r
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