New formulation for compressive strength of CFRP confined concrete cylinders using linear genetic...
Transcript of New formulation for compressive strength of CFRP confined concrete cylinders using linear genetic...
ORIGINAL ARTICLE
New formulation for compressive strength of CFRP confinedconcrete cylinders using linear genetic programming
Amir Hossein Gandomi • Amir Hossein Alavi •
Mohammad Ghasem Sahab
Received: 12 January 2009 / Accepted: 14 October 2009 / Published online: 30 October 2009
� RILEM 2009
Abstract This paper proposes a new approach for
the formulation of compressive strength of carbon
fiber reinforced plastic (CFRP) confined concrete
cylinders using a promising variant of genetic
programming (GP) namely, linear genetic program-
ming (LGP). The LGP-based models are constructed
using two different sets of input data. The first set of
inputs comprises diameter of concrete cylinder,
unconfined concrete strength, tensile strength of
CFRP laminate and total thickness of utilized CFRP
layers. The second set includes unconfined concrete
strength and ultimate confinement pressure which are
the most widely used parameters in the CFRP
confinement existing models. The models are devel-
oped based on experimental results collected from the
available literature. The results demonstrate that the
LGP-based formulas are able to predict the ultimate
compressive strength of concrete cylinders with an
acceptable level of accuracy. The LGP results are
also compared with several CFRP confinement
models presented in the literature and found to be
more accurate in nearly all of the cases. Moreover,
the formulas evolved by LGP are quite short and
simple and seem to be practical for use. A subsequent
parametric study is also carried out and the trends of
the results have been confirmed via some previous
laboratory studies.
Keywords CFRP confinement �Linear genetic programming � Formulation �Concrete compressive strength
1 Introduction
Concrete as a frictional material is considerably
sensitive to hydrostatic pressure. Lateral stresses have
advantageous effects on the concrete strength and
deformation. This means when concrete is uniaxially
loaded and can not dilate laterally, it exhibits
increased strength and axial deformation capacity
indicated as confinement. Concrete confinement can
be generally provided through transverse reinforce-
ment in the form of spirals, circular hoops or
rectangular ties, or by encasing the concrete columns
into steel tubes that act as permanent formwork [1].
Fiber reinforced polymers (FRPs) are also employed
for confinement of concrete columns. Compared to
A. H. Gandomi (&)
The Highest Prestige Scientific and Professional National
Foundation, National Elites Foundation, Tehran, Iran
e-mail: [email protected]
A. H. Alavi
College of Civil Engineering, Iran University of Science
& Technology (IUST), Tehran, Iran
e-mail: [email protected]
M. G. Sahab
College of Civil Engineering, Tafresh University, Tafresh,
Iran
e-mail: [email protected]
Materials and Structures (2010) 43:963–983
DOI 10.1617/s11527-009-9559-y
steel [2], FRPs present several advantages such as
continuous confining action to the entire cross-
section, easiness and speed of application, no change
in the shape and size of the strengthened elements
and corrosive resistance [1]. Typical response of
FRP-confined concrete is shown in Fig. 1, where
normalized axial stress is plotted against axial,
lateral, and volumetric strains. The stress is normal-
ized with respect to the unconfined strength of
concrete core. The figure shows that both axial and
lateral responses are bi-linear with a transition zone at
or near the peak strength of unconfined concrete core.
The volumetric response shows a similar transition
toward volume expansion. However, as soon as the
jacket takes over, volumetric response undergoes
another transition which reverses the dilation trend
and results in volume compaction. This behavior is
shown to be remarkably different from plain concrete
and steel-confined concrete [3]. Carbon fiber rein-
forced plastic (CFRP) is one of the main types of FRP
composites. The advantages of CFRP comprise anti-
corrosion, easy cutting and construction, as well as
high strength to weight ratio and high elastic
modulus. These features caused widely using of
CFRP in the retrofitting and strengthening of rein-
forced concrete structures as one of the most
successfully transferred technologies to the civil
engineering industry for over 50 years. The illustra-
tive figure of CFRP confining concrete cylinder can
be seen in Fig. 2.
Several investigations have been conducted about
the effect of CFRP confinement on the strength and
deformation capacity of concrete columns. On the
basis of these researches, a number of empirical and
theoretical models are proposed [1]. In spite of the
extensive research in this field, there are some
significant limitations such as specific loading system
and conditions and the need for calibration of several
involving parameters on the application of these
empirical models. These limitations, suggest the
necessity of developing more comprehensive math-
ematical models for assessing the behaviour of CFRP
confined concrete columns.
Genetic programming (GP) [4, 5] is a developing
subarea of evolutionary algorithms inspired from
Darwin’s evolution theory. GP may generally be defined
as a supervised machine learning technique that
searches a program space instead of a data space [5].
Fig. 1 Typical response of
FRP-confined concrete [3]
Fig. 2 The illustrative figure of CFRP confining concrete
cylinder
964 Materials and Structures (2010) 43:963–983
In recent years, a particular subset of GP with a linear
structure similar to the DNA molecule in biological
genomes namely, linear genetic programming (LGP)
[6] has emerged. LGP is a machine learning approach
that evolves the programs of an imperative language
or machine language instead of the traditional tree-
based GP [4] expressions of a functional program-
ming language. LGP has significant advantages over
other modeling approaches [6, 7]. There has been just
some little scientific effort directed at applying LGP
to civil engineering tasks such as behavior appraisal
of steel semi-rigid joints [8], performance character-
istics modeling of stabilized soil [9], and soil
liquefaction assessment [10].
The main purpose of this paper is to utilize the LGP
technique to obtain formulas for the determination of
compressive strength of CFRP wrapped concrete
cylinders. A comparison between the proposed
formulations results, as well as 15 existing models
found in the literature, is performed. A reliable
database including previously published compressive
strength of CFRP wrapped concrete cylinder test
results is utilized to develop generic models.
2 Review of previous studies
The characteristic response of confined concrete
includes three distinct regions of un-cracked elastic
deformations, crack formation and propagation, and
plastic deformations. It is generally assumed that
concrete behaves like an elastic-perfectly plastic
material after reaching its maximum strength capac-
ity, and that the failure surface is fixed in the stress
space. Constitutive models for concrete should be
concerned with pressure sensitivity, path dependence,
Table 1 Different models for strength enhancement of FRP confined concrete cylinders
ID Authors Expression
1 Fardis and Khalili [18]f 0cc
f 0co¼ 1þ 3:7 pu
f 0co
� �0:85
2 Mander et al. [19]f 0cc
f 0co¼ 2:254
ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi1þ 7:94pu
f 0co
q� 2pu
f 0co� 1:254
3 Miyauchi et al. [11]f 0cc
f 0co¼ 1þ 3:485 pu
f 0co
� �
4 Kono et al. [12]f 0cc
f 0co¼ 1þ 0:0572Pu
5 Samaan et al. [20]f 0cc
f 0co¼ 1þ 0:6p0:7
u
6 Lam and Teng [21]f 0cc
f 0co¼ 1þ 2 pu
f 0co
� �
7 Toutanji [22]f 0cc
f 0co¼ 1þ 3:5 pu
f 0co
� �0:85
8 Saafi et al. [23]f 0cc
f 0co¼ 1þ 2:2 pu
f 0co
� �0:84
9 Spoelstra and Monti [24]f 0cc
f 0co¼ 0:2þ 3
ffiffiffiffipu
f 0co
q
10 Karbhari and Gao [25]f 0cc
f 0co¼ 1þ 2:1 pu
f 0co
� �0:87
11 Richart et al. [26]f 0cc
f 0co¼ 1þ 4:1 pu
f 0co
� �
12 Berthet et al. [27]
f 0cc
f 0co
¼ 1þ K1
pu
f 0co
� �;
K1 ¼ 3:45 20� f 0co� 50 MPa
K1 ¼ 0:95 f 0co
� ��1=450 � f 0co� 200 MPa
(
13 Vintzileou and Panagiotidou [28]f 0cc
f 0co¼ 1þ 2:8 pu
f 0co
� �
14 Xiao and Wu [29]f 0cc
f 0co¼ 1:1þ 4:1� 0:75
f 02co
El
� �pu
f 0co
15 Li et al. (L-L Model) [30]f 0cc
f 0co¼ 1þ tan 45� � /
2
� �pu
f 0co
� �
/ ¼ 36� þ 1�f 0co
35
� �� 45�
f0co: Compressive strength of unconfined concrete cylinder; f0cc: Ultimate compressive strength of confined concrete cylinder; Pu:
Ultimate confinement pressure Pu ¼ El:ef ¼2t:f 0f
D
� �; El: Lateral modulus; ef: Ultimate tensile strain of FRP laminate; f0f: Ultimate
tensile strength of FRP layer; t: Thickness of FRP layer; D: Diameter of concrete cylinder
Materials and Structures (2010) 43:963–983 965
stiffness degradation and cyclic response. The exist-
ing plasticity models range from nonlinear elasticity,
endochronic plasticity, classical plasticity, and multi-
laminate or micro-plane plasticity to bounding surface
plasticity. Many of these models, however, are only
suitable in a specific application and loading system
for which they are devised and may give unrealistic
results in other cases. Also, some of these models
require several parameters to be calibrated based on
experimental results [3]. Considerable experimental
research has been performed on the behavior of CFRP
confined concrete columns [11–17]. Numerous stud-
ies have concentrated on assessing the strength
enhancement of CFRP wrapped concrete cylinders
in the literature. Some of the most important models in
this field (Eqs. 1 to 15) have been shown in Table 1.
Cevik and Guzelbey [31] presented an application
of neural networks (NN) for the modeling of
compressive strength of CFRP confined concrete
cylinders. Moreover, they obtained the explicit for-
mulation of the compressive strength using the NN
model with 4 neurons in input layer and 15 neurons in
middle layer. Since some of the models in the
literature such as the second formula of Karbhari and
Gao [25] and the modified L-L model [30] require
additional details, they are not used in the compar-
ative study. In recent decade, different models for the
compressive strength of concrete cylinders after FRP
confinement have been proposed [27–31]. The rela-
tive differences between the general forms of the
recently proposed models [27, 29–31] and the older
ones pursue one to challenge for obtaining more
accurate models with newer general forms.
3 Genetic programming
GP is one of the branches of evolutionary algorithms
(EA) that creates computer programs to solve a
problem using the principle of Darwinian natural
selection [32]. GP was introduced by Koza [4] as an
extension of the genetic algorithms, in which pro-
grams are represented as tree structures and expressed
in the functional programming language LISP [4]. GP
has successfully been applied to various kinds of the
civil engineering problems [33–37]. A comprehen-
sive description of GP can be found in Refs. [4]
and [5].
3.1 Linear genetic programming
LGP is a subset of GP that has emerged recently.
Comparing LGP to the traditional Koza’s tree-based
GP, there are some main differences. Linear genetic
programs (LGPs) have graph-based functional struc-
tures and evolve in an imperative programming
language C/C?? [38] and machine code [39] rather
than in expressions of a functional programming
language like LISP [40]. Unlike tree-based GP,
structurally noneffective codes coexist with effective
codes in LGPs.
Noneffective code in genetic programs which is
referred to as ‘‘intron’’, represents instructions
without any influence on the program behavior.
Structural introns act as a protection that reduces the
effect of variation on the effective code. The introns
allow variations to remain neutral in terms of fitness
change [6]. Because of the imperative program
structure in LGP, these noneffective instructions can
be identified efficiently. This allows the correspond-
ing effective instructions to be extracted from a
program during runtime. Since, only effective pro-
grams are executed, evaluation can be accelerated
significantly (see Fig. 3).
The instructions from imperative languages are
restricted to operations that accept a minimum
number of constants or memory variables, called
Fig. 3 Elimination of
noneffective code in LGP.
Only effective programs are
executed [6]
966 Materials and Structures (2010) 43:963–983
registers (r), and assign the result to a destination
register, e.g., r0: = r1 ? 1. A part of a linear genetic
program in C code is represented as follows [6]:
void LGP (double r[5])
{…r[0] = r[5] ? 70;
r[5] = r[0] - 50;
if (r[1] [ 0)
if (r[5] [ 2)
r[4] = r[2] * r[1];
r[2] = r[5] ? r[4];
r[0] = sin(r[2]);
}
where register r[0] holds the final program output.
LGPs can be converted into a functional representa-
tion by successive replacements of variables starting
with the last effective instruction [7]. Automatic
Induction of Machine code by Genetic Programming
(AIMGP) is a particular form of LGP. AIMGP
induces binary machine code directly without any
interpreting steps that results in a significant speedup
in execution compared to interpreting GP systems.
This LGP approach searches for the computer
program and the constants at the same time. The
evolved program is a sequence of binary machine
instructions [39].
The machine-code-based, LGP uses the following
steps to evolve a computer program that predicts the
target output from a data file of inputs and outputs
[6]:
I. Initializing a population of randomly generated
programs.
II. Running a Tournament. In this step four programs
are selected from the population randomly. They
are compared and based on fitness, two programs
are picked as the winners and two as the losers.
III. Transforming the winner programs. After that,
two winner programs are copied and transformed
probabilistically as follows:
• Parts of the winner programs are exchanged with
each other to create two new programs (cross-
over); and/or
• Each of the tournament winners are changed
randomly to create two new programs (mutation).
IV. Replacing the loser programs in the tournament
with the transformed winner programs. The
winners of the tournament remain without
change.
V. Repeating steps two through four until conver-
gence. A program defines the output of the
algorithm that simulates the behavior of the
problem to an arbitrary degree of accuracy.
A brief description of basic parameters, used to
direct the search for a linear genetic program, is
explained below.
3.1.1 Population size
The number of programs in the population that LGP
will evolve are set by the population size. The proper
population size depends on the number of possible
solutions and complexity of the problem.
3.1.2 Crossover
Crossover transforms programs in the population and
exchanges sequences of instructions between two
tournament winners. Two offsprings are the outcomes
of this exchange that are inserted in place of the
loser programs in the tournament. Crossover occurs
between instruction blocks and it can be either
homologous or non-homologous. Reproducing natu-
ral evolution is more closely in homologous cross-
over as a novel approach than traditional crossover.
Figure 4 demonstrates the two-point linear cross-
over used in LGP for recombining two tournament
winners. As shown, a segment of random position and
arbitrary length is selected in each of the two parents
and exchanged. If one of the two children would
exceed the maximum length, crossover is aborted and
restarted with exchanging equally sized segments [6].
Fig. 4 Crossover in LGP [6]
Materials and Structures (2010) 43:963–983 967
3.1.3 Mutation
The mutation operator is used to transform some
randomly selected programs with a small mutation
probability to prevent premature convergence. Three
different types of mutation in LGP are block muta-
tion, instruction mutation and data mutation.
3.1.4 Demes
Based on the EA, the population of individual
solutions may be subdivided into multiple subpopu-
lations that migration of individuals among these
subpopulations causes evolution to occur in the
population. This mechanism was described by biol-
ogists as the island model. Demes are semi-isolated
subpopulations that in comparison to a single popu-
lation of equal size, evolution proceeds faster in
them. The percentage of individuals allowed to
migrate from a deme into another deme during each
generation is limited. Demes are widely used in the
field of EA and GP. The number of them is related to
the way that the population of programs is divided.
3.1.5 Fitness function
The fitness function is a criterion for the evaluation of
the goodness of each individual computer program.
The fitness values are used to determine which
evolved programs survive and reproduce. To evaluate
the fitness of an evolved program, the average of the
squared raw errors is calculated.
3.1.6 Function and terminal sets
The Function and terminal sets are important param-
eters of LGP. The function set for a run may include
the operators such as addition, subtraction, square
root, absolute value and logarithm while the terminal
set comprises of the variables and constants of the
evolving programs.
4 Model development
The main objective of this paper is to explore the
feasibility of using the LGP approach for the
formulation of compressive strength (f0cc) of CFRP
confined concrete cylinders. An experimental
database has been gathered for strength enhancement
of CFRP wrapped concrete cylinders from the
literature. The database contains 101 specimens
obtained from seven separate studies. The complete
list of the data is presented in Table 6 of the
Appendix. The ranges of different input and output
parameters involved in the model development are
given in Table 2.
For the analysis, the data sets are divided into
training and testing subsets (10 data sets were used
for testing and the rest for training). For the LGP-
based models, a computer software called Discipulus
[41] is used. This software works on the basis of the
AIMGP approach. Two LGP-based models (Model I
and Model II) are considered for the assessment of
compressive strength using two different sets of input
data. For each models of I and II, two formulas of
compressive strength of the confined concrete cylin-
der have been obtained. The first function set consists
of nearly all functions (addition, subtraction, division,
multiplication, square root, sine, cosine and tangent)
and the other includes just addition, subtraction,
division, and multiplication in order to obtain short
and very simple formulas. In addition to the men-
tioned function sets, logarithmic function has also
been considered in the LGP predictive models. Since
the best obtained formula considering this form of
function was complex and inaccurate, it has not been
presented here.
The details of developing Model I and Model II
are discussed in the following subsections. Various
LGP involved parameters are population size, muta-
tion type and rate (block mutation rate, instruction
mutation rate, and data mutation rate), crossover type
and rate, function set, number of demes and program
size. The parameter selection will affect the gener-
alization capability of the LGP-based models. For the
development of models, the LGP parameters are
selected based on some previously suggested values
[42] and also after a trial and error approach. The
parameter settings are shown in Table 3. In order to
evaluate the capabilities of the LGP models, the
correlation coefficient (R) and mean absolute percent
error (MAPE) are used.
4.1 Development of Model I
The existing FRP confinement models take into
account the unconfined compressive strength and the
968 Materials and Structures (2010) 43:963–983
ultimate confinement pressure as the main influencing
parameters. The main goal of developing Model I is
to obtain the explicit formulation of the ultimate
strength of concrete cylinders after CFRP confine-
ment (f0cc) by considering the influencing variables
given as follows:
f 0cc ¼ f D; t; f 0f ; f0co
� �ð16Þ
The four input variables to build the model are
listed below:
• diameter of the concrete cylinder (D)
• thickness of the CFRP layer (t)
• ultimate tensile strength of the CFRP laminate
(f0f)• unconfined ultimate concrete strength (f0co)
The first two inputs are geometrical parameters
(Fig. 5) and others are mechanical properties. The
database, presented in Table 6, is used to build Model
I. All specimens used in the database have a length
(L) to diameter (D) ratio of 2. The parameter settings
of Model I are shown in Table 3.
4.1.1 Explicit formulation of compressive strength,
Model I
Formulation of f0cc in terms of the independent
variables, D, t, f0f and f0co, for the best results by the
LGP algorithm are as given below:
f 0cc;I:1 ðMPaÞ ¼ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi2 cos f 0f :t: sin
sin2ðcos2ðf 0co þ D:t=2ÞÞ2
þ 3f 0co
2þ t
� �� �sþ f 0co
ð17Þ
f 0cc;I:2 ðMPaÞ ¼ D
4011
�0:57t � D:f 0f ðð3:6f 0co � 58:7tÞ
�10�8Þ4 þ 11:6 f 0co=100�
ð18Þ
The functions generated for the best results by
LGP to use in the compressive strength prediction
include the effects of all parameters. Comparisons of
the LGP predicted versus experimental compressive
strength of CFRP wrapped concrete cylinder for
Eqs. 17 and 18 are shown in Fig. 6a, b.
In order to evaluate how many times each input
parameters contributes to the fitness of the LGP
Table 2 Ranges of the
parameters in databaseParameters Range
Diameter of the concrete cylinder (mm) 100–153
Thickness of CFRP layer (mm) 0.11–5.04
Ultimate tensile strength of the CFRP laminate (MPa) 1100–3820
Unconfined ultimate concrete strength (MPa) 19.40–82.13
Ultimate confinement pressure (MPa) 3.44–38.38
Confined ultimate concrete strength (MPa) 33.8–137.9
Table 3 Parameter settings
for the LGP modelsParameter Settings
f0cc, I.1, f0cc, II.1 f0cc, I.2, f0cc, II.2
Function set ?, -, *, /, H, sin, cos, tan ?, -, *, /
Population size 10000–25000 10000–25000
Maximum program size 256 256
Initial program size 80 80
Crossover rate (%) 50, 95 50, 95
Homologous crossover (%) 95 95
Mutation rate (%) 90 90
Block mutation rate (%) 30 30
Instruction mutation rate (%) 30 30
Data mutation rate (%) 40 40
Number of demes 20 20
Materials and Structures (2010) 43:963–983 969
programs that contain them (importance of input
parameters), frequency values [43] of the input
parameters of the compressive strength predictive
model (Model I) are obtained and presented in Fig. 7.
A value of 1.00 in this figure indicates that this input
variable appeared in 100% of the best thirty programs
evolved by LGP. To obtain the frequency values, the
data sets are divided into training and testing subsets
as described above. The analysis is performed using
Discipulus software [43]. The frequency values,
presented in Fig. 7, are achieved for the best test R
values of the LGP runs. Figure 7 shows that the
frequencies of D, t, f0f and f0co are 0.15, 0.6, 0.86 and
0.85, respectively. According to these results, it can
be found that the compressive strength of CFRP
wrapped concrete cylinder is more sensitive to f0f and
f0co in comparison with the other inputs.
4.2 Development of Model II
In order to conduct a comparison between this study
and the models found in the literature, the number of
Fig. 5 Geometrical parameters of CFRP concrete cylinder
Fig. 6 Results of the LGP predicted versus experimental compressive strength: (a) Eq. 14, (b) Eq. 15
Fig. 7 Frequency values of input parameters of the compres-
sive strength predictive models (Model I)
970 Materials and Structures (2010) 43:963–983
inputs to build Model II is reduced to two para-
meters. These parameters are the most widely used
parameters in the existing FRP confinement models.
Hence, the formulation of the strength of concrete
cylinders after CFRP confinement as function of
variables will be as follows:
f 0cc ¼ f Pu; f0co
� �ð19Þ
in which the two inputs to build the models are:
• unconfined ultimate concrete strength (f0co)
• ultimate confinement pressure (Pu)
As indicated in Table 1, Pu is a function of the
diameter of the concrete cylinder (D), the thickness of
the CFRP layer (t), and the ultimate strength of the
CFRP layer (f0f) [24]. Therefore, Model II includes
the already mentioned parameters in implicit form.
The parameter settings of Model II are as shown in
Table 3.
4.2.1 Explicit formulation of compressive strength,
Model II
For Model II, f0co and Pu are considered in the
formulation process as the input parameters. The
prediction equations for the best test R values by the
LGP algorithm are given in Eqs. 20 and 21.
f 0cc;II:1 MPað Þ ¼ 7f 0co
18
40cos
ffiffiffi2p
180
ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi90 f 0co � cos 2sin
f 02co
2025
� �8 !
þ f 02co
vuut!þ Pu
!
ð20Þ
f 0cc; II:2 MPað Þ ¼ 7
180pu:f
0co þ
40 f 0co
1þ f 0co
90
� �2
0B@
1CA ð21Þ
Comparisons of the LGP predicted versus exper-
imental compressive strength of CFRP wrapped
concrete cylinder for Eqs. 20 and 21 are shown in
Fig. 8a, b.
Similar to Model I, to obtain the frequency
values, the data sets are divided into training (91
data) and testing (10 data) subsets. Frequency values
of input parameters of Model II for the best test R
values of the LGP runs are presented in Fig. 9. It
can be seen from this figure that that the frequencies
of f0co and Pu are 0.55 and 0.51, respectively.
According to these results, it can be found that
the compressive strength of CFRP wrapped concrete
cylinder is more sensitive to f0co in comparison
with Pu.
Fig. 8 Results of the LGP predicted versus experimental compressive strength: (a) Eq. 17, (b) Eq. 18
Materials and Structures (2010) 43:963–983 971
5 Comparison of CFRP confinement models
The available experimental database is used for
training and testing the LGP-based models. Four
formulas for the compressive strength are obtained
and given in Eqs. 17, 18, 20 and 21. As mentioned
previously, R and MAPE are selected as the target
error parameters to evaluate the performance of the
proposed LGP and other models. A comparison of the
ratio between the predicted compressive strength
values by LGP, the models found in the literature,
and experimental values are shown in Fig. 10a–q.
Performance statistics of the LGP-based formulas and
the other existing models are summarized in Tables 4
and 5.
Comparing the performance of the LGP-based
formulas, it can be seen that Eq. 17 has the best
performance on the training and whole of data. For
the testing data, Eq. 20 has produced better results
followed by Eqs. 17, 18 and 21. Overall perfor-
mance of the LGP models indicates that the
formulas developed using the first function set, as
presented in Table 3, have performed better than
those using the second set of functions as the input
parameters.
When comparison of the overall performance of
the LGP-based formulae with those found in the
literature is taken into consideration, it can be seen
that the best performance is obtained by the NN
model. Comparing the results of the proposed LGP
models with 15 different FRP confinement models,
the LGP-based formulas are found to be more
accurate. In this case, Eq. 4, proposed by Kono
et al. [12], has a slightly better R value than Eq. 21
of Model II. Considering the MAPE values, it can
be seen that Eq. 21 outperforms Eq. 4. In spite of
the better performance of the NN model, the
equation proposed in that study for estimating the
strength enhancement of CFRP wrapped concrete
cylinders is too complex and has long expressions.
On the other hand, the LGP prediction equations are
short and can be used for practical applications.
Details of the NN formulation are shown in
Appendix.
Besides, Eq. 18 evolved by LGP can be expressed
similar to the form of other formulas in Table 1 as
follows:
f 0cc
f 0co
¼ 7 Pu
180þ 1:5
1þ f 0co
90
� �2ð22Þ
This form of equation indicates that the ratio of
f0cc to f0co is more sensitive to Pu in comparison with
f0co. Another agreement for this debate is Eq. 4
which uses only Pu for the determination of the ratio
of f0cc to f0co (as shown in Table 1) and has produced
the best results compared to the other existing
formulas.
6 Parametric study
For further verification of the LGP models, a
parametric study is performed in this study. The
main goal is to find the effect of each parameter,
presented in Table 2, on the values of compression
strength of CFRP wrapped concrete cylinders. Fig-
ures 11a–d and 12a, b present the predicted values of
the strength of concrete cylinders after CFRP con-
finement as a function of each parameter for Model I
and Model II, respectively. The tendency of the
prediction to the variations of the geometrical
parameters (D, t), and the other mechanical properties
(f0f, f0co and Pu) can be determined according to these
figures.
The results of parametric study for Eqs. 17 and
18, presented in Fig. 11b–d, indicate that the
compressive strength continuously increases due to
increasing t, f0f and f0co and slightly decreases due to
increasing D. It is well known that, by inhibiting
lateral expansion of concrete, its strength and
ductility improve significantly [3, 44]. According
Fig. 9 Frequency values of input parameters of the compres-
sive strength predictive models (Model II)
972 Materials and Structures (2010) 43:963–983
to poisson’s effect, for a given value of axial
compression stress, applied on FRP confined con-
crete cylinders, lateral expansion changes depend
on elastic modulus and so tensile strength of
FRP materials. For this reason, there is a direct
relationship between the compressive strength of
CFRP confined concrete cylinders and the tensile
strength of CFRP materials. One can conclude from
Fig. 10 A comparison of the ratio between the predicted and the experimental f0cc values using different methods
Materials and Structures (2010) 43:963–983 973
Fig. 11a that the strength enhancement is not
sensitive to the changes in the values of D. This
can be explained according to the frequency values
for Model I, presented in Fig. 7. Figure 7 indicates
that the strength of CFRP wrapped concrete cylinder
is less sensitive to D compared to the other inputs.
Moreover, the insensitivity of compressive strength
to the changes of D may probably be due to that the
database is poor representative on the range of D.
Considering the results of parametric analysis for
Eqs. 20 and 21, as shown in Fig. 12a, b, it can be
seen that the strength of concrete cylinders after
CFRP confinement continuously increases due to
increasing f0co and Pu. The results of parametric
study are in close agreement with those reported by
other researchers [24, 27, 29, 30, 45].
7 Conclusions and future directions
In this research, a promising variant of GP namely,
LGP was employed to assess the complex behavior of
CFRP confined concrete cylinders. The main focus of
this study is to propose new formulas for determining
the compressive strength enhancement of CFRP
wrapped concrete cylinder as a function of various
influencing parameters. A reliable database including
previously published ultimate strength of concrete
cylinders after CFRP confinement test results was
used for developing the models. Four formulas
of compressive strength were obtained by means of
LGP. In order to evaluate the sensitivity of strength of
concrete cylinders due to variation of the influencing
parameters, a parametric study was also conducted.
The results of the parametric study were confirmed
with the results of experimental studies presented by
other researchers. The results indicate that the
developed correlations are robust and can be used
with confidence. The LGP formulation results were
also compared with the experimental results and
several CFRP confinement models found in the
literature. It was observed that the proposed LGP
models give reliable estimates of the ultimate
strength of concrete cylinders after CFRP confine-
ment. The results demonstrated that, in nearly all
cases, the formulas created by LGP outperform the
models found in the literature. In addition to the
Table 4 Statistical parameters of the LGP models
Models Training Testing
R MAPE R MAPE
LGP, Eq. 17 0.9392 6.62 0.8857 13.19
LGP, Eq. 18 0.9022 7.96 0.8719 13.51
LGP, Eq. 20 0.9016 7.66 0.8961 11.01
LGP, Eq. 21 0.8781 8.74 0.8646 13.43
Table 5 Overall performance of the formulas for the com-
pressive strength prediction
Model R MAPE
NN 0.982 3.02
Eq. 1 0.752 24.04
Eq. 2 0.871 18.19
Eq. 3 0.704 16.91
Eq. 4 0.884 11.34
Eq. 5 0.847 10.12
Eq. 6 0.833 11.09
Eq. 7 0.769 21.62
Eq. 8 0.851 10.11
Eq. 9 0.812 11.81
Eq. 10 0.702 16.28
Eq. 11 0.659 23.16
Eq. 12 0.854 9.8
Eq. 13 0.763 12.86
Eq. 14 0.23 29.43
Eq. 15 0.791 26.5
LGP, Eq. 17 0.929 7.27
LGP, Eq. 18 0.894 7.45
LGP, Eq. 20 0.898 7.1
LGP, Eq. 21 0.882 9.21
974 Materials and Structures (2010) 43:963–983
acceptable accuracy, the LGP-based prediction equa-
tions are quite short and simple and seem to be
practical for use.
Further research can be focused on both the
problem domain and the computing one. As more
data become available, including those for other types
of FRP, the same models can be improved to make
more accurate predictions for a wider range. Also,
more work needs to be conducted for specimens with
squared sections. LGP is quite robust in nonlinear
relationships modeling. However, the underlying
assumption that the input parameters are reliable is
not always the case. Sine fuzzy logic can provide a
systematic method to deal with imprecise and
Fig. 11 Parametric analysis of f0cc in the LGP models (Eqs. 17 and 18)
Fig. 12 Parametric analysis of f0cc in the LGP models (Eqs. 20 and 21)
Materials and Structures (2010) 43:963–983 975
incomplete information, the process of developing a
hybrid fuzzy-LGP model for such problems can be a
suitable topic for further studies.
Acknowledgment The journal reviewers are thanked for
their constructive comments that helped improve this paper.
Appendix
Details of the explicit formulation of the NN model
for the determination of strength enhancement of
CFRP wrapped concrete cylinders [31] (see Table 6):
f 0cc;NNðMPaÞ¼150� 2
1þe�2W�1
� �
W¼0:63� 2
1þe�2U1�1
� �þ0:74� 2
1þe�2U2�1
� ��3:16� 2
1þe�2U3�1
� ��2:62� 2
1þe�2U4�1
� �
�0:68� 2
1þe�2U5�1
� �þ1:16� 2
1þe�2U6�1
� ��1:36� 2
1þe�2U7�1
� �þ0:61� 2
1þe�2U8�1
� �
þ0:83� 2
1þe�2U9�1
� ��0:52� 2
1þe�2U10�1
� ��0:61� 2
1þe�2U11�1
� ��2:57� 2
1þe�2U12�1
� �
þ1:60� 2
1þe�2U13�1
� �þ1:84� 2
1þe�2U14�1
� ��3:77� 2
1þe�2U15�1
� �þ0:25
U1 ¼ ð0:024� DÞ þ ð0:59� tÞ þ ð0:0004� Ef Þ þ ð0:037� f 0coÞ þ 14:02
U2 ¼ ð0:0217� DÞ þ ð1:56� tÞ þ ð�0:0003� Ef Þ þ ð0:0346� f 0coÞ þ 4:42
U3 ¼ ð�0:07� DÞ þ ð�0:1� tÞ þ ð�0:00013� Ef Þ þ ð0:073� f 0coÞ þ 16:12
U4 ¼ ð0:058� DÞ þ ð�0:96� tÞ þ ð�0:0028� Ef Þ þ ð�0:041� f 0coÞ þ 1:42
U5 ¼ ð0:061� DÞ þ ð�0:138� tÞ þ ð�0:0006� Ef Þ þ ð�0:06� f 0coÞ � 4:02
U6 ¼ ð�0:0639� DÞ þ ð�0:6017� tÞ þ ð�0:0014� Ef Þ þ ð�0:0327� f 0coÞ þ 15:32
U7 ¼ ð�0:0365� DÞ þ ð�0:4598� tÞ þ ð0:0004� Ef Þ þ ð0:0691� f 0coÞ þ 2:07
U8 ¼ ð�0:0684� DÞ þ ð0:1734� tÞ þ ð0:0006� Ef Þ þ ð�0:0381� f 0coÞ þ 9:33
U9 ¼ ð0:044� DÞ þ ð0:2966� tÞ þ ð0:0008� Ef Þ þ ð0:0736� f 0coÞ � 6:82
U10 ¼ ð0:0559� DÞ þ ð1:3957� tÞ þ ð0:0004� Ef Þ þ ð0:016� f 0coÞ � 10:58
U11 ¼ ð0:0434� DÞ þ ð�0:7968� tÞ þ ð0:0014� Ef Þ þ ð�0:0164� f 0coÞ þ 3:41
U12 ¼ ð�0:0309� DÞ þ ð�1:0127� tÞ þ ð�0:0014� Ef Þ þ ð�0:0326� f 0coÞ þ 6:09
U13 ¼ ð�0:0638� DÞ þ ð0:7750� tÞ þ ð0:0003� Ef Þ þ ð0:0633� f 0coÞ þ 1:34
U14 ¼ ð0:092� DÞ þ ð�0:6339� tÞ þ ð0:0007� Ef Þ þ ð�0:0032� f 0coÞ � 2:86
U15 ¼ ð�0:0288� DÞ þ ð�0:1202� tÞ þ ð0:0028� Ef Þ þ ð0:0137� f 0coÞ � 5:91
976 Materials and Structures (2010) 43:963–983
Table 6 Experimental database and comparative analysis of experimental and other models results
Ref. D(mm)
t(mm)
f0f(MPa)
f0co
(MPa)
Pu
(MPa)
fccTest(MPa)
NN/
test
Eq. 1/
test
Eq. 2/
test
Eq. 3/
test
Eq. 4/
test
Eq. 5/
test
Eq. 6/
test
[11] 150 0.11 3481 45.2 5.2 59.4 1.01 1.2 1.23 1.06 0.99 1.08 0.94
[11] 150 0.22 3481 45.2 10.08 79.4 0.99 1.15 1.18 1.02 0.9 0.95 0.82
[11] 150 0.11 3481 31.2 5.04 52.4 0.99 1.06 1.08 0.93 0.77 0.95 0.79
[11] 150 0.22 3481 31.2 10.14 67.4 1 1.12 1.1 1 0.73 0.92 0.76
[11] 150 0.33 3481 31.2 15.31 81.7 1 1.15 1.05 1.03 0.72 0.88 0.76
[11] 100 0.11 3481 51.9 7.7 75.2 0.98 1.18 1.23 1.05 0.99 1.02 0.89
[11] 100 0.22 3481 51.9 15.15 104.6 1.02 1.14 1.13 1.01 0.93 0.88 0.79
[11] 100 0.11 3481 33.7 7.57 69.6 1.06 0.98 1 0.87 0.69 0.84 0.7
[11] 100 0.22 3481 33.7 15.39 88 1 1.1 1.02 0.98 0.72 0.84 0.73
[11] 150 0.11 3481 45.2 5.2 59.4 1.01 1.2 1.23 1.06 0.99 1.08 0.94
[12] 100 0.167 3820 34.3 12.77 57.4 1.03 1.55 1.48 1.37 1.04 1.22 1.04
[12] 100 0.167 3820 34.3 12.85 64.9 0.91 1.37 1.31 1.21 0.92 1.08 0.92
[12] 100 0.167 3820 32.3 12.85 58.2 0.97 1.48 1.42 1.33 0.96 1.17 1
[12] 100 0.167 3820 32.3 12.77 61.8 0.91 1.4 1.34 1.25 0.91 1.1 0.94
[12] 100 0.167 3820 32.3 12.67 57.7 0.98 1.49 1.43 1.34 0.97 1.18 1
[12] 100 0.334 3820 32.3 27.69 61.8 1.18 2.23 1.8 2.09 1.37 1.55 1.42
[12] 100 0.334 3820 32.3 35.55 80.2 0.91 2.11 1.7 1.97 1.29 1.46 1.29
[12] 100 0.334 3820 32.3 16.4 58.2 1.25 1.62 1.31 1.51 0.99 1.13 1.12
[12] 100 0.501 3820 32.3 38.33 86.9 1.05 1.96 1.36 1.91 1.19 1.26 1.25
[12] 100 0.501 3820 32.3 38.27 90.1 1.01 1.89 1.31 1.84 1.14 1.21 1.21
[12] 100 0.167 3820 34.8 12.8 57.8 1.03 1.54 1.49 1.38 1.04 1.22 1.04
[12] 100 0.167 3820 34.8 12.67 55.6 1.07 1.6 1.55 1.43 1.08 1.27 1.08
[12] 100 0.167 3820 34.8 12.66 50.7 1.17 1.75 1.7 1.57 1.18 1.39 1.19
[12] 100 0.334 3820 34.8 25.4 82.7 0.97 1.61 1.33 1.49 1.03 1.12 1.04
[12] 100 0.334 3820 34.8 25.46 81.4 0.99 1.64 1.35 1.51 1.05 1.14 1.05
[12] 100 0.501 3820 34.8 38.38 103.3 1.01 1.69 1.2 1.63 1.07 1.08 1.08
[12] 100 0.501 3820 34.8 38.24 110.1 0.94 1.59 1.13 1.53 1.01 1.02 1.01
[13] 150 0.117 2600 34.9 4.08 46.1 1 1.2 1.25 1.07 0.93 1.1 0.93
[13] 150 0.235 1100 34.9 3.44 45.8 1.01 1.15 1.19 1.03 0.91 1.08 0.91
[14] 153 0.36 2275 19.4 10.77 33.8 0.98 1.85 1.65 1.68 0.93 1.51 1.21
[14] 153 0.66 2275 19.4 19.71 46.4 1.01 1.99 1.47 1.91 0.89 1.46 1.27
[14] 153 0.9 2275 19.4 26.87 62.6 1 1.82 1.17 1.8 0.79 1.27 1.17
[14] 153 1.08 2275 19.4 32.2 75.7 0.97 1.72 1 1.74 0.73 1.16 1.11
[14] 153 1.25 2275 19.4 37.32 80.2 1.02 1.81 0.97 1.86 0.76 1.19 1.17
[14] 153 0.36 2275 49 10.68 59.1 1.01 1.66 1.69 1.46 1.33 1.36 1.19
[14] 153 0.66 2275 49 19.77 76.5 1.03 1.72 1.64 1.53 1.36 1.27 1.16
[14] 153 0.9 2275 49 26.85 98.8 0.97 1.59 1.42 1.44 1.26 1.1 1.04
[14] 153 1.08 2275 49 32.3 112.7 1.01 1.56 1.33 1.43 1.24 1.04 1.01
[14] 100 0.6 1265 42 15.21 73.5 0.97 1.45 1.4 1.29 1.07 1.12 0.99
[15] 100 0.6 1265 42 15.21 73.5 0.97 1.45 1.4 1.29 1.07 1.12 0.99
[15] 100 0.6 1265 42 15.15 67.62 1.06 1.58 1.52 1.4 1.16 1.22 1.07
[15] 150 1.26 230 43 3.82 47.3 1 1.33 1.38 1.19 1.11 1.24 1.07
[15] 150 2.52 230 43 7.76 58.91 1 1.35 1.39 1.19 1.05 1.16 0.99
[15] 150 3.78 230 43 11.66 70.95 1 1.33 1.33 1.18 1.01 1.08 0.93
Materials and Structures (2010) 43:963–983 977
Table 6 continued
Ref. D(mm)
t(mm)
f0f(MPa)
f0co
(MPa)
Pu
(MPa)
fccTest(MPa)
NN/
test
Eq. 1/
test
Eq. 2/
test
Eq. 3/
test
Eq. 4/
test
Eq. 5/
test
Eq. 6/
test
[15] 150 5.04 230 43 15.46 74.39 1 1.47 1.42 1.3 1.09 1.13 0.99
[16] 100 0.35 1520 32 10.63 54 0.95 1.44 1.41 1.27 0.95 1.17 0.99
[16] 100 0.35 1520 32 10.69 48 1.07 1.62 1.58 1.43 1.07 1.32 1.11
[16] 100 0.35 1520 32 10.63 54 0.95 1.44 1.41 1.27 0.95 1.17 0.99
[16] 100 0.35 1520 32 10.61 50 1.03 1.56 1.52 1.38 1.03 1.27 1.06
[16] 100 0.16 3790 37 12.2 60 0.99 1.49 1.47 1.33 1.05 1.19 1.02
[16] 100 0.16 3790 37 12.15 62 0.96 1.44 1.41 1.28 1.01 1.15 0.99
[16] 100 0.16 3790 37 12.13 59 1.01 1.52 1.49 1.35 1.07 1.21 1.04
[16] 100 0.16 3790 37 12.11 57 1.05 1.57 1.54 1.4 1.1 1.25 1.07
[17] 150 0.169 2024 25.15 4.63 44.13 0.97 1.06 1.09 0.93 0.72 0.97 0.78
[17] 150 0.169 2024 25.15 4.61 41.56 1.04 1.12 1.15 0.99 0.76 1.02 0.83
[17] 150 0.169 2024 25.15 4.55 38.75 1.11 1.2 1.23 1.06 0.82 1.1 0.88
[17] 150 0.338 2024 25.15 9.11 60.09 0.93 1.07 1.03 0.94 0.64 0.89 0.72
[17] 150 0.338 2024 25.15 9.14 55.93 1 1.15 1.11 1.02 0.69 0.96 0.78
[17] 150 0.338 2024 25.15 9.19 61.61 0.91 1.04 1 0.92 0.62 0.87 0.71
[17] 150 0.507 2024 25.15 13.64 67 1.04 1.2 1.07 1.08 0.67 0.94 0.78
[17] 150 0.507 2024 25.15 13.72 67.27 1.04 1.2 1.07 1.08 0.67 0.93 0.78
[17] 150 0.507 2024 25.15 13.72 70.18 1 1.14 1.02 1.03 0.64 0.89 0.75
[17] 150 0.169 2024 47.44 4.64 72.26 0.91 0.98 1.03 0.89 0.83 0.9 0.79
[17] 150 0.169 2024 47.44 4.61 64.4 1.02 1.1 1.15 0.99 0.93 1 0.88
[17] 150 0.169 2024 47.44 4.57 66.19 0.99 1.07 1.12 0.96 0.9 0.98 0.85
[17] 150 0.338 2024 47.44 9.12 82.36 1.02 1.09 1.11 0.96 0.87 0.92 0.8
[17] 150 0.338 2024 47.44 9.12 82.35 1.02 1.09 1.11 0.96 0.87 0.92 0.8
[17] 150 0.338 2024 47.44 9.08 79.11 1.06 1.14 1.16 1 0.91 0.95 0.83
[17] 150 0.507 2024 47.44 13.79 96.29 0.99 1.12 1.11 0.99 0.88 0.88 0.78
[17] 150 0.507 2024 47.44 13.74 95.22 1.01 1.13 1.13 1 0.89 0.89 0.79
[17] 150 0.507 2024 47.44 13.77 103.9 0.92 1.04 1.03 0.92 0.81 0.82 0.72
[17] 150 0.169 2024 51.84 4.62 78.65 0.94 0.96 1 0.86 0.83 0.88 0.78
[17] 150 0.169 2024 51.84 4.54 79.18 0.93 0.95 0.99 0.86 0.82 0.87 0.77
[17] 150 0.169 2024 51.84 4.57 72.76 1.01 1.04 1.08 0.94 0.9 0.95 0.84
[17] 150 0.338 2024 51.84 9.23 95.4 0.98 0.99 1.03 0.88 0.83 0.84 0.74
[17] 150 0.338 2024 51.84 9.16 90.3 1.04 1.05 1.09 0.94 0.87 0.89 0.78
[17] 150 0.338 2024 51.84 9.02 90.65 1.03 1.05 1.09 0.93 0.87 0.88 0.77
[17] 150 0.507 2024 51.84 13.77 110.5 0.97 1.02 1.02 0.89 0.84 0.81 0.72
[17] 150 0.507 2024 51.84 13.64 103.6 1.03 1.09 1.09 0.95 0.89 0.86 0.76
[17] 150 0.507 2024 51.84 13.65 117.2 0.91 0.96 0.96 0.84 0.79 0.76 0.68
[17] 150 0.845 2024 51.84 22.78 112.6 1.07 1.3 1.22 1.17 1.06 0.94 0.87
[17] 150 0.845 2024 51.84 22.87 126.6 0.95 1.16 1.08 1.04 0.94 0.83 0.77
[17] 150 0.845 2024 51.84 22.67 137.9 0.87 1.06 0.99 0.95 0.87 0.76 0.7
[17] 150 0.169 2024 70.48 4.53 87.29 0.98 1.09 1.1 0.98 1.02 1.01 0.91
[17] 150 0.169 2024 70.48 4.53 84.03 1.02 1.14 1.15 1.02 1.06 1.05 0.95
[17] 150 0.169 2024 70.48 4.53 83.22 1.03 1.15 1.16 1.02 1.07 1.06 0.96
[17] 150 0.338 2024 70.48 9.19 94.06 1.04 1.23 1.28 1.09 1.14 1.05 0.94
[17] 150 0.338 2024 70.48 9.14 98.13 1 1.18 1.22 1.05 1.09 1.01 0.9
978 Materials and Structures (2010) 43:963–983
Table 6 continued
Ref. D(mm)
t(mm)
f0f(MPa)
f0co
(MPa)
Pu
(MPa)
fccTest(MPa)
NN/
test
Eq. 1/
test
Eq. 2/
test
Eq. 3/
test
Eq. 4/
test
Eq. 5/
test
Eq. 6/
test
[17] 150 0.338 2024 70.48 9.22 107.2 0.91 1.08 1.12 0.96 1 0.92 0.83
[17] 150 0.507 2024 70.48 13.7 114.1 0.98 1.17 1.2 1.03 1.1 0.95 0.86
[17] 150 0.507 2024 70.48 13.63 108 1.03 1.24 1.27 1.09 1.17 1 0.9
[17] 150 0.507 2024 70.48 13.48 110.3 1.01 1.21 1.23 1.06 1.14 0.98 0.88
[17] 150 0.169 2024 82.13 4.75 94.08 1 1.15 1.2 1.06 1.11 1.06 0.97
[17] 150 0.169 2024 82.13 5.2 97.6 0.96 1.13 1.18 1.04 1.09 1.04 0.95
[17] 150 0.169 2024 82.13 4.98 95.83 0.98 1.14 1.19 1.05 1.1 1.05 0.96
[17] 150 0.338 2024 82.13 10.15 97.43 1.07 1.36 1.4 1.2 1.32 1.17 1.05
[17] 150 0.338 2024 82.13 9.14 98.85 1.05 1.3 1.34 1.15 1.27 1.12 1.02
[17] 150 0.338 2024 82.13 9.92 98.24 1.06 1.34 1.39 1.19 1.31 1.16 1.04
[17] 150 0.507 2024 82.13 13.59 124.2 0.99 1.19 1.23 1.05 1.18 0.96 0.88
[17] 150 0.507 2024 82.13 13.76 129.5 0.95 1.13 1.18 1.01 1.13 0.92 0.85
[17] 150 0.507 2024 82.13 13.42 120.3 1.08 1.22 1.27 1.08 1.21 0.99 0.91
Bold sets are test
sets
Std.
Dev.
0.06 0.28 0.2 0.29 0.18 0.17 0.16
Mean 1 1.33 1.25 1.2 0.98 1.06 0.94
Ref. Eq. 7/
test
Eq. 8/
test
Eq. 9/
test
Eq. 10/
test
Eq. 11/
test
Eq. 12/
test
Eq. 13/
test
Eq. 14/
test
Eq. 15/
test
Eq. 17/
test
Eq. 18/
test
Eq. 20/
test
Eq. 21/
test
[11] 1.17 1.03 0.91 1.06 1.12 1 0.88 0.80 1.09 1.16 1.12 1.14 1.1
[11] 1.14 0.93 0.93 1.01 1.09 0.9 1.00 0.86 1.17 0.96 0.95 0.96 0.93
[11] 1.03 0.88 0.83 0.93 0.99 0.85 0.94 0.84 1.13 1.12 1.03 0.94 0.94
[11] 1.09 0.86 0.89 0.98 1.08 0.84 1.03 0.97 1.26 1.04 0.92 0.82 0.83
[11] 1.11 0.84 0.88 1.03 1.15 0.81 1.05 1.05 1.37 0.96 0.85 0.75 0.76
[11] 1.17 1 0.94 1.05 1.11 0.97 0.94 0.77 1.11 1.04 0.99 1.19 1.01
[11] 1.12 0.89 0.91 1.01 1.09 0.86 1.02 0.86 1.22 0.87 0.8 1 0.87
[11] 0.97 0.79 0.79 0.86 0.93 0.77 1.00 0.80 1.18 0.87 0.83 0.8 0.8
[11] 1.06 0.81 0.85 0.99 1.1 0.78 1.05 0.98 1.36 0.79 0.75 0.75 0.75
[11] 1.17 1.03 0.91 1.06 1.12 1 0.88 0.80 1.09 1.16 1.12 1.14 1.1
[12] 1.5 1.17 1.21 1.37 1.51 1.13 1.03 1.32 1.29 1.06 1.11 1.11 1.11
[12] 1.32 1.03 1.07 1.21 1.34 1 1.04 1.16 1.30 0.94 0.98 0.98 0.98
[12] 1.45 1.12 1.17 1.32 1.46 1.08 1.04 1.30 1.30 1.02 1.05 1.04 1.04
[12] 1.36 1.06 1.1 1.24 1.37 1.02 1.04 1.23 1.29 0.96 0.99 0.98 0.98
[12] 1.46 1.13 1.17 1.32 1.46 1.09 1.04 1.31 1.29 1.03 1.06 1.04 1.05
[12] 2.15 1.56 1.59 2.07 2.36 1.49 1.02 2.19 1.51 1.13 1.2 1.28 1.28
[12] 2.02 1.47 1.5 1.93 2.22 1.33 1.02 2.07 1.51 0.87 0.92 1.11 1.11
[12] 1.56 1.13 1.16 1.53 1.71 1.19 1.03 1.59 1.51 1.2 1.27 1.11 1.12
[12] 1.88 1.32 1.29 1.89 2.18 1.28 0.98 2.08 1.65 0.92 1 1.06 1.07
[12] 1.81 1.27 1.24 1.82 2.1 1.23 0.98 2.00 1.65 0.89 0.96 1.02 1.03
[12] 1.51 1.18 1.22 1.37 1.51 1.14 1.03 1.32 1.28 1.12 1.11 1.11 1.11
[12] 1.56 1.22 1.27 1.41 1.56 1.18 1.04 1.37 1.28 1.16 1.15 1.15 1.16
[12] 1.71 1.34 1.39 1.55 1.71 1.29 1.04 1.50 1.28 1.27 1.27 1.27 1.27
[12] 1.55 1.13 1.16 1.48 1.68 1.09 1.03 1.54 1.49 0.94 0.94 0.98 0.99
[12] 1.57 1.15 1.18 1.51 1.71 1.11 1.03 1.57 1.49 0.96 0.95 1 1
Materials and Structures (2010) 43:963–983 979
Table 6 continued
Ref. Eq. 7/
test
Eq. 8/
test
Eq. 9/
test
Eq. 10/
test
Eq. 11/
test
Eq. 12/
test
Eq. 13/
test
Eq. 14/
test
Eq. 15/
test
Eq. 17/
test
Eq. 18/
test
Eq. 20/
test
Eq. 21/
test
[12] 1.61 1.14 1.13 1.62 1.86 1.11 0.99 1.75 1.63 0.92 0.87 0.96 0.96
[12] 1.52 1.07 1.06 1.51 1.74 1.04 0.99 1.64 1.63 0.86 0.82 0.9 0.9
[13] 1.19 1.04 0.94 1.06 1.12 1.01 0.90 0.96 1.08 1.25 1.27 1.14 1.14
[13] 1.14 1.01 0.88 1.02 1.07 0.98 0.87 1.11 1.06 1.2 1.3 1.13 1.13
[14] 1.78 1.34 1.39 1.67 1.88 1.29 1.04 1.70 1.40 1.45 1.37 1.08 1.09
[14] 1.91 1.35 1.35 1.88 2.16 1.31 1.00 2.04 1.60 1.29 1.28 0.93 0.94
[14] 1.73 1.2 1.15 1.79 2.07 1.17 0.96 1.97 1.73 1.12 1.12 0.77 0.78
[14] 1.64 1.12 1.04 1.72 2 1.09 0.93 1.92 1.79 0.97 1.03 0.69 0.7
[14] 1.72 1.16 1.05 1.85 2.15 1.14 0.91 2.08 1.85 1 1.06 0.7 0.71
[14] 1.63 1.34 1.33 1.45 1.57 1.29 0.99 0.82 1.17 1.33 1.49 1.46 1.34
[14] 1.67 1.29 1.34 1.53 1.7 1.24 1.04 1.11 1.32 1.19 1.35 1.36 1.26
[14] 1.54 1.15 1.2 1.43 1.61 1.11 1.04 1.16 1.40 1.02 1.16 1.19 1.11
[14] 1.5 1.11 1.15 1.42 1.61 1.07 1.04 1.21 1.45 1.02 1.09 1.13 1.07
[14] 1.41 1.1 1.14 1.29 1.42 1.07 1.04 1.20 1.29 0.99 1.1 1.08 1.07
[15] 1.41 1.1 1.14 1.29 1.42 1.07 1.04 1.20 1.29 0.99 1.1 1.08 1.07
[15] 1.53 1.2 1.24 1.39 1.54 1.16 1.03 1.30 1.28 1.08 1.19 1.17 1.16
[15] 1.32 1.17 1 1.19 1.24 1.14 0.85 0.84 1.06 1.42 1.55 1.31 1.29
[15] 1.32 1.11 1.08 1.18 1.27 1.08 0.97 0.94 1.14 1.17 1.34 1.17 1.14
[15] 1.3 1.05 1.07 1.17 1.28 1.02 1.02 1.01 1.22 1.16 1.19 1.06 1.04
[15] 1.43 1.12 1.16 1.29 1.43 1.08 1.04 1.17 1.28 1.14 1.21 1.1 1.08
[16] 1.4 1.1 1.14 1.27 1.4 1.06 1.04 1.16 1.27 1.04 1.12 1.06 1.06
[16] 1.58 1.24 1.28 1.44 1.58 1.2 1.03 1.30 1.27 1.18 1.26 1.19 1.2
[16] 1.4 1.1 1.14 1.27 1.4 1.06 1.04 1.16 1.27 1.04 1.12 1.06 1.06
[16] 1.52 1.2 1.23 1.37 1.51 1.15 1.03 1.25 1.26 1.13 1.21 1.14 1.15
[16] 1.46 1.15 1.19 1.32 1.45 1.11 1.03 1.23 1.26 1.11 1.1 1.12 1.11
[16] 1.41 1.11 1.14 1.27 1.4 1.07 1.03 1.18 1.26 1.08 1.07 1.08 1.08
[16] 1.49 1.17 1.21 1.34 1.47 1.13 1.03 1.25 1.26 1.13 1.12 1.13 1.13
[16] 1.54 1.21 1.25 1.38 1.52 1.17 1.03 1.29 1.26 1.17 1.16 1.17 1.17
[17] 1.04 0.87 0.84 0.93 1 0.84 0.97 0.87 1.15 1.12 1.04 0.91 0.92
[17] 1.1 0.92 0.89 0.99 1.06 0.89 0.97 0.92 1.15 1.19 1.11 0.97 0.98
[17] 1.18 0.99 0.96 1.05 1.13 0.96 0.97 0.99 1.14 1.28 1.19 1.04 1.05
[17] 1.03 0.81 0.84 0.94 1.04 0.78 1.04 0.94 1.28 0.97 0.88 0.74 0.75
[17] 1.11 0.87 0.9 1.01 1.12 0.84 1.03 1.02 1.29 1.04 0.94 0.8 0.81
[17] 1.01 0.79 0.82 0.92 1.02 0.76 1.04 0.92 1.29 0.95 0.85 0.73 0.73
[17] 1.16 0.87 0.9 1.08 1.21 0.84 1.03 1.13 1.39 0.96 0.88 0.73 0.74
[17] 1.15 0.87 0.9 1.08 1.21 0.83 1.03 1.12 1.39 0.95 0.88 0.73 0.74
[17] 1.1 0.83 0.86 1.03 1.16 0.8 1.04 1.07 1.40 0.91 0.84 0.7 0.71
[17] 0.98 0.87 0.76 0.88 0.92 0.85 0.87 0.58 1.06 0.98 1.06 0.98 0.92
[17] 1.1 0.97 0.84 0.98 1.03 0.94 0.87 0.65 1.06 1.1 1.19 1.1 1.03
[17] 1.07 0.94 0.82 0.96 1 0.92 0.87 0.63 1.06 1.07 1.16 1.07 1
[17] 1.07 0.89 0.87 0.96 1.03 0.86 0.98 0.73 1.16 1 1.02 0.96 0.91
[17] 1.07 0.89 0.87 0.96 1.03 0.86 0.98 0.73 1.16 1 1.02 0.96 0.91
[17] 1.11 0.93 0.9 1 1.07 0.9 0.97 0.76 1.15 1.04 1.07 1 0.94
[17] 1.09 0.88 0.89 0.99 1.08 0.84 1.01 0.83 1.23 0.94 0.95 0.91 0.86
980 Materials and Structures (2010) 43:963–983
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Table 6 continued
Ref. Eq. 7/
test
Eq. 8/
test
Eq. 9/
test
Eq. 10/
test
Eq. 11/
test
Eq. 12/
test
Eq. 13/
test
Eq. 14/
test
Eq. 15/
test
Eq. 17/
test
Eq. 18/
test
Eq. 20/
test
Eq. 21/
test
[17] 1.11 0.88 0.9 1 1.09 0.85 1.02 0.83 1.24 0.95 0.96 0.92 0.87
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[17] 1.11 1.01 0.79 1.02 1.06 1 0.78 0.43 1.05 1.1 1.11 1.02 0.96
[17] 1.12 1.02 0.79 1.03 1.07 1 0.77 0.43 1.05 1.11 1.12 1.03 0.97
[17] 1.22 1.05 0.96 1.07 1.15 1.02 0.91 0.54 1.10 1.1 1.1 1.05 0.99
[17] 1.16 1 0.92 1.02 1.1 0.98 0.92 0.52 1.10 1.05 1.05 1 0.95
[17] 1.06 0.92 0.84 0.94 1.01 0.89 0.91 0.48 1.10 0.96 0.96 0.92 0.87
[17] 1.14 0.95 0.93 1.01 1.11 0.93 0.98 0.61 1.17 0.98 0.99 0.97 0.92
[17] 1.21 1.01 0.99 1.07 1.17 0.98 0.98 0.65 1.16 1.04 1.05 1.03 0.98
[17] 1.18 0.98 0.96 1.04 1.14 0.95 0.98 0.63 1.16 1.02 1.03 1 0.95
[17] 1.16 1.06 0.82 1.03 1.08 1.03 0.77 0.18 1.02 1.1 0.95 0.97 0.9
[17] 1.14 1.04 0.81 1.01 1.06 1.01 0.78 0.18 1.02 1.06 0.92 0.95 0.88
[17] 1.15 1.05 0.81 1.02 1.07 1.02 0.77 0.18 1.02 1.08 0.94 0.96 0.89
[17] 1.34 1.17 1.04 1.17 1.27 1.13 0.89 0.44 1.09 1.14 1.05 1.11 1.05
[17] 1.28 1.12 1 1.12 1.21 1.09 0.89 0.42 1.08 1.12 1.04 1.06 1
[17] 1.32 1.16 1.03 1.15 1.25 1.12 0.89 0.44 1.08 1.13 1.04 1.1 1.03
[17] 1.18 0.99 0.95 1.01 1.11 0.96 0.96 0.48 1.12 0.94 0.92 0.96 0.91
[17] 1.12 0.95 0.91 0.97 1.07 0.92 0.96 0.46 1.13 0.9 0.88 0.93 0.88
[17] 1.21 1.02 0.98 1.03 1.14 0.98 0.96 0.49 1.12 0.97 0.95 0.99 0.94
Bold sets
are test
sets
0.27 0.16 0.19 0.28 0.35 0.16 0.08 0.46 0.18 0.13 0.15 0.15 0.14
1.29 1.03 1.01 1.19 1.31 1 0.97 1.00 1.25 1.03 1.04 1 0.96
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