Next Article in Journal
Research Progress of Urban Floods under Climate Change and Urbanization: A Scientometric Analysis
Next Article in Special Issue
An Exhaustive Search Energy Optimization Method for Residential Building Envelope in Different Climatic Zones of Kazakhstan
Previous Article in Journal
Window View Access in Architecture: Spatial Visualization and Probability Evaluations Based on Human Vision Fields and Biophilia
Previous Article in Special Issue
The Impact of Temporary Means of Access on Buildings Envelope’s Maintenance Costs
 
 
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Article

Novel Fuzzy-Based Optimization Approaches for the Prediction of Ultimate Axial Load of Circular Concrete-Filled Steel Tubes

by
Jinsong Liao
1,*,
Panagiotis G. Asteris
2,*,
Liborio Cavaleri
3,
Ahmed Salih Mohammed
4,
Minas E. Lemonis
2,
Markos Z. Tsoukalas
2,
Athanasia D. Skentou
2,
Chrysanthos Maraveas
5,
Mohammadreza Koopialipoor
6 and
Danial Jahed Armaghani
7
1
School of Construction Management, Chongqing Jianzhu College, Chongqing 400072, China
2
Computational Mechanics Laboratory, School of Pedagogical and Technological Education, 14121 Athens, Greece
3
Department of Engineering, University of Palermo, 90133 Palermo, Italy
4
Civil Engineering Department, College of Engineering, University of Sulaimani, Sulaymaniyah 46001, Iraq
5
Farm Structures Laboratory, Department of Natural Resources and Agricultural Engineering, Agricultural University of Athens, 11855 Athens, Greece
6
Faculty of Civil and Environmental Engineering, Amirkabir University of Technology, Tehran 15914, Iran
7
Department of Urban Planning, Engineering Networks and Systems, Institute of Architecture and Construction, South Ural State University, 76, Lenin Prospect, 454080 Chelyabinsk, Russia
*
Authors to whom correspondence should be addressed.
Buildings 2021, 11(12), 629; https://doi.org/10.3390/buildings11120629
Submission received: 6 November 2021 / Revised: 6 December 2021 / Accepted: 7 December 2021 / Published: 9 December 2021
(This article belongs to the Special Issue Buildings: 10th Anniversary)

Abstract

:
An accurate estimation of the axial compression capacity of the concrete-filled steel tubular (CFST) column is crucial for ensuring the safety of structures containing them and preventing related failures. In this article, two novel hybrid fuzzy systems (FS) were used to create a new framework for estimating the axial compression capacity of circular CCFST columns. In the hybrid models, differential evolution (DE) and firefly algorithm (FFA) techniques are employed in order to obtain the optimal membership functions of the base FS model. To train the models with the new hybrid techniques, i.e., FS-DE and FS-FFA, a substantial library of 410 experimental tests was compiled from openly available literature sources. The new model’s robustness and accuracy was assessed using a variety of statistical criteria both for model development and for model validation. The novel FS-FFA and FS-DE models were able to improve the prediction capacity of the base model by 9.68% and 6.58%, respectively. Furthermore, the proposed models exhibited considerably improved performance compared to existing design code methodologies. These models can be utilized for solving similar problems in structural engineering and concrete technology with an enhanced level of accuracy.
Keywords:
CCFST; hybrid; prediction; FFA; DE; FS

1. Introduction

Concrete-filled steel tube (CFST) members make better utilization of steel and concrete than traditional bare steel or reinforced concrete structures. The steel tube gives confinement to the concrete infill, while the concrete infill prevents the inward buckling of the steel tube. CFST members have a long history of being used in a broad range of construction projects due to their efficiency as structural components. As an example, CFSTs have been utilized as (1) mega columns in super high-rise buildings, (2) chord members in long-span arch bridges, (3) bridge piers, (4) floodwall piling, and (5) underwater pipeline structures, as described by researchers like Wang et al. [1]. For the most part, the CFST components in these situations are utilized to support compressive forces.
When it comes to improving the compressive strength of CFST components, there are primarily two approaches that are used. Using bigger cross sections is one approach. However, it may increase structural weight (and as a result the seismic impact) and decrease useable space, making it a less feasible or cost-effective solution. Alternatively, high strength steel (i.e., with a yield stress higher than 525 MPa) and high strength concrete (i.e., with a compressive strength greater than 70 MPa) are two additional viable methods [AISC 360 [2]].
According to experts like Nishiyama et al. [3], Kim [4] and Han [5] and others, many studies have been carried out to examine the behavior of conventional-strength members of the CFST. Several researchers have experimented with the behavior of high-strength CFST columns facilitating their adoption in practice. For example, Cederwall et al. [6], Varma [7], Uy [8], Liu et al. [9], Mursi and Uy [10], Sakino et al. [11], Lue et al. [12], Aslani et al. [13], and Xiong et al. [14] have performed experimental testing on high-strength rectangular CFST short columns. Lai and Varma [15] reviewed these experiments and provided design equations for calculating the cross-sectional strength of high-strength rectangular CFST columns and also effective stress-strain relationships for the steel tube and concrete infill of such high-strength components.
Additional experimental tests on CFST columns were conducted by Gardner and Jacobson [16], Bergmann [17], O’Shea and Bridge [18], Schneider [19], O’Shea and Bridge [20], Giakoumelis and Lam [21], Sakino et al. [11], Zeghiche and Chaoui [22], Yu et al. [23], de Oliveira et al. [24], Liew and Xiong [25], Chen et al. [26]. The experimental results from previous studies have been employed in this study in order to build an experimental database. It is noted, however, that experiments featuring columns with fibers in the concrete, stainless or aluminum steel tubing, grease on the inner surface of the tubing, or concrete infill alone were excluded from this database.
Machine learning (ML) methods have been widely used in many civil engineering applications [27,28,29,30,31,32,33,34,35,36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,53,54,55], particularly in compressive structures [56,57,58,59]. ML uses databases to develop models that can solve various linear and nonlinear problems with varying degrees of complexity. These methods, using computer processing, help considerably in solving problems more efficiently and quickly, and is introduced as a powerful alternative method for older, experimental and statistical models. An optimization and tree-based approach has been developed by Sarir et al. [60] to find out the maximum capacity of circular CFST members. Short CFST members’ load-bearing capacity was predicted by Ahmadi et al. using an artificial neural network [61,62]. A gene expression model for predicting circular CFST capability was established by Güneyisi et al. [63] and Ipek and Güneyisi [64]. In the study of Moon et al. [65], the load-bearing behavior of circular CFST was also examined using a fuzzy logic model. According to Al-Khaleefi et al. [66], the fire resistance of CFST columns has also been studied using a machine learning method that considers material characteristics and loading circumstances. For sections other than circular, Ren et al. [67] recently published a study on the prediction of square CFST members, using support vector machines and particle optimization methods. While for the same section Tran et al. [68] used a neural network model to predict the ultimate load. Also, Lee et al. [69] used a categorical gradient boosting algorithm to predict the strength of both circular and rectangular CFSTs under concentric or eccentric loading. Zarringol et al. [70] used ANN for the same problem. It can be concluded from these studies that ML methods prove quite promising in investigating the mechanical behavior of structures made up of CFST members.
In this research, the major goal is to develop a regression machine learning model for compressive circular CFST, particularly in contemporary buildings. This was achieved using a hybridizing fuzzy system (FS) with two optimization algorithms known as the firefly algorithm (FFA) and differential evolution (DE). The input data consist of column length, cross-section diameter and steel tube thickness in addition to concrete compressive and steel yield stress. Precise quality metrics such as root mean-squared-error (RMSE), and coefficient of determination (R2) were utilized throughout the model’s testing/validation phase. The FS-FFA and FS-DE models were evaluated and compared with existing design code methodologies to highlight the best predictive model for the examined problem.

2. Research Significance

CFST design can be done using different methods and codes around the world. Accurate, faster, and less costly design is one of the priorities of any structural project. Due to the fact that an accurate CFST design has important effects on the stability of structures, examining different techniques could give a better understanding of their effects and behaviour. Therefore, this research, using a new generation of computational methods developed by learning machines, is aimed at coming up with a practical solution to the aforementioned problem. Using a combination of FS and optimization algorithms (i.e., FFA and DE), new predictive models can be developed to more accurately and quickly evaluate CFST design. Optimal solutions of hybrid models consisting of these conditions can be used for new conditions and provide acceptable results considering practical applications in industrial fields.

3. Short Literature Review on Design Codes

The design of circular CFST columns is already supported by several steel and composite codes, available worldwide. Such codes include EN1994 [71] in Europe, AISC 360 [72] in the USA, AIJ [73] in Japan. Besides providing the squash load that is relevant for short columns, design codes also provide methodologies to predict the resistance against flexural buckling, which becomes the critical failure mode for long, slender columns. Local buckling of the steel tube is also a failure mode relevant for thin-walled steel sections. It is typically covered by placing section slenderness limits and depending on them, either accounting for a reduced effective steel sectional area (i.e., EN1994 [71]), or limiting the ultimate stress the composite section may reach (i.e., AISC 360 [72]). Regarding squash load, which involves the plastic strength of the steel and concrete parts of the CFTS section, the influence of the increased concrete confinement provided by the circular tube is typically expressed through an increase of the concrete strength contribution. The following formulas describe the squash loads, for the EN1994 [71], AISC 360 [72], AIJ [73] design codes (ignoring any safety factors):
N p E N 1994 = { η a f y A s + ( 1 + η c t f y d f c ) f c A c , λ ¯ < 0.5 f y A s + f c A c , λ ¯ 0.5  
N p A I S C 360 = f y A s + 0.95 f c A c  
N p A I J = 1.27 f y A s + 0.85 f c A c  
Factors η a and η c account for the member slenderness λ ¯ . For slender columns, the squash loads given above fail to represent the ultimate compressive load. In such cases, buckling phenomena emerge that cause an earlier failure, depending on the global column slenderness. The methodologies provided by the aforementioned design codes are differentiated in this context. Due to space limitations the relevant expressions are not reproduced herein however.
All design codes place specific limits on their field of application. These are related to material strength limits, steel tube slenderness, global slenderness or steel to concrete ratio. Table 1 presents the relevant application limits for the codes examined.

4. Modeling Approaches

4.1. Fuzzy System (FS)

A chapter titled “fuzzy sets” by Professor Lotfizadeh in 1965 presented the fuzzy theory [74]. Initially, his primary objective was to create a more accurate model of how natural language processing works. Fuzzy sets, fuzzy events, fuzzy numbers, and phases are only a few of the innovations he made to mathematics and engineering thanks to these ideas. A rule base, which includes If–Then rules created by application specialists, constitutes FS’s core component [75]. Membership functions are used to deploy the fuzzy sets. For the FS process, the most popular fuzzifiers are Gaussian, Singleton, and Triangular. In addition, the most often used defuzzifiers in the literature are center of gravity, center average, and maximum. Fuzzy logic principles govern the firing of If–Then rules while the inference engine is operating. A fuzzy rule has the following syntax [76]:
I f   x 1   i s   A 1   a n d   x n   i s   A n   t h e n   Y   i s   B
Fuzzy sets in U R (U is the input space) are Ai and V R (V is the output space) are B, and X is equal to the product of the variables in the input space and the variables in the output space, respectively. There are two types of FS controller: closed-loop and open-loop. The product inference engine and Gaussian fuzzifier were used in the following ways:
f 1 ( x ) = { exp [ 1 2 ( x m 1 σ ) ]     x m 1 1         o t h e r w i s e
f 2 ( x ) = { 1                           x m 2 exp [ 1 2 ( x m 1 σ ) ]         o t h e r w i s e

4.2. Firefly Algorithm (FFA)

Yang was the first to propose FFA as a nature-inspired, meta-heuristic algorithm [77]. Engineers have used this method to address a variety of issues. The most critical aspects of the FFA process are the formulation of attraction and the change in light intensity. Fireflies will operate virtually independently in FFA modelling, which is advantageous for parallel implementation in particular. Fireflies in this algorithm tend to congregate closer to the optimum, making it superior to the particle swarm optimization (PSO) and the genetic algorithm (GA) [76,78]. Figure 1 depicts FFA’s foundation for a better understanding. Several studies, including Yang [77], Zhang and Wu [79], and Apostolopoulos and Vlachos [80], go into great depth regarding FFA. Reviewing past research shows that the FFA may be utilized as a powerful tool for engineering optimization in almost all fields [81,82]. Gholizadeh and Barati [83], for example, used the PSO, FFA, and harmony search (HS) to explore the size and form optimization of truss systems. In terms of optimizing the size and geometry of truss structures, FFA outperformed PSO and HS.

4.3. Differential Evolution (DE)

Storn and Price (1997) first proposed the concept of differential evolution (DE) as a stochastic population-based search technique [84]. NP members are randomly selected from the original population (parents) before the search may begin. Using crossover, mutation, and selection operators, the DE technique then produces a new population (i.e., offspring). This iteration’s members are chosen by comparing how similar they are to the previous iteration’s members. This cycle is repeated until the desired outcome is achieved. The following sections describe the major stages of this algorithm [84].

4.3.1. Generating the Initial Population

If the problem’s decision variables are indicated by D, the initial population vector is produced with a random size N*D inside the decision variables allowed range, according to the following equation:
x i o = x i m i n + r o u n d ( φ i × x i m a x x i m i n ) ,   i = 1 , , N P
There are lower and higher limits on the choice variables ximin and ximax, respectively, while index i is a random number between 0 and 1.

4.3.2. Mutation

To carry out the mutation procedure, the following equation is used:
v i , G + 1 = x r 1 , G + F × ( x r 2 , G x r 3 , G )
There are three randomly selected members of the population in this case, and the scaling factor F ranges from zero to two, giving us a mutant vector v i , G + 1   and three randomly picked members of the population.

4.3.3. Crossover

This operator combines the modified particles with the members of the target group that were chosen in the first stage as follows:
u i j , G + 1 = { v j i , G + 1     r < C r   o r   j = r n i x j i , G         o t h e r w i s e
where j = 1, 2, …, D; ∈ rj [0, 1] is the random number; Cr stands for the crossover constant ∈ [0, 1]; and ∈ rni (1, 2, …, D) is the randomly chosen index.

4.3.4. Selection

Once all operators have been initialised to their respective goal functions, a new measurement vector and target member are created. If the measurement vector’s value exceeds the target member’s, the member is promoted to the next generation. If this does not happen, the target member will be added to the population of the following generation. Figure 2 depicts the DE’s pseudo-code.

4.4. Hybridization of FS

The CCFST is predicted using two hybrid FS-FFA and FS-DE in this research. Five characteristics were utilized as inputs in the hybrid FS modelling procedure, with CCFST ultimate load being the output. The proposed FS-FFA and FS-DE models were trained and tested using 328 datasets of data in the training phase and 82 datasets of data in the testing phase. Fuzzy-based modifications to FFA and DE are suggested in this research to remove or minimize model drawbacks. In this structure, the member (population) of optimization algorithms in each step may affect each other’s movements. For determining progress in the program, we used two metrics to indicate how close the algorithms are getting to the ideal answer. We call this loop counter (iteration) Count and its value is decided by expertise or via trial and error [85]. The fuzzy controller will have to deal with this last problem. The following is an introduction to the delta parameter:
D e l t a i = F ( B e s t i ) F ( T B e s t i 1 )
Iteration i yields Besti, which is the best solution, whereas iteration i−1 yields TBesti−1, which is the best solution. One of the benefits of the hybrid FS is that it regulates the fundamental database, i.e., physics of the examined problem. As a result, convergence speed may be improved by making the appropriate initial adjustments. A MATLAB programme was used to implement the hybrid FS model’s code. The following equation is used to standardize datasets before beginning hybrid FS modelling:
X n o r m = X X m i n X m a x X m i n
where X, Xmin, and Xmax represent the parameters’ real values, minimum and maximum values, respectively, while Xnorm represents the parameter’s normalized value. FS-FFA modeling’s most critical parameters are Npop (swarm size), Alpha (mutation coefficient), Gamma (light absorption coefficient), Beta (attraction coefficient base value) and Maxiter (maximum number of iterations), according to prior research [81,82,85]. Parameters’ number of iteration, crossover constant and population (Npop) are also effective for the DE algorithm [84,86]. Following the trial and error technique, Npop of FFA was set to 50, Npop of DE was set to 80, Alpha was set to 0.25, Gamma was set to 1, crossover constant was set to 0.8, Beta was set to 2, and the number of iterations for both algorithms was set to 500. Figure 3 depicts the steps involved in putting hybrid FS into practice.

5. Data Setup

A variety of sources were used to compile the database for this study such as Wang et al. [87], Geng [88], Dong et al. [89], Wang et al. [90], Chen et al. [91], Yang et al. [92], Wang et al. [93], Wei et al. [94] Hoang and Fehling [95], He et al. [96]. These sources include axial compression tests on circular CFST columns that make up 410 samples in total (whole used datasets for modeling are presented in Appendix A). Several geometrical factors and mechanical characteristics were utilized in these tests to investigate the failure of CFST columns under axial stress. These are column length (L), diameter (D), and thickness (t) as geometrical input variables. Additionally, the steel tube yield stress (fy) and the compressive strength (fc) of the filling concrete are the material specific variables representing their mechanical properties. The only output of the problem is the CFST column ultimate experimental axial compressive load (Pexp). Table 2 shows a statistical examination of the dataset.

6. Development of the Hybrid Models

The performance of FS-FFA and FS-DE models is discussed in this part, presenting how well it can predict the circular CFST ultimate compressive load. In order to do this, three quantitative standard statistical performance measures, namely R2, the a20-index, and RMSE, have been used, as described by Equations (12)–(14) [52,58,97,98,99,100,101,102]:
R M S E = 1 n i = 1 n ( y f r , i y ^ f r , i ) 2
R 2 = 1 i = 1 n ( y f r , i y ^ f r , i ) 2 i = 1 n ( y f r , i y ¯ f r , i ) 2
a 20 i n d e x = m 20 n
where, the predicted and measured values for n data are indicated by y ^ f r , i and y f r , i , respectively, and m20 is the number of samples with a value of (experimental value)/(predicted value) ratio, between 0.80 and 1.20. The best performance of the models is achieved when the errors (RMSE) are zero and the R2 is close to one. The performance of the developed FS-FFA and FS-DE is presented in Table 3 in terms of R2, RMSE, and a20-index. The optimal model values have been optimally picked having as objective to achieve the best possible performance metrics.
In Table 3, it can be shown that the proposed FS-FFA and FS-DE have a good performance for predicting CFST values. In the training section, the performance of the FS-FFA model seems better in terms of RMSE and a20-index, compared to the FS-DE model whereas the latter scores a higher R2 value. However, in the test section, the performance of the two models proves more closely matched, with the FS-FFA achieving slightly better metrics. Given that the FS-FFA model has been able to provide better predictions in both sections, it becomes the preferred one for the estimation of circular CFST ultimate compressive load. Figure 4 and Figure 5 show separately for the training and the testing datasets graphs of predicted vs. experimental loads for both hybrid models. It can be seen that both models exhibit a consistent performance throughout the range of available compressive loads.

7. Discussion

7.1. Comparison against Alternative Hybrid Models

In this section, a comparison is made between the developed hybrid models with the base model and the other two traditional hybrid models. Given that optimization algorithms have different performances for each problem, it is possible to identify their differences and compare their performances by examining several algorithms together. Therefore, two hybrid models, FS-genetic algorithm (GA) and FS-particle swarm optimization (PSO), were developed to compare with the two developed models in this study. The findings showed that the FS-FFA, FS-DE, FS-GA, and FS-PSO models outperformed FS in terms of prediction accuracy for training data by 9.68%, 6.58%, 5.68%, and 1.56% respectively. Among the hybrid models, the FS-FFA model provided the best performance according to the various criteria for predicting circular CFST ultimate load values.

7.2. Comparison against Design Codes

In this section a comparison between the two developed models against the predictions of the three design codes, mentioned earlier in the text (EN1994, AISC360 and AIJ) is presented. The design code calculations were performed ignoring any safety factors. Also, the calculations were not focused on the squash load only but took into account the relevant for more slender columns buckling failure methodologies available in each code.
Table 4 presents the performance indices for the two developed models and the respective ones for the design codes. The results correspond to the designated testing datasets among the specimens in the experimental database, amounting to 82 specimens. The various models in the Table are ranked according to their RMSE index. It appears that the two developed models achieve a considerable improvement in almost all indices, compared to the design codes. In particular the improvement from the best performing code which proves the Japanese AIJ [73], is remarkable for both the RMSE and a20-index. A marginal improvement is also found in terms of R2 index. Among design codes, the AIJ [73] achieves improved performance compared to the other codes.
Figure 6 illustrates for the two hybrid models and for the examined design codes, the individual experimental vs. predicted load values for all specimens in the testing datasets. It can be visually inspected that the FS-FFA hybrid model achieves a better fit to the experimental values, with less outliers, over the entire range of specimens.

7.3. Limitations and Future Works

This research developed several hybrid models using artificial intelligence to predict the ultimate compressive load of CCFST columns. These models are based on data collected from laboratory works of previous research. Given that the structure of models is highly dependent on the number of parameters, their types must be taken into account in measuring and using such data. Laboratory outline data reduce the accuracy of prediction. On the other hand, the purpose of this study is to develop non-linear models to more accurately evaluate the target parameter. Therefore, a balance between the input data and their statistical characteristics must be elaborated. By doing this, a wider range of data can be analyzed and a model with higher power can be developed. Since these models have used two optimization algorithms to improve the performance of the base model, some other optimization techniques such as the whale optimization algorithm can be examined to increase the base model performance. The base model in this research was made using the FS model, which has special features, while by changing the basic model to other predictive models such as neuro-fuzzy, new results can be achieved. The last future direction of this research can be related to increasing the number of data samples with circular cross sections to develop a new model with a level of more generalization.

8. Conclusions

In this study, a novel artificial intelligence-based prediction model is used to correctly evaluate CCFST columns’ axial compression capacity. FS and two recent nature meta-heuristic optimization methods known as FFA and DE were combined to create two hybrid FS-FFA and FS-DE models. It was also combined with two common optimization techniques, the GA and PSO. An extensive database of 410 experimental tests for the CCFST columns was gathered from openly available papers for this research project. A statistical and visual analysis was undertaken to determine the effectiveness and correctness of the findings, and the following conclusions can be reached.
According to the research findings, the suggested hybridization models outperformed the basic FS model when it came to resolving the axial compression capacity problem. The findings showed that the FS-FFA, FS-DE, FS-GA, and FS-PSO models outperformed FS in terms of prediction accuracy for training data by 9.68%, 6.58%, 5.68%, and 1.56%, respectively. According to all performance assessments, the new suggested FS-FFA model is optimal for the prediction of the axial compression capacity of CCFTS columns, with improved RMSE and a20-index compared with FS-DE. Additionally, the proposed model achieved a significantly improved prediction of the ultimate compressive load compared to available design code predictions. In particular, RMSE of the FS-FFA model was reduced by 47% from AIJ [73] and more from the EN1994 [71] and AISC360 [72], whereas a20-index was also considerably increased.
The base model in this research was made using the FS model, which has special features, while by changing the basic model to other predictive models such as neuro-fuzzy, new results can be achieved. The last future direction of this research can be related to increasing the number of data samples with circular cross sections to develop a new model with a greater generalization level.
This model’s performance and machine learning methods are largely reliant on the database used. However, a more sophisticated and bigger database may have significant effects on the hybrid FS model’s final outcomes. Other optimization techniques such as the whale optimization algorithm can be examined to increase the base model performance. Furthermore, other sections’ geometries of CFTS, such as squares and round-ended squares, can also be investigated by the proposed hybrid models in this research. Close form equations of this issue using machine learning models will be very beneficial to engineering in the future.

Author Contributions

Conceptualization, P.G.A., M.K., A.S.M. and D.J.A.; Data curation, P.G.A., M.K., A.S.M., M.E.L., A.D.S. and C.M.; Formal analysis, J.L., M.K., A.S.M., L.C., M.Z.T. and A.D.S.; Supervision, P.G.A., A.S.M. and D.J.A.; Writing—original draft, P.G.A., M.K., A.S.M., D.J.A. and J.L.; Writing—review and editing, P.G.A., L.C., M.K., A.S.M., D.J.A., J.L., M.E.L., M.Z.T. and C.M. All authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

The data presented in this study are available in Appendix A.

Conflicts of Interest

The authors confirm that this article content has no conflict of interest.

Nomenclature

DEdifferential evolution
Ddiameter
HSharmony search
CFSTconcrete-filled steel tubular
CCFSTcircular concrete-filled steel tubular
FSfuzzy systems
FFAfirefly algorithm
fcthe compressive strength
fythe steel tube yield stress
PSOparticle swarm optimization
Lcolumn length
tthickness
GAgenetic algorithm
R2coefficient of determination
RMSEroot mean square error
Pexpultimate axial compressive load
Npoppopulation
MLmachine learning

Appendix A

Table A1. The database used for analysis in this study.
Table A1. The database used for analysis in this study.
Dataset Numberfc (MPa)D (mm)L (mm)t (mm)fy (MPa)Pexp (KN)
134.04601801.48307215
251.3101.9305.73.03371926
334.08601801.48307220
4164.4114.32006.34282866
5103.41003001.94041100
6103.41003001.94041125
7103.41003001.94041170
851.3101.5304.53.03371859
923.1101.6304.83.03371635
1023.2101.6304.83.03371635
1140101.6304.83.03371864
1293.6114.573003.993431308
1334.1101.7203.33.07605.11112.10
1440101.7305.13.03371803
1548.3165562.52.82363.31759
1623101.8305.43.03371679
1723.2101.8305.43.03371632
1840.2101.6304.83.03371864
1951101.9305.73.03371926
2034.08601801.48307215
2125.41083246.478532275
2256.99114.3342.96342.951425.3
2340.51083246.478532402
2443.910812964336839
2543.9210832443361235
26771083246.478532713
2740.51093276.478532446
282511412505.914861177
29371148501.79266515
303711485064861334
3131.9114.09300.53.85343948
3297.2114.263003.933431359
3357.6114.293003.753431067
3431.7114.311433.35287.3563.6
3531.7114.3342.93.35287.3816.2
3631.7114.311436343909.7
3731.7114.3800.163431000.4
3831.7114.3571.563431218.7
3931.75114.3342.93.35287.33816.2
4031.75114.3342.96342.951380
4156.9114.3342.93.35287.33995.7
4225.41083246.478532275
4357114.311433.35287.3904.2
4457114.3571.53.35287.3937
4557114.3342.93.35287.3995.7
4657114.3800.163431244.4
4757114.3571.563431389.3
4886.1114.3342.963431673.9
4986.2114.311433.35287.31200
5086.2114.3571.53.35287.31281.4
5186.2114.3114363431389.1
5286.2114.3800.163431509.3
5386.2114.3571.563431564.7
5486.21114.3342.93.35287.331242.2
5586.21114.3342.96342.951673.9
5688.8114.3342.93.35287.31136.20
5788.8114.3571.53.35287.31180.70
58102.4114.311433.35287.31481.2
59102.4114.3800.13.35287.31513.5
60102.4114.3571.53.35287.31598.9
61102.4114.3342.93.35287.31610.6
62102.4114.3114363431613.5
63102.4114.3800.163431788.9
64102.4114.3571.563431827.1
65102.43114.3342.93.35287.331610.6
66102.43114.3342.96342.951943.4
67107.2114.33002.742351295.10
68107.2114.36005.93551968.10
69164.35114.32006.34282595
70164.35114.32006.34282866
7137.5601801.48307215
72173.5114.32503.64032340
73173.5114.32503.64032422
74173.5114.32506.34032610
7531.4114.433003.98343948
7657.6114.49299.33.753431038
7798.9114.543003.843431359
7840.2101.7305.13.03371803
7934.7114.88300.54.913651380
8089.21153004.923651787
8157.6115.02300.55.023651413
82104.9115.043004.923651787
8323.2101.8305.43.03371679
8434.081203601.48307610
8534.081203601.48307660
8636.615965053902120
8764.21596504.84332210
8856.11655812.82363.32040
89110.612137052952016
90116.712137052951996
9125.41223664.545761509
9225.41223664.545761509
9340.21223664.545761657
9440.51223664.545761657
9540.51223664.545761663
9640.51223664.545761663
97771223664.545762100
9877.21223664.545762100
99110.6127.43905.72952217
100116.7127.43905.72952266
101116.7127.43908.52953106
10242.11334652.9325476
10342.11334654.5325492
10442.11334654.5325576
10542.213327304.5325282
10642.213327304.5325293
10742.213316704.5325335
10842.213316704.5325347
10942.213316704.5325412
11042.213316704.5325430
11142.21334652.9325466
11242.21334652.9325476
11342.21334654.5325500
11442.21334654.5325559
11542.21334654.5325576
11642.21334654.5325591
11742.213318624.5325715
11842.213327934.5325784
11942.213327934.5325800
1209513340552952002
121110.613340552952142
122116.713340552952178
12328.21406356.685372715
12452.51404204.421020.003020
12552.51404208.368134436
12652.514042010.467735420
1271251404206.213593202
1281251404208.193893354
1291251404208.193893398
13012514042011.583674104
13112514042011.583674300
1321251404204.421020.004312
1331251404204.421020.004516
13412514042016.723895120
1351251404206.271153.005386
1361251404208.368135502
13712514042010.467736187
13812514042010.467736339
13940.51494472.963081080
140771494472.963081781
14177.11494472.963081781
142951524655.52952662
143116.71524655.52952851
144170152.4942.98.8392.63919.9
145170152.4551.98.8392.64200.8
146178.4152.4940.26.3373.43584.7
147178.4152.4552.76.3373.44033
148178.8152.4943.88.8392.64099.8
149180.9152.4949.75445.93383.4
150182.8152.4950.55445.93995.7
151182.8152.4540.75445.94224
152185.7152.4947.36.3373.43535.3
153185.7152.4554.76.3373.43808
154185.7152.4951.38.8392.64178.7
155185.7152.4559.78.8392.64288.5
156185.8152.4951.35445.93724.1
157185.8152.4548.55445.93997.5
158188.1152.45536.3373.43692.8
159188.1152.4948.56.3373.43861.1
16042152.6304.94.93633.42909.10
16143.4152.6304.94.9633.42913.60
16237.51203601.48307660
16336.61596506.84022830
16436.6159650103553400
16564.11596504.84332210
166381655712.82363.31649
16737.51203601.48307660
16848.31906581.52306.11841
16948.2165562.52.82363.31759
17064.51596504.84332240
17193.615965053902970
17293.6159650103553400
17393.815965053902970
17493.81596506.84023410
175106159.635004.982701454
17671159.725005.22811562
177101159.730004.972751636
17870159.820005.012831650
17973159.830005.12761468
180100159.825005.012751818
181102159.840004.972701333
18245159.940004.982811091
18340160.120004.982801261
18474160.135004.982761326
185100160.12004.992752550
18641160.225004.962811244
18771160.240005.022811231
18843160.3300052701236
18999160.320005.032812000
190158.46164.26522.53773501
19164.31596504.84332210
19238.11655712.82363.31649
19364.21596504.84332240
19448.1165562.52.82363.31759
19538.11906571.13185.71308
19637.51203601.48307610
197341203601.48307660
19895.8168.66453.93633339
19956.41655812.82363.32040
20067.91655002.763502250
20167.941655002.813502160
20267.941655002.763502250
203771655711.82363.32608
20434.081805401.483071280
20580.2165580.52.82363.32295
206108165577.52.82363.32673
20774.7190663.50.86210.72451
20829.5165.22003.73661630.56
20943.5165.22003.73661676.42
21043.5165.22003.73661737.94
21158165.22003.73662094.15
21258165.22003.73662221.62
21381.6165.22003.73662511.3
21481.6165.22003.73662922.24
215158.7168.16458.14095254
21648.21906581.52306.11841
21736.2168.66453.93631771
21856.31655812.82363.32040
21995.8168.66453.93633339
220165.49168.66483.93634216
22177.11906640.86210.72553
222158.75168.76455.24054751
223151.9168.86505.74524930
22456.4190664.50.86210.71940
225167.871696454.83994330
22638.21655712.82363.31649
227341805401.483071280
22838.2216.5649.56.614524200
22934.081805401.483071311
23037.21805401.483071280
23164.41596504.84332210
23237.51805401.483071311
233158.4618975633984837
23438190657.50.86210.71240
235381906571.13185.71308
23638.1190657.50.86210.71240
2371081906601.94256.43360
23838.1190659.51.94256.41652
23938.2190657.50.86210.71240
24041.13009002.962793277
24177.11655712.82363.32608
24248.11906581.52306.11841
243151.91168.86505.74524930
24477.21906561.94256.43083
24556.1190664.50.86210.71940
24656.2190661.51.13185.71862
24756.2190664.50.86210.71940
24856.2190655.51.94256.42338
24956.4190661.51.13185.71862
250165.5168.66483.93634216
25137.51805401.483071280
25274.2190657.50.86210.72433
253113.51906602271.93360
254113.5165577.53364.32673
25574.7190663.51.94256.42592
256771906640.86210.72553
257771906581.52306.12830
258772226666.478437304
259167.91696454.83994330
26077.11906581.52306.12830
26177.11906561.94256.43083
26239.2318.4955.210.373357742
26324.3216.5649.56.614523568
26480.1190662.51.13185.72295
26580.2190663.51.52306.12602
26680.2190658.51.52306.12870
26785.14501350.002.9627911,665
2681081906611.13185.73220
269108190661.51.52306.13260
27038.2190659.51.94256.41652
271108.1190661.51.13185.73220
27240.52226666.478435714
273113.51906601.15184.83058
274113.51906620.95211.23070
275113.5190661.51.55315.33260
27625.43371011.006.478238475
27746.7216.4649.26.614524283
27824.1216.5649.56.614523568
27956.4190655.51.94256.42338
28038.1216.5649.56.614524200
28141.133710116.478239835
2821082197086.33005410
283148.8219.16006.33006838
284163219.16006.33006915
285174.5219.16006.33007569
286175.4219.16006.33007407
287185.1219.160053807837
288185.1219.1600103819085
28925.42226666.478434964
290108.21906611.13185.73220
29126.95501000.001654628,830
292772226666.478437304
29377.21906581.52306.12830
29440.52387144.545073583
29540.52387144.545073647
29625.42397174.545073035
29774.7190657.50.86210.72433
29834.082407201.483072150
29934.082407201.483072300
30041.13371011.006.478239668
30137.52407201.483072150
30241.136110834.545257260
30338.21906571.13185.71308
30425.43019032.962792382
30580.33019032.962795540
30652.2318.3954.910.373359297
30739.1318.4955.210.373357742
308771906561.94256.43083
30924.2318.5955.510.373356901
31092.3323.91000.005.6443.911,481
31125.433710116.478238475
31234.012407201.483072300
31341.133710116.478239668
314158.75168.16458.14095254
31537.52407201.483072300
31641.13371011.006.478239835
31785.133710116.4782313,776
31841.136010804.545257045
31985.136010804.5452511,505
32037.22407201.483072300
32141.13611083.004.545257260
32225.445013502.962794415
32341.145013502.962796870
32441.145013502.962796985
32585.145013502.9627911,665
3261081906601.13185.73058
32740.52226666.478435714
32826.95501000.001654629,590
32937.5601801.48307215
330103.41003001.94041085.00
33151.3101.5304.53.03371859
33233.9101.7203.33.07605.11067.60
33323.2101.8305.43.03371632
33440.51093276.478532446
3352511412805.944861285
336371148503.35291785
337371148504.44332902
33831.7114.3800.13.35287.3736.8
33931.7114.3571.53.35287.3749.4
34031.7114.3342.963431380
34131.9114.33003.85343998
34257114.3800.13.35287.3932.9
34357114.3114363431141.3
34457114.3342.963431425.3
34586.2114.3800.13.35287.31206.5
34686.2114.3342.93.35287.31242.2
347102.4114.3342.963431943.4
348105.5114.3571.53.35287.31407.10
349105.5114.3342.93.35287.31453.10
350107.2114.36002.742351296.60
351107.2114.33005.93551989.90
352173.5114.32506.34032633
35398.9114.37299.53.853431182
35434.7114.433003.82343929
35584.1114.53003.843431359
35679.6114.63003.993431308
35777.11906621.13185.72630
35895127.43908.52952544
359110.6127.43908.52952623
36042.213327304.5325268
36142.213316704.5325416
36242.21334654.5325568
36342.21334654.5325582
36442.213318624.5325882
36552.51404206.271153.004274
3661251404206.213593215
36712514042016.723895135
3681251404206.271153.005354
36995127.43905.72952078
37025.41494472.96308941
37140.51494472.963081064
372110.61524655.52952734
373178.8152.4549.88.8392.64354.1
37493.8159650103553400
37577.1190662.51.13185.72630
37680190658.51.52306.12870
377158.5164.26522.53773501
37867.91655002.813502160
37941160.235004.972731193
38029.5165.22003.73661428.32
38136.2168.66453.93631771
382158.7168.76455.24054751
383158.518975633984837
38438.2190659.51.94256.41652
38556.4190661.51.13185.71862
38656.4190655.51.94256.42338
38774.7190657.50.86210.72433
38877.11906640.86210.72553
38993.81596506.84023410
3901251404208.368135531
39177.11906621.13185.72630
392771655712.82363.32608
39380.2190658.51.52306.12870
3941081906620.86210.73070
39546.7216.4649.26.614524283
39625.42226666.478434964
39740.42226666.478435638
39840.52226666.478435638
399772387144.545075578
400772387144.545075578
40141.13009002.962793152
40280.33019032.962795540
40352.2318.3954.910.373359297
40424.2318.5955.510.373356901
40585.13371011.006.4782313,776
40641.13601080.004.545257045
40785.13601080.004.5452511,505
40825.23611083.004.545255633
40925.436110834.545255633
41026.95501000.001654629,050

References

  1. Wang, F.; Han, L.; Li, W. Analytical behavior of CFDST stub columns with external stainless steel tubes under axial compression. Thin-Walled Struct. 2018, 127, 756–768. [Google Scholar] [CrossRef]
  2. Design, A.S. Specification for structural steel buildings. AISC Dec. 1999, 27, 1–210. [Google Scholar]
  3. Nishiyama, I. Summary of Research on Concrete-Filled Structural Steel Tube Column System Carried out under the US-Japan Cooperative Research Program on Composite and Hybrid Structures; Building Research Institution: Uttarakhand, India, 2002. [Google Scholar]
  4. Kim, D.K. A Database for Composite Columns. 2005. Available online: http://hdl.handle.net/1853/7126 (accessed on 20 May 2005).
  5. Han, L.H. Concrete Filled Steel Tube Structures-Theory and Application; Science Press: Beijing, China, 2007. [Google Scholar]
  6. Cederwall, K.; Engstrom, B.; Grauers, M. High-strength concrete used in composite columns. Spec. Publ. 1990, 121, 195–214. [Google Scholar]
  7. Varma, A.H. Seismic Behavior, Analysis, and Design of High Strength Square Concrete Filled Steel Tube (CFT) Columns; Lehigh University: Bethlehem, PA, USA, 2001. [Google Scholar]
  8. Uy, B. Strength of short concrete filled high strength steel box columns. J. Constr. Steel Res. 2001, 57, 113–134. [Google Scholar] [CrossRef]
  9. Liu, D.; Gho, W.-M.; Yuan, J. Ultimate capacity of high-strength rectangular concrete-filled steel hollow section stub columns. J. Constr. Steel Res. 2003, 59, 1499–1515. [Google Scholar] [CrossRef]
  10. Mursi, M.; Uy, B. Strength of slender concrete filled high strength steel box columns. J. Constr. Steel Res. 2004, 60, 1825–1848. [Google Scholar] [CrossRef]
  11. Sakino, K.; Nakahara, H.; Morino, S.; Nishiyama, I. Behavior of centrally loaded concrete-filled steel-tube short columns. J. Struct. Eng. 2004, 130, 180–188. [Google Scholar] [CrossRef]
  12. Lue, D.M.; Liu, J.-L.; Yen, T. Experimental study on rectangular CFT columns with high-strength concrete. J. Constr. Steel Res. 2007, 63, 37–44. [Google Scholar] [CrossRef]
  13. Aslani, F.; Uy, B.; Tao, Z.; Mashiri, F. Behaviour and design of composite columns incorporating compact high-strength steel plates. J. Constr. Steel Res. 2015, 107, 94–110. [Google Scholar] [CrossRef]
  14. Xiong, M.-X.; Xiong, D.-X.; Liew, J.Y.R. Axial performance of short concrete filled steel tubes with high-and ultra-high-strength materials. Eng. Struct. 2017, 136, 494–510. [Google Scholar] [CrossRef]
  15. Lai, Z.; Varma, A.H. High-strength rectangular CFT members: Database, modeling, and design of short columns. J. Struct. Eng. 2018, 144, 4018036. [Google Scholar] [CrossRef]
  16. Gardner, N.J.; Jacobson, E.R. Structural behavior of concrete filled steel tubes. J. Proc. 1967, 64, 404–413. [Google Scholar]
  17. Bergmann, R. Load introduction in composite columns filled with high strength concrete. In Tubular Structures VI; Routledge: Oxfordshire, UK, 2021; pp. 373–380. [Google Scholar]
  18. O’Shea, M.D.; Bridge, R.Q. Circular thin-walled tubes with high strength concrete infill. In Proceedings of the Composite Construction in Steel and Concrete III, New York, NY, USA, 9–14 June 1996; pp. 780–793. [Google Scholar]
  19. Schneider, S.P. Axially loaded concrete-filled steel tubes. J. Struct. Eng. 1998, 124, 1125–1138. [Google Scholar] [CrossRef]
  20. O’Shea, M.D.; Bridge, R.Q. Design of circular thin-walled concrete filled steel tubes. J. Struct. Eng. 2000, 126, 1295–1303. [Google Scholar] [CrossRef]
  21. Giakoumelis, G.; Lam, D. Axial capacity of circular concrete-filled tube columns. J. Constr. Steel Res. 2004, 60, 1049–1068. [Google Scholar] [CrossRef]
  22. Zeghiche, J.; Chaoui, K. An experimental behaviour of concrete-filled steel tubular columns. J. Constr. Steel Res. 2005, 61, 53–66. [Google Scholar] [CrossRef]
  23. Yu, Q.; Tao, Z.; Wu, Y.-X. Experimental behaviour of high performance concrete-filled steel tubular columns. Thin-Walled Struct. 2008, 46, 362–370. [Google Scholar] [CrossRef]
  24. de Oliveira, W.L.A.; De Nardin, S.; de Cresce El, A.L.H.; El Debs, M.K. Influence of concrete strength and length/diameter on the axial capacity of CFT columns. J. Constr. Steel Res. 2009, 65, 2103–2110. [Google Scholar] [CrossRef]
  25. Liew, J.Y.R.; Xiong, D.X. Effect of preload on the axial capacity of concrete-filled composite columns. J. Constr. Steel Res. 2009, 65, 709–722. [Google Scholar] [CrossRef]
  26. Chen, G.; Xu, Z.; Yang, Z.; Tian, Z. Experimental study on behavior of short steel tubular columns filled with ultra-high strength concrete mixed with stone-chip subjected to axial load. J. Build. Struct. 2011, 32, 82–89. [Google Scholar]
  27. Tang, D.; Gordan, B.; Koopialipoor, M.; Jahed Armaghani, D.; Tarinejad, R.; Thai Pham, B.; Huynh, V. Van seepage analysis in short embankments using developing a metaheuristic method based on governing equations. Appl. Sci. 2020, 10, 1761. [Google Scholar] [CrossRef] [Green Version]
  28. Ye, J.; Koopialipoor, M.; Zhou, J.; Armaghani, D.J.; He, X. A novel combination of tree-based modeling and monte carlo simulation for assessing risk levels of flyrock induced by mine blasting. Nat. Resour. Res. 2020, 30, 225–243. [Google Scholar] [CrossRef]
  29. Yang, H.; Wang, Z.; Song, K. A new hybrid grey wolf optimizer-feature weighted-multiple kernel-support vector regression technique to predict TBM performance. Eng. Comput. 2020, 1–17. [Google Scholar] [CrossRef]
  30. Zhou, J.; Chen, C.; Wang, M.; Khandelwal, M. Proposing a novel comprehensive evaluation model for the coal burst liability in underground coal mines considering uncertainty factors. Int. J. Min. Sci. Technol. 2021, 31, 799–812. [Google Scholar] [CrossRef]
  31. Zhou, J.; Qiu, Y.; Khandelwal, M.; Zhu, S.; Zhang, X. Developing a hybrid model of Jaya algorithm-based extreme gradient boosting machine to estimate blast-induced ground vibrations. Int. J. Rock Mech. Min. Sci. 2021, 145, 104856. [Google Scholar] [CrossRef]
  32. Zhou, J.; Li, X.; Mitri, H.S. Classification of rockburst in underground projects: Comparison of ten supervised learning methods. J. Comput. Civ. Eng. 2016, 30, 4016003. [Google Scholar] [CrossRef]
  33. Asteris, P.G.; Cavaleri, L.; Ly, H.-B.; Pham, B.T. Surrogate models for the compressive strength mapping of cement mortar materials. Soft Comput. 2021, 25, 6347–6372. [Google Scholar] [CrossRef]
  34. Harandizadeh, H.; Armaghani, D.; Asteris Panagiotis, G.; Gandomi, A.H. TBM performance prediction developing a hybrid ANFIS-PNN predictive model optimized by imperialism competitive algorithm. Neural. Comput. Appl. 2021, 33, 16149–16179. [Google Scholar] [CrossRef]
  35. Mohammed, A.S.; Asteris, P.G.; Koopialipoor, M.; Alexakis, D.E.; Lemonis, M.E.; Armaghani, D.J. Stacking ensemble tree models to predict energy performance in residential buildings. Sustainability 2021, 13, 8298. [Google Scholar] [CrossRef]
  36. Armaghani, D.J.; Mamou, A.; Maraveas, C.; Roussis, P.C.; Siorikis, V.G.; Skentou, A.D.; Asteris, P.G. Predicting the unconfined compressive strength of granite using only two non-destructive test indexes. Geomech. Eng. 2021, 25, 317–330. [Google Scholar]
  37. Ke, B.; Khandelwal, M.; Asteris, P.G.; Skentou, A.D.; Mamou, A.; Armaghani, D.J. Rock-burst occurrence prediction based on optimized Naïve Bayes models. IEEE Access. 2021, 9, 91347–91360. [Google Scholar] [CrossRef]
  38. Asteris, P.G.; Lourenço, P.B.; Hajihassani, M.; Adami, C.-E.N.; Lemonis, M.E.; Skentou, A.D.; Marques, R.; Nguyen, H.; Rodrigues, H.; Varum, H. Soft computing-based models for the prediction of masonry compressive strength. Eng. Struct. 2021, 248, 113276. [Google Scholar] [CrossRef]
  39. Yang, H.; Koopialipoor, M.; Armaghani, D.J.; Gordan, B.; Khorami, M.; Tahir, M.M. Intelligent design of retaining wall structures under dynamic conditions. STEEL Compos. Struct. 2019, 31, 629–640. [Google Scholar]
  40. Asteris, P.G.; Lemonis, M.E.; Le, T.-T.; Tsavdaridis, K.D. Evaluation of the ultimate eccentric load of rectangular CFSTs using advanced neural network modeling. Eng. Struct. 2021, 248, 113297. [Google Scholar] [CrossRef]
  41. Nguyen, N.-H.; Vo, T.P.; Lee, S.; Asteris, P.G. Heuristic algorithm-based semi-empirical formulas for estimating the compressive strength of the normal and high performance concrete. Constr. Build. Mater. 2021, 304, 124467. [Google Scholar] [CrossRef]
  42. Asteris, P.G.; Lemonis, M.E.; Nguyen, T.-A.; Van Le, H.; Pham, B.T. Soft computing-based estimation of ultimate axial load of rectangular concrete-filled steel tubes. Steel Compos. Struct. 2021, 39, 471. [Google Scholar]
  43. Colesanti, C.; Wasowski, J. Investigating landslides with space-borne Synthetic Aperture Radar (SAR) interferometry. Eng. Geol. 2006, 88, 173–199. [Google Scholar] [CrossRef]
  44. Asteris, P.G.; Skentou, A.D.; Bardhan, A.; Samui, P.; Lourenço, P.B. Soft computing techniques for the prediction of concrete compressive strength using Non-Destructive tests. Constr. Build. Mater. 2021, 303, 124450. [Google Scholar] [CrossRef]
  45. Asteris, P.G.; Skentou, A.D.; Bardhan, A.; Samui, P.; Pilakoutas, K. Predicting concrete compressive strength using hybrid ensembling of surrogate machine learning models. Cem. Concr. Res. 2021, 145, 106449. [Google Scholar] [CrossRef]
  46. Bardhan, A.; Gokceoglu, C.; Burman, A.; Samui, P.; Asteris, P.G. Efficient computational techniques for predicting the California bearing ratio of soil in soaked conditions. Eng. Geol. 2021, 291, 106239. [Google Scholar] [CrossRef]
  47. Parsajoo, M.; Armaghani, D.J.; Mohammed, A.S.; Khari, M.; Jahandari, S. Tensile strength prediction of rock material using non-destructive tests: A comparative intelligent study. Transp. Geotech. 2021, 31, 100652. [Google Scholar] [CrossRef]
  48. Parsajoo, M.; Armaghani, D.J.; Asteris, P.G. A precise neuro-fuzzy model enhanced by artificial bee colony techniques for assessment of rock brittleness index. Neural. Comput. Appl. 2021, 1–19. [Google Scholar] [CrossRef]
  49. Pham, B.T.; Nguyen, M.D.; Nguyen-Thoi, T.; Ho, L.S.; Koopialipoor, M.; Quoc, N.K.; Armaghani, D.J.; Van Le, H. A novel approach for classification of soils based on laboratory tests using Adaboost, Tree and ANN modeling. Transp. Geotech. 2020, 27, 100508. [Google Scholar] [CrossRef]
  50. Mohamad, E.T.; Koopialipoor, M.; Murlidhar, B.R.; Rashiddel, A.; Hedayat, A.; Armaghani, D.J. A new hybrid method for predicting ripping production in different weathering zones through in-situ tests. Measurement 2019, 147, 106826. [Google Scholar] [CrossRef]
  51. Cai, M.; Koopialipoor, M.; Armaghani, D.J.; Thai Pham, B. Evaluating slope deformation of earth dams due to earthquake shaking using MARS and GMDH techniques. Appl. Sci. 2020, 10, 1486. [Google Scholar] [CrossRef] [Green Version]
  52. Huang, J.; Koopialipoor, M.; Armaghani, D.J. A combination of fuzzy Delphi method and hybrid ANN-based systems to forecast ground vibration resulting from blasting. Sci. Rep. 2020, 10, 1–21. [Google Scholar] [CrossRef] [PubMed]
  53. Guo, H.; Zhou, J.; Koopialipoor, M.; Armaghani, D.J.; Tahir, M.M. Deep neural network and whale optimization algorithm to assess flyrock induced by blasting. Eng. Comput. 2019, 37, 173–186. [Google Scholar] [CrossRef]
  54. Xu, C.; Gordan, B.; Koopialipoor, M.; Armaghani, D.J.; Tahir, M.M.; Zhang, X. Improving performance of retaining walls under dynamic conditions developing an optimized ANN based on ant colony optimization technique. IEEE Access 2019, 7, 94692–94700. [Google Scholar] [CrossRef]
  55. Yang, H.Q.; Xing, S.G.; Wang, Q.; Li, Z. Model test on the entrainment phenomenon and energy conversion mechanism of flow-like landslides. Eng. Geol. 2018, 239, 119–125. [Google Scholar] [CrossRef]
  56. Huang, L.; Asteris, P.G.; Koopialipoor, M.; Armaghani, D.J.; Tahir, M.M. Invasive weed optimization technique-based ANN to the prediction of rock tensile strength. Appl. Sci. 2019, 9, 5372. [Google Scholar] [CrossRef] [Green Version]
  57. Lu, S.; Koopialipoor, M.; Asteris, P.G.; Bahri, M.; Armaghani, D.J. A novel feature selection approach based on tree models for evaluating the punching shear capacity of steel fiber-reinforced concrete flat slabs. Materials 2020, 13, 3902. [Google Scholar] [CrossRef]
  58. Asteris, P.G.; Koopialipoor, M.; Armaghani, D.J.; Kotsonis, E.A.; Lourenço, P.B. Prediction of cement-based mortars compressive strength using machine learning techniques. Neural Comput. Appl. 2021, 33, 13089–13121. [Google Scholar] [CrossRef]
  59. Gao, J.; Koopialipoor, M.; Armaghani, D.J.; Ghabussi, A.; Baharom, S.; Morasaei, A.; Shariati, A.; Khorami, M.; Zhou, J. Evaluating the bond strength of FRP in concrete samples using machine learning methods. Smart Struct. Syst. 2020, 26, 403–418. [Google Scholar]
  60. Sarir, P.; Chen, J.; Asteris, P.G.; Armaghani, D.J.; Tahir, M.M. Developing GEP tree-based, neuro-swarm, and whale optimization models for evaluation of bearing capacity of concrete-filled steel tube columns. Eng. Comput. 2019, 37, 1–19. [Google Scholar] [CrossRef]
  61. Ahmadi, M.; Naderpour, H.; Kheyroddin, A. ANN model for predicting the compressive strength of circular steel-confined concrete. Int. J. Civ. Eng. 2017, 15, 213–221. [Google Scholar] [CrossRef]
  62. Ahmadi, M.; Naderpour, H.; Kheyroddin, A. Utilization of artificial neural networks to prediction of the capacity of CCFT short columns subject to short term axial load. Arch. Civ. Mech. Eng. 2014, 14, 510–517. [Google Scholar] [CrossRef]
  63. Güneyisi, E.M.; Gültekin, A.; Mermerdaş, K. Ultimate capacity prediction of axially loaded CFST short columns. Int. J. Steel Struct. 2016, 16, 99–114. [Google Scholar] [CrossRef]
  64. Ipek, S.; Güneyisi, E.M. Ultimate axial strength of concrete-filled double skin steel tubular column sections. Adv. Civ. Eng. 2019, 2019. [Google Scholar] [CrossRef] [Green Version]
  65. Moon, J.; Kim, J.J.; Lee, T.-H.; Lee, H.-E. Prediction of axial load capacity of stub circular concrete-filled steel tube using fuzzy logic. J. Constr. Steel Res. 2014, 101, 184–191. [Google Scholar] [CrossRef]
  66. Al-Khaleefi, A.M.; Terro, M.J.; Alex, A.P.; Wang, Y. Prediction of fire resistance of concrete filled tubular steel columns using neural networks. Fire Saf. J. 2002, 37, 339–352. [Google Scholar] [CrossRef]
  67. Ren, Q.; Li, M.; Zhang, M.; Shen, Y.; Si, W. Prediction of ultimate axial capacity of square concrete-filled steel tubular short columns using a hybrid intelligent algorithm. Appl. Sci. 2019, 9, 2802. [Google Scholar] [CrossRef] [Green Version]
  68. Tran, V.-L.; Thai, D.-K.; Kim, S.-E. Application of ANN in predicting ACC of SCFST column. Compos. Struct. 2019, 228, 111332. [Google Scholar] [CrossRef]
  69. Lee, S.; Vo, T.P.; Thai, H.-T.; Lee, J.; Patel, V. Strength prediction of concrete-filled steel tubular columns using Categorical Gradient Boosting algorithm. Eng. Struct. 2021, 238, 112109. [Google Scholar] [CrossRef]
  70. Zarringol, M.; Thai, H.-T.; Thai, S.; Patel, V. Application of ANN to the design of CFST columns. Structures 2020, 28, 2203–2220. [Google Scholar] [CrossRef]
  71. The European Union. European C. for Design of Composite Steel and Concrete Structures; CEN: Salt Lake City, UT, USA, 1994. [Google Scholar]
  72. Committee, A. Specification for Structural Steel Buildings; ANSI/AISC 360-10; American Institute of Steel Construction: Chicago, IL, USA, 22 June 2010. [Google Scholar]
  73. AIJ. Recommendations for design and construction of concrete filled steel tubular structures. Open J. Civ. Eng. 1997, 3, 3. [Google Scholar]
  74. Zadeh, L.A. A fuzzy-algorithmic approach to the definition of complex or imprecise concepts. Int. J. Man. Mach. Stud. 1976, 8, 249–291. [Google Scholar] [CrossRef]
  75. Wang, L.-X. A Course in Fuzzy Systems; Prentice-Hall International, Inc.: Hoboken, NJ, USA, 1999. [Google Scholar]
  76. Ali, M.M.; Khompatraporn, C.; Zabinsky, Z.B. A numerical evaluation of several stochastic algorithms on selected continuous global optimization test problems. J. Glob. Optim. 2005, 31, 635–672. [Google Scholar] [CrossRef]
  77. Yang, X.-S. Firefly algorithm, stochastic test functions and design optimisation. Int. J. Bio-Inspired Comput. 2010, 2, 78–84. [Google Scholar] [CrossRef]
  78. Kaur, M.; Ghosh, S. Network reconfiguration of unbalanced distribution networks using fuzzy-firefly algorithm. Appl. Soft Comput. 2016, 49, 868–886. [Google Scholar] [CrossRef]
  79. Zhang, Y.; Wu, L. A novel method for rigid image registration based on firefly algorithm. Int. J. Res. Rev. Soft Intell. Comput. 2012, 2, 141–146. [Google Scholar]
  80. Apostolopoulos, T.; Vlachos, A. Application of the firefly algorithm for solving the economic emissions load dispatch problem. Int. J. Comb. 2010, 2011. [Google Scholar] [CrossRef] [Green Version]
  81. Koopialipoor, M.; Fahimifar, A.; Ghaleini, E.N.; Momenzadeh, M.; Armaghani, D.J. Development of a new hybrid ANN for solving a geotechnical problem related to tunnel boring machine performance. Eng. Comput. 2019, 36, 345–357. [Google Scholar] [CrossRef]
  82. Koopialipoor, M.; Noorbakhsh, A.; Noroozi Ghaleini, E.; Jahed Armaghani, D.; Yagiz, S. A new approach for estimation of rock brittleness based on non-destructive tests. Nondestruct. Test. Eval. 2019, 34, 354–375. [Google Scholar] [CrossRef]
  83. Gholizadeh, S.; Barati, H. A comprative study of three metaheuristics for optimum design of trusses. Int. J. Optim. Civ. Eng. 2012, 2, 3. [Google Scholar]
  84. Hancer, E.; Xue, B.; Zhang, M. Differential evolution for filter feature selection based on information theory and feature ranking. Knowl. Based Syst. 2018, 140, 103–119. [Google Scholar] [CrossRef]
  85. Bidar, M.; Sadaoui, S.; Mouhoub, M.; Bidar, M. Enhanced firefly algorithm using fuzzy parameter tuner. Comput. Inf. Sci. 2018, 11, 26–51. [Google Scholar] [CrossRef]
  86. Mai, S.H.; Seghier, M.E.A.B.; Nguyen, P.L.; Jafari-Asl, J.; Thai, D.-K. A hybrid model for predicting the axial compression capacity of square concrete-filled steel tubular columns. Eng. Comput. 2020, 1–18. [Google Scholar] [CrossRef]
  87. Wang, Y.; Geng, Y.; Ranzi, G.; Zhang, S. Time-dependent behaviour of expansive concrete-filled steel tubular columns. J. Constr. Steel Res. 2011, 67, 471–483. [Google Scholar] [CrossRef]
  88. Geng, Y.; Wang, Y.; Chen, J. Time-dependent behaviour of steel tubular columns filled with recycled coarse aggregate concrete. J. Constr. Steel Res. 2016, 122, 455–468. [Google Scholar] [CrossRef]
  89. Dong, J.F.; Wang, Q.Y.; Guan, Z.W. Structural behaviour of recycled aggregate concrete filled steel tube columns strengthened by CFRP. Eng. Struct. 2013, 48, 532–542. [Google Scholar] [CrossRef]
  90. Wang, Y.; Chen, J.; Geng, Y. Testing and analysis of axially loaded normal-strength recycled aggregate concrete filled steel tubular stub columns. Eng. Struct. 2015, 86, 192–212. [Google Scholar] [CrossRef]
  91. Chen, J.; Wang, Y.; Roeder, C.W.; Ma, J. Behavior of normal-strength recycled aggregate concrete filled steel tubes under combined loading. Eng. Struct. 2017, 130, 23–40. [Google Scholar] [CrossRef]
  92. Yang, Y.-F.; Ma, G.-L. Experimental behaviour of recycled aggregate concrete filled stainless steel tube stub columns and beams. Thin-Walled Struct. 2013, 66, 62–75. [Google Scholar] [CrossRef]
  93. Wang, Y.; Geng, Y.; Chang, Y.; Zhou, C. Time-dependent behaviour of recycled concrete filled steel tubes using RCA from different parent waste material. Constr. Build. Mater. 2018, 193, 230–243. [Google Scholar] [CrossRef]
  94. Wei, J.; Luo, X.; Lai, Z.; Varma, A.H. Experimental behavior and design of high-strength circular concrete-filled steel tube short columns. J. Struct. Eng. 2020, 146, 4019184. [Google Scholar] [CrossRef]
  95. Le Hoang, A.; Fehling, E. Numerical study of circular steel tube confined concrete (STCC) stub columns. J. Constr. Steel Res. 2017, 136, 238–255. [Google Scholar] [CrossRef]
  96. He, L.; Zhao, Y.; Lin, S. Experimental study on axially compressed circular CFST columns with improved confinement effect. J. Constr. Steel Res. 2018, 140, 74–81. [Google Scholar] [CrossRef]
  97. Koopialipoor, M.; Jahed Armaghani, D.; Haghighi, M.; Ghaleini, E.N. A neuro-genetic predictive model to approximate overbreak induced by drilling and blasting operation in tunnels. Bull. Eng. Geol. Environ. 2017, 78, 981–990. [Google Scholar] [CrossRef]
  98. Koopialipoor, M.; Ghaleini, E.N.; Tootoonchi, H.; Jahed Armaghani, D.; Haghighi, M.; Hedayat, A. Developing a new intelligent technique to predict overbreak in tunnels using an artificial bee colony-based ANN. Environ. Earth Sci. 2019, 78, 165. [Google Scholar] [CrossRef]
  99. Yu, C.; Koopialipoor, M.; Murlidhar, B.R.; Mohammed, A.S.; Armaghani, D.J.; Mohamad, E.T.; Wang, Z. Optimal ELM–Harris Hawks optimization and ELM–Grasshopper optimization models to forecast peak particle velocity resulting from mine blasting. Nat. Resour. Res. 2021, 30, 2647–2662. [Google Scholar] [CrossRef]
  100. Koopialipoor, M.; Nikouei, S.S.; Marto, A.; Fahimifar, A.; Armaghani, D.J.; Mohamad, E.T. Predicting tunnel boring machine performance through a new model based on the group method of data handling. Bull. Eng. Geol. Environ. 2018, 78, 3799–3813. [Google Scholar] [CrossRef]
  101. Armaghani, D.J.; Koopialipoor, M.; Bahri, M.; Hasanipanah, M.; Tahir, M.M. A SVR-GWO technique to minimize flyrock distance resulting from blasting. Bull. Eng. Geol. Environ. 2020, 79, 4369–4385. [Google Scholar] [CrossRef]
  102. Armaghani, D.J.; Yagiz, S.; Mohamad, E.T.; Zhou, J. Prediction of TBM performance in fresh through weathered granite using empirical and statistical approaches. Tunn. Undergr. Space Technol. 2021, 118, 104183. [Google Scholar] [CrossRef]
Figure 1. Base of firefly algorithm (FFA).
Figure 1. Base of firefly algorithm (FFA).
Buildings 11 00629 g001
Figure 2. Pseudo-code of the differential evolution (DE).
Figure 2. Pseudo-code of the differential evolution (DE).
Buildings 11 00629 g002
Figure 3. The general flowchart developed in this research.
Figure 3. The general flowchart developed in this research.
Buildings 11 00629 g003
Figure 4. Results of training phase: (a) FS-FFA model, (b) FS-DE model.
Figure 4. Results of training phase: (a) FS-FFA model, (b) FS-DE model.
Buildings 11 00629 g004
Figure 5. Results of testing phase: (a) FS-FFA model, (b) FS-DE model.
Figure 5. Results of testing phase: (a) FS-FFA model, (b) FS-DE model.
Buildings 11 00629 g005
Figure 6. Experimental vs. predicted ratios: (a) the FS-FFA model, (b) the FS-DE model, (c) the AIJ design code model [73], (d) the EN1994 design code model [71], (e) the AISC360 design code model [72].
Figure 6. Experimental vs. predicted ratios: (a) the FS-FFA model, (b) the FS-DE model, (c) the AIJ design code model [73], (d) the EN1994 design code model [71], (e) the AISC360 design code model [72].
Buildings 11 00629 g006
Table 1. Design codes application limits, related to circular CFSTs.
Table 1. Design codes application limits, related to circular CFSTs.
Code f y
(MPa)
f c
(MPa)
Section SlendernessOther
EN1994 [71] 235 f y 460 25 f c 50 d t 90 235   MPa f y 0.2 A s f y N p 0.9
AISC 360 [72] f y 525 21 f c 69 d t 0.31 E s f y A s 0.01 A s c
AIJ [73] 235 f y 355 18 f c 60 d t 1.5 23500   MPa min { f y ; 0.7 f u } L e B 50
Asc, As, and Ac are the areas of the total cross section, the steel tube and the concrete core, respectively Le is the column effective length.
Table 2. General information of dataset.
Table 2. General information of dataset.
ParameterUnitMinAverageMaxSDT
Lmm180720.734000594.56
Dmm60169.4155074.04
tmm0.864.4716.722.59
fyMPa184.8388.381153170.29
fcMPa23.274.98188.144.01
PexpKN2152992.71295903213.2
Table 3. The final result of hybrid fuzzy system (FS) models.
Table 3. The final result of hybrid fuzzy system (FS) models.
ModelTrainingTesting
a20-IndexR2RMSEa20-IndexR2RMSE
FS-FFA0.96040.9854482.03620.86590.9880415.4471
FS-DE0.96340.9571655.47080.86590.9876419.4502
Table 4. Performance indices on the testing datasets.
Table 4. Performance indices on the testing datasets.
RankingModela20-IndexR2RMSE
1FS-FFA0.86590.9880415.4471
2FS-DE0.86590.9876419.4502
3AIJ [73]0.63410.9842786.3858
4EN1994 [71]0.57320.96811119.6477
5AISC 360 [72]0.36590.98141330.6249
Publisher’s Note: MDPI stays neutral with regard to jurisdictional claims in published maps and institutional affiliations.

Share and Cite

MDPI and ACS Style

Liao, J.; Asteris, P.G.; Cavaleri, L.; Mohammed, A.S.; Lemonis, M.E.; Tsoukalas, M.Z.; Skentou, A.D.; Maraveas, C.; Koopialipoor, M.; Armaghani, D.J. Novel Fuzzy-Based Optimization Approaches for the Prediction of Ultimate Axial Load of Circular Concrete-Filled Steel Tubes. Buildings 2021, 11, 629. https://doi.org/10.3390/buildings11120629

AMA Style

Liao J, Asteris PG, Cavaleri L, Mohammed AS, Lemonis ME, Tsoukalas MZ, Skentou AD, Maraveas C, Koopialipoor M, Armaghani DJ. Novel Fuzzy-Based Optimization Approaches for the Prediction of Ultimate Axial Load of Circular Concrete-Filled Steel Tubes. Buildings. 2021; 11(12):629. https://doi.org/10.3390/buildings11120629

Chicago/Turabian Style

Liao, Jinsong, Panagiotis G. Asteris, Liborio Cavaleri, Ahmed Salih Mohammed, Minas E. Lemonis, Markos Z. Tsoukalas, Athanasia D. Skentou, Chrysanthos Maraveas, Mohammadreza Koopialipoor, and Danial Jahed Armaghani. 2021. "Novel Fuzzy-Based Optimization Approaches for the Prediction of Ultimate Axial Load of Circular Concrete-Filled Steel Tubes" Buildings 11, no. 12: 629. https://doi.org/10.3390/buildings11120629

Note that from the first issue of 2016, this journal uses article numbers instead of page numbers. See further details here.

Article Metrics

Back to TopTop