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Published in: International Journal of Concrete Structures and Materials 3/2012

Open Access 01-09-2012 | Article

Effective Prediction of Thermal Conductivity of Concrete Using Neural Network Method

Authors: Jong-Han Lee, Jong-Jae Lee, Baik-Soon Cho

Published in: International Journal of Concrete Structures and Materials | Issue 3/2012

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Abstract

The temperature distributions of concrete structures strongly depend on the value of thermal conductivity of concrete. However, the thermal conductivity of concrete varies according to the composition of the constituents and the temperature and moisture conditions of concrete, which cause difficulty in accurately predicting the thermal conductivity value in concrete. For this reason, in this study, back-propagation neural network models on the basis of experimental values carried out by previous researchers have been utilized to effectively account for the influence of these variables. The neural networks were trained by 124 data sets with eleven parameters: nine concrete composition parameters (the ratio of water–cement, the percentage of fine and coarse aggregate, and the unit weight of water, cement, fine aggregate, coarse aggregate, fly ash and silica fume) and two concrete state parameters (the temperature and water content of concrete). Finally, the trained neural network models were evaluated by applying to other 28 measured values not included in the training of the neural networks. The result indicated that the proposed method using a back-propagation neural algorithm was effective at predicting the thermal conductivity of concrete.

1 Introduction

Many accidental and environmental factors continue to produce and change heat flow within concrete structures. The magnitude of the temperature variance and resulting thermal behaviors primarily depend on the accuracy of thermal conductivity of concrete (TCC). Since concrete is a composite material composed of water, cement, fine aggregate, coarse aggregate, and other admixtures, the thermal conductivity value changes according to the combination of the concrete compositions including the volume faction and the unit weight of the constituents, and the ratio of water to cement. In addition to the mix proportion and constituents of concrete, many other variables such as quality control, water content, and temperature are directly associated with the value of the TCC. Consequently, the prediction of the TCC is limited and imprecise in the heat transfer and thermal structure analysis of concrete structures.
The age of concrete hardly affects the change in the TCC except for very early age of about two days due to hydration (Kim et al. 2003). Toyokazu and Yoshiro (1976) also found that the conductivity of concrete slightly increased during the first three days and became almost constant after the age of three days. Thus, this study focused on the value of the TCC in the dry state and accounted for the important variables, such as the mix proportioning, moisture and temperature status, and unit weight of concrete.
The testing methods and procedure for the measurement of the TCC are also complicated and time-consuming. In general, there are three methods of measuring the TCC: the two-linear parallel probe method, the plane heat source method, and the hot guarded plate method (Morabito 1989; Carslaw and Jaeger 1959; Nevile 1995). All the three methods based on similar basic principles require additional efforts to cut the specimen thin and firmly place the thermal probe on/in the specimen, as well as long time control of the dependent and independent variables during the entire testing. Moreover, the conditions of concrete structures exposed to real environmental conditions might differ from those experimentally controlled. Therefore, for the evaluation of temperature distributions and thermal behaviors in the current state of concrete structures, an accurate prediction of the value of the TCC that can account for all these characteristics of the concrete is essential but very complex. For this reason, to investigate the complexity and influences of numerous factors on the TCC, we have employed a back-propagation neural algorithm that emerged as a new alternative to complicated pattern recognition in many fields such as the medical and biochemistry field.
The neural network, a prediction method for the estimation of the TCC, was constructed and trained using 124 experimental data obtained by previous studies (Kim et al. 2003; Morabito 1989; Harmathy 1983; Yamazaki et al. 1995; Lie and Kodur 1996; Van Geem et al. 1997; Khan et al. 1998; Khan 2002; Kodur and Sultan 2003). Based on their data sets, the developed neural network model was trained with regard to eleven parameters: nine parameters representing the composition of concrete constituents, which were the water–cement ratio, the fine aggregate percentage, the coarse aggregate percentage, the unit water weight, the unit cement weight, the unit fine aggregate weight, the unit coarse aggregate weight, the unit fly ash weight, and the unit silica fume weight, and two parameters representing the state of concrete, which were the temperature of the concrete and the water content in the concrete. Finally, the TCC estimated by the neural network model was compared with 28 randomly-selected measured data not included in the neural network training. As a result, the neural network model, trained by the eleven parameters, accurately estimated the values of the TCC. Therefore, this study demonstrated that the proposed prediction method based on a neural network algorithm could be used as a reliable and effective technique for determining thermal conductivity in the thermal design and analysis of concrete structures.

2 Construction of Neural Network

2.1 Principles of Neural Network

As problems such as pattern recognition, system identification, and system control became difficult to solve using conventional computing methods, the concept of neural networks was inspired by the biological learning and decision-making process of the human neuron system. In civil engineering, neural networks were well applied to the detection of structural damage (Feng and Bahng 1999), the identification and control of structural systems (Feng and Bahng 1999; Chen et al. 1995), the modeling of material behavior (Adeli and Park 1995), and the proportion of concrete mixtures (Oh et al. 1999). In addition, the compressive strength of concrete (Kim et al. 2004; Kim et al. 2005) was effectively estimated by several researchers, including the authors of this paper, who have applied the neural networks. The main advantage of the neural network approach is easily to perform the predictions, which depend on multiple variables and find difficult to develop an analytical model.
In this paper, we have used feed forward neural networks based on a backward propagation algorithm for the learning of the network. The basic processing elements of the network are artificial neurons and connecting weights, and the complex relationships between input data and corresponding target values are trained to find patterns in data. During the training of the network, the connecting weights are updated in accordance to a particular learning rule until the difference between the predicted values from the feed forward process and the target values meets a tolerance limit. Calculations are conducted from the input of network toward the output data, and errors computed in the output layer are then propagated backward to the input layer. After that, the trained neural network is applied for predicting the outcome of new independent input data.

2.2 Structure of Neural Network

To develop the relationships between the TCC and the eleven parameters, this study created a two-layer network with twenty neurons, presented in Fig. 1. Each layer is fully connected to the succeeding layers through the connection weights. The neural network can be expressed as
$$ {\text{net}}\,{ = }\,f\left( {\sum\limits_{i} {W_{ji} P_{i} + B_{j} } } \right) $$
(1)
in which P i is the element of input sets, and W ji and B j are the connection weights and biases of the neurons. The input data for the development of the neural network model, which play a key role to reach a satisfactory quality of the neural network approach, were obtained from the literature (Kim et al. 2003; Morabito 1989; Harmathy 1983; Yamazaki et al. 1995; Lie and Kodur 1996; Van Geem et al. 1997; Khan et al. 1998; Khan 2002; Kodur and Sultan 2003).
The sets of input data with initial weights were passed through the network layer, and then the weights and biases were trained using activation functions, which represented a tangent sigmoid function in the first layer,
$$ f^{1} (x) = \frac{{{\text{e}}^{x} - {\text{e}}^{{ - {x}}} }}{{{\text{e}}^{x} + {\text{e}}^{{ - {x}}} }} $$
(2)
and a linear transfer function in the second layer,
$$ f^{2} (x) = x $$
(3)
During the training of the network, the weights and biases of the network were iteratively adjusted to minimize the network performance with a back-propagation algorithm. The network performance was based on the mean squared error, MSE, defined as
$$ {\text{MSE}} = \frac{1}{N}\sum\limits_{k = 1}^{N} {\left( {T_{k} - a_{k} } \right)^{2} } $$
(4)
in which T k is the calculated value in the network, a k is the desired thermal conductivity of concrete, and N is the number of the output neurons. The errors associated with desired output data are adjusted in the way that reduces these errors in each neuron from the output to the input layers. The error function was minimized by the Levenberg–Marquardt back-propagation algorithm, which combines the gradient decent and the Gauss–Newton method. When the solution is far from the correct one, the weights are updated in the direction of the negative gradient. When the solution is close to the correct one, the Gauss–Newton method is applied to the training because it is more accurate and faster near an error minimum than the gradient decent method.
The available data sets obtained from the literature were divided into two sets; the training and testing sets. A total of the experimental data sets are 152, of which 124 data (accounting for 80 % of the total data) were randomly selected for the training of the neural network model, and the remaining 28 data (accounting for 20 %) were utilized for the testing of the network performance. The neural network modeling program was implemented in MATLAB 7.01 software. The number of neurons in the input and the output layers is equal to the number of the input and output data sets. Optimal number of the neurons in the hidden layer was determined to be twenty by training the networks with increases in the number of the neurons.

2.3 Training of Neural Network

To train the neural network of the TCC, this research utilized experimental data reported by previous researchers from the 1980’s to the 2000’s. The training data of the network were composed of 124 sets from Harmathy (1983), Morabito (1989), Yamazaki et al. (1995), Lie and Kodur (1996), Van Geem et al. (1997), Khan et al. (1998), Khan (2002), Kodur and Sultan (2003) and Kim et al. (2003). Table 1 presents samples of the data sets used in the training of the network with eleven parameters: the water–cement ratio, the fine aggregate percentage, the coarse aggregate percentage, the unit water weight, the unit cement weight, the unit fine aggregate weight, the unit coarse aggregate weight, the unit fly ash weight, the unit silica fume unit weight, the temperature of concrete, the water content in concrete.
Table 1
Samples of the input data sets for the training of the neural network.
Researchers
TC (W/m K)
Water–cement ratio
Fine aggregate (%)
Coarse aggregate (%)
Unit weight (kg/m3)
Water content (%)
Temperature (°C)
Water
Cement
Fine aggregate
Coarse aggregate
Fly ash
Silica fume
Harmathy (1983)
0.6
0.50
0
0
510
1,020
0
0
0
0
0
33
0.7
0.50
0
0
510
1,020
0
0
0
0
0
100
0.9
0.33
0
0
432
1,308
0
0
0
0
0
310
1.0
0.33
0
0
432
1,308
0
0
0
0
0
35
1.1
0.44
31
46
170
387
736
1,115
0
0
0
22
1.3
0.44
31
46
170
387
736
1,115
0
0
0
150
1.3
0.49
30
46
190
385
701
1,096
0
0
0
305
1.4
0.49
30
46
190
385
701
1,096
0
0
0
20
1.6
0.62
29
51
183
294
701
1,236
0
0
0
165
1.7
0.62
29
51
183
294
701
1,236
0
0
0
30
Morabito (1989)
1.1
0.50
46
16
175
350
700
250
0
0
100
20
1.2
0.50
57
0
292
583
1,167
0
0
0
0
20
1.3
0.50
36
32
175
350
700
250
0
0
100
20
1.7
0.50
23
60
175
350
700
1,850
0
0
100
20
1.8
0.50
30
48
175
350
700
250
0
0
0
20
Yamazaki et al. (1995)
1.1
0.48
30
51
145
242
707
1,204
60
0
0
385
1.1
0.48
30
51
145
242
707
1,204
60
0
0
435
1.2
0.48
30
51
145
242
707
1,204
60
0
0
295
1.2
0.48
30
51
145
242
707
1,204
60
0
0
345
1.3
0.48
30
51
145
242
707
1,204
60
0
0
245
Lie and Kodur (1996)
1.0
0.37
26
48
161
439
621
1,128
0
0
0
385
1.4
0.37
26
48
161
439
621
1,128
0
0
0
32
1.4
0.37
26
48
161
439
621
1,128
0
0
0
190
1.5
0.37
26
48
161
439
621
1,128
0
0
0
75
1.5
0.37
26
48
161
439
621
1,128
0
0
0
110
Khan et al. (1998)
1.1
0.50
33
44
178
355
790
1,040
0
0
0
37
1.2
0.50
33
44
178
355
790
1,040
0
0
0
25
1.7
0.25
29
44
133
494
720
1,105
0
46
0
82
1.8
0.25
29
44
133
494
720
1,105
0
46
0
73
Van Geem et al. (1997)
1.6
0.22
24
43
144
564
593
1,068
0
89
0
30
1.7
0.29
27
44
160
475
659
1,068
59
24
0
30
1.9
0.29
28
44
155
487
676
1,068
0
47
0
30
2.2
0.23
24
43
151
475
593
1,068
104
74
0
149
2.3
0.28
26
44
158
564
647
1,068
0
0
0
30
Khan et al. (1998)
1.9
0.60
56
0
191
318
635
0
0
0
0
25
2.0
0.60
26
53
191
318
635
1,270
0
0
0
25
2.2
0.60
27
52
191
318
635
1,256
0
0
0
25
2.3
0.60
26
53
191
318
635
1,274
0
0
0
25
2.3
0.60
27
52
191
318
637
1,260
0
0
0
25
Kodur and Sultan (2003)
1.0
0.26
28
44
140
500
700
1,100
0
50
0
600
1.2
0.26
28
44
140
500
700
1,100
0
50
0
500
1.8
0.26
28
44
140
500
700
1,100
0
50
0
200
1.9
0.26
28
44
140
500
700
1,100
0
50
0
100
2.0
0.26
28
44
140
500
700
1,100
0
50
0
23
Kim et al. (2003)
1.1
0.35
0
0
524
1,498
0
0
0
0
100
60
1.2
0.25
0
0
440
1,762
0
0
0
0
100
20
1.2
0.30
0
0
486
1,619
0
0
0
0
100
40
1.4
0.40
10
16
420
1,050
206
321
0
0
100
60
1.6
0.40
17
26
340
850
345
546
0
0
100
60
1.9
0.40
25
40
220
550
559
880
0
0
100
60
2.0
0.40
25
40
220
550
559
880
0
0
100
40
2.4
0.40
39
32
181
452
887
729
0
0
100
20
2.4
0.40
28
44
181
452
630
989
0
0
100
40
2.5
0.40
31
48
140
350
702
1,103
0
0
100
40
During the training of the neural network, the weights and biases of the network were updated until its mean squared error was less than a target mean squared error. This study investigated the performance of the neural networks on the basis of four different target errors: 0.10, 0.05, 0.01, and 0.005. The prediction performance of the networks was evaluated using the mean squared error (MSE) and the statistical correlation coefficient (R). Figure 2 displays the variations in the mean squared errors and the correlations of the entire training data. The neural network, trained by the 0.10 target error, presents a 0.086 error and a 0.850 correlation between the network outputs and the training sets. As the target errors decreased from 0.10 to 0.005, the mean squared errors also decreased from 0.086 to 0.003. In addition to the mean squared errors, the correlations between the network outputs and the training data increased to 0.928, 0.983, and 0.995 in the target errors 0.05, 0.01, and 0.005, respectively. Furthermore, as represented in Fig. 3, the distributions of the network errors, the difference between the network outputs and the training data sets, showed the decreases as the target errors decrease from 0.10 to 0.005. The neural networks, trained by the target errors 0.01 and 0.005, find that most network errors are in the range of −0.1 to 0.1 W/m K. Since the difference range is sufficiently accurate in the thermal analysis of concrete structures, this study determines that the two neural networks can be applied as optimum models to the prediction of the TCC.

3 Comparison of Estimated and Measured Thermal Conductivity of Concrete

Since the training of the neural networks exhibited similarly good performance in the 0.01 and 0.005 target errors, this study evaluated the applicability of the two neural networks to the estimation of the TCC. To evaluate the trained neural networks, this study randomly selected 28 experimental values not included in the training process of the neural networks from the research results of Harmathy (1983), Yamazaki et al. (1995), Lie and Kodur (1996), Van Geem et al. (1997), Khan et al. (1998), Kodur and Sultan (2003) and Kim et al. (2003). Table 2 shows the details of the 28 experimental values with the eleven parameters: the ratio of water–cement, the percentage of fine and coarse aggregate, the unit weight of water, cement, fine aggregate, coarse aggregate, fly ash, and silica fume, and the temperature and the water content of concrete.
Table 2
Experiment data sets for the evaluation of the neural network.
Researchers
TC (W/m K)
Water–cement ratio
Fine agg. percentage
Coarse agg. percentage
Unit weight (kg/m3)
Water content (%)
Temperature (°C)
Water
Cement
Fine aggregate
Coarse aggregate
Fly ash
Silica fume
Harmathy (1983)
0.3
0.50
0
0
510
1,020
0
0
0
0
0
660
0.7
0.25
0
0
392
1,568
0
0
0
0
0
560
0.9
0.25
0
0
392
1,568
0
0
0
0
0
100
1.2
0.44
31
46
170
387
736
1,115
0
0
0
280
1.3
0.62
29
51
183
294
701
1,236
0
0
0
330
1.5
0.49
30
46
190
385
707
1,096
0
0
0
155
Yamazaki et al. (1995)
1.0
0.48
30
51
145
242
707
1,204
60
0
0
485
1.3
0.48
30
51
145
242
707
1,204
60
0
0
195
Khan et al. (1998)
1.6
0.30
34
42
135
421
820
1,025
0
34
0
28
1.8
0.25
29
44
133
494
720
1,105
0
46
0
25
Lie and Kodur (1996)
1.0
0.37
26
48
161
439
621
1,128
0
0
0
490
1.2
0.37
26
48
161
439
621
1,128
0
0
0
290
Van Geem et al. (1997)
1.8
0.29
27
43
160
475
359
1,068
59
24
0
370
1.9
0.22
24
43
144
564
593
1,068
0
89
0
150
2.0
0.29
28
44
155
487
676
1,068
0
47
0
150
2.1
0.23
24
43
151
475
593
1,068
104
74
0
30
Kodur and Sultan (2003)
1.4
0.26
28
44
140
500
700
1,100
0
50
0
400
1.6
0.26
28
44
140
500
700
1,100
0
50
0
300
Kim et al. (2003)
1.0
0.30
0
0
486
1,619
0
0
0
0
0
20
1.3
0.30
0
0
486
1,619
0
0
0
0
100
20
1.3
0.40
17
26
340
850
345
546
0
0
0
40
1.4
0.40
10
16
420
1,050
206
321
0
0
100
20
1.7
0.40
17
26
340
850
345
546
0
0
100
40
1.8
0.40
23
35
260
650
490
768
0
0
100
60
1.8
0.40
28
44
181
452
630
989
0
0
0
60
2.2
0.40
28
44
181
452
630
989
0
0
100
60
2.3
0.40
28
44
181
452
630
989
0
0
100
20
2.4
0.40
36
36
181
452
810
806
0
0
100
20
The values of the TCC obtained in the previous experiments were compared with those estimated by the neural networks. Table 3 shows the differences between the measured and estimated values. The results indicate that all of the estimated values based on the eleven parameters show good agreement with the measured ones in both neural networks. In the neural networks with the target error 0.01, nine estimates matched the measured values, eighteen represented a 0.1 W/m K difference, and the last one showed a 0.2 W/m K difference. The neural network, trained by the target error 0.005, showed that twelve estimated values were the same as the measured ones and that the remaining values represented the difference of 0.1 W/m K. In addition, Fig. 4 presents the mean squared errors of the neural networks and the correlations between estimated and measured thermal conductivity. The errors of the neural networks were found to be quite small: 0.008 in the target error 0.01 and 0.007 in the target error 0.005. For the correlation values, the two neural networks exhibited extremely high values of 0.985 and 0.987 in the target errors 0.05 and 0.005, respectively. As a result, the proposed neural networks, developed and trained by the eleven parameters, estimated the TCC with high accuracy. Therefore, this estimation method can provide an efficient technique for obtaining the TCC.
Table 3
Comparisons between the estimated and experimental values.
Researchers
Data no.
Concrete thermal conductivity (W/m K)
Measured
Estimated by the target 0.01 network
Estimated by the target 0.005 network
Harmathy (1983)
1
0.3
0.4 (0.1)
0.3 (0.0)
2
0.7
0.8 (0.1)
0.8 (0.1)
3
0.9
1.0 (0.1)
0.9 (0.1)
4
1.2
1.2 (0.0)
1.1 (0.0)
5
1.3
1.5 (0.2)
1.4 (0.1)
6
1.5
1.4 (0.1)
1.3 (0.1)
Yamazaki et al. (1995)
7
1.0
1.0 (0.1)
1.1 (0.1)
8
1.3
1.3 (0.0)
1.3 (0.0)
Khan et al. (1998)
9
1.6
1.7 (0.1)
1.7 (0.1)
10
1.8
1.8 (0.0)
1.7 (0.1)
Lie and Kodur (1996)
11
1.0
1.1 (0.1)
1.0 (0.0)
12
1.2
1.3 (0.1)
1.2 (0.0)
Van Geem et al. (1997)
13
1.8
1.9 (0.1)
1.9 (0.1)
14
1.9
1.8 (0.1)
1.9 (0.0)
15
2.0
1.9 (0.1)
2.0 (0.0)
16
2.1
2.2 (0.1)
2.1 (0.0)
Kodur and Sultan (2003)
17
1.4
1.5 (0.1)
1.5 (0.1)
18
1.6
1.7 (0.1)
1.7 (0.1)
Kim et al. (2003)
19
1.0
0.9 (0.1)
0.9 (0.1)
20
1.3
1.2 (0.1)
1.2 (0.1)
21
1.3
1.3 (0.0)
1.2 (0.1)
22
1.4
1.4 (0.0)
1.5 (0.1)
23
1.7
1.7 (0.0)
1.7 (0.0)
24
1.8
1.9 (0.1)
1.8 (0.0)
25
1.8
1.7 (0.1)
1.9 (0.1)
26
2.2
2.2 (0.0)
2.2 (0.0)
27
2.3
2.3 (0.0)
2.4 (0.1)
28
2.4
2.4 (0.0)
2.4 (0.0)
The values in parenthesis present the differences between the measured and estimated thermal conductivity.

4 Conclusions

The determination of the TCC is essential to the analysis of its thermal behavior. However, the conductivity value depends on numerous variables, including the composition, the temperature, and the water content of concrete. Thus, this paper proposed an effective prediction method based on a back-propagation neural algorithm and investigated the influences of all the factors on the TCC. The neural network model was trained using 124 data sets, obtained experimentally in previous research, with regard to eleven parameters: the ratio of water to cement, the percentage of fine and coarse aggregate, the unit content of water, cement, fine aggregate, coarse aggregate, fly ash content, and silica fume, and the temperature and the water content of the concrete.
To determine the optimum neural network model for the estimation of the TCC, this study investigated the variations and distributions of the network errors as the target errors decreased from 0.10 to 0.005. Since the two neural networks, trained by the 0.01 and 0.005 target errors, showed similarly good performance, the two neural networks were used to estimate the 28 previously measured values not included in the training of the neural networks. The estimated values by the proposed neural networks were very close to the measured values. For the 0.01 neural network, ten estimated values were the same as the measured ones, seventeen differed by 0.1 W/m K, and the last one differed by 0.2 W/m K. The neural network of the 0.005 target error showed that twelve values were the same as the measured ones and that the remaining values differed by 0.1 W/m K. The differences in the two proposed neural network models are accurate enough to determine the precise temperature distributions of concrete structures. In addition, the correlations between the estimated and measured values were found to be very high: 0.985 and 0.987 in the target error 0.05 and 0.005, respectively.
In conclusion, the back-propagation neural networks include the influence of multiple factors such as the composition of concrete constituents and the temperature and water content of the concrete in the estimation of the TCC. Based on the estimated results, the proposed network models provide an efficient method for the determination of the TCC. Furthermore, as new data are added to the current training data sets, the performance of the proposed method should dramatically increase.

Acknowledgments

This work is a part of the research project “Development of an Integrated Design Solution based on Codes and Field Data for the Advancement of the Plant Industry (No. 10040909),” supported by the Korea Government Ministry of Knowledge Economy.
Open AccessThis article is distributed under the terms of the Creative Commons Attribution 2.0 International License (https://​creativecommons.​org/​licenses/​by/​2.​0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
Literature
go back to reference Adeli, H., & Park, H. S. (1995). Neural dynamics model for structural optimization—theory. Computers and Structures,57(3), 383–390.CrossRefMathSciNetMATH Adeli, H., & Park, H. S. (1995). Neural dynamics model for structural optimization—theory. Computers and Structures,57(3), 383–390.CrossRefMathSciNetMATH
go back to reference Carslaw, H. S., & Jaeger, J. C. (1959). Conduction of heat in solids (3rd ed.). Oxford: Clarendon Press. Carslaw, H. S., & Jaeger, J. C. (1959). Conduction of heat in solids (3rd ed.). Oxford: Clarendon Press.
go back to reference Chen, H. M., Tsai, K. H., Qi, G. Z., Yang, C. S., & Amini, F. (1995). Neural network for structure control. Journal of Computing in Civil Engineering,9(2), 168–176.CrossRef Chen, H. M., Tsai, K. H., Qi, G. Z., Yang, C. S., & Amini, F. (1995). Neural network for structure control. Journal of Computing in Civil Engineering,9(2), 168–176.CrossRef
go back to reference Feng, M. Q., & Bahng, E. Y. (1999). Damage assessment of jacketed RC columns using vibration tests. Journal of Structural Engineering,125(3), 265–271.CrossRef Feng, M. Q., & Bahng, E. Y. (1999). Damage assessment of jacketed RC columns using vibration tests. Journal of Structural Engineering,125(3), 265–271.CrossRef
go back to reference Harmathy, T. Z. (1983). Properties of building materials at elevated temperatures, DBR Paper No. 1080. National Research Council of Canada Division of Building Research. Harmathy, T. Z. (1983). Properties of building materials at elevated temperatures, DBR Paper No. 1080. National Research Council of Canada Division of Building Research.
go back to reference Khan, M. I. (2002). Factors affecting the thermal properties of concrete and applicability of its prediction models. Building and Environment,37(6), 607–614.CrossRef Khan, M. I. (2002). Factors affecting the thermal properties of concrete and applicability of its prediction models. Building and Environment,37(6), 607–614.CrossRef
go back to reference Khan, A. A., Cook, W. D., & Mitchell, D. (1998). Thermal properties of transient thermal analysis of structural members during hydration. ACI Materials Journal,95(3), 293–303. Khan, A. A., Cook, W. D., & Mitchell, D. (1998). Thermal properties of transient thermal analysis of structural members during hydration. ACI Materials Journal,95(3), 293–303.
go back to reference Kim, K. H., Jeon, S. E., Kim, J. K., & Yang, S. C. (2003). An experimental study on thermal conductivity of concrete. Cement and Concrete Research,33, 363–371.CrossRef Kim, K. H., Jeon, S. E., Kim, J. K., & Yang, S. C. (2003). An experimental study on thermal conductivity of concrete. Cement and Concrete Research,33, 363–371.CrossRef
go back to reference Kim, J. I., Kim, D. K., Feng Maria, Q., & Yazdani, F. (2004). Application of neural networks for estimation of concrete strength. Journal of Materials in Civil Engineering,16(3), 257–264.CrossRef Kim, J. I., Kim, D. K., Feng Maria, Q., & Yazdani, F. (2004). Application of neural networks for estimation of concrete strength. Journal of Materials in Civil Engineering,16(3), 257–264.CrossRef
go back to reference Kim, D. K., Lee, J. J., Lee, J. H., & Chang, S. K. (2005). Application of probabilistic neural networks for prediction of concrete strength. Journal of Materials in Civil Engineering,17(3), 353–362.CrossRef Kim, D. K., Lee, J. J., Lee, J. H., & Chang, S. K. (2005). Application of probabilistic neural networks for prediction of concrete strength. Journal of Materials in Civil Engineering,17(3), 353–362.CrossRef
go back to reference Kodur, V. K. R., & Sultan, M. A. (2003). Effect of temperature on thermal properties of high-strength concrete. Journal of Materials in Civil Engineering,15(2), 101–107.CrossRef Kodur, V. K. R., & Sultan, M. A. (2003). Effect of temperature on thermal properties of high-strength concrete. Journal of Materials in Civil Engineering,15(2), 101–107.CrossRef
go back to reference Lie, T. T., & Kodur, V. K. R. (1996). Thermal and mechanical properties of steel-fibre-reinforced concrete at elevated temperatures. Canadian Journal of Civil Engineering,23(2), 511–517.CrossRef Lie, T. T., & Kodur, V. K. R. (1996). Thermal and mechanical properties of steel-fibre-reinforced concrete at elevated temperatures. Canadian Journal of Civil Engineering,23(2), 511–517.CrossRef
go back to reference Morabito, P. (1989). Measurements of the thermal properties of different concretes. High Temperatures–High Pressures,21(1), 51–59. Morabito, P. (1989). Measurements of the thermal properties of different concretes. High Temperatures–High Pressures,21(1), 51–59.
go back to reference Nevile, A. M. (1995). Properties of concrete (4th ed.). UK: Longman. Nevile, A. M. (1995). Properties of concrete (4th ed.). UK: Longman.
go back to reference Oh, J. W., Lee, I. W., Kim, J. T., & Lee, G. W. (1999). Application of neural networks for proportioning of concrete mixes. ACI Materials Journal,96(1), 61–67. Oh, J. W., Lee, I. W., Kim, J. T., & Lee, G. W. (1999). Application of neural networks for proportioning of concrete mixes. ACI Materials Journal,96(1), 61–67.
go back to reference Toyokazu, S., & Yoshiro, M. (1976). Thermal properties of mortar and concrete in hardening process. Transactions of the Architectural Institute of Japan,241, 1–8 (in Japanese). Toyokazu, S., & Yoshiro, M. (1976). Thermal properties of mortar and concrete in hardening process. Transactions of the Architectural Institute of Japan,241, 1–8 (in Japanese).
go back to reference Van Geem, M. G., Gajda, J., & Dombrowski, K. (1997). Thermal properties of commercially available high-strength concretes. Journal of Cement, Concrete, and Aggregates,19(1), 38–54.CrossRef Van Geem, M. G., Gajda, J., & Dombrowski, K. (1997). Thermal properties of commercially available high-strength concretes. Journal of Cement, Concrete, and Aggregates,19(1), 38–54.CrossRef
go back to reference Yamazaki, N., Yamazaki, M., Mochida, T., Mutoh, A., Miyashita, T., Ueda, M., Hasegawa, T., Sugiyama, K., Hirakawa, K., Kikuchi, R., Hiramoto, M., & Saito, K. (1995). Structural behavior of reinforced concrete structures at high temperatures. Nuclear Engineering and Design,156(1–2), 121–138.CrossRef Yamazaki, N., Yamazaki, M., Mochida, T., Mutoh, A., Miyashita, T., Ueda, M., Hasegawa, T., Sugiyama, K., Hirakawa, K., Kikuchi, R., Hiramoto, M., & Saito, K. (1995). Structural behavior of reinforced concrete structures at high temperatures. Nuclear Engineering and Design,156(1–2), 121–138.CrossRef
Metadata
Title
Effective Prediction of Thermal Conductivity of Concrete Using Neural Network Method
Authors
Jong-Han Lee
Jong-Jae Lee
Baik-Soon Cho
Publication date
01-09-2012
Publisher
Korea Concrete Institute
Published in
International Journal of Concrete Structures and Materials / Issue 3/2012
Print ISSN: 1976-0485
Electronic ISSN: 2234-1315
DOI
https://doi.org/10.1007/s40069-012-0016-x

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