Computational intelligent strategies to predict energy conservation
Transcription
Computational intelligent strategies to predict energy conservation
Applied Thermal Engineering 102 (2016) 432–446 Contents lists available at ScienceDirect Applied Thermal Engineering journal homepage: www.elsevier.com/locate/apthermeng Research Paper Computational intelligent strategies to predict energy conservation benefits in excess air controlled gas-fired systems Alireza Bahadori a,⇑, Alireza Baghban b, Meysam Bahadori c, Moonyong Lee d, Zainal Ahmad e, Mehrasa Zare f, Ehsan Abdollahi g a School of Environment, Science and Engineering, Southern Cross University, Lismore, NSW, Australia Young Researcher and Elite Club, Fasa Branch, Islamic Azad University, Fasa, Iran National Iranian Drilling Co, Kish, Iran d School of Chemical Engineering, Yeungnam University, Gyeungsan, Republic of Korea e School of Chemical Engineering, Universiti Sains Malaysia (USM), Engineering Campus, Seri Ampangan, 14300 Nibong Tebal, Penang, Malaysia f Salman Farsi University, Kazerun, Iran g Department of Gas Engineering, Ahwaz Faculty of Petroleum Engineering, Petroleum University of Technology (PUT), Ahwaz, Iran b c h i g h l i g h t s Intelligent models are applied to predict combustion efficiency of natural gas in gas-fired systems. The developed models were examined using experimental data, and a reasonable match was attained. The models have been tested and validated using around 100 data points. Hybrid algorithm is used to determine parameters of membership function in ANFIS approach. a r t i c l e i n f o Article history: Received 11 September 2015 Revised 10 March 2016 Accepted 2 April 2016 Available online 2 April 2016 Keywords: Conservation benefits Combustion efficiency Artificial neural network Adaptive neuro fuzzy inference system Support vector machine a b s t r a c t Gas-fired systems and boilers are the noteworthy energy consumers in industries for energy production. The mostly applied factor in systems which contain boilers is the combustion efficiency. This parameter has widely applied to determine important information about exhaust gas such as CO2 and O2. This study plays importance on applying the predictive techniques based on the Adaptive Neuro-Fuzzy Inference System (ANFIS), Multi-Layer Perceptron Artificial Neural Network (MLPANN), Support Vector Machine (SVM), and simple correlation for predicting the combustion efficiency of natural gas at extensive range of excess air fraction and stack temperature rise. The developed tools can be of great assessment for engineers dealing with combustion to have a rapid check on combustion efficiency of natural gas at broad range of applications without the requirement of any unit as pilot plant. The Levenberg–Marquardt algorithm is employed to optimize the bias and weight values of the ANN model. In addition, Hybrid algorithm (coupling of back propagation and least square methods) is used to determine parameters of membership function in the ANFIS approach. Hyper variables of the SVM technique (i.e., C, K and e) are determined using tried and error procedures. To that end, a database including 72 data points has been collected from the energy management handbook. Approximations are recognized to be in high approbation with reported data points. Furthermore, potential of aforementioned models has been evaluated through statistical analyses. The developed models were examined using several data, and a reasonable match was attained showing a good potential for the proposed predictive tools in estimation of the combustion efficiency of natural gas at extensive range of excess air fraction and stack temperature rise. Ó 2016 Elsevier Ltd. All rights reserved. 1. Introduction ⇑ Corresponding author. E-mail address: Alireza.bahadori@scu.edu.au (A. Bahadori). http://dx.doi.org/10.1016/j.applthermaleng.2016.04.005 1359-4311/Ó 2016 Elsevier Ltd. All rights reserved. Nowadays, the main part of global energy production is from the combustion of fossil fuels [1–3]. The concentrations of carbon dioxide in the atmosphere have been steadily increasing over the A. Bahadori et al. / Applied Thermal Engineering 102 (2016) 432–446 433 Nomenclature AAD ANFIS ANN ARD BP C Cal. Exp. FLS GA HGAPSO ICA K Average Absolute Deviation Adaptive Neuro Fuzzy Inference System Artificial Neural Network Average Relative Deviation Back Propagation penalty factor calculated experimental Fuzzy Logic System Genetic Algorithm hybrid genetic algorithm and particle optimization imperialist competitive algorithm kernel function parameter swarm LSSVM MF MLP MRE MSE PSO R2 RBF RMSE STD SVM TST UPSO e Least Square Support Vector Machine Membership Function multi-layer perceptron Mean Relative Error Mean Square Error particle swarm optimization R squared Radial Basis Function Root Mean Square Error Standard Deviation Support Vector Machine Twu–Sim–Tassone unified particle swarm optimization insensitive coefficient Fig. 1. Construction of typical ANFIS. years, mainly due to emission of CO2 from the burning of fossil fuels. The ever increasing concentration of CO2 is starting to have significant effects on the global climate and the effect will continue to multiply if the problem is not addressed [4]. Moreover, air contamination, acid rain, and health risks can be occurred due to Nitrogen oxides, Sulphur oxides, polycyclic aromatic hydrocarbons (PAHs), carbon monoxide emissions [5,6]. Hence, using new methods is crucial to attain high combustion efficiency with the minimum quantity of contaminant emissions. To that end, monitoring of combustion processes or adjusting of the fuels can great help [4]. According to obtained results from researchers and engineers who study on boiler in industry, excess air is an important parameter and it has great effect on thermal efficiency and operation of boilers [4]. Due to the increase in the excess of air value in the furnace, the adiabatic flame temperature is diminished. Also, due to the flue gas temperature reducing, the heat transfer coefficients are increased quickly for all the convective equipment. Because of rising of the flame temperature in the boiler, the more the concentration of oxygen in the main combustion zone, the more the Fig. 2. Flowchart diagram of proposed models. excess air ratio. It causes that the temperature in the boiler radiation area is dropped [7,8]. The chemical reaction between oxygen and fuel is carried out during combustion and the heat and light are released [9]. 434 A. Bahadori et al. / Applied Thermal Engineering 102 (2016) 432–446 Table 1 Tuned coefficients used in Eq. (16). Coefficient Optimal value a1 a2 a3 a4 a5 a6 0.8969 3.743e05 0.0002801 5.208e08 3.275e06 2.684e08 hy o þs Ao ¼ 4:77 c þ 4 2 Ai Ao X¼ Ao Fig. 3. Flow diagram of SVM approach. Table 2 Obtained values of MSE and R2 through raising the number of neurons. Neuron MSE R2 1 2 3 4 5 0.000039 0.000002 0.000001 0.000001 0.000001 0.9853 0.9994 0.9995 0.9997 0.9998 Generally the fuel is a hydrocarbon and the required oxygen is prepared from ambient air. To have complete combustion, the sufficient oxygen is required for converting the fuel to carbon dioxide and water [10]. If the fuel is partially combusted and other products instead of CO2 and H2O such as carbon monoxide, hydrogen, etc. are produced, incomplete combustion occurs. Representation of complete combustion of typical carbon-based fuel compound presents in Eq. (1) [10]. hy o C c Hhy Oo Ss Nn þ c þ þ s O2 4 2 n hy H2 O þ ðsÞSO2 þ N2 ! ðcÞCO2 þ 2 2 Air is formed approximately 20.9% oxygen on a dry base. Therefore, 4.77 mol of air is supplied from 1.0 mol of oxygen. Using this strategy to methane, 9.54 mol of air is required for every mole of methane. Eq. (2) denotes the calculation of theoretical required air for carbon-based fuel, in moles of air per mole of fuel (Ao) and this is derived following stoichiometry [9,10]: ð1Þ ð2Þ ð3Þ where in Eq. (3), Ao denotes the theoretical required air of fuel, in moles of air per mole of fuel, Ai denotes the inlet air in moles of air per mole of fuel and X represents the fraction of excess air. The more combustion air must be used than theoretical required air in a boiler for safeguarding that combustion is completed and operation is safe. Due to the very low rate of air, carbon monoxide will be released rapidly in the flue gas and, in dangerous conditions, smoke will be appeared [11]. Simultaneously, the efficiency of boiler has very close relation with the excess air rate. Hence, amount of excess air must be low in practice for reducing the amount of extra air that is released heat at the stack temperature [11,12]. The quantity of excess air in the flue gas and the stack temperature rise above the inlet air temperature are important to determine the efficiency of the combustion process. To control the ratio of air-to-fuel, a widely used approach namely, excess oxygen measured in the exhaust stack is applied. Moreover, to guarantee the best performance, it should be considered the importance of furnace operation. Also, achieving ideal control over unnecessary losses can obtain through measuring of the excess air continuously [13]. Taking into account the aforementioned subjects, evolving a precise and simple-to-apply approach which is more simplify than present methods for forecasting the efficiency of natural gas combustion as a function of excess air fraction and stack temperature rise is essential. Bahadori and Vuthaluru developed a correlation based on principle component analysis (PCA) and partial least square (PLS) [14]. They estimated the efficiency of natural gas combustion as a function of excess air fraction and stack temperature rise. While, this aforementioned approach is able to estimate efficiency of natural gas combustion accurately, using of obtainable technique is usually limited to this case. It means that this model requires some parameters which are tuned and they must be determined according experimental data points. Actually, these parameters are not generally acceptable in the absence of experimental data points. In such conditions, evolving and employing wide-ranging models is desirable to estimate the efficiency of natural gas combustion. The most significant embranchment of computational intelligence paradigms is the Artificial Neural Network (ANN) that can be a benefit application for phase equilibrium modeling. Artificial neural networks are non-parametric and statistical modeling tools that do not require any pre assumption between inputs and output [15–17]. To approximate any non-linear systems, artificial neural networks have these abilities with high interpolation capacity [18,19]. In addition, the fuzzy logic system is one of the embranchment of computational intelligence paradigms that has been created to category the concept of partial truth-truth values between completely true and completely false [20,21]. Another embranchment of computational intelligence paradigms was created by combining of the learning capability of neural networks [22–24] with the knowledge of Fuzzy Logic summarizes in the ANFIS method which is abbreviate of adaptive neuro-fuzzy inference systems [25–27]. Recently, Support Vector Machines (SVMs) 435 A. Bahadori et al. / Applied Thermal Engineering 102 (2016) 432–446 Fig. 4. Performance plot of ANN model. Table 3 Weight and bias values of the ANN model. Neuron Input Layer Output Layer Weight 1 2 3 4 5 Bias Weight Bias Stack temperature rise Excess air fraction b1 Combustion efficiency b2 0.690115 8.9921 1.42943 47.792 1.52882 0.18594 3.38592 0.32808 33.80368 0.34798 1.6166 15.93858 0.210648 24.3715 0.160937 1.195993 0.708773 4.075821 0.0023 3.39472 0.52819 Table 4 Details of proposed intelligent models. ANN ANFIS Type Value/comment Type Value/comment No. of training data No. of testing data Transfer function Hidden layer neuron Hidden layer Optimization method Epoch 18 54 Logsig 5 1 Levenberg–Marquardt 1000 No. of training data No. of training data Membership function No. of MF parameters No. of clusters Optimization method Initial step size Step size increase 18 54 Gaussian 60 10 Hybrid 0.01 1.1 SVM Type Value/comment No. of training data No. of training data Kernel function C 18 54 RBF 1000 0.0005 0.0002 e K are a popular learning technique for classification, regression, and other learning task [28]. Unlike traditional artificial neural network technique, the quadratic programming (QP) with linear limitations is formulated in SVM problems [29,30]. Moreover, simplifying the optimization processes of the SVMs can be performed through a modification version of the SVM namely Least Square Support Vector Machine (LSSVM) [31–33]. So as to create optimum construction of these intelligent schemes, their related parameters can be obtained by using of different mathematical optimization techniques including: Back Propagation (BP) [34], Genetic Algorithm [35], Particle Swarm Optimization (PSO) [36,37], Hybrid Particle Swarm Optimization and Genetic Algorithm (HPSOGA) [38], Unified Particle Swarm Optimization (UPSO) [22] and Imperialist Competitive Algorithm (ICA) [39]. There are lots of studies regarding application of these computational strategies in different fields. Esen et al. applied two models based on the ANFIS and ANN for predicting performance of a solar ground source heat pump system [40]. Their results indicated better capability of the ANFIS against the ANN 436 A. Bahadori et al. / Applied Thermal Engineering 102 (2016) 432–446 model. Moreover, Baghban et al. used the ANFIS, ANN, SVM, and LSSVM techniques as modeling tools for different applications such as predicting phase behavior of carbon dioxide in ionic liquids, estimation of semi-clathrate hydrate conditions of seven gases in TBAB, prediction thermal conductivity of supercritical CO2, and approximation of air dew point temperature [41–44]. In this study, the Adaptive Neuro Fuzzy Inference System (ANFIS), Multi-Layer Perceptron Artificial Neural Network (MLPANN), Support Vector Machine (SVM), and simple-to-use correlation have been developed to predict the efficiency of natural gas combustion as a function of excess air fraction and stack temperature rise. Obtained results indicate ability of the proposed intelligent approaches for predicting of energy conservation benefit with satisfactory accuracy in comparison with the experimental reported data in the database (see Appendix A) [45]. 2. Theory 2.1. Adaptive Neuro Fuzzy Inference System (ANFIS) In this part, the basic theory of the ANFIS is submitted. ANFIS base on a five layers adaptive network-based fuzzy inference system proposed by Jang and Sun [46]. A typical fuzzy inference system based on subtractive clustering has been trained by both back propagation and hybrid learning methods frequently [47]. In Artificial Neural Networks (ANN), the most commonly used algorithms is Back Propagation (BP). However, other computational algorithm such as Genetic Algorithm, and Particle Swarm Optimization can be applied for optimizing structure of the ANN. The goal of these optimization algorithms is determine difference between corresponding target value and output value in the training set of data which was introduced to the network is calculated [44,48]. A combination of back propagation method and the least square method is applied in the typical ANFIS in order to train the ANFIS to follow a training set of data. The training process happens when the difference between testing and training errors are in a definite range. A typical ANFIS structure has shown in Fig. 1. The adapted parameters by the ANFIS are located in premise and consequent parameters while other parameters are constant in other layers. The ANFIS obligation is that it can only simulate single output systems. Suppose a system with two input parameters and one output. The Takagi–Sugeno simulation of such system is structured by five layers. The detail of hybrid learning process presented here Fig. 5. The performance of ANN and ANFIS predictive tools in comparison with experimental data for calculating combustion efficiency. A. Bahadori et al. / Applied Thermal Engineering 102 (2016) 432–446 that all equation in this ANFIS modeling are proposed by Jang and Sun [46]. The first layer equations for each node i: o1i ¼ lAi ðxÞ; For i ¼ 1; 2 or o1i ¼ lBi2 ðyÞ; For i ¼ 3; 4 ð4Þ In this equation x and y are input parameters for nodes and each node can be parameterized with a function membership with range of 0–1. For example the Gaussian membership function [46,49]: lA ðXÞ ¼ ðxc Þ2 i e 2ri 2 ð5Þ where c and r are the input membership function parameters. In the second layer all of the nodes are fixed nodes labeled p output shown the weight of a rule [50]. r2i ¼ xi ¼ lAi ðxÞlBi ðyÞ; For i ¼ 1; 2 ð6Þ The third layer nodes labeled N are fixed and the equation of this layer are: r3i ¼ xi ¼ xi ; For i ¼ 1; 2 x1 þ x2 ð7Þ 437 The fourth layer membership function equation is: r4i ¼ xi f i ¼ xi ðpi x þ qi y þ ri Þ; For i ¼ 1; 2 ð8Þ where pi ; qi and r i are output membership function parameters. The output f function is a constant or linear. The single node in the final layer is a fixed node that computes all nodes and summation of them. r5i ¼ X i P xf xi f i ¼ Pi i i i xi ð9Þ 2.2. Artificial neural network An interesting potential of the ANN is the Non-linear modeling by back-propagation learning approach called multi-layer perceptron (MLP). Via the ANN, we are capable to make complex and nonlinear relations between forecasters as input variables and estimated variables which are the outputs of network. Also, we can obtain precise and complicate information from typical databases. Detecting capability of the ANN leads to find all possible interactions between input and output variables [51–55]. In the Fig. 6. The performance of correlation and SVM predictive tools in comparison with experimental data for calculating combustion efficiency. 438 A. Bahadori et al. / Applied Thermal Engineering 102 (2016) 432–446 ANN, input and output variables Communicate with each other without needing any assumptions about mathematical demonstration of the system which should be simulated. Furthermore, capability of the ANN for generalizing leads to process incomplete and noisy data that defines the problem to be modeled. There are three layers including: input layer, hidden layer and output layer in the MLP structure. Each layer consists of several nodes called neurons. There are directed connections between each neuron in one layer and neurons of the next layer. These neurons have unique weight and bias and via the optimization algorithm, these values should be optimized and updated. Also, through activation functions which are used in each layer, the values of input weight and bias are converted to output values [44,56]. There are several activation functions for converting values of weigh and bias. Among them, hyperbolic tangent sigmoid function (tansig), log-sigmoid transfer function (logsig) and linear transfer function (purelin) are the mostly used transfer functions in many practical applications. In order to Back Propagation (BP) optimization algorithm which commonly applied in the ANN, different mathematical optimization methods including: Genetic Algorithm [32], Particle Swarm Optimization (PSO) [57], Hybrid Particle Swarm Optimization and Genetic Algorithm (HPSOGA) [24], Unified Particle Swarm Optimization (UPSO) [22] and, Imperialist Competitive Algorithm (ICA) [23,39] can be applied to create optimum configuration of ANNs related parameters such as weights and biases. 2.3. Support Vector Machine (SVM) Based on statistical learning theories, support vector machine (SVM) is a global learning method and its construction firstly was introduced by Vapnik [58]. Furthermore, it has been mostly used to solve regression problems and the obtained result is often more accurate and better than other machine learning methods such as multi-layer perceptron artificial neural network and fuzzy logic system [59–61]. Based on the principle of risk minimization theories, SVM takes the fitting of training data and the complexity of the training sample into consideration [62]. Moreover, it can predict the regression problem by using a collection of kernel functions which are specified in a high dimensional feature space. Since the optimality problem is convex, a unique solution is delivered. This is an advantage of the SVM over Neural Networks, which have multiple solutions associated with local minima [63]. To describe regression with the SVMs, Support vector regression (SVR) is used Fig. 7. Experimental versus predicted combustion efficiency by: (a) ANN and (b) ANFIS. 439 A. Bahadori et al. / Applied Thermal Engineering 102 (2016) 432–446 in literature. Based on a given data bases (xi, yi)n, estimating with SVR is applied to forecast a function, where xi and yi represents the input and output vectors respectively and the total number of data bases is represented by n, (in this work, the input vectors (xi) refer to stack temperature rise and excess air fraction, whereas the target value (yi) refers to combustion efficiency of natural gas). As formulated in Eq. (10), the following function is used as the linear regression function: where C is a positive parameter and represents a parameter of extra capacity control that specifies the trade-off between the complication of model and the amount up to which an error larger than e is tolerated. The term of Euclidean norm, ||x||2 represents the regularization parameter and the empirical risk is measured by Le which denotes insensitive loss function. Accordingly, by minimizing a function in Eq. (11) subject to Eq. (12), a non-linear regression function is given at following: f ðxÞ ¼ x /ðxÞ þ b f ðx; a; a Þ ¼ ð10Þ where /(x) is a nonlinear function similar to linear, polynomial, radial basis and Sigmoid functions, the parameter of weight vector and bias have been represented by b and x respectively that should be predicted from the data set. As formulated in Eqs. (11) and (12), through a non-linear mapping, linear regression is exhibited in a high dimensional feature space and the bias and weight values are predicted by minimizing the sum of the empirical risk and a complexity term. n X 1 Le ðf ðxi Þ; yi Þ kxk2 2 i¼1 0 for jf ðxi Þ yi j < e Le ðf ðxi Þ; yi Þ ¼ jf ðxi Þ yi j e otherwise R¼C ð11Þ ð12Þ X ða a Þkðxi ; xÞ þ b ð13Þ with ai ai ¼ 0 and ai ai P 0 for i = 1, . . ., N and the kernel function k (xi,x) defines the internal product in the D-dimensional feature space kðx; yÞ ¼ D X /j ðxÞ/i ðyÞ ð14Þ i¼1 Also, the coefficients ai ai are obtained by maximizing the following form: Rðaa Þ ¼ N N X X 1 X ðai þ ai Þ þ yi ðai ai Þ ðai þ ai Þ 2 i¼1 i;j¼1 ðai þ ai Þkðxi ; xj Þ Fig. 8. Experimental versus predicted combustion efficiency by: (a) correlation and (b) SVM. ! ð15Þ 440 A. Bahadori et al. / Applied Thermal Engineering 102 (2016) 432–446 On the other hand, one of the major disadvantages of the SVM is the requirement to solve a large scale quadratic programming problem [64]. To reduce the complexity of optimization process and solving linear equations instead of quadratic programming problems, a modified version of the traditional SVM called leastsquares SVM (LS-SVM), has been developed to overcome this drawback [65,66]. 2.4. Description of simple correlation According to Eq. (16), easy-to-use correlation has been developed to calculate amount of combustion efficiency of natural gas (g) as a function of stack temperature rise (DT) and excess air fraction (E). The unit of stack temperature rise used in this correlation is °C. There are six tuned coefficients in this correlation. The notations of these coefficients are a1–a6 and they summarize in Table 1. Through minimizing summation of squared errors (difference between correlation output and experimental value), optimal values of these coefficients are determined. g ¼ a1 þ a2 E þ a3 DT þ a4 E2 þ a5 EDT þ a6 DT 2 ð16Þ 3. Development of models The accurate experimental databases are needed to develop computational models. In the current cooperation, the combustion efficiency of natural gas, stack temperature rise and excess air fraction which were reported in the previous published papers were applied and presented in Table A1 (see Appendix A) [45]. The combustion efficiency ranges from the 0.655 to 0.88 and the ranges of excess air fractions and stack temperature rises are 0–1 and 150–700 °F. After identifying and assembling the data set, the following step was the selection of input parameters, which are the model’s independent variables. In this regard, the excess air fraction and stack temperature are considered as input variables and combustion efficiency is introduced as target variable. The data set which contains 72 data points, have been divided into training data set (75% of total data points) and testing data set (25% of total data points) randomly. It should be noted the test data set has been used to investigate the efficiency of the proposed models. In this research, three different computational paradigms including the Adaptive Neuro Fuzzy Inference System (ANFIS), Multilayer Perceptron Artificial Neural Network (MLP-ANN), Support Vector Machine (SVM) and, a simple-to-apply correlation Fig. 9. Regression plots prediction of combustion efficiency using: (a) ANN and (b) ANFIS models. 441 A. Bahadori et al. / Applied Thermal Engineering 102 (2016) 432–446 have been developed to predict the combustion efficiency of natural gas. There are three parameters that require to be set in SVM model before training, namely, penalty factor (C), insensitive coefficient (e) loss function and, corresponding parameter of the kernel function (K). To select an appropriate type of kernel function and its parameters, we should consider application-domain knowledge which reflects distribution of input values of the training data bases [35,36]. In addition, the ANFIS approach has membership functions and its parameters should be determined based of membership function type. The commonly and mostly applicable membership functions are the Gaussian, Triangular mf, Trapezoidal mf, Generalized bell mf, zmf, pimf and, smf. Moreover, the multi-layer perceptron artificial neural network contains some parameters, i.e. bias and weight parameters which should be optimized according to applied optimization method and transfer functions types. A schematic diagram of proposed models is shown in Fig. 2. In order to examine the performance of abovementioned models, the Mean Squared Errors (MSEs), Mean Relative Errors (MREs), Average Absolute Error (AAE), Standard Deviations (STD), Root Mean Square Error (RMSE), and the correlation coefficient (R) have been carried out between the experimental and predicted values. The formulations of these statistical analyses have been shown in Eqs. (17)–(22). MSE ¼ N 1X ðaexp acal Þ2 N i¼1 ð17Þ MRE ¼ N 1X jaexp acal j N i¼1 aexp ð18Þ AAE ¼ N 1X jaexp acal j N i¼1 STDerror ¼ RMSE ¼ N 1 X ðerror errorÞ2 N 1 i¼1 !0:5 N 1X 2 ðaexp acal Þ N i¼1 ð19Þ !0:5 Pn i¼1 f½aexp aexp ½acal acal g qP ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi R ¼ qffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi Pn n i¼1 ½aexp aexp i¼1 ½acal acal ð20Þ ð21Þ ð22Þ where aexp is the experimental data point and acal is the calculated data point by models. Also, N denotes the number of data points. Fig. 10. Regression plots prediction of combustion efficiency using: (a) correlation and (b) SVM models. 442 A. Bahadori et al. / Applied Thermal Engineering 102 (2016) 432–446 Fig. 11. The percentage of relative deviation between model results and experimental values for: (a) ANN and (b) ANFIS models. 4. Results and discussions In the current study, the Radial Basis Function (RBF) is applied as the kernel function of SVM approach. Its parameters greatly affect the number of support vectors and there is close relation between its parameters and the performance of SVM and training elapsed time. If the number of support vectors increase more than enough, over fitting might be occur. However, three parameters of the SVM algorithm (C, e and k) have been determined optimally by evaluating them in a user-defined manner based on prior knowledge and experience. Flow diagram of the proposed SVM model has been shown in Fig. 3. Firstly, we introduced these three parameters to algorithm and according to specified training data points, the SVM is trained and extracts the outputs. Hence, the MSEs between the outputs and corresponding target variable of training data points (combustion efficiency) have been considered as stop criterion of algorithm. Based on specific stop criterion that we define it, the parameters of SVM are tuned. Moreover, to design the ANN architecture, it is vital to note that the optimal number of hidden layers and the number of neurons throughout every layer should be used. Based on results obtained from a guideline regarding overfitting problem, the number of data points should be 10 times the number of connections in the ANN. Hence, as presented in Table 2, through raising the number of hidden neurons, the values of R2 and MSE were determined. Results showed that the optimal number of hidden neurons as gave the minimum deviation should be considered 5 neurons in its hidden layer. Owning to great capability of the Levenberg–Marquardt algorithm, this technique was applied for training process of the ANN model. Moreover, as indicated in Fig. 4, the performance of training stage, which is the MSE, was decreased by raising epochs and the best values obtained 0.000001. To determine optimal construction of the ANN, its parameters namely, bias and weight should be optimized. Levenberg–Marquardt algorithm is used in order to optimize these parameters. Table 3 lists the optimal values of bias and weight for the ANN model. In addition, another model based on the ANFIS was created in order to combustion efficiency estimation. Owning to remarkable features of the Gaussian function, it was employed as membership function of the ANFIS. Based on 10 clusters which have been considered for this system and the number of inputs and output variables, the total number of membership function parameters obtained 60. In more details, each membership functions have two parameters and the number of input and output variables were 2 (stack temperature rise and excess air fraction) and 1 (combustion efficiency) respectively. So, based on ten clusters and three variables, the total number of membership function parameters obtained from Eq. (23). NT ¼ Nc NV Nmf ð23Þ where Nc , N V ; and N mf refer to the number of clusters, number of variables and number of each membership function parameters. A. Bahadori et al. / Applied Thermal Engineering 102 (2016) 432–446 443 Fig. 12. The percentage of relative deviation between model results and experimental values for: (a) correlation and (b) SVM models. Table 5 Statistical analyses obtained from proposed models. Network ANN Analysis Training Testing ANFIS Training Testing MSE R2 MRE% RMSE STD 0.000001 0.9998 0.071294 0.000760 0.000502 0.000002 0.9996 0.142110 0.001428 0.000920 0.000000 1.000 0.026332 0.000283 0.000194 0.000004 0.9985 0.168241 0.002071 0.001595 Network SVM Analysis Training Testing Correlation Total Data MSE R2 MRE% RMSE STD 0.000000 1.0000 0.062801 0.000498 0.000017 0.000000 1.0000 0.062140 0.000494 0.000029 0.000002 0.9992 0.121108 0.001437 0.001108 Optimizing these parameters was carried out by hybrid algorithm (combination of least square and back propagation) in the ANFIS. The stop criterion of this optimization technique was the RMSEs between the actual and predicted combustion efficiency. Details of aforementioned models have been presented in Table 4. As a visual demonstration, the experimental against predicted combustion efficiencies by aforementioned models have been shown as function of the stack temperature rise and excess air fraction in Figs. 5 and 6. The more excess air fractions and stack temperature rises the less the combustion efficiencies. A comparison was shown in Figs. 7 and 8 between the experimental and predicted combustion efficiently using the ANN, SVM, and ANFIS models for both training and testing stages and a model based on simple correlation. The strength of the developed models was remarkably confirmed by the close match between the predicted and experimental data points in assessing the predictive tools for the training and testing steps. A popular technique, which is commonly used in order to modeling, is the regression analysis. Hence, Figs. 9 and 10 have been prepared to show the regression analysis for the present models. The R2 value is an indication of the relationship between the model outputs and actual values. If R2 = 1, this indicates that there is an exact linear relationship between the model outputs and actual values. If R2 is close to zero, then there is no linear relationship between the model outputs and actual values. A close-fitting of data points about the 45° line for the models indicate their accuracy. With the aim of above point, there are great linear relationships between the output of models and actual values. According to statistical viewpoints, Eqs. (24)–(27) are generated as the linear regressions for test data set of the ANFIS, ANN and SVM models and total data set of simple correlation model respectively. 444 A. Bahadori et al. / Applied Thermal Engineering 102 (2016) 432–446 Table 6 Comparison of the proposed models with Bahadori and Vathaluru correlation [14]. Excess air, fraction Stack temperature rise, °C Reported combustion efficiency, fraction Bahadori and Vuthaluru model ANN model ANFIS model SVM model Correlation 0 0 0 0.2 0.2 0.2 0.2 0.4 0.4 0.4 0.4 0.6 0.6 0.6 0.6 0.8 0.8 0.8 0.8 0.8 1 1 1 1 1 1 1 65.5 204.4 371.1 93.3 232.2 315.5 371.1 65.5 176.6 232.2 343.3 93.3 204.4 315.5 371.1 65.5 121.1 260 315.5 371.1 65.5 121.1 148.8 204.4 232.2 315.5 371.1 0.88 0.84 0.789 0.864 0.814 0.784 0.764 0.867 0.82 0.7995 0.751 0.8495 0.796 0.742 0.717 0.8595 0.828 0.75 0.72 0.69 0.8525 0.819 0.8005 0.769 0.751 0.7 0.655 0.8792 0.8384 0.7898 0.8636 0.8144 0.7841 0.76338 0.8678 0.8216 0.798 0.7514 0.8497 0.7953 0.7417 0.7167 0.8582 0.8272 0.7509 0.72049 0.6898 0.8541 0.8173 0.8006 0.7684 0.7522 0.6989 0.6572 0.8815 0.8386 0.7895 0.8640 0.8127 0.7836 0.7644 0.8675 0.8214 0.7986 0.7509 0.8497 0.7959 0.7425 0.7149 0.8585 0.8273 0.7503 0.7200 0.6900 0.8529 0.8188 0.8019 0.7684 0.7517 0.6992 0.6550 0.8780 0.8396 0.7894 0.8641 0.8128 0.7838 0.7652 0.8684 0.8200 0.7995 0.7509 0.8497 0.7959 0.7418 0.7170 0.8530 0.8280 0.7501 0.7177 0.6900 0.8526 0.8187 0.8009 0.7686 0.7517 0.7000 0.6550 0.8784 0.8385 0.7893 0.8636 0.8144 0.7844 0.7642 0.8683 0.8219 0.7984 0.7510 0.8498 0.7959 0.7414 0.7139 0.8579 0.8275 0.7508 0.7198 0.6887 0.8527 0.8187 0.8016 0.7673 0.7501 0.6982 0.6635 0.8795 0.8395 0.7895 0.8635 0.8135 0.7845 0.7645 0.8665 0.8195 0.799 0.7515 0.849 0.7964 0.7425 0.7175 0.859 0.8275 0.7505 0.7205 0.6905 0.852 0.8185 0.8 0.7695 0.7515 0.7005 0.6555 Table A1 Experimental data used in this study [45]. Excess air 0% Excess air 20% Excess air 40% Excess air 60% Excess air 80% Excess air 100% DT (°F) g DT (°F) g DT (°F) g DT (°F) g DT (°F) g DT (°F) g 150 200 250 300 350 400 450 500 550 600 650 700 0.88 0.87 0.8625 0.855 0.848 0.84 0.83 0.821 0.812 0.806 0.799 0.789 150 200 250 300 350 400 450 500 550 600 650 700 0.874 0.864 0.854 0.844 0.834 0.824 0.814 0.804 0.794 0.784 0.774 0.764 150 200 250 300 350 400 450 500 550 600 650 700 0.867 0.857 0.845 0.833 0.82 0.81 0.7995 0.788 0.774 0.761 0.751 0.74 150 200 250 300 350 400 450 500 550 600 650 700 0.8625 0.8495 0.837 0.822 0.809 0.796 0.783 0.77 0.754 0.742 0.73 0.717 150 200 250 300 350 400 450 500 550 600 650 700 0.8595 0.8415 0.828 0.812 0.796 0.7805 0.766 0.75 0.735 0.72 0.705 0.69 150 200 250 300 350 400 450 500 550 600 650 700 0.8525 0.836 0.819 0.8005 0.784 0.769 0.751 0.735 0.717 0.7 0.682 0.655 DT: stack temperature rise, g: combustion efficiency. y ¼ 1:0035 x 0:002; R2 ¼ 0:9985 ð24Þ 2 ð25Þ 2 y ¼ 0:9924 x þ 0:006; R ¼ 1:0000 ð26Þ y ¼ 0:999 x þ 0:00007; R2 ¼ 0:9992 ð27Þ y ¼ 0:9861 x þ 0:011; R ¼ 0:9996 Some popular statistical techniques such as the Mean Squared Errors (MSEs), Mean Absolute Errors (MAEs), Standard Deviations (STD), Root Mean Square Error (RMSE), and R-Squared (R2) have been used to examine the models. The percentage of relative deviations between the experimental and predicted combustion efficiency by the models have been shown in Figs. 11 and 12. These figures indicated behavior of models in terms of accuracy. Deviation ranges of SVM approach have been shorter than other predictive models. The percentage of Average Relative Deviations (ARDs) of testing data set for the ANN and ANFIS models are 0.142110 and 0.168241 respectively. In addition, these values obtained 0.062140 and 0.121108 for the SVM model and simple correlation respectively. The values of Mean Square Errors (MSEs), Average Relative Deviations (ARDs), Standard Deviations (STD), Root Mean Square Errors (RMSEs) and, R-squared (R2) have been summarized in Table 5 for both testing and training data set of aforementioned models. Moreover, as presented in Table 6, we compared the combustion efficiency values at different excess air fractions and stack temperature rises that are determined from the models used in this study with the Bahadori and Vuthaluru correlation that was only previous work regarding estimation of natural gas combustion efficiency. Accordingly, all of models can predict combustion efficiency of natural gas with high satisfactory precision. 5. Conclusion Predicting energy conservation benefits in excess air controlled gas-fired systems is as an interesting subject that was well organized in this contribution. The present study plays importance on applying the computational models such as the Adaptive Neuro Fuzzy Inference System (ANFIS), Multi-Layer Perceptron Artificial A. Bahadori et al. / Applied Thermal Engineering 102 (2016) 432–446 Neural Network (MLPANN), Support Vector Machine (SVM) and, simple correlation based of data gathered from the energy management handbook. These aforementioned strategies can be of great assessment in practice for chemical engineers to have a rapid prediction of natural gas combustion efficiency at wide ranges of applications. The present tools can predict natural gas combustion efficiency as function of stack temperature rise and excess air fraction. The Levenberg–Marquardt algorithm indicated satisfactory performance to optimize the bias and weight values of the ANN model. Hybrid algorithm which is the combination of back propagation and least square was used as great optimization tool to determine membership function parameters of the ANFIS approach. In addition, based on experience knowledge, the optimal values of C, e and, K were determined in the SVM approach. Approximations are recognized to be in high approbation with experimental data points. Based on figures accompanied with the statistical analyses, although the SVM approach achieves much better in accuracy than the other proposed models in order to combustion efficiency estimation, other approaches also had great accuracy. In addition, results obtained from the present models and previous work carried out by Baharori and Vuthaluru confirmed their acceptable precisions. These artificial intelligence methods promise noteworthy advantages in order to combustion efficiency of natural gas modeling. Moreover, unlike complex mathematical techniques for predicting combustion efficiency, the proposed models are simple-to-apply and would be of great help for petroleum engineers especially those dealing with the gas-fired systems. Appendix A Experimental data bases that used in this study are presented in this section. The stack temperature rise (DT), excess air fraction (E) and combustion efficiently of natural gas (g) are presented in Table A1. References [1] X. Xu, C. 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