Research Article  Open Access
A SelfTuning ProportionalIntegralDerivativeBased Temperature Control Method for DrawTexturingYarn Machine
Abstract
Owing to the fast timevarying characteristics, the temperature control for drawtexturingyarn (DTY) machine has higher technical difficulties and results in challenges for system energy optimization. To address the matter, a selftuning proportionalintegralderivative (STPID) based temperature control method is proposed. Referring to the technical procedures of DTY machine, a thermodynamic model is set up. Then, a STPID minimum phase control system is constructed by the polepoint placement method. Subsequently, an artificial neural network based forgetting factor searching (ANNFFS) algorithm is developed to optimize the system parameter identification. The numerical cases show that the proposed ANNFFS algorithm can improve the parameter identification process, and the average identifying efficiency () can increase by more than 50%; compared with the fuzzy PID controller, the proposed STPID method can increase the control accuracy nearly 3 times for the static temperature ascending. The experimental results prove that the proposed STPID method has better abilities of characteristics tracing and antiinterference and can restrain the temperature fluctuation caused by objective switching and the factual control accuracy reaches 3 times that of fuzzy PID method.
1. Introduction
Drawtexturingyarn (DTY) machine can induce tensile strain for long polyester fiber and make the fiber have higher elasticity. For the above operation, heating is an indispensable technical procedure, in which the temperature of heating cabinet is a key control objective. The control precision of temperature will influence the fiber quality parameters containing curl degree, coloration rate, and shrinkage ratio, and it should be limited to less than ±2°C [1].
A DTY machine is of many production channels, in which the processing velocity is commonly higher than 500 m/min [2]. Apparently, it is a classical fast timevarying control objective and brings forward challenges for temperature control systems. Moreover, the working temperature of DTY machine is prone to being influenced by peripheral environmental factors, such as fiber material, fiber moisture percentage, tensile speed, ambient temperature, and heating power. Therefore, the fast timevarying temperature control for DTY machine has higher technical difficulties.
Related research works suggested that proportionalintegralderivative (PID) is an effective temperature control approach for different engineering areas. For the timevarying objectives, the digital PID algorithms with selfadapting abilities are developed to improve the control accuracy [3–7]. Attaran et al. put forward an energy efficiency optimization method for heating, ventilating, and air conditioning (HVAC) system by using a radial basis function neural network (RBFNN) combined with the epsilon constraint (EC). The method adopted the advanced algorithm of RBFNN for the HVAC system to estimate the residual errors, increased the control signal, and reduced the error results [8]. Trafczynski et al. proposed PIDcontrolled heat exchangers to analyze the influence of fouling on the dynamic behavior and proved that, at changed thermal resistance of fouling, the values of tuning parameters should be changed [9]. Moradi et al. developed a temperature controller for the linearized plant based on decoupled fuzzy PID and fuzzy PDtype methods. The results proved that the decoupled fuzzy PID controller could guarantee the robust performance against the modelbased parametric uncertainties, and the poleplacement controller could lead to the less energy consumption [10]. Li et al. provided a GPCPIDbased control strategy for laminar cooling process, which could control the global temperature curve to produce high quality steel, and set up a TS fuzzy model to improve the temperature prediction accuracy [11]. Kanagalakshmi et al. proposed a multimodelbased PID controller for the realtime temperature control of injection molding machine to improve the operator setup time and product quality [12]. Zhang et al. presented a multiinput multioutput (MIMO) selftuning temperature sensing and control system for efficiently modulating the temperature environment within a multimodule instrument, in which the internal temperature of the instrument converged to a target without the need of a system model, thus making the control robust [13]. Pamela and Godwin Premi presented a hot air temperature controller in oven for sterilization using fuzzy PID controller and adaptive smith predictor, which could maintain the optimum temperature in hot air ovens from a farther distance [14]. Zhang developed an improved PID controller based on predictive functional control (PFC) to test the chamber pressure in an industrial coke furnace. The experimental results showed that the controller had the better ensemble performance compared with traditional PID controllers [15].
From the above references, it can be inferred that the key matter of PIDbased temperature control is tracing the characteristic variation of control objective and obtaining the accurate control parameters to guarantee the control effectiveness. For the fast timevarying characteristics of DTY machine channel (heating cabinet), the problems of dynamical parameter identification might become apparent. Consequently, to address the issue, we propose a selftuning proportionalintegralderivative (STPID) based temperature control method for DTY machine.
To accomplish the above research target, the technical route is described as follows. Referring to the thermodynamic characteristics of DTY machine heating cabinet, a discrete mathematics model is set up. A STPID controller for DTY heating cabinet is designed, and the corresponding minimum phase control system is constructed by the polepoint placement method. An artificial neural network based forgetting factor searching (ANNFFS) algorithm is developed to improve the computation efficiency of system parameter identification. A STPID controller is developed based on embedded system technologies, and the control effects are checked by the comparative experiments.
In general, the key scientific contribution of the paper is providing a STPID modeling method and a dynamical parameter identifying method for the fast timevarying temperature objectives. This research not only can offer theoretical references to the control system modelingsolving and energy conservation of fast timevarying process, but can supply direct technical evidences for control system development and energy optimization of related industrial applications.
This paper is organized as follows. In Section 2, the temperature control objective of DTY machine is described, and a thermodynamic model is set up. In Section 3, the digital PIDbased temperature control method is presented, and the STPID controller for DTY machine is designed. In Section 4, the minimum phase system of STPID controller is constructed, and the ANNFFS algorithm is proposed. In Section 5, the numerical instances are provided, and the results are discussed. In Section 6, a STPID controller is developed, and the comparative experiments are performed to verify the effectiveness of the proposed method. In Section 7, the conclusions are presented.
2. Control Objective and Thermodynamic Model
The working procedure of DTY machine is shown in Figure 1. By the mechanical transmission structures, a bunch of fiber enters heating cabinet, where the tensile strain is induced by resistance heating and mechanical stretching. Then, the fiber passes through the heating pipe for shape setting and curls into a fiber package. With respect to the above operations, the fiber transmission process is of higher line velocity (>500 m/min), so it is a classical fast timevarying objective.
Heating cabinet is the key control objective of DTY machine, as shown in Figure 2, and it contains three functional layers: constant temperature layer, heating layer, and thermal insulation layer. The resistance is activated and heats the atmosphere of the heating cabinet. Consequently, the temperature of heating cabinet increases, and the heat radiation of thermal insulation layer will rise. If the heating power equals the heat radiation rate, the temperature of heating cabinet tends to be stable.
For the heating cabinet, the physical conditions are as follows: the initial voltage and power of the resistance are 220 V and 5 kW, respectively, the upper limit temperature is 200°C, and the heating length is 1.5 m. Consequently, we set up a thermodynamic model, as shown in Figure 3, where 1, 2, and 3 represent the air cell, insulation layer, and outside air, respectively; are the temperatures of air cell, insulation layer, and outside air; are the specific heats correspondingly; is the input heat power; and , are the thermal transmission quantities from air cell to insulating layer and insulating layer to outside air, respectively, [16–20].
Based on the above model, the following thermodynamic expression can be obtained: where , represent the heat transfer coefficient, , are the masses of air cell and insulating layer, and , are the heat transfer areas. Since , , , are constants, they are recorded as , , , [21–24].
3. SelfTuning PID Temperature Control Method for DTY Machine
3.1. Digital PID Control Method
Related research works suggested that temperature control can be described by the model of singleorder inertia with lag annulus: where is the system gain factor, is the lag time, is the time constant, is system specific heat, and is radiating coefficient [3, 4, 25–27]. Therefore, it will be with apparent variations according to the different control objectives and environmental conditions. Regarding the temperature objectives of industrial applications, the lag annulus is apt to arouse system overshoot and oscillation. Accordingly, the parameters of temperature objectives will be subjected to largescale changes. For example, during the course of electric furnace heating, since the cooler parts are placed into the furnace continuously, the temperature control model of electric furnace will be varied, and the high control accuracy is hard to achieve.
PID is a linear controller, which is one of the most widely used temperature control methods. Referring to the control effects of proportionalintegralderivative of output temperature error, it can be expressed as where is the time variable, is the error between the ideal output and factual output , is the proportional constant, is integral time constant, and is derivative time constant. Related research works prove that PID can obtain better control effectiveness for some industrial applications and has two merits as follows. Firstly, it is of simple principle and structure and is easy to implement. Moreover, it can match the requirements of different industrial applications and is of higher robust performance [8–10, 28–31].
The current PID control methods can be divided into two modes: digital control and analogue control. The digital control method is prone to being realized by computer, and it has many technical advantages such as good flexibility, low cost, and reliable performance. The transformation of incremental digital PID can be described as
As shown in Figure 4, the incremental digital PID controller only outputs the increment of control objective, that is, ; then the following expression can be obtained:where , and it contains the coefficients about sampling period, proportional ratio, integral time constant, and derivative constant.
3.2. SelfTuning PID Temperature Control Method for DTY Machine
The selftuning control is an effective method that can resolve the nonlinearities and timevarying objectives of complex systems, as shown in Figure 5.
Parameter tuning is the key matter of DTY machine temperature controller and can make the target system have an expected closedloop characteristic equation. Regarding a linear timevarying objective, where , , and are the system undetermined parameters. For the incremental digital PID controller, its transform expression iswherewhere , , and are the system control parameters. To guarantee the closedloop stability, a filtering element needs to be introduced:Accordingly, the system closedloop control diagram is shown in Figure 6.
For the openedloop stable minimum phase system, the polezero cancellation for the forward transform function is performed; that is,where
With respect to some industrial applications, the model order can set and , respectively. Subsequently, the pole points can be denoted by the control parameters , , and , and let thenThe closedloop transfer function can be expressed aswhere is a constant (). By the recursive least square (RLS) method, the control law of selftuning controller is obtained aswhere , , and are the system parameters to be identified. According to (14) and (15), if and are selected adequately, the expected closedloop pole points will be acquired. Selftuning controller is of better characteristics tracing ability to adapt different control objectives, especially for temperature control.
Based on the above hypothesis, the transfer function of temperature control method for DTY machine is described as where , , , and .
The step response of the temperature control objective is shown in Figure 7, and there is no oscillation phenomenon. Therefore, it can be inferred that , and (16) can be revised as where , , and are real roots. Concerning the factual temperature control, (17) needs to be processed by transform with zeroorder hold (ZOH), and the discrete system model is described aswhereThen, let and ; the system difference model is expressed as where represents the lagging sampling period number. Subsequently, referring to (20), the system control diagram is shown in Figure 8.
4. Parameter Identification and PolePoint Assignment Method
4.1. System Parameter Identification
Parameter identification is the key task for the effectiveness of the proposed selftuning PID temperature control method. Regarding the temperature control model in Section 3, to reduce the computation load, the RLS method is adopted to restrict the error of parameter estimation values and factual observation values and approximate it to the factual system output [32–35].
According to the control objective characteristics of DTY machine, we can obtain the closedloop control block diagram of system parameter identification, as shown in Figure 9.
The transfer function expression of the above model isEquation (21) can be represented as
From the above formulae, we can find that the system parameter identification model is a secondorder controller, and the order number equals the order number of temperature control objective of DTY machine. Therefore, it can satisfy the parameter conditions of closedloop systems.
4.2. PolePoint Assignment
System point assignment is an essential factor to the factual working performance of the proposed selftuning PID temperature controller. Pole assignment of selftuning controller is based on normal control strategy, and the steps are described as follows: acquiring the expected polepoint position of a closedloop system; estimating and identifying the system parameters online; obtaining the parameters of controller; calculating the efficiency of controller. As mentioned in Section 4.1, the temperature control objective of DTY machine is a secondorder system, so the closedloop transfer function can be expressed by
Form (23), the zero points of control targets transfer function are located in the lefthalf plane of root plane, so it is a classical minimum phase system. For the above system, we can letwhere , , and .
Consequently, we can acquire the relationship of objective parameters and controller parameters, and the expression is described as where , , , and are the system parameters obtained by online identification, respectively. So the PID control parameters can trace the variation of control objectives, and the system control effectiveness can be improved.
During the RLSbased system parameter identification, the data saturation can influence the identifying accuracy and cause negative effects for the temperature control system [36, 37]. To address the matter, an ANNbased forgetting factor searching (ANNFFS) algorithm is proposed, and the steps are described as follows.
A RLS model for parameter identification is set up:where is the iteration error that is the difference between the current output and expected output.
In an empirical forgetting factor dataset, the initial values of weights and thresholds are selected, and the neural network is initialized.
The feature data of the target object is input by the input layer neurons, and, after the transition actions of weights, thresholds, and the action function, the network output is obtained.
If is less than the expected error, then the algorithm ends; otherwise, it proceeds to the next step.
The connection weights from the output layer to the hidden layer and the output layer neuron thresholds are modified by the following expressions:where is the connection weights from the hidden layer to output layer, is the number of modifications, is the iterative interval, are the neuron errors of hidden layer, is the momentum factor, is the neuron threshold of the output layer, is the number of iterations, and is a positive integer.
The connection weights from the input layer to the hidden layer and the hidden layer neuron thresholds are modified by the following expressions:where are the connection weights from the input layer to the hidden layer, is the neuron error of the output layer, and is the neuron threshold of the hidden layer.
Does the algorithm arrive at the maximum number of training processes? If so, the iteration ends; otherwise, it returns to step .
5. Numerical Simulation and Results Discussion
5.1. Forgetting Factor Searching
Related research works suggested that the forgetting factor selection is connected with the system gain factor. For the larger gain factor, the forgetting factor should select smaller values; on the contrary, the larger forgetting factors should be configured. Consequently, the proposed ANNFFS algorithm can adapt the gain variations of different systems and output better identification results.
To check the effectiveness of the proposed ANNFFS algorithm, the two groups of comparative experiments for the four parameters (, , , and ) have been performed, the parameter truth values are listed in Table 1, and the results are shown in Figures 10–13.

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According to the identification results of in Figure 10, the following results can be obtained. The two methods can perform parameter identification in less than 650 iteration steps, and the proposed ANNFFS algorithm is of better convergence performance, especially for the case with smaller gain factor. In Figure 10(a), the convergence step numbers of ANNFFS and pole assignment are 498 and 612, respectively, so the proposed method can increase the identification efficiency by 18.6%, with smaller error oscillation range. In Figure 10(b), the two methods can converge in less than 400 steps, and the parameter identification is apt to be performed for larger gain factor. The convergence step numbers of the two methods are 365 and 387, respectively, so the convergence advantage of the proposed method tends to be lower.
From the identification curves of in Figure 11, we can conduct the following conclusions. Like the identification results of , the two methods can obtain the expected parameter value in less than 600 iteration steps. The proposed ANNFFS algorithm has higher parameter identification efficiency, and the advantage becomes apparent by the increment of gain factor. In Figure 11(a), the iteration error curve of pole assignment shows remarkable oscillation, and the proposed method can obtain more stable iteration results. The convergence step numbers of the two methods are 382 and 598, respectively, so the proposed method can increase the identification efficiency by 36.1%. In Figure 11(b), the two methods can also converge in less than 400 steps, but the iteration error oscillation still exist on the identification curve of pole assignment. The convergence step numbers of the two methods are 358 and 385, respectively, so the convergence advantage of the proposed method decreases to 7%.
Referring to the identification iteration process about (shown in Figure 12), the following results can be obtained. Compared with the identification results of and , identification iteration for needs lower computation load. The two methods can converge in less than 500 iteration steps, without apparent iteration error oscillation phenomena. The proposed ANNFFS algorithm also can be of better identification efficiency, especially for smaller gain factor. In Figure 12(a), the convergence step numbers of ANNFFS and pole assignment are 175 and 218, respectively, so the proposed method can increase the identification efficiency by 19.7%. In Figure 12(b), different from the results of and , the two methods can converge in more than 300 steps, which proves that the parameter identification for larger gain factor requires more iteration steps. The convergence step numbers of the two methods are 258 and 542, respectively, so the convergence advantage of the proposed method can reach more than 52%.
The identification results for parameter are shown in Figure 13, and the following conclusions can be acquired. In Figure 13(a), the iteration curves of the two methods take on apparent oscillation phenomena. For the pole assignment method, the identification computation requires the max iteration step number: 823. The proposed ANNFFS algorithm can perform parameter identification in less than 600 iteration steps, and the identification efficiency can be increased by more than 27%. In Figure 13(b), the convergence step numbers of ANNFFS and pole assignment are 261 and 745, respectively, so the proposed method can obtain the best identification efficiency improvement (65.0%). The above results prove that the computation load of pole assignment method increases obviously, and the proposed method can perform more stable convergence performance.
5.2. Static Temperature Ascending Process
The static temperature ascending process is the indispensable working procedure of DTY machine heating cabinet and can reflect the primary control performance of the proposed temperature control system. Concerning the issue, the comparative numerical instances with the fuzzy PID method for different working velocities are performed, and the results are shown in Figure 14.
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The simulated experimental conditions are set as follows: the fiber material is polyester, the moisture percentage is 30%, the working velocities () are 600 m/min, 700 m/min, and 800 m/min, respectively, the original temperature is 20°C, the control target temperature is 180°C, and the control accuracy threshold is ±1°C.
From the numerical results of static temperature ascending in Figure 14, the following conclusions can be obtained. The proposed STPID method and fuzzy PID method can match the control accuracy range (±1°C) in less than 500 s. By the increment of working velocity, the timevarying characteristics of the control objective tend to be remarkable, so the convergence process for static temperature ascending requires more heating time. In Figure 14(a), the temperature curve of fuzzy PID is of oscillation phenomenon, and the proposed method can obtain more stable control results. The convergence heating time of the two methods is 255 s and 345 s, respectively, so the proposed method can increase the temperature ascending efficiency by 26.1%. The two methods can all have better control effects, and the control accuracy ranges are ±0.25°C and ±0.45°C, respectively. In Figure 14(b), the proposed method requires lower heating time to perform the temperature ascending convergence. Because of the limited objective tracing ability, the control accuracy of fuzzy PID method decreases apparently, and the accuracy ranges of the two methods are ±0.27°C and ±0.68°C, respectively. In Figure 14(c), owing to the increment of working velocity, the two methods require more than 400 s to match the temperature ascending convergence. The control accuracy of fuzzy PID method decreases continuously to ±0.85°C. The proposed method can keep stable control effects, and the control accuracy can increase nearly 3 times compared with the fuzzy PID method.
6. Industrial Experiments and Results Discussion
6.1. Embedded STPIDBased Temperature Control System
To check the industrial effectiveness of the proposed STPID temperature control method, an embedded STPID temperature control system for DTY machine is developed [38–41]. The control system is composed of CortexM3 embedded processor, LCD human computer interface (HCI), field programmable gate array (FPGA), RAM memory, A/D converter, multichannel switch, driver circuit, power amplification device, and temperature sensors, as shown in Figure 15.
As indicated in Section 1, a DTY machine not only has the fast timevarying characteristics, but possesses many working channels, that is, the heating cabinets. Therefore, the temperature controller can hold the multichannel control points, with the abilities of multichannel selection, input and output. To address the issue, a FPGA is adopted to extend the I/O ports of embedded processor (shown in Figure 15), and the multichannel temperature control for DTY machine is performed.
Since the working temperature of DTY heating cabinet is apt to be disturbed by the environmental factors of fiber material, fiber moisture percentage, tensile speed, ambient temperature, and heating power, the antiinterference scheme is an indispensable component of the temperature control system [42–45]. Considering the above matter, two methods are adopted to resolve it. In the facet of hardware, some antiinterference measures such as optoelectronic isolating should be implemented. For the software, the system selfcheck program is developed according to related working conditions, in which the monitor timer (watch dog) and interrupt program are adopted to improve the system stability. As shown in Figure 16, by the monitor time and interrupt program, the system control procedure can be divided into three independent branches: main program, A/D interrupt program, and timer interrupt program. The above scheme can perform parallel task processing and mutex operation for the data acquisition and temperature control.
6.2. Comparative Experiments and Results Discussion
6.2.1. Temperature Ascending Process
As mentioned in Section 5, as a key technical procedure of DTY machine, the static temperature ascending process can characterize the fundamental control effects of the developed temperature control system. Consequently, the comparative experiments with the fuzzy PID method for the static temperature ascending process at different working velocities are performed, and the results are shown in Figure 17. The experimental conditions are described as follows: the fiber moisture percentage is 33%, the average working velocities () are 620 m/min, 730 m/min, and 810 m/min, respectively, the original temperature is 40°C, the control target temperature is 180°C, and the control accuracy threshold is ±1°C. If the control accuracy exceeds ±2°C, it cannot satisfy the practical technical requirement of fiber heating.
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According to the comparative experimental results of temperature ascending in Figure 17, we can obtain the following conclusions. The experimental results are in accord with the numerical simulation results in Figure 14. The proposed STPID method and fuzzy PID method can match the expected control range (±1°C) in less than 600 s. By the increment of working velocity, the heating time for the expected temperature threshold increases apparently. Compared with the numerical results, the factual static temperature ascending process requires more heating time due to the peripheral environmental factors. In Figure 17(a), the temperature variation range of fuzzy PID method exceeds ±1°C in the earlier 300 s, and the proposed method can obtain more stable control effects with the control accuracy ±0.27°C. Different from the numerical results, the control accuracy of fuzzy PID decreases to ±0.75°C, which proves that it is apt to be influenced by the environmental interferences. In Figure 17(b), the proposed STPID method can obtain better static temperature ascending efficiency. The temperature curve of fuzzy PID still shows oscillation phenomenon, and the control accuracy decreases to ±0.75°C. For the objective tracing ability and antiinterference scheme, the control accuracy of the proposed method shows only a slight decrease, and the accuracy range is ±0.30°C. In Figure 17(c), owing to the increment of working velocity, the two methods require the max heating time to match the temperature ascending threshold. The control accuracy of fuzzy PID method decreases continuously to ±0.98°C. The proposed method can keep the accuracy range to less than ±0.32°C, and the control accuracy can increase more than 3 times.
6.2.2. Steady State Control Effects
Steady state control effects are the most important technical indexes of control systems. In order to verify the validation and superiority of the proposed STPID control method, the comparative experiments with the fuzzy PID control method have been implemented.
During the course of the experiments, by the increasing of temperature, the fiber moisture percentage will decline continuously. When the moisture percentage decreases to 20%, the evaporation rate tends to be accelerating, and the thermal conductivity of fiber will decline rapidly. The above physical process can cause the remarkable variation of control objective and can be regarded as an objective switching process. Accordingly, to check the objective tracing and antiinterference performances of the proposed STPID method, the selected time segments for steady control experiments contain the objective switching process, and the results are shown in Figure 18.
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From the comparative results of steady state control effects in Figure 18, the following conclusions can be inferred. For the moisture stage, the proposed STPID method and fuzzy PID method can match the expected control range (±1°C), that is, keeping the steady state variation trend after the temperature ascending. At the moment of objective switching, the temperature curves of fuzzy PID method show severe fluctuation, and the fluctuation amplitude increases with the increment of working velocity. On the contrary, since the proposed STPID method is of the better abilities of characteristics tracing and antiinterference, it can adapt the remarkable variation of objective and restrain the temperature fluctuation in the range of ±0.85°C. For the dried stage, the control accuracy of fuzzy PID method decreases apparently, even exceeding the expected control range. The proposed method can have stable control effects, and the temperature variation can be limited in the range of ±0.55°C. In Figure 18(a), the temperature fluctuation of fuzzy PID at 900 s is larger than ±1.50°C, and the control accuracy range narrowly satisfies the expected threshold. The temperature curve of the proposed method shows apparent fluctuation, and the steady control accuracy is less than ±0.40°C. In Figure 18(b), the temperature switching fluctuation of fuzzy PID can reach ±2.20°C, which will cause negative influence to normal textile production. The steady control accuracy of fuzzy PID has exceeded the expected threshold, while the proposed method can make the steady accuracy be in the range of ±0.45°C. In Figure 18(c), by the increment of working velocity, the temperature switching fluctuation of fuzzy PID can reach ±2.80°C, and the steady control accuracy decreases to ±1.50°C. The proposed method can keep stable control effects, and the control accuracy can increase nearly 3 times.
7. Conclusion
DTY machine has multiple production channels and fast timevarying characteristics, which bring forward technical challenges for the temperature control systems. This paper addresses the issue by proposing a STPIDbased temperature control method. With respect to the above research target, the corresponding research works have been performed, and the main conclusions are as follows.
According to the thermodynamic characteristics of DTY machine heating cabinet, a discrete mathematics model is set up, and the heat transfer results of the control objective are acquired.
A STPID temperature controller for DTY machine is designed, and the minimum phase control system is constructed by the pole assignment method. To improve the parameter identification efficiency, an ANNFFS algorithm is proposed, which can resolve the data saturation of identification computation.
Two numerical cases are provided, and the simulated results show that the proposed ANNFFS algorithm can optimize the parameter identification process, and the average identifying efficiency for different gain factors (; ) can increase by more than 25% and 50%, respectively, compared with the pole assignment method; the proposed STPID method can obtain stable control effects for the static temperature ascending process, and the control accuracy can increase nearly 3 times, compared with the fuzzy PID controller.
An embedded STPID temperature control system for DTY machine is developed, and the comparative industrial experiments have been performed. The experimental results prove that the proposed STPID method has better abilities of objective characteristics tracing and antiinterference and can restrain the temperature fluctuation caused by objective switching; it can obtain stable steady state control effects, and the factual control accuracy reaches 3 times that of fuzzy PID method.
To sum up, the key scientific contribution of the paper is providing a STPID modeling method and a dynamical parameter identifying method for the fast timevarying objectives. This research not only can offer theoretical references to the control system modelingsolving and energy conservation of fast timevarying process, but can supply direct technical evidences for control system development and energy performance optimization involved in the industrial areas of metallurgy automatic control, mechatronic system monitoring, and pressure vessel maintenance. The subsequent research works will be performed on the computational fluid dynamics (CFD) based heat transfer modeling and realtime parallel control methods.
Nomenclature
:  System output parameters 
:  Heat transfer area from air cell to insulating layer 
:  Heat transfer area from insulating layer to outside air 
:  Radiating coefficient 
:  System excitation parameters 
:  Specific heat constant from input to air cell 
:  Specific heat constant insulating layer to outside air 
:  System specific heat 
:  Air cell specific heat 
:  Insulation layer specific heat 
:  Outside air specific heat 
:  Time constant 
:  Lagging sampling period number 
:  transformation of incremental digital PID 
:  Natural constant 
:  System error 
:  Incremental error 
:  Filtering element 
:  Zeroorder control parameter 
:  Firstorder control parameter 
:  Secondorder control parameter 
:  System transfer function 
:  Incremental step 
:  Heat transfer constant from air cell to insulating layer 
:  Heat transfer constant from insulating layer to outside air 
:  System gain factor 
:  STPID gain factor 
:  Heat transfer coefficient from air cell to insulating layer 
:  Heat transfer coefficient from insulating layer to outside air 
:  Proportional constant 
:  Air cell mass 
:  Insulating layer mass 
:  Positive integer 
:  Iteration number 
:  Input heat power 
:  Heat from air cell to insulating layer 
:  Heat from insulating layer to outside air 
:  Ideal output 
:  Complex domain variable 
:  System real roots 
:  Time variable 
:  Air cell temperature 
:  Insulation layer temperature 
:  Outside air temperature 
:  Derivative time constant 
:  Integral time constant 
:  PID expression 
:  Incremental digital PID expression 
:  Experimental working velocity 
:  Simulated working velocity 
:  Factual output 
:  transformation variable. 
:  Momentum factor 
:  Neuron errors of hidden layer 
:  Neuron error of the output layer 
:  Iteration error 
:  Damping coefficient of STPID 
:  Original iterative value 
:  Iterative interval 
:  Neuron threshold of the output layer 
:  Neuron threshold of the hidden layer 
:  Weights from the hidden layer to output layer 
:  Weights from the input layer to the hidden layer 
:  System lag time. 
Disclosure
The funders had no role in study design, data collection and analysis, decision to publish, or preparation of the manuscript.
Conflicts of Interest
The authors declare that there are no conflicts of interest regarding the publication of this paper.
Acknowledgments
The authors wish to acknowledge the financial supports of the Zhejiang Provincial Health Department Program under Grant no. 2015KYA067 and the Zhejiang Provincial Education Science Plan under Grant nos. 2013SCG386 and 2017SCG028.
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Copyright © 2017 Rong Song and Shuting Chen. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.