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Active-Disturbance-Rejection-Control for Temperature Control of the HVAC System ()

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*Intelligent Control and Automation*,

**9**, 1-9. doi: 10.4236/ica.2018.91001.

1. Introduction

HVAC (heating, ventilation, and air conditioning, HVAC) is a typical complex system with non-linear, strong coupling and strong disturbance influence. The study on HVAC system is significant for the energy efficiency in buildings, and its control strategies are the major concern [1] [2] . Generally, PID control method is adapted in the temperature control of the zone in traditional HVAC system. The overshooting of the temperature often appears. When the special system has high requirement for the thermal and humidity of the zone, the overshooting of the thermal and humidity cannot satisfy the high precision requirement, and the unnecessary energy consumption is produced. In order to solve the above problem, some researches on the control strategies of HVAC system are done, such as fuzzy control of a simple HVAC model [3] [4] , tuning parameters of fuzzy control based on genetic algorithm in HVAC system [5] . Although the studies of HVAC system have obtained some good performances, there are some deficiencies.

Active-rejection-disturbance-control (ADRC) algorithm was proposed by Han Jingqing in 1998 [6] . Compared with traditional control approaches, ADRC shows good control performances, such as robustness [7] , decoupling capability [8] [9] , and so on. Some researches show that ADRC is suitable for the control of complex system with non-linear, strong coupling and disturbance rejection capabilities [10] [11] [12] . The main idea of ADRC approach is that the whole disturbances, including the internal and external, are actively estimated using an extended state observer (ESO) and compensated during each sampling period, and eliminated by controller.

Original ADRC consists of non-linear ESO and non-linear controller, and has strong robustness and disturbance rejection capabilities. However, the development of ADRC is limited by the complicated structure and difficult parameters tuning. In 2001, non-linear ADRC is simplified to linear active rejection disturbance control (LADRC) by Gao [13] . LADRC is simple, and the stability and disturbance rejection capabilities of ADRC are remained, and LADRC is applied widely. Some researches on ADRC of HVAC can be found. ADRC is applied in the temperature control of a zone in HVAC system [14] [15] . However, the structure of non-linear controller is complex and the tuning parameter is a problem.

In the paper, the physical model of HVAC system is built, including the zone, fan, heating coil, duct and sensor. LADRC with strong disturbance rejection capabilities, self-decoupling and simple structure is applied in temperature control of the HVAC system. The design of LADRC in the system is proposed. Simulation in Matlab/Simulink is done. Simulation results are compared with PID and Integral-Fuzzy control. Simulation results show that LADRC has priority to PID and integral-Fuzzy control in rising time, overshooting and rejecting the step disturbance. The study can provide fundamental basis for high-precision requirement, rejection strong disturbance and reduce energy consumption of HVAC system.

2. HVAC Model

In this paper, the temperature control of the HVAC system in winter operation season is chosen, when the disturbances of the system appear, in order to keep the temperature of the zone in 20˚C, actuator adjusts the water supply of internal coil of air handling unit. HVAC model is composed of zone, fan, heating coil and temperature sensor, the structural diagram is showed in Figure 1.

2.1. Zone Model

In this paper, a typical zone is chosen. Its volume is 36 m^{3}. Two people with 150 W

Figure 1. Structural diagram of the HVAC.

load and two lamps with load 500 W are considered. Based on energy and mass balance governing equations of the zone, the equation [5] can be obtained

${\rho}_{a}{C}_{pa}V\frac{\text{d}{T}_{z}}{\text{d}t}={m}_{a}{C}_{pa}\left({T}_{s}-{T}_{z}\right)+KF\left({T}_{o}-{T}_{z}\right)+q\left(t\right)$ (1)

where its parameters is showed in Table 1.

The Laplace transform of the Equation (1) is:

$$ ${T}_{z}\left(s\right)={G}_{z}\left(s\right)\left[\lambda T\left(s\right)+\gamma {T}_{o}\left(s\right)+q\left(s\right)\right]$ (2)

where ${G}_{z}\left(s\right)=\frac{1}{{\rho}_{a}{C}_{pa}Vs+{m}_{a}{C}_{pa}+KF}=\frac{1}{45.23s+60.24}$ , $\lambda ={m}_{a}{C}_{pa}$ , $\gamma =KF$ ,

the diagram of the zone is showed in Figure 2.

2.2. Fan and Sensor Model [16]

Heat transfer from the fan motor to air is considered, and causes air temperature to increase about 1˚C - 2˚C normally. The transfer function of the fan is a first

order function: ${G}_{F}\left(s\right)=\frac{1}{s+1}$ . The sensor measure the actual temperature of

the zone, and transfer to the controller for the control of the temperature, its

transfer function is written as ${G}_{S}\left(s\right)=\frac{1}{s+1}$ .

2.3. Heating Coil Model [16]

In this study, the winter operation season is chosen. Heating coil is water to air heat exchanger, which provides conditioned air for ventilation purposes in buildings. In order to build the simplified model of the heat coil, it has been assumed that the mass flow rate of the water inside the coil and the temperature of the air out from the coil are constants, the balance equation can be obtained:

${C}_{ah}\frac{\text{d}{T}_{co}}{\text{d}t}={f}_{sw}{\rho}_{w}{C}_{pw}\left({T}_{wi}-{T}_{wo}\right)+{\left(UA\right)}_{ah}\left({T}_{o}-{T}_{co}\right)+{f}_{sa}{\rho}_{a}{C}_{pa}\left({T}_{m}-{T}_{co}\right)$ (3)

where the information of the parameters is described in Table 2.

Table 1. Information of the parameters in Equation (1).

Table 2. Information of the parameters in Equation (3).

Figure 2. Diagram of the zone.

The Laplace transform of the Equation (3) is expressed by

${T}_{co}\left(s\right)={G}_{A}\left(s\right)\left[\alpha {T}_{wi}\left(s\right)+{\left(UA\right)}_{ah}{T}_{o}\left(s\right)+\beta {T}_{m}\left(s\right)\right]$ (4)

where ${G}_{A}\left(s\right)=\frac{1}{{C}_{ah}s+\left[{\left(UA\right)}_{ah}+\beta \right]}=\frac{1}{4.5s+0.28}$ .

Similarly, the transfer function of the humidifier can be expressed by

${G}_{p}\left(s\right)=\frac{1}{0.63s+0.21}$ .

In this paper, the values of the parameters in the HVAC system are showed in Table 3.

3. Temperature Control of the HVAC System

3.1. Active-Disturbance-Rejection-Control of the HVAC System

In the temperature control of the zone, a first order ESO and second order controller of the LADRC are chosen, ESO is expressed by

$\{\begin{array}{l}{\stackrel{\dot{}}{z}}_{1}={z}_{2}+{\beta}_{1}\left(-{z}_{1}+y\right)+{b}_{0}u\\ {\stackrel{\dot{}}{z}}_{2}={\beta}_{2}\left(-{z}_{1}+y\right)\end{array}$ (5)

where u and y are the input and output respectively, ${\beta}_{1}$ and ${\beta}_{2}$ are the gains of the observer, ${z}_{1}$ and ${z}_{2}$ are the estimators of the output y and the whole disturbances, second order controller is expressed by

$\{\begin{array}{l}u=\left(-{z}_{2}+{u}_{0}\right)/{b}_{0}\\ {u}_{0}={k}_{p}\left({T}_{r}-{z}_{1}\right)\end{array}$ (6)

The diagram of the LADRC is showed in Figure 3 and Figure 4.

3.2. Integral-Fuzzy Control in the Temperature of HVAC System

In practice, fuzzy control [17] is adopted in many process controls. The steady-state error of the output is a problem in traditional fuzzy controller. Hence, the error integral is added to the fuzzy controller in this study, the fuzzy controller is called integral-fuzzy controller.

Table 3. The parameter values in HVAC model.

Figure 3. Diagram of LADRC.

Figure 4. Structural diagram of LADRC for HVAC system.

1) Design of the fuzzy controller

The inputs in the integral-fuzzy controller of the HVAC system are the error e and its change-in-error
$\text{d}e/\text{d}t$ of return air temperature T_{z} and the set point of the temperature in the zone. The scale of the error
$e\in \left[-2,2\right]$ (˚C), the linguistic value of e is expressed by {neglarge, negsmall, zero, possmall, poslarge} = {NB, NS, ZE, PS, PB}, membership function of the e is triangle; the scale of
$\text{d}e/\text{d}t\in \left[-0.5,0.5\right]$ , the linguistic values of the
$\text{d}e/\text{d}t$ is expressed by {neglarge, negsmall, zero, possmall, poslarge} = {NB, NS, ZE, PS, PB}, membership function of the
$\text{d}e/\text{d}t$ is triangle, the linguistic value of the output u is the following {close, minor-open, half-open, small-open, big-open} = {CB, CS, M, OS, OB}, membership function of the u is trapezoid, the membership functions are drew in Table 4.

Rule base of the fuzzy controller is showed in Table 5.

Table 4. Membership functions of inputs and output for the fuzzy controller.

Table 5. Rule base of the fuzzy controller.

2) Integral of the error

In order to eliminate the steady-state error in the control of the HVAC system, the integral of the error is chosen as a part of the controller, the diagram of the integral-fuzzy controller is showed in Figure 5.

3.3. Simulation of the HVAC System

Supposed that the temperature outside is 0˚C, set point of the temperature of the zone is 20˚C, simulation modules are established in Matlab/Simulink environment, include the traditional PID controller, integral-fuzzy controller and LADRC. When the HVAC system approaches steady state, there are disturbances outside, such as open the door and windows, and so on. A step disturbance is added to the system in t = 500 s in order to check the rejection disturbance capabilities. The tuning parameters of the controllers based on the experience is adapted, the values of the parameters is showed in Table 6.

Simulation result is showed in Figure 6, comparisons in overshot. Rising time and the rising time in step disturbance are showed in Table 7.

Figure 5. Diagram of the integral-fuzzy controller for HVAC system.

Figure 6. Simulation curves of HVAC system.

Table 6. Parameters of the temperature controllers for the HVAC system.

Table 7. Comparison belong three control methods of HVAC system.

4. Conclusion

In the temperature control of the HVAC system, three approaches, including PID control, integral-fuzzy control and LADRC, are designed. Simulation results show that the LADRC obtains a good performance in the rising time and no overshooting; when the step disturbance is added to the system in t = 500 s, the LADRC can quickly and smoothly reach the steady state in 80 s and shows good disturbance rejection capability. In the temperature control of the HVAC system, the LADRC represents in rising time, strong disturbance rejection and high precision. The study provides fundamental basis for the control of the HVAC system and energy conservation.

Project

The project is supported by the Science & Technology Program of Beijing Municipal Commission of Education (No. KM201611417007) and the National Natural Science Foundation of China (No. 51578065).

NOTES

*Corresponding author.

Conflicts of Interest

The authors declare no conflicts of interest.

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