Kong Xiangdong (孔祥东), Song Yu, Ai Chao, Li Yanpeng, Tian Dezhi
(*Key Laboratory of Advanced Forging & Stamping Technology and Science (Yanshan University),Ministry of Education of China, Qinhuangdao 066004, P.R.China)(**Hebei Provincial Key Laboratory of Heavy Machinery Fluid Power Transmission and Control,Yanshan University, Qinhuangdao 066004, P.R.China)(***School of Mechanical Engineering, Yanshan University, Qinhuangdao 066004, P.R.China)
Adaptive friction compensation for large diameter electro-hydraulic proportional valve cores based on LuGre①
Kong Xiangdong (孔祥东)②******, Song Yu***, Ai Chao***, Li Yanpeng***, Tian Dezhi***
(*Key Laboratory of Advanced Forging & Stamping Technology and Science (Yanshan University),Ministry of Education of China, Qinhuangdao 066004, P.R.China)(**Hebei Provincial Key Laboratory of Heavy Machinery Fluid Power Transmission and Control,Yanshan University, Qinhuangdao 066004, P.R.China)(***School of Mechanical Engineering, Yanshan University, Qinhuangdao 066004, P.R.China)
This paper presents an adaptive friction compensation method based on LuGre model for large diameter electric-hydraulic proportional valves in which the valve core contains friction. A mathematic model of the electric-hydraulic proportional valve is established, and the friction characteristics are described based on the LuGre model. The global asymptotic stability of the control system with the adaptive friction compensation controller is guaranteed over Lyapunov theorem. The adaptive compensation of the friction on LuGre friction model is verified by simulation and experiment. The steady-state error is about [-4.23×10-5m, 5.91×10-5m] and [-2.5×10-4m, 2.6×10-4m] on simulation and experiment, the position tracking accuracy is higher, and the lag time of the main valve through the dead zone is shorter. The result proves that the adaptive friction compensation method can effectively compensate for the negative effects of nonlinear friction.
electric-hydraulic proportional valve, pilot stage, LuGre, adaptive friction compensation, experimental identification
As the requirement for hydraulic control system increases gradually, higher requirements are put forward for the electro-hydraulic proportional valve[1]. Research institutions and scholars have promoted the static and dynamic characteristics of the proportional valve by improving the working principle and structure all around the world. Due to the friction characteristics of valve cores, the flow characteristics of valve port and the hysteresis characteristics of coil of the proportional valve, the proportional valve core cannot get accurate displacement control and limits the precision of the control system. Among them, the nonlinear friction characteristic of the valve core is the most important influence factor. The existence of the nonlinear friction leads to the limit cycle oscillation and low speed crawl phenomenon, therefore the static and dynamic characteristics of the proportional valve are affected badly. Reducing the negative impact of the valve core friction is an effective way to improve the proportional valve’s dynamic and static performance.
Based on the structure of optimizing valve core, the nonlinear friction compensation also attracts extensive attention[2]. When the radial force of the proportional valve core is balanced, valve core and valve body fluid port are completely concentric and the clearance around is uniformly distributed between valve core and valve body, only friction caused by Newtonian fluid shear force exists. However, in engineering, certain shape error and deformation exists in valve core and valve body fluid port, inevitably the valve core radial hydraulic pressure distribution is not uniform, and a large numerical friction is formed. Friction is a function of velocity discontinuity, and it is the main factor of high precision motion control[3,4]. Therefore, to improve the performance of proportional valve, the appropriate control method must eliminate the influence of friction.
Nonlinear PID control strategy is a common compensation method. Adjusting the PID parameters by the working state is better to restrain friction, such as analyzing PID control for valve-controlled hydraulic motor positioning control system[5], and friction compensation for the electric cylinder[6]. With the integral element, PID control can eliminate system static error theoretically, but low speed friction nonlinear characteristics, the memory of integral element will lead to the emergence of the limit cycle in position control system. In the following control system, when speed steering happens, the integral loop will lead output torque and static friction to get into the same direction, so as to increase the influence of friction[7]. At present, domestic and foreign scholars put forward some adaptive friction compensation methods, one example is that the coulomb friction is expressed as a function of time, and making up for the defects of fixed coulomb friction model by improving the observer gain[8]. Another method is to present the observer gain as a function of velocity, and the constraint condition of gain function is deduced by Lyapunov function[9]. However, the friction model based on velocity function can’t describe the nonlinear characteristic of friction in static, and the control effect is limited. With the consideration of Stribeck effect in compensation method, a more precise description of the friction phenomenon[10]is given to the ultra-low speed period. Since the above friction model is the static one and its dynamic characteristic of friction compensation effect is limited, its application is restricted.
The LuGre friction model is a relatively complete dynamic friction model. All kinds of static and dynamic characteristics of friction can be accurately described, which has become a hotspot in the research of theory and application[11-13]. Basically, the adaptive control strategy of friction is designed on the basis of Layapunov stability proved in this paper, which enables adaptive compensation of the friction on LuGre friction model.
1.1 Mathematics model of hydraulic proportional valve
The hydraulic principle diagram of large diameter electro-hydraulic proportional valve is shown in Fig.1. It comprises of a proportional amplifier, a pilot stage, a relief valve and a main stage. According to the principle diagram, the mathematical model of the components is established.
1) The proportional amplifier: The proportional amplifier is used to regulate the electro-hydraulic proportional valve which is an important unit. The mathematical model is described by
(1)
where, i is the driven current of the proportional electromagnet, ksis proportional coefficient, e is the input deviation signal, Tiis the integration time constant, Tdis the differential time constant, kais the power amplification coefficient, uiis the bias current, udis the amplitude of chatter signal.
1 The pilot stage; 2 The main stage; 3 The relief valve; 4 The proportional amplifier
2) The pilot stage: The pilot stage uses direct proportional direction throttle valve in this paper. The valve core of power level is driven by the proportional electromagnet directly, and the flow rate and direction are controlled.
The proportional electromagnet is described by
Fph=kei
(2)
where, Fphis the force of the proportional electromagnet, keis the conversion coefficient of the proportional electromagnet.
The force equilibrium equation of pilot valve is described by
(3)
where, mpis the pilot valve core and the equivalent mass in the pilot valve, xpis the displacement of the pilot valve, Bppis the viscosity damping coefficient of the pilot valve, kpkis the centered spring rigidity of the pilot valve, Fptis the steady-state fluid force of the pilot valve, Fptis the transient flow force of the pilot valve, and Fpfis the friction force of the pilot valve.
According to the pilot valve core and valve body dimension relations, the pilot valve opening degree is described by
(4)
where, xpiis the opening degree of the pilot valve port i, xpivis the overlap degree of the pilot valve port i, xpsis the maximum displacement of the pilot valve.
The flow equation is described by
qL=kqxpi-kcpL
(5)
where, qLis the load flow of the pilot valve, pLis the load pressure of the pilot valve, kqis the flow gain, kcis the pressure gain.
3) The main stage: The flow continuity equation of the main valve is described by
(6)
where, Amis the efficient working area of the main valve, xmis the displacement of the main valve core, Ctpis the integrated leakage coefficients, Vtis the total compressed volume and βeis the effective volume elastic modulus.
The force equilibrium equation of the main valve is described by
(7)
where, mmis the main valve core and the equivalent mass in the pilot valve, Bmpis the viscosity damping coefficient of the main valve, kmkis the centered spring rigidity of the main valve, Fmk0is the pre-tightening force of the centered spring, Fmsis the steady-state fluid force of the main valve, Fmtis the transient flow force of the main valve and Fmfis the friction force of the main valve.
4) The displacement sensor: The linear variable differential transformer (LVDT) and modulation-demodulation measuring and amplifying circuit are adopted in this paper. The mathematical model is described by
uf=kmdxm
(8)
where, ufis the feedback voltage of the displacement sensor, kmdis the conversion coefficient of the displacement amplifier circuit.
According to the mathematical model of components, the block diagram of large diameter electro-hydraulic proportional valve is concluded and shown in Fig.2.
The pilot valve controlling main valve is the typical valve control cylinder model with elastic load, the spring- quality-damping system is composed of hydraulic spring, centralizing spring and the mass of main valve. The simplified model of the main valve output displacement is shown in Eq.(9).
Xm=
(9)
where, kceis the flow-pressure coefficient, kce=kc+Ctp, kpis the pressure gain, kp=kq/kce, wris the turning frequency of the pilot valve controlling main valve, ζ0is the integrated damping ratio of the pilot valve control the main valve.
Fig.2 The block diagram of the piloted large diameter electro-hydraulic proportional valve block diagram
1.2 The LuGre model
From relatively static to the relative motion, four experienced stages of the friction of the main valve core are the stage of interface elastic deformation, the stage of boundary lubrication, the stage of partial fluid lubrication and the stage of completely fluid lubrication. In these four stages, the friction and the relative velocity are in steady-state corresponding relationship between contact surfaces, namely the Stribeck model, and the curve is shown in Fig.3.
The steady-state of the LuGre model is consistent with the Stribeck model, which is a relatively complete dynamic model, and the static and dynamic characteristics of nonlinear friction can be described and predicted accurately, and the dynamic compensation effect of the friction is better[14]. In dynamic the LuGre model
Fig.3 The curve of the Stribeck
regards the friction contact surface as elastic mane with stochastic behavior in microscopic[15].
The friction of LuGre model is produced by the mane of deflection, the parameters of which are shown in Eqs(10)~(12).
(10)
(11)
σ0g(v)=Fc+(Fs-Fc)e-(v/vs)2
(12)
where, σ0is the friction rigidity coefficient, z is the average deformation of the bristle, σ1is the damping coefficient of the friction, σ2is the viscous friction coefficient, Fcis the coulomb friction force, Fsis the static friction force, vsis the critical velocity of Stribeck, v is the valve core velocity, g(v) is a bounded function more than zero.
The large diameter electro-hydraulic proportional valve control system monitors the performance and parameters of a controlled object with friction compensation controller, and feeds back acquisition data to the controller, then makes the proportional valve system work in optimal state. When the friction compensation controller is designed, this paper assumes that the special-shaped composite non-circular opening valve has reduced the fluid force of the main valve, and viscous damping coefficient is neglected. Eq.(7) has been simplified, thus the force equilibrium equation of main valve is described by
(13)
By linking Eq.(13) with Eqs(10) and (11), the LuGre model is described by
(14)
where, σ=σ1+σ2>0.
The observer equation is described by
(15)
(16)
The observer error equation is described by
(17)
(18)
(19)
By linking Eq.(19) with Eq.(14) , the equation is described by
(20)
(21)
Define the Lyapunov function for the system
(22)where, r0, r1, r2is the adaptive gain, r0, r1, r2>0.
(23)
The control rate is described by
(24)
(25)
(26)
l0=-ε
(27)
(28)
By linking Eq.(20) with Eqs(21)-(25), the equation is described by
(29)
Therefore, according to the Lyapunov theorem, the adaptive control rate can guarantee global stability for the system.
Through the method of experimental identification, the static and dynamic parameters of the LuGre friction model are obtained.
3.1 The static parameters identification of the friction model
When the system works in steady state (dz/dt=0), by Eq.(13), static friction Ffssis described by
Ffss=pLAm-kmkxm-Fmk0
(30)
the least square method, the results are shown in Fig.4 and Fig.5, the static friction parameters are shown in Table 1.
Fig.4 Fitting curve of the static friction model in positive direction
Fig.5 Fitting curve of the static friction model in negative direction
DirectionThestaticparameters Fs(N)Fc(N)vs(mm/s)σ2(N/(mm/s))Positive151.0767122.184510.690.5475Negative-141.0647-102.6461-9.890.5475
3.2 Dynamic parameters identification of the friction model
(31)
When the motion stops
(32)
where, xsis the steady-state displacement in the region of static friction.
Based on the identification results, xs=0.04029mm is obtained by a small step signal response, then σ0is got.
(33)
By applying the Laplace transform, Eq.(34) is described by
(34)
(35)
where, ωnis the natural frequency of second-order oscillation, ξ is the damping ratio of second-order oscillation, the best damping ratio is 0.7.
By linking Eq.(34) with Eq.(35), the function is described by
(36)
By linking Eq.(33) with Eq.(36), the dynamic friction parameters as shown in Table 2.
Table 2 The identification parameters of the LuGre dynamic friction model
4.1 Joint simulation model for the friction compensation
The joint simulation model of AMESim and MATLAB/Simulink for the piloted large diameter electro-hydraulic proportional valve is shown in Fig.6.
Fig.6 Joint simulation model of AMESim and MATLAB/Simulink
4.2 The simulation analysis of the friction compensation
The low speed crawl phenomenon of the main valve turns up in the process of low speed movement. The paper contrasts the friction compensation effect of the feed-forward compensation and the adaptive compensation. The displacement of main valve core and error response to the sine input (y=7.5×10-3sin0.1π) are shown in Fig.7 and Fig.8.
As shown in Fig.7 and Fig.8, the low speed crawl phenomenon of the main valve core is basically eliminated to the sine input. Under the feed-forward compensation control, the steady-state error is [-1.51×10-4m, 0.76×10-4m]. The friction compensation has a better effect. However, the main valve reversing
Fig.7(a) The response to the sine input
Fig.7(b) The enlarged drawing of Ⅰ
Fig.7(c) The enlarged drawing of Ⅱ
Fig.8 The error curve
in the full scale position, the polarity of the proportional valve has not changed. The main valve high pressure is reduced to the level of the passivity force with the corresponding throttle, and the valve core gets to the dynamic force balance. Therefore, the main valve has a sensitive area, and forms the phenomenon similar to a “flat top”. At the same time, due to the “dead zone”, the biggest tracking error appears at 10s.
The adaptive friction compensation tracking performance is obviously better than the friction feed-forward compensation, its steady-state error is near zero, about [-4.23×10-5m, 5.91×10-5m]. The position tracking accuracy is higher, and the lag time of the main valve through the dead zone is shorter than the feed-forward compensation control. By analyzing the effect of the friction compensation method, the adaptive compensation based on LuGre friction model has obvious advantages in terms of friction compensation, which greatly improves the low speed tracking performance of the position control system.
4.3 The experimental analysis of the adaptive friction compensation
The nonlinear friction compensation hydraulic principle diagram and test bed are shown in Fig.9 and Fig.10.
The friction characteristics change along with the change of system operation conditions and environment, and the friction model parameters changes as well. It is very difficult to achieve satisfactory effect for the feed-forward compensation with fixed parameters. The adaptive friction compensation is combined with friction model parameters estimation and adaptive friction compensation controller, the changes of the friction model parameters and the object system model parameters can be compensated in real time. It achieves satisfactory compensation effect and meets the requirements of control accuracy, experiment curves of which are shown in Fig.11 and Fig.12.
Fig.9 The hydraulic principle diagram of the proportional valve test bed
Fig.10 The test bed of the proportional valve
Fig.11(a) The response to the sine input
Fig.11(b) The enlarged drawing of Ⅰ
Fig.11(c) The enlarged drawing of Ⅱ
Fig.12 The error curve
As shown in Fig.11 and Fig.12, the actual location tracking is essentially overlapped with the given position under the adaptive friction compensation, its steady-state error is near zero, about [-2.4×10-4m, 2.6×10-4m]. The experiment results and simulation results have certain difference due to the change of oil temperature, oil elastic modulus, abrasion of valve core and so on in experiment. The result of the experiment still proves that the adaptive friction compensation method can effectively compensate for the negative effects of nonlinear friction. It is able to achieve location tracking quickly with good stability. Compared with the feed-forward friction compensation method, the compensation effect is better, and it is suitable for high precision positioning control and frequent reversing conditions.
Based on the Lyapunov stability the adaptive law of the friction parameters is designed, and the adaptive compensation model based on LuGre friction model is built. The accurately joint simulation model of large diameter electro-hydraulic proportional valve is established, and the effectiveness of the friction nonlinearity compensation strategy is analysed.
The adaptive friction compensation based on LuGre friction model gives full consideration to the dynamic friction problem of large diameter electro-hydraulic proportional valve core. The adaptive friction compensation method can accurately compensate for the negative effects of nonlinear friction, and it is able to achieve location tracking quickly with good stability. It is a feasible solution to improve the dynamic control performance of large diameter electro-hydraulic proportional valve.
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Kong Xiangdong, born in 1959. He received his Ph.D degrees in Metallurgical Mechanics Department of Northeast Heavy Machinery Institute (Yanshan University) in 1991. He also received his B.S. degree from Zhejiang University in 1982 and received his M.S. degree from Northeast Heavy Machinery Institute in 1985. His research interests include the fluid transmission and control, the design and optimization of hydraulic component.
10.3772/j.issn.1006-6748.2015.04.001
①Supported by the National Key Basic Research Program of China (No. 2014CB046405), Key Projects in the National Science & Technology Pillar Program during the Twelfth Five-year Plan of China (No. 2014BAF02B00, 2011BAF09B04).
②To whom correspondence should be addressed. E-mail: xdkong@ysu.edu.cn Received on Oct. 11, 2014
High Technology Letters2015年4期