REJECTION OF REPEATABLE AND NON-REPEATABLE DISTURBANCES FOR DISK DRIVE ACTUATORS

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Proceedingsof the AmericanControl Conference San Diego, California June 1999 REJECTON OF REPEATABLE AND NON-REPEATABLE DSTURBANCES FOR DSK DRVE ACTUATORS Jianwu Li Tsu-Chin Tsao Department of Mechanical and ndustrial Engineering University of llinois at Urbana-Champaign Urbana, L 6181 j-li4@uiuc.edu t-tsao@uiuc.edu ABSTRACT This paper presents an application of two-parameter robust repetitive control (TPRRC) in disk drive servo control, where the repeatable rrmout (RRO) and non-repeatable runout (NRRO) are rejected simultaneously. The repeatable disturbances are rejected by tbe internal model structure of TPRRC, while the nonrepeatable disturbances are attenuated by the robust performance specification. The design procedure of TPRRC is given. A simple structure of tbe robust performance weighting function WP(j@ is proposed and the relationship between the coefficients of WP@iS) and the performance specification over the non-repeatable disturbance is discussed too. The simulation results using the measured position error signals (PES) of a disk drive as output disturbance are presented to show the effectiveness of the disturbance rejection of disk drive servo control and demonstrate that it is a cost effective way to improve the track density of disk drives. Keyword Disk Drive Servo Control, Repetitive Control and Disturbance Rejection. 1. NTRODUCTON The capacity of magnetic hard disk drive has increased significantly in recent years, while the size of the hard disk drive is keeping smaller and smaller. This trend is probably to continue in the near future. t is estimated that a high track density of 25 tracks per inch (TP) will be expected by the end of this century [2]. This will require better performance of disk drive servo control. The read/write operation of a disk drive is usually categorized into the track-seeking mode and the track-following mode. n track-seeking mode, the head positioning servo control loop moves the head to the vicinity of a target track. n trackfollowing mode, the head positioning servo control loop precisely positions the head on the desired track for reading or writing of data. As the track density increases, the disk drive servo control becomes more difficult since various disturbances caused by manufacturing processes will limit the performance improvement of the servo control. The disturbances can be divided into repeatable and non-repeatable disturbances. For example, in track following, the eccentricity of the spindle will cause the repeatable runout (RRO). The disk vibration and bearing defects will cause the non-repeatable runout (NRRO). Much research has been done to deal with the repeatable disturbances. The internal model based repetitive control is one of the well-known methods and has been demonstrated to be effective in rejecting repeatable disturbances in disk drives [3] [6]. However, this repetitive control using zero phase error tracking controller (ZPETC) can reject only the repeatable disturbance of a fundamental frequency and its harmonics. n order to achieve high track density, we have to deal with those NRRO. One way is to reduce the NRRO during the disk drive manufacturing processes. The disadvantage is that it will increase the cost of disk drive significantly. The other way is to design abetter control algorithm with the capability to reject both RRO and NRRO simultaneously. Guo(1997) proposed a disturbance rejection controller based on the repetitive controller using ZPETC, where two polynomials of R(z) and S(z) are added to do frequency shaping of sensitivity function over the frequency range of NRRO [4]. However, considering the uncertainty of the model, which is inevitable in practice, the structures of R(z) and S(z) are constrained in order to achieve robustness. Therefore the frequency shaping of sensitivity function based on R(z) and S(z) is limited and the tradeoff between robustness and performance is not elucidated. Li and Tsao (1998) proposed a framework for the synthesis and analysis of robust repetitive controller using structured singular values [8]. t provided a systematic way to tradeoff between robustness and performance by converting the repetitive control design into a standard problem in linear fractional transformation (LFT) form. The robust performance can be achieved not only to the repeatable signal of fundamental frequency and its harmonics, but also to the non-repeatable signals whose frequency range is determined by the performance weighting WP@). To make the controller realizable in practice, a fictitious uncertainty was introduced to substitute the big delay term of repetitive control, such that the designed controller is low order and can be implemented efficiently. To further push the robust performance, Li and Tsao (1998) also presented a two-parameter robust repetitive controller (TPRRC) [9]. An additional design freedom was added to improve the robust performance over the non-repeatable signals. Since TPRRC cart deal with both repeatable and non-repeatable signals, it is a good alternative for disk drive servo control. The challenge is that the non-repeatable disturbances in disk drive servo control (NRRO) usually locate in the high frequency, around 4 Hz as reported in [4] [7] [1]. -783-499-6/99 $1, @1999 AACC 3615

r.... ---- TPRRC ; ~ ------, Figure 1. The Block Diagram of TPRRC @-:@ ~- - 1T%Z-M 1 Q +1 : 1 -. - 1 - - - J Figure 2. The Design Framework of TPRRC This paper presents the repeatable and non-repeatable disturbances rejection in disk drive servo control using TPRRC. t demonstrates that it is a cost-effective way to improve the track density of disk drives by improving the performance of the servo control. n section 2, a brief review of TPRRC and design procedure is given. n section 3, the issues of selection of control model and performance weighting for disk drive servo control are discussed. The relationship between the coefficients of Wp(jtil) and the performarw specification over the non-repeatable disturbance is discussed too. The simulation results using the measured position error signal (PES) of disk drives as output disturbance are presented in section 4 to show the effectiveness of repeatable and non-repeatable disturbances rejection in disk drive servo control. Finally, conclusions are given in section 5. 2. TWO PARAMETER ROBUST REPETTVE CONTROL (TPRRC) There are two objectives in TPRRC: (a). Perfectly reject the repeatable disturbance and its harmonics. n discrete time domain, the repeatable signals are governed by f(k+n)=f(k) for V k (1) where k stands for time and N is the period of the repeatable signal. (b). Achieve robust performance over non-repeatable signals, which is specified by following inequality b p (ja)s TpRRC (ja) <1 for VOS (2) where S-c is the sensitivity function of the closed loop system of TPRRC. W$j@ is the performance weighting. The block diagram of TPRRC is shown in figure 1, where P. is the nominal plant, Wr is the weighting of unmodeled dynamics. The unmodeled dynamics A, is assumed stable and the norm of A, is less than or equal to 1, i.e. A, E91H_ and A)< 1. The actual plant is P. ( + W, A). Where N, + N,= N, N is the period of repeatable signal and N,ssNa. Q is a low pass filter, which is necessary for robustness of the closed loop system. The task is to design controller K, and ~, such that the closed loop system is stable and inequality (2) is satisfied. t is easy to show that the closed loop system can reject the repeatable signals with period of N and its harmonics by internal model A, f)akct ~ [ o (J Af ~ P big [K1K2] Figure 3. The LT Form of TPRRC principle, since there is a periodic signal generator in the structure of TPRRC. n order to design a low order controller which can be realized efficiently, the proposed design framework is shown in figure 2, where the big delay term of repetitive control is substituted by a fictitious uncertainty ~, where 4 is assumed stable and the norm of L is less than or equal to 1, i.e. L e!lih_ and 11411S 1. The design procedure of TPRRC is following: (1). Design the controller K, and 1$ under the design framework of Figure 2, which is converted into a standard problem in LFT form as shown in figure 3, such that sup ~AP(~(p~,(j~)> [K, (@) ~(@)]) < 1 (s) m where AP := {diag ( A,, 4, Ar), A, C, L GC, A~ C).This is a standard wsynthesis problem and can be solved systematically in Matlab. (2). mplement the TPRRC in figure 1, using the controller K, and ~ designed in step (1). (3). t is guaranteed that the TPRRC in figure 1 will achieve the two objectives, i.e. perfectly reject the repeatable signal with period of N and its harmonics, and the sensitivity function of the closed loop system of TPRRC is shaped by inequality (2). Please refer to [9] for proof. 3. SYSTEM MODEL AND PERFORMANCE WEGHTNG 3.1 System Model. A lot of researchers have tried to get an accurate mathematical model of disk drive [1], [1]. These models in complex mathematical form describe the dynamics of each component of disk drive, such as the multiple flexible disks, spindle, bearing and etc.. These models help us to have more 3616

1 ; ;;;;;;;: ; ;:,,,,,,,.,.!!.,,,!,,,,4!!!,,!!!!! 4,,,,,,,,,,,,,,,,,,,,,,,,,,,,,,, n u,,,,,,,,,,,,,,,,,,,!. o - -5~,,,,,,,,,,,,!,,,!. -2 -.!., ~-l:m -2 1 12 13 14 Frequency(Hz) Figure 4. The Frequency Response of System Model insight of the dynamics of disk drive and can be used to predict the resonance of the unbalanced mode and forced response analytically. However, for a control engineer, a simplified model is preferred because of the complexity of controller, speed limit of DSP and other implementation issues. A conventional disk drive actuator has ball bearings and a voice coil motor (VCM). A simplified form of the actuator stransferfunction is proportional to a double integrators.however, the nonlinear dynamics due to the actuator s ball bearings and pivot friction affects the form of the transfer function. A second order model with damp is popular in the design of disk drive servo control. n this paper, the following second order model is used. d -4,,,,,,,,,.,,,!!!!!!!!!,! 1 1 1 1 12 1 Frequency (Hz) Figure 5. The Frequency Response of Performance Weighting Wp@S) T-$=+$-l Figure 6. The Block Diagram of a Disk Drive Control assigning appropriate values of the parameters to,, & K and m, of (5). The relationship between the parameters and the performance specification over non-repeatable disturbances are described as following: tis,: t if~roughly approximates the frequency of non-repeatable disturbances, when it is the middle value of the frequency range where the non-repeatable disturbances locate. KptDp2 P(s) = (4) S2+25JJPS+mpz The frequency response of the model is shown in figure 4. 3.2 PerJorwrance Weighting WP(jti7).As we know, the repeatable signals are taken care of by the internal model structure of periodic signal. However, the performance over non-repeatable signals is described by inequality (2). So, the selection of performance weighting WP@O depends on the performance specification over the non-repeatable signals. Figure 7 shows the measured track-following position error signal (PES) of a disk drive running at 54 rpm. The power spectrum of the PES is shown in Figure 8, where there is a strong non-repeatable disturbance at 42 Hz as predicted by mathematical analysis. A weighting function as simple as possible is preferred, such that the control system is low order and can be implemented efficiently. n this paper, a third order weighting function is used. Wp( jos ) = mn2 * KOSL (5) (ja)2+xmn(ja)+mn2 jgs+gjl The reason choosing the third order timction of (5) as the performance weighting is that we can easily specify the performance specification over non-repeatable signals by ~ ~ corresponds to the performance weight placed on the rejection of the non-repeatable disturbances. ~ is less than 1. The smaller the ~, the heavier weight we place on the rejection of non-repeatable disturbances. K: K specifies the performance weight over the low frequency. f a small steady state error at low frequency is desired, a high gain of K is used. tij~:tis, specifies the low frequency below which small steady state error is desired. The frequency response of the weighting function Wp(jtD)is shown in figure 5. 4. SMULATON RESULTS The simulation is conducted in Simulink of Matlab. To simulate the real disk drive servo system as accurate as possible, a sampled-data control system is constmcted. The block diagram of the sampled-data control system is shown in figure 6, where P(s) is the transfer function of the disk drive servo loop in continuous time domain. The C-c(z) is the discrete time controller of TPRRC, designed in discrete time domain. A zero-order hold is used to connect discrete and continuous signals. The disturbanm d used in the simulation is a measured and normalized trackfollowing position error signal (PES) of a disk drive running at 54 rpm. The PES in time domain is shown in figure 7. The 3617

e,!!, 11,,!.. 4.- 2.- -2 4!!!! -e o,5,1,15.2,25.3,35,4 Time (Secoti) Figure 7. Time Trace of PES (rms=l.788).5.1,15,2.25.3,35 Time (aecocd) Figure 9. The Time Trace of Output of ZPETC (rms=l.683).3, 1 Soo ----- :-.---. ---- -----: ---- 4 ----- -, -----,- ----, -----,--- - 3 -----.-----, - ----, --------- - 6 ----:-.--. -- --- ----- ----- 5----- ----- - L --- ----- ----- 4----- --.-- - --- ----- ----- 3 ---- J-----,- ---, -----, ----- 2 -----.-----, ----, -----, ----- 1 -----.-----,- --- An 2 4 8 8 1 Fmquenoy (Hz) Figure 8. The Power Spectrum of PES 2 4 (loo Boo 1 1 Figure 1. The Power Spectrum of Output of ZPETC RMS of PES is 1.78. To understand the characteristics of the PES, analysis in frequency domain is preferred. The power spectrum of the PES is shown in figure 8. t is obvious that there is a strong non-repeatable runout around 42 Hz, which is not a harmonic of fundamental frequency 9 Hz. For easy comparison, a repetitive controller based on ZPETC is designed for the same system. Figure 9 shows the trackfollowing PES in time domain. We can see that the RMS of PES decreases a little bit from original 1.78 to 1.61. The power spectrum of the PES of ZPETC is shown in figure 1. t is clear that the repeatable disturbance and its harmonics are rejected. However, the non-repeatable disturbance at 42 Hz and other nonharmonics are amplified, which explains why the RMS of PES is only decreased by 1 percent. A TPRRC is designed for the disk drive servo system to reject both repeatable and non-repeatable disturbances. The performance weighting Wn@$ of figure 5 is used and the frequency response of the sensitivity function (i.e. the transfer function from disturbance d to system output y) is shown in figure 11. The sensitivity function keeps the shape of repetitive control at the fundamental frequency 9 Hz and its harmonics and is also shaped to attenuate the non-harmonics around 42 Hz. From the frequency response of sensitivity function, we can see that the non-repeatable disturbances in the frequency range from 3 Hz to 5 Hz will be attenuated. The PES in time domain is shown in figure 12. The RMS of PES is reduced from original 1.78 to.655, which is a 63 percent improvement of RMS. The power spectrum of the output is shown in figure 13. t is obvious that TPRRC reject not only the repeatable disturbance of 9 Hz an its harmonics, but also the non harmonics. n this application, the non-repeatable disturbances around 42 Hz are attenuated dramatically. 5. CONCLUSONS The two-parameter robust repetitive control (TPRRC) is successfully applied to disk drive servo control, such that both repeatable runout (RRO) and non-repeatable runout (NRRO) can be rejected simultaneously. The systematic design procedure of TPRRC and a simple structure of performance weighting function WP(j@ are presented. The relationship between the coefficients of WP(j@ and the performance specification over the non-repeatable disturbances is discussed. The simulation results using the measured position error signal (PES) of a disk drive are presented to show the effectiveness of the disturbance rejection in disk drive 3618

[6] Kempf, C., Messner, W., Tomizuka, M. And Horowitz, R., ----.- --..-..-. 1993, A Comparison or Pour Luscrete- l lmekepetmve Control Algorithms, EEE Control System Magazine, Vol. 13, pp 48-54. [7] Lee, H.S. and Guo, Lin, 1998, Servo Performance Prediction 1:::::: for High Capacity Disk Drives, Proceedings of the 1998 American Control Conference, Philadelphia, USA. [8] Li, Jiartwu and Tsao, T.C. 1998, Robust Performance Repetitive Control Design Using Stmctured Singular Values and ts mplementation, Proceedings of the ASME Dynamic Systems and Control Division, DSC-VO1.64, pp 347-353. [9] Li, Jianwu and Tsao, T.C. 1998, A Two Parameter Robust Repetitive Control Design Using Structured Singular Values, Proceedings of the 37 EEE Conference on Decision and Control, Tampa, Florida, USA, December 1998, pp 123-1235,5,1,15.2.25.3 [1] Shen,. Y.,1997, Closed-Form Forced Response of a Time (Sbcond) Damped, Rotating, Multiple Disks/Spindle System, Journal of Figure 12. Time trace of output (rms=o.6554) Applied Mechanics, VO1.64, pp 343-352. [11] Takaishi, K., mamura, T., Mizoshita, Y., Hasegawa, S., Ueno, T. And Yamada, T., 1996, Microactuator Control for Disk Drive, EEE Transactions on Magnetics, VO1.32, No.3, pp 1863-1866. sl,,, 4.--,----,----S-- -.---~----,-- 2-2.4-6 6 5 ------ ----- --- -- ---------- 4. -----: -----:--- --,----- ;---- 3 -----------, --- --,---------- 2 ----- J ----- --- -- -----!---- 1 ------, -----,--- --,----- ;---- n 2 4 6 8 1 Fmqwncy (Hz) Figure 13. The Power Spectrum of PES of TPRRC servo control and demonstrate that it is a cost-effective way to improve the track density of disk drives. REFERENCE [1] Chen, J.S. and Bogy, D.B., 1992, Effeds of Load Parameters on the Natural Frequencies and Stability of a Flexible Spinning Disk with a Stationary Load System, ASME Journal of Applied Mechanics, VO1.59, pp23-235. [2] Chew, K.K., 1996, Control System Challenges to high track density Magnetic Disk Storage, EEE Transactions on Magnetics, VO.32, No.3, pp 1799-184. [3] Chew, K.K. and Tomizuka, M., Digital Control of Repetitive Errors in Disk_Drive Systems, EEE Control System Magazine, Vol. 1, pp 16-2. [4] Guo, Lin, 1997, Reducing the Manufacturing Costs Associated with Hard Disk Drives - A New Disturbance Rejection Control Scheme EE.?YASME Transactions on Mechatronics, VO1.2, NO.2, June 1997, pp 77-85. [5] Hwartg, D.S., Peng, S.C. and Hsu, P.L., 1994, An ntegrated Control/Diagnostic System for a Hard Disk Drive, EEE Transactions on Control Systems Technology, VO1.2, No.4, pp 318-326. 3619