The present invention relates to data storage systems, and more particularly to a control scheme for a dual stage control system in a data storage system. Still more particularly, the present invention relates to a method and control scheme for compensating the coarse actuators undesired transients in dual stage control systems.
In several data storage systems, such as hard disk drives, the recording head (or heads) is positioned over the disk surface by a rotary or linear actuator. The actuator is moved, or positioned, by a motor. With disk drive systems, a voice coil motor moves the actuator. A voice coil motor is, in simple terms, a coil between two magnets. To move the actuator, a current is applied to the coil to induce a force, and this force moves the actuator.
A recording head reads data from, and/or writes data to, the disk. So positioning the recording head accurately is very important in data storage systems. Typically, the recording head is located at one end of the actuator. But accurate positioning of the recording head can be difficult due to the transient motion created when the actuator and head are moved. Since the actuator is similar to a long beam, moving it causes the actuator to oscillate, or resonate. And this in turn causes the recording head to oscillate. This oscillation, or resonance, makes accurate positioning of the recording head difficult.
One conventional method for compensating for the oscillations of the recording head is to determine the structure of the actuator and recording head in detail. Once known, the movement of the actuator and head can be determined and the resonant frequencies calculated. A control system can then be designed to cause the motor to move in a direction contrary to the transient motion, thereby minimizing, or canceling, the resonance frequencies. A limitation to this method however, lies in the fact that the actuator and recording head oscillate in several directions, thus creating a high number of differing resonance frequency states. Unfortunately, this causes the control system to be complex, which in turn causes the cost of developing and manufacturing such a control system to be high.
To overcome the limitations of the one stage control system described above, dual stage control systems have been proposed. In a dual stage control system, a microactuator is combined with a coarse actuator. A coarse actuator is usually a conventional actuator, while a microactuator typically moves the recording head only. In this type of control system, the actuator is used for the coarse positioning of the recording head, while the microactuator is used for high speed, high accuracy positioning of the recording head.
The design of dual stage control systems, however, is much more complicated than the single stage control system. Anticipating and effectively compensating for the high frequency transient motion of the actuator and recording head is challenging. The undesired transient motion is usually generated by the actuator, suspension, and gimball resonances
A typical method of compensation utilizes transfer function models of the coarse actuator and the microactuator. One conventional control scheme for compensating the coarse actuators undesired transients in dual stage control systems in shown in the block diagram of
The control scheme 100 includes a controller 102, a coarse actuator 104, and a microactuator 106. The coarse actuator 104 is comprised of a Vnom block 108 and a Vres block 110. Vnom is usually an ideal frictionless model, or transfer function, of the coarse actuator 104. For voice coil motor actuators, such as the ones found in hard disk drives, the most frequently used transfer function for the nominal model is Vnom(s)=1/s2, where s is the Laplace transform operator. The resonant portion of the coarse actuator, Vres, is usually determined via finite element analysis of the mechanical structure and/or frequency domain measurements.
The controller 102 is comprised of a control block 112 and a filter 114. Controller 102 is typically a state variable feedback controller. Certain types of microactuators 106 allow explicit measurement of their displacement, and this measurement may be fed back to the controller 102 via line 115.
The position of the recording head relative to the storage medium is measured by means of special servo marks written on, or formed in, the storage medium. The current position of the recording head (y) is fed back as input into controller 102 via line 116. A previously presented position for the recording head (a previously presented specific location where the head is to be moved to) is input into the controller via line 118. Control block 112 then generates two signals, one on line 120 and the other on line 122. The signal on line 120 is input into anti-resonance filter 114 to generate a previously presented signal, uv, on line 123. Filter 114 is used to compensate for the resonance of the coarse actuator, and is described in greater detail below.
The signal uv is input into the coarse actuator 104, where the transfer functions Vnom and Vres are applied to the signal uv to generate a signal yv on line 124. In hard disk drive systems, uv is the current used to move the coarse actuator, and the signal yv represents the positioning motion of the coarse actuator. The signal um on line 122 is input into microactuator 106 and causes the microactuator 106 to move. The microactuator 106 then generates a signal ym on line 126, which represents the positioning motion of the microactuator 106. The position of the recording head (y) on line 128 is the sum of the coarse actuator's motion yv and the microactuator's motion ym, as shown in block 130.
To simplify the controller structure and the design procedure, the controller 102 is usually designed for the nominal portion of the coarse actuator (Vnom), neglecting the resonances, Vres. To minimize the influence the resonances have on the system, a cascade anti-resonance filter 114 is applied. The anti-resonance filter 114 approximates the inverse of the resonance model, i.e. C(s)=1/Vres(s). Thus, the resonant portion of the coarse actuator is cancelled out by inverting the resonance transfer function, Vres.
One limitation to this method, however, is that in many cases Vres contains unstable (right half s-plane) zeros. When an unstable zero is inverted, an unstable pole is created. This results in an unstable pole-zero cancellation, which makes the system unstable (i.e., can not control the motion), and may result in complete failure of the control system.
The present invention overcomes the limitations of the prior art by utilizing a compensation element in a feedforward line from a first positioning element's control signal to a second positioning element's input. In an exemplary embodiment the first positioning element is a coarse actuator and the second positioning element is a microactuator, so that the compensation element is utilized from the coarse actuator's control signal uv to the microactuator's input um. In the exemplary embodiment described herein, the compensation element is a transfer function. This transfer function is defined as:
where ^Vnom (z) is a transfer function model of the nominal portion of the first positioning element, ^Vres (z) is a transfer function model of the resonance portion of the first positioning element, and ^M(z) is a transfer function model of the second positioning element dynamics. The compensation element generates a compensation signal that is input into the second positioning element to compensate for the undesired transient motion from the first positioning element.
The novel features believed characteristic of the invention are set forth in the appended claims. The invention itself, however, as well as a preferred mode of use, and further objects and advantages thereof, will best be understood by reference to the following detailed description of an illustrative embodiment when read in conjunction with the accompanying drawings, wherein:
The present invention relates to a method and control scheme for compensating the coarse actuators undesired transients in dual stage control systems. The following description is presented to enable one of ordinary skill in the art to make and use the invention and is provided in the context of a specific embodiment, namely a hard disk drive system. However, the present invention is not limited to this embodiment. Various modifications to the specific embodiments will be readily apparent to those skilled in the art and the generic principles herein may be applied to other implementations that require very accurate positioning in a control system having dual stages of control. Thus, the present invention is not intended to be limited to the embodiment shown but is to be accorded the widest scope consistent with the appended claims and with the principles and features described herein.
For clarity only one recording disk 202 is shown in
Storage system controller 204 may randomly access a specific logical location on recording disk 202 via a particular track address and a particular sector address. Tracks 116 are very closely spaced in order to maximize storage capacity and economy. The mechanical precision of the movement of recording disk 202 and the movement of recording head 210 is critical to accessing the proper data storage location on recording disk 202. Storage system controller 204 thus requires some means for precisely positioning recording head 210 quickly and accurately over tracks 216 for subsequent storage and retrieval operations.
Referring to
The control scheme 300 includes a controller 302, a first positioning element 304 (e.g. a coarse actuator), and a second positioning element 306 (e.g. a microactuator). Microactuator 306 in this embodiment moves only the recording head, typically in distances that are microns in length. In another exemplary embodiment, the microactuator 306 moves the slider to which the recording head is mounted on.
The coarse actuator 304 is comprised of a Vnom block 308 and a Vres block 310. Vnom is usually an ideal frictionless model, or transfer function, of the coarse actuator 304. For voice coil motor actuators, such as the ones found in hard disk drives, the most frequently used transfer function for the nominal model is Vnom(s)=1/s2, where s is the Laplace transform operator. The resonant portion of the coarse actuator, Vres, is usually determined via finite element analysis of the mechanical structure and/or frequency domain measurements.
The controller 302 is comprised of a control block 312 and a compensation element 317. In this exemplary embodiment, the compensation element 317 is comprised of a first transfer function block 314 and a second transfer function block 316. Controller 302 is typically a state variable feedback controller. As discussed earlier, certain types of microactuators 306 allow explicit measurement of their displacement, and this measurement may be fed back to the controller 302 via line 313 Measurement of the current head position is fed back into the controller 302 via line 315.
The position of the recording head relative to the storage medium is measured by means of special servo marks written on, or formed in, the storage medium. A new position for the recording head is input into the controller 302 via line 318. Control block 312 then generates two signals on lines 320 and 322, respectively. The signal uv on line 320 is input into the coarse actuator 304 and causes the coarse actuator to move. The signal uv is also input into a feedforward line 324, where the compensation element 317 generates a compensation signal on line 326 that compensates for the coarse actuator's transient motion. In this exemplary embodiment, the compensation element 317 is a transfer function defined as:
This transfer function is applied to the signal uv. ^Vnom (z) is a transfer function model of the nominal portion of the coarse actuator, ^Vres (z) is a transfer function model of the resonance portion of the coarse actuator, and ^M(z) is a transfer function model of the microactuator dynamics. The transfer function from uv to y is as follows:
Assuming that ^Vnom≈Vnom, ^Vres≈Vres, and ^M≈M, this transfer function becomes:
Thus, the control scheme of the present invention effectively compensates for the resonances of the coarse actuator.
Returning to
A new position for the recording head (Pn) is also input into microprocessor 406 via signal line 416. In this exemplary embodiment, the microprocessor 406 performs the calculations described with reference to
The digital values are then converted to analog signals via digital-to-analog converters (D/A) 408, 410. As discussed earlier, this embodiment is described with reference to a hard disk drive. Thus, current is input into the actuator and microactuator (not shown) in order to move these two elements. So the voltage values output by D/As 408, 410 are converted to current values via voltage-to-current converters (V/I) 412, 414. The output of V/I converter 412 is the signal uv described above. The output of V/I converter 414 is signal um, also described above.
In an alternative embodiment, a voltage signal is input into a microactuator, and not a current signal. In this alternative system the voltage-to-current converter 414 is not used, and the output of the digital-to-analog converter 410 is fed directly into the microactuator via an appropriate amplifier stage.
While the invention has been particularly shown and described with reference to a preferred embodiment, it will be understood by those skilled in the art that various changes in form and detail may be made therein without departing from the spirit and scope of the invention.
This is a continuation under 35 U.S.C. 371 of PCT/US00/26289 filed 22 Sep. 2000, which claims priority to U.S. Provisional patent application No. 60/155,680 filed 23 Sep. 1999.
Filing Document | Filing Date | Country | Kind | 371c Date |
---|---|---|---|---|
PCT/US00/26289 | 10/12/2001 | WO | 00 | 10/12/2001 |
Publishing Document | Publishing Date | Country | Kind |
---|---|---|---|
WO01/22409 | 3/29/2001 | WO | A |
Number | Name | Date | Kind |
---|---|---|---|
3657524 | Bakke | Apr 1972 | A |
3924268 | McIntosh et al. | Dec 1975 | A |
4200827 | Oswald | Apr 1980 | A |
4736353 | Kasai et al. | Apr 1988 | A |
5177652 | Yamaguchi et al. | Jan 1993 | A |
5189578 | Mori et al. | Feb 1993 | A |
5305158 | Ueda et al. | Apr 1994 | A |
5317550 | Semba | May 1994 | A |
5402400 | Hamada et al. | Mar 1995 | A |
5452275 | Ogawa | Sep 1995 | A |
5623461 | Sohmuta | Apr 1997 | A |
5710497 | Yanagimachi | Jan 1998 | A |
5745319 | Takekado et al. | Apr 1998 | A |
5796558 | Hanrahan et al. | Aug 1998 | A |
5856896 | Berg et al. | Jan 1999 | A |
5862015 | Evans et al. | Jan 1999 | A |
5920441 | Cunningham et al. | Jul 1999 | A |
6005742 | Cunningham et al. | Dec 1999 | A |
6049441 | Ottesen | Apr 2000 | A |
6088187 | Takaishi | Jul 2000 | A |
6101058 | Morris | Aug 2000 | A |
6160676 | Takaishi | Dec 2000 | A |
6295184 | Takekado | Sep 2001 | B1 |
6320720 | Hattori | Nov 2001 | B1 |
6470225 | Yutkowitz | Oct 2002 | B1 |
6490118 | Ell et al. | Dec 2002 | B1 |
6493177 | Ell et al. | Dec 2002 | B1 |
6583964 | Huang et al. | Jun 2003 | B1 |
6587303 | Bui et al. | Jul 2003 | B1 |
6600619 | Morris et al. | Jul 2003 | B1 |
Number | Date | Country |
---|---|---|
0924689 | Jun 1999 | EP |
2-263369 | Oct 1990 | JP |
Number | Date | Country | |
---|---|---|---|
20020171967 A1 | Nov 2002 | US |
Number | Date | Country | |
---|---|---|---|
60155680 | Sep 1999 | US |