History of Moving Coil Actuators in Disk Drives
- Slides: 70
History of Moving Coil Actuators in Disk Drives Presented at SJSU 5/19/18 IEEE Magnetics Monthly Meeting J. Arthur Wagner, Ph. D. Prof. Emeritus in Electrical Engineering SJSU
Basic Purpose of Disk drive Moving Coil Actuators • Disk drives store data magnetically. • The data is stored and located on concentric tracks on surfaces of disks. • Magnetic heads “fly” over the disk surfaces to write or read data to or from magnetic media on a disk. • The purpose of disk drive moving coil actuators is to position the magnetic heads over a track.
Contents • The basic magnetics of a moving coil actuators • Historical cases of actuators
IBM • • • Started operations in San Jose in c. 1956 First location: downtown San Jose First product: RAMAC c. 1956 IBM spawned other disk drive companies In the 1970 s IBM introduced the moving coil actuator using a 14” diameter disk.
Disks • • 24” RAMAC 1956 50 disks 3. 75 MB 14” flying heads 10” 8” 5 ¼” 3 ½” 2 ½” Today’s size 1. 8”
Voice Coil Motor: Like the short air gap, long coil, linear disk drive actuator Leads attached to a moving Coil mounted onto a cylinder. Air gap at inner edge of plate. Axially magnetized ferrite magnet. End plate
IBM Linear Actuator, Like a voice coil motor, “Long Coil”, probably weighed 25 lbs There was a shorted turn on this actuator, not shown. Explain purpose.
Location of the actuator Memorex 360
ISS Ferrite Magnet Linear Actuator • Exchange ferrite for Alnico to reduce the cost • Rectangular coil • Shorted turn • Magnets on the two longer sides of the rectangular coil
ISS Magnetics and Disk Ferrite magnets Center pole Shorted turn Flux path completed through an end plate
Crucial Design Parameter Airgap (allows the coil to move)
ISS or Priam, c. 1981, 14” Disk, Rectangular Coil, Rectangular wire, Aluminum wire
Edge view 6 layers Rectangular wire Aluminum Two coil sides in the air gap ISS 14” Coil
Flux Lines: Cross section for the shown Rectangular Coil linear actuator f = el I X B Head carriage on this end (not shown)
Next step • Multiple disk drives in one box • HDA or EMA • Spindle motors become “direct drive” on the shaft
Linear Actuator ISS Cabinet with Four EMAs ~500 MB spindle motor-”direct drive”
IBM 3370 - Double Actuator
Design of a Linear Cylindrical Actuator Design goal: For fixed outside dimensions, minimize seek time by adjusting the thicknesses of the steel, magnet, clearance, coil, and shorted turn.
Enter 8” Disks
Linear Cylindrical Actuator 8” c. 1986
8” Linear Actuator, Coil, and Shorted Turn Flat aluminum wire Ferrite magnet in three arc segments
From 8” to 5 ¼” disks • The linear actuator was known. • In a 5 ¼” disk drive format, the linear actuator was too long. • Resulted in linear dual coil actuators followed by rotary actuators.
CAST, Dual Coil Actuator 5 ¼” Disks “half high”, c. 1983 Go over geometry Bg = 0. 20 T Ferrite magnets shorted turn coil carriage rails
Seagate, c. 1985, 5 ¼” full high, 20 MB, dual coil linear actuator, coils and carriage not shown Steel Magnets, Ferrite, Shorted turns Bg = 0. 18 T Flux leakage from front plates toward disks Top rail clamped on (not shown) Bottom rail
Siemens (? ) mid 80 s, 5 ¼” full high, Race-track Coil, Circular ferrite magnets, fabricated in two halves. One coil was shared by the halves Bg = 0. 28 T
Enter Samarium Cobalt Magnets • Phased out the ferrite magnets • Sm. Co magnets expensive • Over about a 2 -year span
5 ¼” Floppy Spindle motor Bg = 0. 17 T access Media access One head, each side of media Dual coil Rectangular wire Aluminum Shorted turn (not shown) Sm. Co magnets
Enter the rotary moving coil actuator • The rotary moving coil actuator did not protrude as did the linear actuator. • Designers were wary initially, because of the first torsional resonance mode (low frequency).
Early Rotary Actuator: The magnetics still resembled magnetics of a linear actuator. A pivot was added. The coil had to clear the center pole over its arc. The head arm (flexure) and head were adapted from a linear actuator.
Early Rotary, c. 1985 Siemens head arm mounts (heads not rotated) pivot shorted turn coil magnet Bg = 0. 22 T 1 st torsional mode
DEC, Colorado Springs, 5 ¼”, full high, c. 1988 Pivot point, ferrite magnets, center pole, flux flow Rotary actuator Coil and shorted turn not shown. Coil expensive, but actuator was quite stiff and had a level Kt (torque factor) Bg = 0. 31 T
Rotate the Head 90 deg: Actuator pivoted on an axis (more controllable than bearings on linear rods) c. 1989 Rotating the head and getting the head and flexures was a major, timeconsuming redesign. The flex cable loop inserted a bias into the sum of torques on the actuator.
Syquest removable cartridge. Rotary actuator, Rectangular coil, Counterweight, Head ramp, Troublesome actuator modes, Removable disk format perpetuated the actuator design
Enter the flat coil rotary actuator • • The coil is in a plane. Disk drives were getting smaller. Fit better in the critical, height (z-) direction. Neodymium Iron Boron (Nd. Fe. B) magnet material made thin, flat magnets possible
Early Flat Coil Design Shorted turn not required because of a larger effective airgap, which extends through both magnets and the mechanical gap.
(Quantum) Plus, The rotary actuator head mimicked the linear actuator head orientation pivot balance weight flat coil Successful Product for Quantum. The actuator was nonsymmetrical introducing vibration modes.
Flat Coil Actuator (Samsung) Flat Coil, molded to actuator Parking magnetics Bg = 0. 73 T 3 1/2” Flat Coil on a bobbin Mounted the coil on arms
Flat Coil Actuator, Introduced c. 1989 Shown: Samsung, 3 1/2 inch c. 2006
3 1/2 inch Actuator and Disk
3 1/2 inch Actuator--no Shorted Turn Necessary Magnets on both sides of the coil. Parking latch. Worked using leakage fields.
Enter the 2 ½” disk • Disk drives getting smaller. • This disk size is the main disk now. • Tweaks on the diameter for special disk drives. • A 1. 8” disk was introduced and used briefly in camcorders.
Iota (Syquest) 2 1/2” Removable Disk Late 80 s Flat coil actuator Head ramp (uncommon at the time in fixed HDDs) Bg = 0. 55 T Disk insertion
Dual (Two Stage) Actuator in an HDD, 2013
Summary • Showed the development of the moving coil actuator from c. 1980 • Linear voice coil motors were used on 14”, 8” disk drive products. • The actuator transitioned to rotary beginning with the 5 ¼” disk drive. • The actuator moved to a flat coil midway in the 5 ¼” production. • The flat coil actuator was used, and is now used, in the 3 ½” and 2 ½” disk drives.
References • Boettcher, De Callafon, Talke, “Modeling and Control of a Dual Stage Actuator Hard Disk Drive”, Journal of AMDSM, 2010. • D. Abramovitch and G. Franklin, “A brief history of disk drive control”, IEEE Control Systems Magazine, June 2002. (60 references) • R. K. Oswald, “Design of a disk file head-positioning servo, ” IBM J Res Development, vol. 18, pp. 506 -512, Nov. 1974. • J. Arthur Wagner, “The shorted turn in the linear actuator of a high performance disk drive”, IEEE Transactions on Magnetics, vol. 18, issue: 6, pp. 1770 -1772, Nov. 1982.
Back Up
Servo Data • Servo surfaces (one disk surface) c. 1970 s until c. 1995 – Very high sample rate -- “linear” control system theory – A-B bursts -- A half track right, B half track left • Embedded servo data c. 1995 until today, 2015 – Sampled data control system theory – Sample rates, lower mechanical modes due to rotary actuator
Embedded Servo -- c. 1995
Servo Writing (position data onto disks) • Servo surface and sector servo -- 1970 s -- c. 1999 – – “Servowriter” -- External device positioned head(s) One clock track head and VCM current biased actuator against a pin e. g. laser interferometer guides VCM to servo track • Self servo-track writing -- c. 1999 -- today, 2015 – “Seed” tracks are prewritten by the HDD or externally – Position reference is regenerated from previously written tracks -- close VCM loop and position offset – Servo pattern propagates (error propagates)
2013 Advancement: Dual (Two Stage) Actuator • Track following accuracy • Vibration suppression – Primary actuator • conventional electromagnetic actuator (VCM) • coarse displacement – Secondary actuator • Piezoelectric push-pull • To fine tune the head position
Fundamentally Unchanged by 2015 • Seek Mode • Track Follow Mode – Control Laws in Each • Flat coil rotary actuator (since c. 1989)
Incremental Changes by 2015 • Flat coil, rotary actuator – 3 D Magnetics Analysis – Coil arm manufacturing techniques • Seek mode – Acoustics – Smoother seek profiles--access time trade off
Incremental Changes by 2015 • 2 1/2 in. HDD in 3 1/2 in. footprint • Four disks – Thinner base plate and cover – Lower frequency resonances – Filter out resonances in track following
Will SSDs replace HDDs? • Yes, gradually, but not completely. • SSDs more rugged, more expensive, limited rewrites, lighter weight, lower access time • SSDs may place between RAM and HDD in memory hierarchy • HDDs still lots cheaper. • HDDs moving toward large, long-term, stationary storage • One buys an SSD for its convenience. • Tape storage is still used.
San. Disk (SSDs) • 1991 1 st SSD 20 MB, $1000, $50/MB – went into cameras – eventually replaced 1. 8 HDDs in video cameras • 2002 1 GB Compact Flash Card – demise of film • 2002 1 st USB drive. – replaced spinning flexible media like Iomega’s Clik and Zip drives
San. Disk (SSDs) cont. • 2007 1. 8” and 2. 5” SSDs began replacing HDDs in notebook computers • 2015 SSDs entering PCs and enterprise servers • 2015 Fry’s: random sample – HDD 3 TB $110 – SSD 120 GB (0. 12 TB) $95
Next HDD Technologies • Flash memory caches interior to an HDD, now • Helium-filled space (thinner disks), now • Shingled Magnetic Recording (SMR) 2015 in “mostlyread” applications • Heat-assisted Magnetic Recording (HAMR) 2018 • Two Dimensional Magnetic Recording (TDMR) 2017 • Bit Patterned Media (BPM) 2022 - never • Heated-dot Magnetic Recording (HAMR+BPM) 2022
RAMAC Two heads per arm Head position detent at track Arms position detent at disk Arms move horizontally Carriage moves vertically Drive Capstan Magnetic powder counter rotating clutches Linear potentiometer – vertical position – wiper proportional to distance to go. Velocity control system until near disk Head positioning – same control system
Control Modes • Seek -- Velocity feedback • Track-follow -- Position feedback • Major Electromechanical Parameters – Mass M [kg] or J [kg m^2] – Force Factor Kf [N/A] or Torque Factor Kt [Nm/A] – BEMF Factor Ke [V/m/s] [V/rad/s] (Kt = Ke)
Linear Actuator Models State variables, position X, velocity U, current I s coil shorted turn magnetizing inductance K = force factor U = velocity Z = coil impedance I 1 = Z^(-1)*(Vs - K*U)
Kf Variation Control Design Lived with
Servo Surface: Bottom and Middle of Disk Stack
Velocity Generator (Oswald) z = arbitrary variable can be used for velocity and acceleration (proportional to current)
Phase Plane -- Seek
Trajectory Generator
Beginning of a Seek ISS
128 Track Seek Waveforms ISS
Seek--Showing Velocity Command too steep
Seek Waveforms IBM 3350
IBM type, “Short Coil” steel Cu shorted turn
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