CA1286768C - "delta" magnetic head-slider - Google Patents

"delta" magnetic head-slider

Info

Publication number
CA1286768C
CA1286768C CA000526439A CA526439A CA1286768C CA 1286768 C CA1286768 C CA 1286768C CA 000526439 A CA000526439 A CA 000526439A CA 526439 A CA526439 A CA 526439A CA 1286768 C CA1286768 C CA 1286768C
Authority
CA
Canada
Prior art keywords
slider
fluid
bar
trailing edge
cavity
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Fee Related
Application number
CA000526439A
Other languages
French (fr)
Inventor
Michael A. Verdone
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Unisys Corp
Original Assignee
Unisys Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Unisys Corp filed Critical Unisys Corp
Application granted granted Critical
Publication of CA1286768C publication Critical patent/CA1286768C/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Landscapes

  • Adjustment Of The Magnetic Head Position Track Following On Tapes (AREA)

Abstract

ABSTRACT OF THE DISCLOSURE

Described are Delta-shaped magnetic recording "sliders", some being provided with a "back-bar" and associate "purge channel", the air bearing surface area of the sliders increasing gradually from a minimum at its nose to a maximum at its trailing edge.

Description

Ç;7~

"DELTA" MAGN~TIC HEAD-SLIDER

A '~Delta slider" for flying a magnetic head on a fluid bearing above moving magnetic recording media is disclosed in which an air bearing surface ABS includes a generally planar, but divergent, fluid support surface extending generally transver~e to the direction MM of media movement, with ABS area increasing in direction MM.
The leading-edge of this ABS is relatively narrow and pointed. A method of making such a Delta slider is also disclosed.
lQ The present invention relates to magnetic head-slider assemblies, ana more particularly to air bearing slider assemblies used for noncontact recording in magnetic disk files and the like.

Magnetic head assemblies, comprising sliders carrying magnetic transducers, are widely and extensively used in magnetic recording apparatus, particularly disk recording apparatus. Various types of head/slider arrangements that fly on a fluid or air bearing film over the moving recording media surface are well known in the art. In order to maximize the density of stored data on such magnetic disks, the flying height of the transducer above the media is made as small as is practical, with the requirement that a substantially constant height be maintained. Conventionally, the sliders are designed such that they experience, from their support arms, a constant pressure toward the disk surface, with the lifting force of the air bearing serving to hold the slider and transducer away from the disk surface the desired amount when the disk is rotating.
An object of this invention is to provide a novel and improved air bearing slider for a flying magnetic head assembly that maintains a substantially constant spacing relative to a moving magnetic medium during transducing operation.
Another object is to provide a head slider assembly that is insensitive to skew and disk curvature or flutter and has a high degree of bearing stiffness and stability.

7~

Magnetic head assemblies that fly relative to magnetic media have been used extensively. The objectives for improving the noncontact transducing relationship between a magnetic transducer and a magnetic recording medium, such as a rotary disk, are to attain ~ery close spacing between the transducer and the disk, and to maintain a stable constant spacing.
The close spacing, when used with very narrow ~ransducing gaps and very thin magnetic record films, allows short wavelength, high frequency signals to be recorded, thereby affording high density, high storage capacity recording. As the data recording technology progresses, it becomes more desirable to fly magnetic heads more closely to the magnetic disk surface in order to increase data packing density.
Workers are aware of prior art techniques to utilize magnetic head-slider assemblies. In such an air bearing slider assembly, magnetic transducers are affixed thereto for non-contact recording on a passing magnetic disk. Workers know how to mount such magnetic head assemblies (having air bearing sliders) onto carriages -- e.g., to be used in integrated data modules for storage of information in a magnetic disk file.
Efforts now abound to increase the density of storage on such magnetic disks -- e.g., workers are trying to narrow disk-track width.
.

Among the various types of known slider configurations are those of Garnier, et al. U.S. 3,855,625 self-loading), Roscamp, et al U.S. 4,081,846 and the trimaran structures of Warner U.S. 3,823,416 and Piper, S et al. 3,754,104, where the transducing head is supported relative to a record medium by three pads spaced apart from one another in triangular formation.
~ne type of slider which has been developed and which may possess some self-loading characteristic is that shown in the Garnier, et al. patent. This slider, having what is known as a taper-flat configuration with a ramped portion at the leading edge and two air bearing rails extending therefrom to the trailing edge with a rectangular recess therebetween, has provided satisfactory operation in many respects. The structure is substantially self-loading in that the rectangular recess provides a low pressure area to counteract some of the lift provided by the air bearing side rails such that the device tends to fly a distance above the moving media surface which can be controlled by the relationship between the rectangular recess and the fluid bearing rails. However, the Garnier, et al. structure possesses several major disadvantages both in fabrication and in operation. Since the recessed area of that structure is rectangular and is enclosed on three sides by walls, fabrication of the device requires surface etching to produce the necessary configuration.
The requirement for such etching severely restricts the ~ ~ ~~7~3 types of material tha-t may be used. And, the e-lyes are substantially perpendicular to the air bearing surface and act as collectors of dust, debris and foreign material. A build-up of such material in this cavi-ty can change the operating conditions of the slider and head assembly significantly.
Even the slider configurations of Roscamp, et al.
and Warner require expensive processes such as grinding and lapping within confined areas between side rails.
Such requirements not only increase the manufacturing costs but also may have adverse effects upon the production yield.
The present invention provides a "Del-ta slider"
which overcomes many of the disadvantages of the prior art devices. It is an object of this invention to provide a novel Delta slider for flying a mangetic head at a substantially constant spacing from the moving magne-tic media during operation.
It is another object of this invention to provide a Delta slider which resists roll.
A further object is to provide such a slider which is easy and economical to manufac-ture.
To achieve the foregoing, as well as other objects which will become apparent below, the present invention provides a Delta-shaped slider Ass for flying a magnetic head on a fluid bearing relative to magnetic recording media moving in a predetermined direction, which slider includes a slider ABS whose area increases as one proceeds fore-to-aft.

Embodiments of the present invention will now be described, by way of e~ample, with reference to the accompanying drawings (not necessarily to scale), wherein like reference symbols denote like elements.
FIG. 1 depicts, in schematic perspective, a prior art self-loading ("modified Winchester") type slider while FIG. 2 similarly depicts a like known slider whose ABS
pressure profile is given in FIG. 3;
FIG. 4 depicts in plan view a like self-loading slider, shown in side and end views respectively in FIGS.
5, 6, with different pressure profiles thereof given in FIGS. 7 and 8, these being idealized pressure-profiles along respective axes of this slider;
FIG. 9 schematically indicates operational attitude (side view) of such an embodiment, while FIG. 10 indicates the same without a back-bar;
FIG. 11 is a highly-schematic, generalized view (plan, side) of a Delta slider with Back-bar;
FIG. 12-A is an enlarged plan view of a like slider, shown in side view on FIG. 12-B, in associated plan view if FIG 13-A and end-view in FIG. 13-B, with a like plan view in FIG. 14-b and idealized pressure profile across some portions thereof plotted in FIG. 14-A;
FIG. 15 reproduces a photograph of a Delta slider flying over a (transparent) disk;
FIG. 16 idealizedly relates the orientation of pressure pads on a Delta slider;
FIG. 17 very schematically shows a multi-slider workpiece in side view; this shown in idealized fragmentary plan view in FIGS. 1~ and 19; and FIGS. 20/21 show respective modified Delta sliders very schematically and in plan view.

' ~, '....

Illustrated in FIG. 1 is a prior art ~self-loading"
slider 20' of the conventional, taper-flat configuration with ramps 22' leading into air bearing support side rails 24' which run the length of the slider. At the leading edge of the slider a cross rail 26' (emphasizes negative pressure and self-loading of cavity 30') extends between the two side rails 24'. Suitable magnetic transducers 28', schematically illustrated in phantom, are provided at the trailing edge of the transducer.
In this prior art slider 20' the flying height is controlled by the provision of a rectangular negative-pressure cavity 30' bounded on three sides by the side rails 24' and the cross rail 26'. This cavity 30' is generally formed by various etching techniques, is disadvantageous in that the manufacturing processes form side walls 32' and 34' between the base of the cavity 30' and the side rails 24' and transverse rail 26', which side walls are generally perpendicular to the surfaces of the side rail and transverse rail. The abrupt break between the fluid bearing support surfaces and the side walls, as well as the corners at the leading edge of the recess 30' have tended to trap dust and debris and to make continued control of the flying height difficult. As noted above, the necessity for forming such a structure by etching has also limited the materials from which the slider could be fabricated and has complicated the manufacturing process.
FIG. 2 shows an air bearing head slider formed from a substantially rectangular block 110 made of ceramic, by way of example. The slider may be configured with an air bearing surface that is flat, taper-flat, or other variations of geometry. The slider configuration has two spaced side rails 112 and 114 and a cross-rail 16. The leading portion of each rail 112 or 114, relative to a moving data track, is formed as tapered sections 118 and 120 respectively. Between the tapered sections and at the leading end of the slider adjacent to the cross rail 16, a recessed step 119 is configured.
. ~
. ~

Magnetic transducer elements 122a, 122b, which may be thin film assemblies, are bonded to the ends of the rails 112 and 114 at the trailing end 113 of the slider relative to the path of movernent of the data tracks as found for example on a rotating magnetic disk (not shown), The transducing gaps of the elements 122a,b are flush with the surface of the side rails 112 and 114. The slider assembly, when it is urged by a load means toward the surface of a rotating magnetic disk, establishes a thin air lubricating film which separates the gaps of the transducer elements from the disk by a very small, but constant distance.
A negative pressure zons 2~ is formed by the configuration of the side rails and cross-rail. The negative pressure zone is rnade in the recessed region following the cross-rail 116 and between the two side rails 112 and 114 to the same depth as the step 119, which may be in the order of 10 microns.
To provide optimum opposing load forces, and to realize mechanical stability with insensitivity to skew and disk curvature or flutter while preserving high stiffness, reliefs or recessed areas 126 and 128 may be formed on the exposed surfaces of the side rails and at the air bearing surface of the slider. The recesses 126 and 128 are formed, by etching for example, to a depth in the side rails which produces a condition of essentially ambient or slightly subambient pressure across the side rails in the recess areas 126, 128 during flying operation of the head slider. The recesses 126, 128 are preferably formed to a depth in the range of 0.5 to 3 microns. The cross-rail 116 may also be relieved to the same depth as the recesses below the surface of the side rails, during the same fabrication step.

~ ~67~j~
g _ FIG. 3 depicts a trailing edge isometric view of the pressurP profile observed with the implantation of the inventive slider described with reference to FIG. 2. For reference, the outer slider boundaries are at ambient pressure. The zones between the pressure peaks (136 and 144, and 134 and 142) have average pressures essentially equal to ambient, and relate to the side rail relieved zones 126 and 128 respectively. The two projecting positive pressure areas 134 and 136 relate generally to the trailing end surfaces 138 and 140 of the side rails 112 and 114, respectfully, and the positive pressure areas 142 and 144 relate to the front portions 146 and 148 respectively of the side rails. This illustrates "4-point" slider-record contact (see also U.S. 4,218,715).

., . ~ .

67~-~

Descrl~tion of Bac~-bar; feature:
FIGS. 4-6 schematically illustrate a "self-loading"
type slider assembly 20 constructed and modified according to a back-bar feature. This, and other related S techniques and means discussed for all embodiments, will generally be understood as constructed and operating as presently known in the art, except where otherwise specified. And, except as otherwise specified, all materials, methods and devices and apparatus herein will be understood as implemented by known expedients according to present good practice.
More particularly, FIGS. 4-6 will be understood as schematically depicting such a slider 20 which is improved to include a prescribed "full back bar" 21 and associated "purge channel" 23 extending transverse to the direction of slider flight (arrow). Slider 20 will be recognized by workers as otherwise conventional, comprising a ceramic body 1 with a leading edge portion 20-L and a trailing edge portion 20-TR, a pair of (positive-pressure) side-rails 20-R, 20-R' (including projecting, ramped lead-tips 20-T, 20-T'), plus a very shallow interior aerodynamic cavity 20-C (or "negative-pressure channel") of prescribed precise dimensions (usually, up to several hundred ,u-in.).
It has been found that advantageous effects may be produced by a prescribed e~tension of the slider length to accommodate a "back-bar" 21 and intervening "purge channel" 23 of proper dimensions, designed to 9 ~~67~;~

reduce the pressure to zero (atmosphere) -- and yield such effects as flushing the dirt particles away from the transducer end. Workers know that one must guard against detritus clogging slots P, R or cavity L le.g., this can lead to a catastrophic head crash). Now, some detritus build-up is virtually certain with such sliders. For instance, the best filters ["99.999%"
type] correctly used with such equipment will customarily exclude all atmospheric contaminants larger than about 12 ~u". This should eliminate most smoke particles (usually -~250,u"). But smaller airborne contaminants abound and can readily build-up in shallow cavity L (especially at its trailing edge) and/or in slots P, R [e.g., commonly: oil vapor from the disk drive bearings, particles from the media -- also smog, atmospheric dust and fumes, rosin smoke, metallurgical dust and fumes, viruses, etc.]. Thus, the art needs a better contaminant-free slider which avoids, or mitigates, such problems. This is one salient objective of my invention.
Thus, as one feature hereof, an improved, more contaminant-free flying slider is provided with a "back-bar" and associated transverse flush-cavity (purge channel) adapted to better accommodate multiple heads at the lowest point of slider's flying face (above disk), to reduce pitch angle, to better "flush" the slider (cf. more reliable way of keeping "negative-pressure-orifice" clean), to facilitate fabrication of thin film ; ` ' g"~ 7~;~

heads (lower cost, yet high reliability due to accuracy of masking techniques), and to effect improved "purging" (at the R/W gap).
In particular, this allows multiple transducer means to be located anywhere across the "back bar"
(compared with conventional sliders). This "back bar"
extends the full width of the slider (trailing edge) --i.e., to be a "full back bar" (no advantage to less than full width) -- and it may be of any suitable width talong direction of axis A) depending on pitch angle required (e.g., here, several mils width was found suitable).
The "purge channel" 23 is cut just upstream (forward) of the back-bar 21 along the slider ABS face 20-f. Channel 23 will be located (along axis A) such as to terminate cavity L and to distribute positive and negative (dynamic) forces as understood by workers.
Channel 23 may in some instances be cut in two segments.
Channel 23 is preferably cross-sectionally rectangular (square-corners as in FIG. 5, e.g., for fabrication convenience) or virtually any other suitable shape.
For instance, satisfactory operation has been observed with a self-loading slider like slider 20 (FIGS. 4-6) about 170 mils in length L (Lc = 93 mils) by 40 mils in height h (hc = 25 mils), by 110 mils in width w (WC ~ 30 mils); with rails having a width wr of about 15 mils [ramp hp about 0.175 mils in height hr;
tips 20-T about 20 mils in lengthr te ~~ bar 20-L about ~ 7~

20 mils in length, fe] with inner "flying-cavity" 20-c about 500 micro-inch in depth dc and 80 mils in width wc.
For this slider, under relatively conventional "flying" conditions (e.g., disk surface-velocity at mid-track a~out 1500 inch/sec -- 3600 rpm 4"-7" disk band), it is found satisfactory to make "back bar" 21 about 5 mils wide (Wb) and "square" in cross-section (cf. FIG. 5) with a purge channel 23 about 10 mils wide (wp) and about 4 mils deep (dp) and "s~uare-cut". This afforded a stable flying height of about 5-7 micro-inch (at trailing edge, along back-bar), and showed fine "self-flushing" characteristics -- such that workers would likely be surprised.
--Operation of this Embodiment (see FIGS. 7, 8):
FIG. 9 diagrammatically suggests how such a slider 20 is intended to function, as opposed to a like slider 30 lacking the "back-bar" and "purge channel"
(both sliders assumed to be flying above a disk at a desired attitude, for read/write operations). The trailing corner 31-Tc of conventional (self-load) slider 30 in FIG. 10 will be visualized as allowing relatively little air (compressed by slider flight) to escape, and wil~ be seen as approaching so close ("trailing corner" 31-Tc of flying-face 30-f at trailing-edge 31) to the passing disk surface (see plane M'---M') as to readily be occluded by debris build-up -- such as to "block" the desired, necessary purge of its "negative-pressure-channel" 30-c.

~ 7 By comparison, when analogous embodiment 20 is provided with a back-bar 21 and associated purge channel 23 (see FIG. 9) to purge its "negative-pressure-channel" 20-c of debris, air can readily and quickly escape to atmosphere, so the slider 20 may purge itself of debris quite easily. [Note the relatively "massive"
dimensions of purge-channel 23 compared with the miniscule depth of n-p channel 20-c]. Such "purging"
along such a relatively massive channel (cut transverse to the flying direction) is found different from (and superior to) other proposed air escape configurations such as "parallel slots" through bar 20-B. This proposed design is not as practical or economical, etc., as I
would like.
Thus, this "full back-bar/transverse purge channel" design improves operational and other characteristics of the usual "self-load" slider, giving a massive air purge conduit across to the air beari~g surface (to very effectively flush cavity 20-c) and parallel to the back-bar. The "positive pressure" and the "negative pressure" regions provide the "net load"
across the air bearing surface (compare FIGS. 7, 8 with FIG. 4). The positive pressure surfaces (along axis B;
cf. FIG. 8) fully flank the medial negative pressure area (e.g., along axis A; cf. FIG. 7). The resultant (net, loading) force due to these pressures provides a relatively constant load over the slider bearing. Changes in air flow or disk speed will have negligible effect on this loading; hence, a more stable air bearing surface is realized.

~6,7~

The positive loads due to positive pressure distribution along the side rails and the "back-bar"
control the "bearing stiffness" o the slider. The sum of these positive loads tends to increase the "net load", resulting in a higher air-bearing-stiffness (see FIGS. 7, 8 for pressure profiles plotted along axis A, axis B of slider of FIG. 4).
Workers will note that as cavity depth (cd) increases the flying height (fh) increases and becomes less linear vs load change -- and tends to approach the characteristics of a more conventional slider OW
~ordinary Winchester, no Back-Bar) -- something novel in the art -- also, suction decreases as cd increases.
Thus, a worker would likely prefer a MIN cd design (e.g., 100 u"); however, for ease and reliability of rendering such miniscule "cd cuts", we prefer a cd of about 300 u" (or slightly more~.
The positive pressure distributed along the back-bar surface will increase slider stiffness. This added stiffness will tend to improve control of the slider and inhibit undesirable "roll" (e.g., about axis A, FIG. 4). The presence of such positive back-bar pressure also acts to reduce the "pitch restoring moment", and thus reduce "pitch angle" where pitch angle is plotted vs load for a "zero load full back bar" slider.
Workers will be surprised to note that, unlike the ordinary slider, such "back bar sliders" are so relatively insensitive to changes in load (especially the smaller cd, at least for such minor load changes). A
like (surprisingly) insensitivity to disk-velocity is also observed (e.g., 1500-2500 ips).

7~

Initial Delta Embodiment FIG. 11 indicates some broad features of the subject "delta slider" here shown rather generally as - delta slider SL depicted in pitched "flying condition"
flying on an air bearing film past associated magnetic recording medium M. Slider SL will be understood as pitched-up by positive hydrodynamic ~orces on forward pad PD (situated just aft of ramp R) and supported elsewhere by the positive forces on tail section TL as well as some forces from the rail members l-RL enclosing cavity CV -- cavity CV acting as a negative pressure force as with the typical self-floating slider urging slider SL relatively toward passing medium M~ A "Delta slider" will be understood as having a somewhat pointed (reduced width) nose with gradually increasing ABS area going aft therefrom. (The non-ABS
parts of the slider need not follow this Delta-profile, though such is prefeFred).
TABLE A
As further detailed below, many desired characteristics inhere in this "delta slider", such as:
1. It provides a slider with a "three point force profile" and greater stability (less roll, etc; see discussion of FIG. 13 below).
2. The delta shape provides a maximum tail area for mounting read/write heads (as much as with the best - conventional sliders), whereas the overall slider mass (weight) is radically reduced (about one-half of a conventional slider such as in FIG. 1 or in U.S. 3,855,625, etc.).

7~
3. This great reduction in mass is accompanied by a significant decrease in production cost and an increase in the "natural frequency" of the slider --this latter acting to increase the servo band width associated with the head carriage (e.g., when mounted on the same load beam as slider of U.S. 3,855,625, the delta has a natural frequency 5% higher).
4. The delta design is particularly stable, especially laterally and is quite resistant to disturbance from surface asperities, being nimble in negotiating such, without problems.
5. Delta operation is par-ticularly clean, even "self-cleaning", since its "plow-shaped nose" is adapted to thrust particles (dirt, etc.) to one side.
A particularly preferred version of such a delta slider is shown in FIG. 12A in plan view as delta slider l-SL, in associated side view in FIG. 12B and in similar plan view in FIG . 1 3A with a schematic end view in FIG . 1 3B showing the transducer means mounted on the tail.
Thus, slider l-SL has a ramp means 1-R across its forward air bearing surface ("ABS"1, terminating in a somewhat nose portion 1-N which is somewhat pointed as illustrated (the ramp section being relatively conventional as known by workers, both in structure and in function). A positive pressure pad ABS 1-PD is provided just aft of ramp 1-R. A negative pressure cavity l-CV is disposed aft of pad l-PD, and is defined laterally by a pair of thin rail means l-RL.

A back bar arrangement preferably terminates this structure with a back bar slot l-CT just aft of cavity l-CV (and adapted to "purge" l-CV), with the other side of slot l-CT defined by a back bar member ABS l-PB presenting a tail edge l-TL on which transducer means are mounted (e.g., about five as shown schematically in FIG. 13B~. Of course, features like the Back-bar/slot, ramp, etc. are not always necessary for a Delta slider, as workers will perceive.
The slider material may be made of any known "slider material" as known in the art; for instance, a ceramic like Sumitomo No. SCS-AC2 (by Sumitomo Co.) which, as finished, in the illustrated form may be the order of .150 to .160" long by about .120 to .130" wide at tail l-TL and about .034" high with cavity l-CV for instance being 350 to 400 u-in. deep and slot l-CT
being the order of .004" deep by about .010" wide.
Rail walls l-RL will be kept thin (e.g., about .005").
The angle of divergence of the sides (see AA angle, FIG. lOA) may be the order of 20 to 22.
-~Results:
Workers will be surprised at how clean, nimble, stable and effective a slider such as l-SL can be in operation. For instance, FIG. 15 is a photograph taken of such a delta slider flying above a glass disk (photographed from under the disk) with the forward area 12-A flying at about 14 u-in. and the tail area at 12-T flying at about 2 u-in. in very stable condition.

g.2~7~

One reason for the great stability and particularly strong resistance to roll is presented in the analysis summarized by FIG. 14A, a plotting of ideal pressure profiles for a slider air bearing like 5 l-SL, illustrated in associated FIG. 14~. Here, it will be understood that the positive pressure thrusting the slider away from the medium is principally exerked by the "front pad" l-PD and to a lesser degree by thé aft ABS, or "rear pad" (including back bar l-PB and rails l-RL flanking cavity l-CV). This "rear pad" ABS pressure profile will be seen as presenting minor peaks PK, PK' determined principally by the additive function of rails l-RL. These positive pressures will be understood as resisted by the oppositely urging negative pressures of cavity l-CV (see "cavity" in the profile plot).
TABLE B
Some novel features of this delta slider (ABS) appear to be:
1. CLEAN: A triangular or "Delta" shape (in plan-cross-section) together with a properly pitched flying attitude (leading edge flies at greater height than trailing edge above media) appears to give this design a particular self-cleaning aspect. Any dirt particles encountered (at head-disk interface) will likely be deflected to either side of the slider.
2. STABLE: The slider is supported as it flies on the medium by three main pressure points (see discussion re FIG. llA above) with consequent great improvement in i7~

slider stability, especially in the lateral direction (vs. roll).
Thus, as opposed to a conventional "rectangular profile" slider (as slider 20 in FIG. 1), there is virtual complete elimination of "wobble" tendencies (i.e., a lateral "seeking" of a plane of stabilization while flying, with associated oscillation back and forth in the roll direction, e.g., when one rail ABS l-RL is not exactly coplanar with the other). Radical reduction of rail ABS area helps to provide this stability too.
2A. SELF-RIGHTING: Pitch attitude of such a delta slider should be largely determined by the pressure differential under the leading pad ABS (l-PD) vs. that of the trailing edge ABS (l-TE) -- the size of the leading pad l-PD is probably a significant factor determining the air bearing pressure attained (here a pitch of about 80 to 90 micro-radians is assumed).
As long as the air bearing surface adjacent the trailing edge is sufficiently flat, the pressure peaks near the edges of the slider should be relatively equal (see FIG. 12, peaks PK, PK,); this balance of forces will tend to keep the plane of the air bearing surfaces ABS
parallel to the plane of the passing disk.
Further, the fact that the forward pad l-PD has a reduced-length lateral "lever arm" significantly reduces roll tendencies. The pressure peak on this leading pad will be centered on the slider's center line. If the plane of leading pad l-PD is different than the plane of the trailing pad, then leading pad l-PD will tend to 7~i~

exert a roll force on the slider. This is indicated schematically in FIG. 3 where the large ~orce Fl on the leading pad is directed symmetrically on ~he pad, that is on the center line of the slider. Since there is only one force applied to this pad, there is very little (other than the spatial extent of the force) to affect the orientation of the pad with respect to the disk.
The trailing pad, however, has a relatively uniform support along the entire slider width; and this tends to keep its ABS parallel to the disk surface. Since the moment arm of the leading pad tending to roll the slider is so small, the overall roll forces will always be much reduced and relatively trivial and the slider will typically tend to return to its "no-roll" equilibrium state even when perturbed (a "self-righting"
characteristic).
2B. EDGE-FORCES BALANCED: Workers will understand that as this Delta ABS rushes across a disk (or other flat) surface, very very close thereto, a type of "exhaust" is commonly thrown-up about its sides from air escaping the entrapment induced by "wedging" between the up-pitched slider and the passing record. Such "exhaust"
can readily tip a slider ABS to one side (undesired roll) and upset stability. A Delta slider ABS is desensitized to such exhaust-induced roll and related instabilities. Also, the simple "cuneiform" ABS shape makes it much easier for a worker to ascertain the magnitude of such lateral forces.

.-~

Also, a "Delta ABS" is more stable under low transport velocities le.g., flying a few u" above a 3~" or 5~" disk at low rpm -- cf over sputtered recording surface).
3. NIMBLE: Such a delta slider seems to have interesting compliance features that make it more forgiving of media imperfection (e.g., surface asperities~, being lighter and more nimble in dodging-around such surface discontinuities (this also results from its three point pressure contact as well as its somewhat pointed nose and reduction in forward ABS area in the lateral direction (i.e., "forward attentuation"
or "pointing").
--Alternative structures:
Where the Delta ABS pre~erably is somewhat pointed at its leading edge (cf ramp R, FIG. 11), it may merely be snub-nosed in appropriate cases (e.g., see slider II, FIG. 20). hikewise, where the back-bar/slot feature and/or the ramp are not needed, these can be eliminated (see FIG. 20 also, where Delta slider II is like slider I in FIG. 11 except for eliminating ramp and back bar/slot, and exhibiting a relatively blunt nose).
Also, where symmetry of the ABS about center axis ~ ~Ax ~~ Ax FIG. 20) is commonly desired, in some instances it may not be. For instance, one may orient the ABS
sides at different angles; e.g., to nullify unequal "exhaust" or like lateral forces. Thus, FIG. 21 shows a Delta ABS like II in FIG. 20 except that one side diverges from its center axis Ax ~~ A at about 24 (aa) - (vs. larger side-thrust on ABS) while the other diverges at about 24 (bb). Likewise, the size and orientation/
shape of the side rails flanking cavity C~ may be modified. Also, one could adapt this delta ABS for a non-self-loading slider (cf where the cavity CV has the blocking wall on its forward section pierced or removed), though, as usual, such must be downward urged for proper loading.
--Manufacturing methods:
A delta slider (e.g., like slider l-SL discussed above) presents a number of attractive manufacturing features as well. For instance, when using typical slider production techniques, one may expect about twice the yield from a given workpiece, with little or no significant increase in manufacturing time or costs.
This is a very significant advantage of course as workers will ~cknowledge. It is somewhat schematically illustrated in FIG. 15 where a first linear array of delta sliders SL will be seen as formed by common treatment steps on a single multi-slider workpiece 15-P
(see FIGS. 17-19), being first formed there and later cut-out or sliced away (diced). Where sliders SL
(e.g., rectangular) might convent onally be formed from 15-P, the "delta" configuration facilitates doubling the yield approximately, to also form sliders SL', for example. That is, a second identical set of sliders SL' is likewise formed in the interstices between primary sliders SL; these second sliders SL' however are faced in the opposite direction so that their air bearing surfaces ABS are on the opposite side of this plan view.

2~J~3~~

~ 24 -According to known techniques, such a work-piece 15-P may be clamped at both ends, and an array of transducers for each slider set formed along the appropriate edge ( that is lower edge 15-E for sliders SL and the opposite side, and upper edge for transducers of the second slider set SL'). Work-piece 15-P may comprise a three inch thick wafer with the thin film heads deposited on these edges, and with both sides being sputtered and electroplated simultaneously, or at least at the same s*ation, thus reducing the process time by about one-half. Both sides of the wafer would thus be masked (resist deposition and removal in common), washed, cleaned and annealed together, etc; these being performed on both sides of the wafer at the same station (and possibly simultaneously). Then t~.e two slider sets SL, SL' could be cut away for the finished form, yielding approximately twice the number of sliders for little more than essentially the same processing time and trouble-expense.
Workers will be particularly attracted to this feature of "delta sliders", especially the possibility of forming two sets of sliders together, with associated transducers deposited on both sides of the wafer.
Automatic laser machining or ion etching may be used to conveniently define the air bearing geometry.
One may typically find that the leading ABS pad and the trailing ABS pad need not be coplanar in all instances (vs. 4-point pressure profile, as FIG. 3 G~

which requires co-planarity) -- one other advantage of the 3-point pressure profile of a Delta slider (see al80 FIGo 16). "Imperfect flatness" of the leading pad may not be significant in affec~ing Delta slider attitude or stability -- the 3-point pressure profile is more tolerant of changes in such.
Special fixturing and transfer tooling would of course would be advisable. Also, it might not be feasible to attempt to obtain a precise alignment of the "zero-throat" line on both sides of the substrate --thus, it may be pruaent to orient the masks on the "second side" of the workpiece 180 degrees from those on the front side, even where trying to maintain alignment as close as possible. Thus, it is necessary to have access to both cut surfaces on the workpiece as each surface will be machined to form ABS pads, though one need not perform these operations simultaneously. After the sliders are cut from the workpiece, each ~lider can be marXed on a bar-by-bar basis using the negative force cavity l-CV surface as a reference.
FIG. 17 shows a side view of such a workpiece 15-P as described above, clamped top and bottom, while FIG. 19 shows in plan view somewhat greater detail of such a workpiece 15-P. For instance, with a tail-spacing 16-S of about 12 mils one day typically laser-etch an outline each of the sliders (cf step L-l) about 315 + 100 u-in. One may also laser etch the back bar channel (cf step L-2), e.g., about 4 mils deep. One may also laser etch the center cavity l-CV (cf. step L-3), e.g., about 350 + 50 u-in. deep.

- ~ ~!3~

Thus, in summary workers will appreciate that there has been described a novel "delta slider" and associated advantageous manufacturing techniques and that these involve a number of surprising features and advantages, such as those above mentioned.
For instance, such a low mass delta slider is appropriate for use on some state of the art disk drive units. The slider may in some cases even be mounted on conventional support mechanisms such as the "Watrous flexure-load beam" or like flexure-spring cantilever.
Such a light slider will exhibit less momenttlm and be more nimble, thus more readily negotiating a nodule on a disk surface without being destabilized, etc. thereby.
Reduced mass will also increase the slider's natural frequency.
The delta slider forms an advantageous "zero load"
(or negative load) air bearing member and as such it may be appropriate for a wide range of implementations (e.g., 3.5 in. to 14 in. disks); varying head-disk velocities (e.g., from 500 to 2500 ips) and even for use as a "launched" head in a disk drive unit.
And where the back bar is used it is conducive to the placement of a plurality of read/write transducers on the device.
The "three point" medium-contact feature will provide greater stability and less tendency to roll.
Dust particles and the like can be more readily negotiated and/or diverted out of the slider path by the light slider and its pointed nose. And, the pointed nose should slice through the air with less disturbance and oscillation.

9 2~3~

Manufacturing advantages have also been mentioned such as the fact that approximately twice the number of sliders and associated thin film heads can be produced on a given wafer (both sides) with a consequent reduction in wafer cost and processing steps (e.g., heads electroplated in a single step).
Operating with the mentioned slider embodiment (cf. disk velocity of 1508 in/sec; positive pressure rails 15 mil wide and 500 u-inch negative air-pressure cavity), an escape passage 23 as in FIGS. 4-6 and 10 x 4 mils in cross section (for a flying height of 5 to 7 u-inch under the back-bar) increased bearing stiffness (e.g., by about 10~), gave better control and less "roll", while reducing "pitch angle" (e.g., from 130 u-radians to 90 u-radians).
It will be understood that the preferred embodiments described herein are only exemplary, and that the invention is capable of many modifications and variations in construction, arrangement and use without departing from the spirit of the invention.
Workers will appreciate that such "Delta ABS"
features are apt for use with negative pressure type sliders which fly at less than 10 u" (as is back bar).
Workers will also appreciate that, in appropriate instances, one may alternatively use such design (e.g., and back bar/purge channel) with low flying, positive-pressure or zero-pressure (Winchester) sliders.

2.~6~7 .
Further modifications of the invention are also possible. For example, the means and methods disclosed herein are also applicable for flying Delta ABS over other record surfaces. Also, the present invention is applicable for providing a precision-flying ABS in association with other forms of low-mass recording and/or reproducing systems, such as those in which data is recorded and reproduced optically.
The above examples of possible variations of the present invention are merely illust,rative.
Accordingly, the present invention is to be considered as including all possible modifications and variations coming within the scope of the invention as defined by the appended claims.

Claims (29)

1. A "Delta slider" for flying a magnetic head on a fluid bearing relative to magnetic recording media moving in a predetermined direction in the fluid, comprising:
a slider body having means defining a wedge-shaped fluid bearing surface having leading and trailing edges for flying above the moving media, the fluid bearing surface defining means comprising:
a generally cuneiform planar fluid support surface extending generally transverse to the predetermined direction of movement of said media; the area of this surface increasing continuously from a minimum at the leading edge to a maximum at the trailing edge.
2. The combination as recited in claim 1, wherein at least a portion of said slider leading edge defines a ramp angled away from the plane of said fluid support surface and said media.
3. The combination as recited in claim 2, wherein the slider is also characterized by a cavity formed in said fluid support surface and spaced from said leading edge while being positioned adjacent said slider trailing edge, whereby the cavity may serve to create a controlled reduced-pressure area on the fluid bearing surface when the slider is flying above the moving media to urge the slider closer to the media.
4. The combination as recited in claim 1, wherein one or several transducer elements are mounted on, or adjacent to, the trailing edge.
5. An air bearing head slider for supporting transducer elements comprising:
a support structure having a wedge-shaped air bearing surface and a longitudinal axis along said surface, and leading and trailing edges;
side rails disposed along the side edges of said air bearing surface;
a cavity disposed between said side rails;
said air bearing surface area increasing gradually from a minimum at the leading edge to a maximum at the trailing edge; and transducer means mounted along said trailing edge.
6. An air bearing head slider as in claim 5, wherein said side rails and cross-rail define a first relatively deep recessed section disposed towards the trailing edge portion adjacent to one side of said cross rail, said first recessed section being closed on three sides by said rails.
7. The combination as recited in claim 5, wherein a back-bar slot is provided adjacent said trailing edge.
8. A "Delta slider" for flying magnetic transducer means on a fluid bearing relative to magnetic recording media moving in a predetermined direction in the fluid, comprising:
a slider body having means defining a cuneiform fluid bearing surface having leading and trailing edges for flying above the moving media, the fluid bearing surface defining means comprising:
a generally planar fluid support surface extending generally transverse to the predetermined direction of movement of said media and having a minimum area at the leading edge, increasing gradually to a maximum area adjacent the trailing edge;
a portion of said slider leading edge defining a ramp angled away from the plane of said fluid support surface and said media, said transducer means being mounted on said trailing edge.
9. The combination as recited in claim 8, wherein the fluid support surface is also characterized by cavity means formed in said fluid support surface and spaced from said leading edge, and adapted to create a controlled reduced-pressure area on the fluid bearing surface when the slider is flying above the moving media.
10. The slider of claim 9, wherein said cavity means has an opening into said slider trailing edge, whereby fluid within the cavity may be exhausted through the trailing edge opening.
11. The slider of claim 9, wherein the cavity is terminated by back bar means disposed across the trailing face of the slider, this back bar means including purge channel means in fluid communication between the cavity and the ambient atmosphere whereby to better purge the cavity of gas and associated contaminants, a plurality of R/W transducer means being mounted along the back bar means.
12. The combination as recited in claim 11, wherein the back bar means includes a bar member extending fully across the cavity exit zone and across the slider width normal to flying direction and wherein the purge channel means comprises a prescribed shallow groove between said bar member and the exit zone of the cavity, this groove communicating with the sides of the slider and extending relatively transverse said flying direction.
13. The combination as recited in claim 12, wherein the slider is a "self-loading" type.
14. A magnetic recording head-slider assembly for flying magnetic transducer means on a fluid bearing relative to an information storing medium moving in a predetermined "flight-direction" in the fluid comprising:
a support body including means defining a fluid bearing surface having leading and trailing edges and which is adapted to overfly the moving medium, said fluid bearing surface defining means increasing in area from a minimum at the leading edge to a maximum at the trailing edge, and having;
a number of spaced parallel planar fluid support rails extending in the same direction as the predetermined direction of movement of said media;
a flat fluid support surface extending transverse to the predetermined direction of movement of said medium and extending between and substantially planar to the fluid support rails near the trailing edge; and a ramp surface extending from said flat fluid support surface and between said spaced fluid support rails and having a slope of a preselected angle to form a wedge shaped chamber having an opening located between the leading edges of the fluid support rails and magnetic transducer means mounted on, or adjacent, the trailing edge.
15. The combination as recited in claim 14, wherein the assembly is also characterized by:
at least one purge channel means between the ramp surface and the support surface and adapted to direct air flow transverse the "flight-direction"
whereby to quickly purge the flow over the ramp surface, cleaningly; with the magnetic transducer means mounted at the trailing edge of said body and positioned with the gap of each transducer on, and in alignment with, said flat fluid bearing surface; said ramp surface being operative to receive fluid at the open end of said wedge shaped chamber and direct the same toward the flat fluid support surface producing a lifting force thereagainst which causes said support body to over-fly said moving medium on a fluid bearing formed between the spaced parallel fluid support rails adjacent said moving media and the flat fluid support surface extending between said spaced parallel fluid support rails.
16. The slider of claim 15, wherein said channel means defines a fluid release bypass aperture adjacent the trailing edge of the body, and having a diameter selected to purge essentially all the fluid from said wedge shaped chamber to control the thickness of the fluid bearing formed between the body and moving media and the flying height of the slider relative to the moving medium.
17. A multi-channel "Delta-shaped" magnetic transducer-slider assembly comprising:
a ceramic member having a cuneiform bottom slider face having leading and trailing edges, and which is adapted to ride on a thin fluid film a predetermined distance in a flight direction above a moving medium, said bottom slider face defining first and second substantially planar fluid bearing rail surfaces which extend in spaced alignment along the edges of the member and extend toward a third flat fluid support surface which is located between, and offset from, said first and second fluid bearing rail surfaces, said bottom slider face including means defining a ramp surface extending from said third flat fluid support surface and having a slope of a preselected angle to form a wedge-shaped chamber having an opening located between the leading edges of the fluid support rails and having an "exit end" located adjacent said flat fluid support surface;
a plurality of magnetic transducers each having a gap width of a preselected dimension, these being disposed at a predetermined uniform spacing therebetween, said magnetic transducers being mounted on the trailing edge of said ceramic member at the third fluid bearing surface and positioned with the gap of each adjacent to and in alignment with said third fluid bearing surface;

said plurality of magnetic transducers and said ceramic member co-acting with a moving medium to enable said bottom slider surface and magnetic transducers to be supported on a fluid film formed between said first, second and third bearing surfaces, said ramp surface and the surface of a moving medium; and purge channel means between the exit end of the ramp surface and the third support surface, said channel means being adapted to direct fluid flow from said ramp surface transverse said flight-direction, purgingly;
said ramp surface being operative to receive fluid at the open end of said wedge-shaped chamber and direct the same past the flat fluid support surface producing a lifting force thereagainst to position said plurality of transducers a predetermined distance above the surface of said media equal to the thickness of said fluid film to position said transducers across a moving medium forming a plurality of tracks thereon wherein the width of each track is substantially equal to the preselected gap width of each magnetic transducer and the spacing between each track is substantially equal to the predetermined spacing between each magnetic transducer.
18. A Delta-shaped magnetic recording slider having a prescribed shallow "flying cavity" on its medium-confronting face, this cavity being terminated by back bar means disposed across the trailing face of the slider face, and adapted to present a full-width trailing edge for mounting any number of transducer means, this back bar means including purge channel means in fluid communication between the cavity and the ambient atmosphere whereby to better purge the cavity of gas and associated contaminants; the area of this face increasing from a minimum at the slider leading portion to a maximum at its trailing edge;
a plurality of thin film R/W transducer means being so disposed along the back bar means, the back bar surface terminating at the trailing edge, being sufficiently wide to reduce pitch angle to a prescribed value, inhibit roll and increase slider stiffness a prescribed amount.
19. The combination as recited in claim 18, wherein the back bar means includes a bar member extending fully across the cavity exit zone and across the slider width, measured normal to flying direction, the cavity being flanked by a pair of slider rails; and wherein the transducer means comprise thin film heads fabricated on the bar member.
20. A method of fabricating a "Delta slider" means for flying a magnetic head on a fluid bearing relative to magnetic recording media moving in a predetermined direction in the fluid, this slider means comprising:
a slider body having means defining a wedge-shaped fluid bearing surface having leading and trailing edges for flying above the moving media, the fluid bearing surface defining means comprising:
a generally cuneiform planar fluid support surface FSS, the method including:
providing a rectangular bar of slider material, this bar including a pair of elongate planar parallel "top" and "bottom" faces defined between opposing parallel sides;
forming a row of identical relatively adjacent triangular slider pieces, including forming air bearing surfaces and associated cavities and other elements in common, the sliders being disposed in alternating reversed juxtaposition along the row; and severing the sliders so formed from the bar.
21. The combination as recited in claim 20, wherein identical arrays of thin film transducers are formed, in common, along each slider base before severing.
22. The combination as recited in claim 21, wherein the sliders are defined and their elements so formed in common so as to be juxtaposed in alternatingg face-up/bottom-up relation, wherein an adjacent slider is up-ended and also face reversed, whereby every even number slider ABS faces up on one bar face while every odd number slider ABS faces up on the opposite bar face.
23. The combination as recited in claim 22, wherein a row of self-loading Delta sliders are so formed in common, with each ABS including a negative-pressure cavity.
24. The combination as recited in claim 23, wherein the ABS cavities and convergent sides of each slider are defined by laser means.
25. A method of fabricating a number of identical magnetic recording Delta sliders in common, including the steps of:
providing an elongate bar of slider material having a pair of parallel elongate edges and a pair of parallel elongate opposed top and bottom faces lying between these edges;
defining at least one row of said sliders on at least one bar-face with adjacent sliders being defined in up-ended relation so that a first slider presents its trailing edge along a first bar edge, and the adjacent slider presents its trailing edge along the opposite bar edge, etc.;
depositing identical sets of thin film transducers along each bar edge, one set along the trailing edge of each slider;
forming the rest of the slider elements in common on the bar; and severing the so-formed sliders.
26. The combination as recited in claim 25, where each slider row is arranged to present adjacent slider air bearing surfaces (ABS) on opposite bar-faces.
27. The combination as recited in claim 26, where the sliders are so defined and separated in common by laser cutting means.
28. The combination as recited in claim 27, wherein a like negative-pressure cavity is formed on each slider ABS, to thus produce self-loading sliders.
29. The combination as recited in claim 28, wherein the thin film transducers are deposited along both slider faces.
CA000526439A 1985-12-30 1986-12-29 "delta" magnetic head-slider Expired - Fee Related CA1286768C (en)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
US81493185A 1985-12-30 1985-12-30
US814,931 1985-12-30

Publications (1)

Publication Number Publication Date
CA1286768C true CA1286768C (en) 1991-07-23

Family

ID=25216385

Family Applications (1)

Application Number Title Priority Date Filing Date
CA000526439A Expired - Fee Related CA1286768C (en) 1985-12-30 1986-12-29 "delta" magnetic head-slider

Country Status (2)

Country Link
JP (1) JP2539206B2 (en)
CA (1) CA1286768C (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4802042A (en) * 1987-02-05 1989-01-31 Magnetic Peripherals Inc. Side-vented magnetic head air bearing slider

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5266418U (en) * 1975-11-12 1977-05-17
JPS60186562U (en) * 1984-05-18 1985-12-10 株式会社日立製作所 magnetic head slider
JPS6158463A (en) * 1984-08-29 1986-03-25 Fanuc Ltd Rectilinear driving gear

Also Published As

Publication number Publication date
JPS62264490A (en) 1987-11-17
JP2539206B2 (en) 1996-10-02

Similar Documents

Publication Publication Date Title
US4644641A (en) Fabrication of "Delta" magnetic head-sliders
EP0015383B1 (en) Magnetic head slider assembly
US5473485A (en) Tripad air bearing magnetic head slider
US4802042A (en) Side-vented magnetic head air bearing slider
EP0237752B1 (en) An air bearing slider
US5479306A (en) Methods for providing back bar and boss for slider
US6147838A (en) Air bearing slider with shaped taper
US5406432A (en) Air bearing magnetic head sliders with separate center rail segments
JPH0359512B2 (en)
US6525909B1 (en) Disc head slider having deeply recessed corners
US20040228029A1 (en) Tape head with thin support surface and method of manufacture
US5748408A (en) Flight slider for magnetic recording
EP0753843A2 (en) Altitude insensitive air bearing slider
EP0558983B1 (en) Tripad air bearing magnetic head slider
EP0238727B1 (en) Magnetic head-slider and method of fabricating the same
US6608735B1 (en) Asymmetric tapered air bearing slider
CA1286768C (en) "delta" magnetic head-slider
US5774304A (en) Disc head slider having center rail with asymmetric edge steps
EP0231625B1 (en) Taper-flat slider
EP0847044A1 (en) Altitude insensitive air bearing slider
EP0076361B1 (en) Air bearing slider for a transducer
US5889637A (en) Air bearing magnetic head slider
CN1084617A (en) Air bearing magnetic head slider
JP2872384B2 (en) Magnetic head slider and magnetic disk device
WO1998032129A1 (en) Slider having terminated side rails with trailing edge cuts

Legal Events

Date Code Title Description
MKLA Lapsed