CA1151748A - Flatness control in hot strip mill - Google Patents

Abstract

FLATNESS CONTROL IN HOT STRIP MILL

ABSTRACT OF THE DISCLOSURE
The flatness of metal strip being rolled in a hot strip mill is improved by applying higher than normal interstand tensions with maximum permissible tensions being based upon pre-established maximum allowable width reductions due to interstand tensions.
The relationships between interstand tension and interstand plastic deformation are predetermined functions of strip material properties, strip temperature, and assumed tensile stress distribution across the strip width.

Description

FLATNESS CONTROL IN HOT STRIP MILL
WORKPIECE SHAPE CONTROL, U.S. Patent No.
4,137,741 - issued February 6, 1979 - Fapiano et al and assigned to the assignee of the present invention.

COMPUTER CONTROLLED SYSTEM FOR METALS ROLLING
MILL, U.S. Reissue Patent No. 26,996 - issued December 8, 1970 - Beadle et al and assigned to the assignee of the present invention.
The present invention relates to the rolling of metal strips and, more particularly, to techniques for maintaining the strips flat during the rolling process.
Sheet metal is produced by rolling slabs, bars, or other relatively massive workpieces into thin, elongated strips. Although finish rolling often occurs near room temperature (cold rolling), the intial workpiece reduction from its slab form is done at elevated temperature in a facility known as a hot strip mill. The product of the hot strip mill may be further processed and further reduced in thickness, or it may be sold directly for applications requiring thicker strip materials. Where hot-rolled strip ~517~8

- 2 _ 21-DSS-2505 is an intermediate produce subject to furthér rolling, its width and thickness dimensions may be somewhat less critical than where it is the final product. In either case, however, its flatness, or freedom from waviness, is important since excess waviness interfers with both subsequent processing and eventual fabrication of the strip into a finished product.
waviness in rolled strip results from unequal elongation across the strip width due to une~ual percentage thickness reduction across the strip width. A region of strip which is elongated more-than other strip regions will exhibit waviness.
In order to reduce the thickness of the strip, the strip is passed between successive stands having two opposed rolls which are designed to support large rolling forces. In a "two high" stand only two rolls are present, while in a "four high" stand upper and lower work rolls contact the strip and are themselves contacted by upper and lower backup rolls of much larger diameter. Even the relatively rigid "four high" assembly experiences deflect-ion under the bending effort of rolling forces which rangerom 500 to 3000 tons in strip rolling applications. To compensate for deflection the work rolls may be ground, or contoured, so that their diameters at mid-length are greater than their diameters at the ends. This diameter difference is referred to as roll "crown".
Roll crown is not constant during a rolling operation, but varies as the roll temperature increases or decreases through contact with (a) the hot workpiece and (b) cooling water used in the process. Roll crown changes due to nonuniform temperature variations across the roll may exceed 0.01 inch. During the rolling process, the roll crown is further altered by surface wear in the regions of contact with the workpiece. Work rolls are changed relatively frequently to maintain good surface conditions but may exhibit wear in excess of 0.01 inch. In addition rA~ t l9 21 -DS S - 2 5 0 5 to work roll dimension changes, backup rolls wear due to friction from their contact with the work rolls. Although backup roll wear rates are much lower than work roll wear rates, the time between bac~up roll changes is sufficiently S greater that the accumulated wear may be of the same order as work roll wear.
These roll crown-influencing facto~s combine at each mill stand to produce some strip thickness variation across strip width. The difference between strip thickness near its edge and at its center is referred to as "strip crown". With the exception of roll wear, all of the factors which influence roll crown and roll deflection can be used to control strip crown. Roll temperature can be controlled by the use of roll coolant. ~eflection can be controlled by proper choice of thickness reduction which determines the associated roll separating force. Roll grinding practices normally are chosen to be compatible with the planned rolling practice. Finally, supplementary roll ' bending sys~ems can be provided to alter the effective roll crown by applying bending moments to the work rolls or backup rolls with hydraulic cylinders.
Whatever the method of controlling roll crown and strip crown, the strip crowns in successive rolling ~tands must result in essentially equal elongation of all elements of the strip across its width or waviness eventually will result. Equal element elongation will be achieved if all strip elements receive identical percentage thickness reductions in each rolling stand. Expressed another way, the percent strip crown must be maintained essentially constant during the successive reductions in thickness.
These concepts are well understood in the context of both cold rolling and hot rolling. In hot rolling, most recent techniques have attempted to meet the constant per-centage thickness reduction require.~ent by proper choice ofthickness reduction and associated rolling force. These _ 4 _ methods attempt to model mathematically the thermal roll crown changes in the work rolls, the wear pattern in the work rolls and backup rolls, and the deflection of the work rolls under nonuniform roll separating forces. These 5 methods then attempt to choose a thickness reduction such that the combination of roll crown factors and roll deflection factors produces a delivery strip crown which bears the proper relationship to the entry strip crown at each rolling stand. In some variations of this strategy, the calculations are limited to the last three or four rolling stands.
While this prior art strategy produces somewhat better results than strategies which take no account of entry and delivery strip crown relationships~ it is obvious that in the absence of flatness feedback, the results often will be unreliable. That is, the prior techniques are "predictive" because they calculate in advance the expected regult8 of a rolling schedule and do not rely on measured values to determine if in fact the proper strip crown relationghips are being produced. The difficulties lnherent in a predictive approach can be appreciated by recognizing that a workpiece 0.1 inch thick produced with a ~trip crown 0.001 inch greater than a crown produced under conditions of uniform elongation will experience approximately 0.1 percent less eiongation at the center than at the edges. The extra edge elongation will produce an edge waviness of about 0.8 inch amplitude, in the abgence of tension.- Since uncertainties in the actual loaded roll surface configuration will often exceed 0.001

3~ inch, it is clear that waviness easily can occur with even the most sophisticated predictive technigue.
Prior art strip crown control techniques in hot strip mills have analyzed the waviness problem without taking tension between roll stands into account or by assuming that interstand tension is negligible. It is well known in cold rolling to provide substantial tension , , . _ ...... ........ ..

- ~ , . ~ , .. .

` 1~51748 _ 5 _ between successive roll stands. This is done primarily to reduce the roll force required to effect the desired thickness reduction. It also is recognized that in.erstand tension acts as an aid to fla~ness control. The use of relatively high interstan~ tension has been possible in cold rolling because the elastic lim~ts of a typical workpiece at or near room temperature are very high.
Interstand tensile stresses m2y therefore be maintained correspondingly high without exceeding the elastic limits of the strip and, therefore, without causing undesirable interstand plastic deformation.
It ia fur~her known in cold rolling applications that nonuni~orm tension distributions which would have resulted from nonuniform elongation across stri~ width are attenuated by an amount which depends upon the length of the arc of contact, the thickness of the wor~piece and the elastic moduli of the workpiece and rolls. Davies ~"Preduction and Control of Strip Flatness in Cold Rolling~
-W. E. Davies, et al, etals Technology, October 1975) give~ the following expression for attenuation, A, o' roll crown errors in the presence of tension:

A ~ 1 + 6 ~ E
wherein:
Q = arc of contact h = outgoing thic~ness ES = elastic modulus of strip ER = elastic modulus of roll.
In this res~ect, interstand tenfiion influences are ~i~ilar for hot and cold rolling ~pplications. The fact that interstznd tension exhibits this flatness correcting e ect in hot rolling applications has probably been neglected because (1) it has been generally assumed that interstand tension levels are negligible in hot rolling, and (2) it has been incorrectly assumea that the mo2ulus of elasticity of the 3~ workpiece at rolling tempera.ures is too low to sisnif}cantly l~S179~8 influence tension profiles.
In hot rolling, moreover, prior attempts to employ other than minimal interstand tensions, insufficient to have any noticeable effect on strip flatness, have met with inconsistent and sometimes highly unsatisfactory results. Because the factors governing interstand plastic deformation have been insufficiently understood, the results of these prior attempts have varied so that in some instances no appreciable effect was observed, while at other times severe reductions in width, or nec~ing resulted. In extreme cases, interstand plastic deformation has been so drastic as to result in breaking of the strip.
Summ æ~ of the Invention It is, therefore, an object of the present invention to provide a method for employing interstand tension as an active flatness control parameter in a hot metal rolling mill.
It is another object to provide a method of flatness control in a hot metal rolling process which employs relatively high controlled interstand tensions derived as a unction of determinable workpiece characteristic3.
It is a further object to provide a method of flatness control in a hot metal rolling mill which employs appreciable interstand tension in a controlled and pre-dictable manner.
The foregoing and other objects are achieved in accordance with the method of the present invention which overcomes the major problems associated with the use of high interstand tensions and provides an effective, controllable technique for improving strip flatness in hot strip mills. Essentially, the invention first determines an acceptable wor~piece width reduction due to plastic flow between each pair of roll stands. Based on (a~ the acceptable width reduction, (b) the initial strip width, (c) the transport time between each pair of . .

J~lS1748 roll stands, and (d) an assumed relationship between transverse and longitudinal strain, longitudinal strain rates are calculated. These strain rates then are used to select allowable tension levels from stored S relationships between stress and strain rate for the particular grade of material and for the average temperature in each interstand space. The selected tensile stresses are converted to interstand tensile force and applied as references to a conve~tionally supplied interstand tension regulation system.
In a preferred em~odiment, interstand stress levels are stored as linear functions o~ the logarithm of strain rate for representative opesating temperatures and for material groups having similar tension-strain rate characteristics. Preferably, the stress levels are reduced to compensate for some amount of tension non-uniformity, since nonuniform tension produces more width reduction than does uniform tension.
Brie~ Description of the Drawing While the present invention is described in particularity in the claims annexed to and forming a part o~ thls spe~ification, a better understanding of the ~nvention can be had ~y reference to th~ following description t~ken in conjunction with the accompanying drawing in which:
Fig. 1 is a simplified schematic view of a hot strip mill in which the present invention may be practiced;
Fig. 2 is a schematic representation of the interaction between interstand ten9ion distribution and rolling force distribution;
Fig. 3 schematically represents the relationship between interstand tension distribution and interstand plastic ~low;
Fig. 4 is a plot of stress versus logarithm of strain rate for a metal strip under uniform tension across its width;

115174~

Fig. ; is a plot of percent strip width reduction ~ersus tension at a 2,000 foot per munute strip delivery speed for a uniform strip tension profile;
Fig. 6 is a plot of tension in the strip across the width of the strip when the center of the strip is under greatest tension;
Fig. 7 is a plot of tension in the strip across the width of the strip when the edges of the strip are under greatest tension;
Fig. 8 is a plot of percent strip width reduction versus tension at a 2,000 foot per minute strip delivery speed for different strip tension profiles;
Fig. 9 is a plot of strip tension versus mill stand location, a typical prior art tension level being plotted and a tension level according to the invention being plotted; and, Fig. 10 is a block diagram representing the methodology of the present invention and its implementation in a hot strip mill.
Description of the Preferred Embodiment In a hot strip mill, the initial reductions of the thickness of a metal slab are taken in a set of tandem mill stands known collectively as a roughing train.
Fig. 1 shows in greatly simplified form the last stand of a roughing train 10 along with other components in a hot strip mill. As the slab emerges Erom the stand ~ , it moves across a mill table 12 toward a finishing train 20 consisting of mill stands Fl, F2, F3, F4, F5, F6 and F7 arranged in tandem. The final reductions in thickness are taken in the finishing train 20 to produce a metal strip 22 which may be, for example, 1,000 or more feet in length, two to seven feet in width, and 0.05 to 0.5 inch in thickness.
As a typical example, during its passage through the roughing train 10 and the finishing train ~0, the strip ~.~517~fl _ g _ 22 gradually is cooled from its initial temperature of about 2200 degrees Fahrenheit (F). By the time the strip 22 reaches stand F7, it has cooled to around 1600~
to 1700F. As the strip 22 emerges from the last stand F7 in the finishing train 20, it traverses a cooling or runout table 24 before being coiled by a coiler 26.
Strip tension during the coiling operation is maintained a pair of pinch rolls 28, 30 located at the coiler end of the runout table 24.
As illustrated in Fig. 1, each stand in the finishing train 20 includes an upper work roll 40 and a lower work roll 42. Upper and-lower backup rolls 44, 46 are pressed against the upper and lower work rolls 40, 42, respectively, during a rolling operation to prevent excessive distortion of the work rolls 40, 42. This configuration is known as a four high mill. Each mill stand includes roll-adjusting screws 48 to regulate the opening between the upper and lower work rolls 40, 42.
The rolls of each mill stand are rotated by independently controllable electric motors having motor controls, all indicated schematically by the numeral 50. By rotating the motors 50 at different speeds with respect to each other, the tension applied to a strip 22 passing through the finishing train 20 can be controlled. Customarily, in a modern autcmated mill, the determination of the individual motor ~roll) speeds is the result of computations performe~ by a suitable computer 51 (for x/p ~ example, a ~oneywell 4000 Series). The computations employ various parameters of the strip itself tfor example, composition, size, temperature, etc.) as well as operating parameters of the mill tfor example, roll force, thickness reduction, etc.) all as is well known in the art. As an example, reference is made to the Computer Control Patent.
The control link between the motors and their controls 5~
and the computer 51 is schematically illustrated by a bus 49.

~ ~S~7413 ( A metal sensor 52 is located a short distance upstream of the first mill stand Fl. The metal sensor 52 is positioned above the mill table 12 and senses when the beginning and the end of a strip 22 are approaching the first mill stand Fl. The metal sensor 52 generates a signal which is sent to the computer Sl via a line 53.
A looper 54 is positioned midway between each mill stand and is in contact with the underside of a strip 22 during its passagé through the finishing train 20. The loopers 54 are in communication with the computer 51 by way of a line 55. The loopers 54 serve to maintain a desired strip loop between mill stands as well as a desired preset tension. Looper positions are maintained through adjustments of the adjacent work roll speeds. The strip tension is determined by the looper and strip geometry and by looper torque motor current. Alternatively, a suitable tensiometer such as is known in the art may be used to sense interstand tension and provide the requisite feedback signals.
29 Fig. 2 is a schematic representation of a metal strip 22 as it i9 deformed during its passage through the finishing train 20. Only the lower work roll 42 is shown for purposes of clarity. Under normal rolling conditions, the work rolls 40, 42 are subjected to roll separating ~5 forces of between 500-3,000 tons. The work rolls 40, 42 are supported along their entire length by the backup rolls 44, 46 to prevent excessive bending. Even though the resulting roll assembly is relatively rigid, the large roll separating forces produce roll deflections which are signiicant when compared with the thickness of the strip being rolled. Since the backup rolls 44, 46 are supported only at their ends by the roll adjusting screws 48, deflections tend to be greater near the center of the workpiece than near the edge of the workpiece. Typically, the work rolls 40, 42 are contoured to have a slightl~
larger diameter at their midlength than at their ends in 1.~51~4~3 an attempt to compensate for expected roll deflections.
Furthermore, the combined action of roll cooling water, which is distributed over the full length of the work rolls 40, 42, as well as heat conducted from the strip 22 causes relatively more thermal expansion at the mid-length of the rolls 40, 42 than at the ends of the rolls 40, 42.
This th~rmal expansion is influenced by the length of the rolling contact arc, the temperature of the strip 22, the temperaturé of the rolls 40, 42, the temperature of the cooling water, the rolling speed, and the width of the strip 22, among other factors. The effective roll crown is ~urther influenced by surface wear of the work rolls 40, 42 which also is nonuniform and is influenced by many unpredictable factors. The backup rolls 44, 46 wear more slowly than the work rolls 40, 42 but the backup rolls 40, 46 are retained longer in the mill stand and experience accumulated wear comparable to that of the work rolls 4~, 42. Although mathematical models have been proposed for calculating roll thermal crowns, none of these models have been completely effective in the presence of the unmeasurable variations in many of the controlling factors.
All of the foregoing actors combine to produce a thickness variation across the width of the strip 22 as the strip Z2 is reduced in thickness between the work rolls 40, 42. It is well known that the crown imparted to the strip 22 (strip crown) as the strip 22 exits the work rolls 40, 42 must bear a specific relationship to the strip crown upon entry to the work rolls 40, 42 if good strip flatness is to be maintained. Specifically, the percentage strip crown must be maintained approximately constant at each stage of strip thickness reduction from the initial to final thickness in the hot strip mill. In the earlier stands, some deviation from constant percent crown is permissible, the amount of deviation depending upon the thickness, width and temperature of the strip 22.

.

In the latter stands, particularly when rolling thin, wide strips, ver~ little deviation from constant percent crown is permissible.
As earlier indicated, interstand tension can improve strip flatness in a rolling mill through inter-action with r~ll gap forces. In hot rolling, the gap force tension interaction is supplemented by two additional mechanisms associated with interstand flow.
~ig. 2 illustrates the relationship between interstànd tension and roll force profiles when the roll gap configuration is such as to produce more elongation at workpiece center than at workpiece edges. In the presence of interstand tension this condition will reduce the tension at workpiece center and increase the tension at workpiece edges as illustrated by the arrows 58.
Since the wor~piece yields when the combined stress equals the yield stress, the tension profile will produce the nonuniform force profile illustrated by the arrows 57.
The higher roll separating force in the workpiece central region will produce more roll deformation there than in the regions corresponding to the workpiece edge~. As a result, the wor~piece crown will be increased and the elongation at workpiece center reduced compared to that which would have occurred in the absence of tension. ~he 2S reduced elongation is re~resented in Fig. 2 by dimension ~, the dotted line representing the condition which would have occurred in the absence of intérstand tension. This is similar to that occurring in cold rolling, as previously noted.
It will be understood from the previous illustration that the average interstand tension level is significant since higher tension will accommodate larger tension differéntials before any element of wor~-piece width falls to zero tension and manifest waviness appears.

~1517~8 21-~SS-2505 It is in the interstand wor~piece behavior that ~he differences between hot and cold rolling applications become most significant Interstand flow in the presence of tension is nonexistent in cola rolling but may be ~ 5 significant in hot rolling. ~his interstand flow influences width, which is generally considered undesirable, while it has two be~eficial i~fluences on flatness. Fig.3 illustrates one of these actions. Consider an element of strip le2~ing one or a pa_, of mill stands io with excessi~e elongation as shown by section 56 Tensile s'.ress at the workpiece edges woul2 be grezter than at the centerline, the tension distribution taking the for~
illustsated ~y the ærrows 60 During the t~me interval in which the workpiece section proceeds from a first to a second o the stand pairs all of the workpiece section expesiences some flow~or creep, the regions of the sections under greater tension experiencing greater flow When the wor~piece element arri~es at the second stand, its edges have been elongated more than its center and the conditions which would have given rise to waviness thus have been partially compensated as demonstrated at 61 wherein the dotted lines again show the condition in the absence of tension.
While not shown in Fig 3, it will be understood that the edge regions of the workpiece in this example will not only have undergone more elonsation that the central regions, but additionally the edge thic~ness will have been reduced more than the central thickness and the transverse flow or width reduction in the edge regions will be sreater than that in the cent-al resions The thickness changing ~n'luence o' _he in~erstznd tension differenti21 acts to 'ur.her ampli'y the roll force pattern illustr2ted in ~ig 2 The s~eater ~eduction of edge gzuge reduces the relative reduction and associated roll separating force in the edge regions, assisting the b)~ , ~5~74l9 previously described action of the tension profile.
A quantitative understanding of these phenomena requires knowledge of the "creep" or strain~rate behavior of the workpiece at rolling temperatures and practical interstand tensile stress levels. The Journal of Applied Mechanics, June 1941, "High-Speed Tension Tests at Elevated Temperatures - Parts II and III" by Nadai et al gives some data for mild steel. Additional laboratory results performed by the assignee of the present invention are in general agreement with the earlier published results but cover a broader range of materials.
Fig. 4 shows typical-actual experimental results for mild steel at temperatures of 1700F and 1800F.
These data can be expressed as a log-linear equation.
For stresses in the 1000 to 10,000 psi range, the stress V8. strain-rate (i.e., time rate of change of strain) relation can be expressed as a log-linear equation of the form:
(1) C~ = Rl + K2 ln(e) 20 wherein, a= stress (psi) e - strain-rate (in/in/sec) Kl & R2 = constants representing the intercept and slope of the equation for a particular material at a particular temperature.
For mild steel at 1700F, as an exa~ple, and in the region of 1% strain, the relationship is approximately:
(2) cr = 10200 1 1100 l~e) For mild steel at 1800F, the relationship will be approximately:
(3) CJ , 8600 1 1040 ln(e).
Experimental data for the values of Kl and K2 have been developed for a range of temperatures and materials and such data can be duplicated in any metallurgical ~S174~

testing facility by well-known methods such as that set forth in the l~adai et al article cited above.
These relationships can be stored in a computer (i.e., computer 51 in Fig 1) in any convenient form such as tabular or as equations such as those cited above.
Equations (1), (2) and (3) describe the relationship between stress and axial strain rate for conditions of axial tension. It is necessary that this information be correlated to width reductions for various conditions of interest. An assumption can be made that, for small interstand strains, the percent width reduction and percent thickness reduction are each half of the percent length increase. This is a reasonable assum~tion because Poisson's Ratio, the ratio of transverse strain to axial strain, approaches one-half because volume remains substantially constant in plastic deformation.
~aving thus determined the relationship between axial tension and trans~erse strain rate, the percent width reduction due to axial tension also can be determined.
Fig. 5 is derived from equation (2) and is a plot of percent width reduction between mill stands versus average interstand tension for an average inter-stand temperature of 1700aF and a transit time corresponding to a wor~piece speed of 2,000 feet per minute. In order to plot the cur~e of Fig. 5, it has been assumed that the mill stands are spaced a known constant distance and that the tensiGn applied across the width of the strip 22 is uni~orm. A significant problem exists, however, because it is difficult, if not impossible, to achieve uniform tension across the width of the strip under day to day operating conditions. It therefore is necessary to determine the effect of non-uniform tensile stresses on width reduction before high interstand tension levels can be effectively applied.
Figs. 6 and 7 illustrate "tight center" and "tight edge"

~iS3~7~19 conditions, respectively, of a typical strip 22 being roll~ed in a hot strip mill. The distributions are assumed to be parabolic and the depictions indicate that for a strip being rolled at a mean tension of 2000 psi, and under greatest tension at its center, the maximum tension differential which can be tolerated before waviness appears is 3000 psi. wa~iness will appear in a strip being rolled whenever tension in a portion of the-strip drops to zero. Fig. 7 illustrates that a '10 strip having more tension at its edges than at its center can tolerate a maximum tension differential of 6000 psi before waviness appears.
The importance of these curves becomes apparent when the width reduction for a given strip under different tensile loadings is explored. In Fig. 8, a family of curves is plotted for a particular grade of strip steel at 1700F and under three different tensile loadings:
uniform loading, tight edge loading and tight center ' loading. It has been assumed that the strip is being rolled at a speed of 2000 feet per minute and that the mill stands are spaced a known constant distance.
Because the temperature of the strip decreases as it passes through the mill, a temperature of 1700F
approximates that in a ty,pical strip mill in the last interstand space The cuxves of Fig. 8 for the tight center and tight edge conditions are derived from the uniform width reduction case, for example, by integration by parts.
According to thls technique, the percentage width reduction at each element of the strip due to the local tension there is calculated from a cur~e similar to that of Fig. 5 for the particular material and temperature under consideration. The calculated percentage width reduction at that particular element is multiplied by the width of that element. The calculation is repeated for each of llS174~3 the other elements across the width of the strip and a family of curves li~e thzt in Fig. 8 can be plo'ted.
The curves thus plotted can be stored in tzbular form or can be converted back into log-linear relationships like thzt o' equation (l). For example, mild steel in the region of one percent strain and under tisnt center conditions, will yield zn approximate relationship.

(4) a = 7830 1 800 ln(e~, at 1700~F.
Various relationships like those of equations (2), (3) and (4) can be calculated and s.ored by the computer 51.
Three zspects of these relationships are of particular interest. Firs., there is a pronounced "~nee"
in these curves, above which strain inc~eases sharply with - tension. Second, the allowable s~ress levels drop quickly as the ups~ream stands are approached due to the com~ined effects of increasing temperature and increasing transit time between mill stands. The third aspect relates to the uniform tension assumption. All nonuniform tension distributions produce greater width reductions than uni.orm tension distributions because of the nonlinear stress-strain rate relationship. Because the tight edse tension distribution produces more extreme stress concentration than the tisht center condition, the corresponding width reduction may be substantizlly greater.
For example, at a mean tension of 3000 psi, z uniform tension distribution shows only a ~.04 percent width reduction, while a tisht center tension distribution shows a 0.07 percent width reduction. A tisht edse tension distribution, however, shows a 0.56 percent width _eduction. Clearly, i' a strip is being rolled under tight edge conditions and ~nte_stand tensions z~e permitted to reach even into the 3000 psi .ange, width reductions of one percent or more are possi~le. 3ased on ~he foregoing phenomenon, which until the present invention 3~ hzs not been understood, at least in the context o' hot ., ~pJ .

......... . .. ........ . .. . . .. ...... . .... ........... ................................................................. ...

4~9 ( strip mill operation, hot strip mill practice has been to reduce interstand tension levels to the order of a maximum of 1500 psi in order to avoid any tension-induced problems. Stated differently, in the absence of a clearer understanding of interstand plastic flow relation-ships, the only reliable recourse has been to reduce interstand tension to levels which produce acceptable width reduction under the most unfavorable combinations of tension distribution, temperature and rolling speed.
As a result, the flatness-producing mechanisms which require the presence of high interstand tension have been substantially unused.
The invention contemplates a technique for calculating optimum interstand tension levels for the conditions which exist at each interstand space, and for controlling the interstand tension regulation means to produce the calculated optimum tension levels. Essentially, an acceptable width reduction of a strip 22 due to tension lmposed between roll stands is sought from predetermined conBiderations. In a typical hot strip mill, an acceptable width reduction might be 0.5 inch from the mill stand Fl through the mill stand F7. Because the rolling process might widen the strip 22 about 0.25 inch, the total acceptable tension-induced width reduction from mill stand Fl through mill stand F7 might be about 0.75 inch. The tension~induced reduction is distributed over the interstand spaces, favoring the~latter stands where the percentage elongation errors and flatness problems are most troublesome. A typical distribution of tension-induced width reduction might be, for example, 50 percentin the F6-F7 space, 30 percent in the F5-F6 space, and 20 percent in the F4-F5 space. Tension levels upstream of mill stand F4 would remain at their normal, low levels.
Rolling speeds and temperatures are determined in advance of workpiece arrival at the finishing train 22.

17~8 The Computer Control Patent describes one such technique.
For a typical steel wor~piece, rolling speeds leaving the last mill stand F7 will be 1000 to 3000 feet per minute and corresponding temperatures will range from 1600F to 170pF. The transit times for the F6-F7 space typically - are 0.~ to 1.5 seconds. For each interstand space, values for the workpiece temperature entering that space and the workpiece velocity while traversing that space can be calculated and stored by the computer 51.
A further objective of the rolling schedule calculation is to achieve approximately uniform elongation in the successive reductions. A method for accomplishing this through proper choice of (strip) reductions is - described in the Shape Control PatentO Computer calculated reduction schedules employing this or similar strategies can avoid (extreme) tight e~dge tension distributions.
Manually controlled ~ cannot be relied upon to avoid undesirable tension distributions.
The thickness reduction schedule and/or roll bending techniques are usually employed in a manner to produce a desired tension distribution. By erring in the direction of tight center conditions, excessively high local tensions are avoided.
Mean tension levels have been calculated for each interstand location. Referring to Fig. 9, typical conventional interstand tension levels are illustrated by the line marked "An. These tens~ion levels between mill stands Fl and F2 are approximately 500 psi and increase tp approximately 1050 psi between mill stands F6 and F7.
Presently available mill control equipment automatically maintains tension in the strip at preselected low levels such as that shown in Fig. 9. Ten~ions calculated and used in accordance with this invention will fall into the range illustrated by the shaded area bounded by curves C
and D in Fig. 9.

~5J~74~3 Fig. 10 is a block diagram representation of the technique by which the tension levels according to the invention are calculated and by which the hot strip mill is controlled to achieve desirable flatness properties in a strip 22. The computer 51 is indicated in outline form. As part of the computer 51, a calculator 62 determines the maximum allowable per uni~ width reduction (~ W/W) based on a predetermined acceptable width change ~ W. A calculator 64 determines the maximum allowable length increase (~ L/L) based on the equation:

(5) ~ L/L = 2 (~ W~W).
Rnowing the properties of the material being rolled, its temperature, and its rolling speed, axial strain rate, ea,can be determuned from the equation-

(6) ea= 2 (~tW/W) = (~ L/L) wherein, t - time required for a point on the strip to traverse the interstand space.
Equation (6) ~g solved by the calculator 66.
Ba~ed on the value of eacalculated by the calculator 66, a calculator 68 solves an equation like that of equation (1) to determine axial stress. The calculator 6a can be programmed in advance for different values of Rl and K2 depending upon the properties of the particular material being rolled, i'ts temperature, its strain level and so forth. In essence, equations (2), (3), (4) and other similar appropriate equations can be developed for all expected operating temperatures and materials and the equations, or equivalent tables, can be stored in the computer 51. Accordingly, during rolling of a particular strip 22, the calculator 68 will only ha~e to select the proper stored relationship to determine axial stress as a function of axial strain rate.

~151~4~3 ~

Axial stress is tra~slated into ir.terstand tension through multiplication, in calculator 70, by the cross sectional area of the strip. The interstand tension is then applied as a re'erence to a normally included tension cont~ol means o' any suitable type ~nown in the art, for example, cons'~nt .ension loopers 54 ~Fig. 1). The tension establishea ~y ~he constant tension loopers is deten~ined by torque motors and by the zngle made by the looper znd stri?. This angle is io maintained constant by adjustins crive motor speed with speed control means 50 to maintain co~s'ant loo?er position. Other means such as airect control o' tension by interstand tensiometer working through stand speed control can also be employed . During acceleration of the mill to stezdy -~tzte rolling speeds, the permissible in~er-stand tension levels are recalculated and tension levels zre raised to the maximum permissible extent after ezch recalculation. The ~ethodology described schematically in Fig. 9 is repezted separztely for each interstand space in which high tension levels are desired. Typioally, this woula ~e between mill stands F4-F5, F5-F6 and F6-F7.
Tension levels between the ~receedi~g m~ll stands would be set accoraing to presently eY~isting techniques.
Exam~le -Steel having 0.09~ car~on and 0.~0% mzng2nese exhibited the 'ollowins s.ress ve~sus strain-rate relationship at 1700F, for uni'orm tension:

(7) cr = 10200 + 11001n(ea).
Allowing ~or the worst czse tension profile simil2r to thzt ~o in ~ig. 6, t~e re7ztionship is ~djusted ~o:

(8) C~ = 7830 + 8001n(ea).
It will ~e assumed thzt 50% o~ a ~otal width reduction of 0.;0 inch is allowab~e in s?ace F6-~7 and that the strip 22 is 80 inches wide, C~lculator 62 will determ~ne the max_mum allowzble pe--~nit width reduction .*~

,, .. , .......... ,, .. .. ... , .......... ,. _ ._ .....................................................

- ~151748 ( as 0.003125. Calculator 6~ will compute the maximum per-unit allowable length increase as 0.00625. Assuming that mill stands F6 and F7 are 18 feet apart and strip is traversing the F6-F7 space at 2000 feet per minute, an element of strip would require 0.54 seconds to travel from F6 to F7. The calculator 66 will calculate the axial strain-rate during this interval as 0.01157 per-unit per second.
Rnowing the material and temperature, the calculator 68 will select from among stored relationships the relationship given by equation (8), in this example, and calculate the allowable axial stress at 4263 psi.
Accordingly, an interstand tension reference corresponding to an axial stress of 4263 psi could be applied to the interstand tension regulating means 54. This procedure would be repeated for all interstand spaces, resulting in a tension practice illustrated as curve B in Fig. 7.
Provided the interstand tension levels are m2intained at or slightly below the tension levels calculated in this manner, width reductions will be acceptable and waviness problems will be reduced. Since width reductions due to tension are predictable, they ob~iously may be compensated by corresponding increases in the strip width produced in the roughing mill 10.
Equally obvious is the fact that higher tensions need not be employed where strip dimensions are such that flatness problems are not usually e'ncountered.
Although the invention has been described in its prçferred form with a certain degree of particularity, it will be understood that the present disclosure of the preferred embodiment has been made only by way of example and that numerous changes may be resorted to without departing fxom the true spirit and scope o~ the invention as hereinafter claimed. It is intended that the patent shall cover, by suitable expression in the appended claims, whatever features of patentable novelty exist in the invention disclosed.

Claims (12)

The embodiment of the invention in which an exclusive property or privilege is claimed are defined as follows:

1. In a hot strip mill having at least two mill stands where a metal workpiece is compressed and reduced in thickness to form a strip, each mill stand having rolls, the rolls of each mill stand being rotatable at selected speeds by means of a mill control system so that the strip can be placed under tension during its passage between mill stands, a method for improving strip flatness, comprising the steps of:
a) selecting a predetermined maximum width reduction which the strip will be permitted to undergo during its passage between adjacent mill stands;
b) calculating, from predetermined relationships between stress and strain-rate, the tensile stress which will produce this width reduction; and, c) regulating interstand tensile stress at or below the calculated tensile stress level.

2. The method of Claim 1 wherein the relation-ship between stress and strain-rate is defined by equation:
.sigma.= K1 + R2 ln(?) wherein, .sigma. = stress ? = strain-rate K1 and K2 = constants representing the intercept and slope of the equation for a particular material at a particular temperature.

3. In a hot strip mill having at least two mill stands where a metal workpiece is compressed and reduced in thickness to form a strip, each mill stand having rolls, the rolls of each mill stand being rotatable at selected speeds by means of a mill control system so that the strip can be placed under tension during its passage between mill stands, a method for improving strip flatness, comprising the steps of:
a) selecting a predetermined maximum width reduction which the strip will be permitted to undergo during its passage between adjacent mill stands;
b) calculating the transverse strain-rate in the strip resulting from the selected width reduction;
c) calculating the axial strain-rate in the strip corresponding to the calculated transverse strain-rate in the strip based upon a predetermined relationship between transverse strain-rate and axial strain-rate;
d) calculating the axial stress in the strip which will produce the calculated axial strain-rate; and, e) regulating the speed of the rollers in adjacent mill stands to apply axial stress to the strip at a level at or below the calculated axial stress.

4. The method of Claim 3 wherein the calculated axial stress is calculated as a function of strain-rate, strip material and strip temperature.

5. The method of Claim 3 wherein the relation-ship between axial strain-rate and axial stress also is corrected to allow for tension nonuniformity across the strip width.

6. In a hot strip mill having at least two mill stands where a metal workpiece is compressed and reduced in thickness to form a strip, each mill stand having rolls, the rolls of each mill stand being rotatable at a selected speed so that the strip may be placed under tension during its passage between mill stands, a method for improving strip flatness during the rolling process, comprising the steps of a) selecting a predetermined maximum width reduction which the strip will be permitted to undergo during its passage between mill stands;
b) establishing the degree of transverse strain-rate in the strip needed to achieve the selected width reduction as a function of a fixed mill stand spacing and a predeter-mined strip speed between adjacent mill stands;
c) establishing the degree of axial strain-rate in the strip corresponding to the established transverse strain-rate in the strip based on a predetermined relationship between transverse strain-rate and axial strain-rate;
d) establishing the axial stress in the strip which will produce the established axial strain-rate; and, e) regulating the speed of the rollers in adjacent mill stands to apply axial stress to the strip such that the established axial strain-rate is not exceeded.

7. The method of Claim 6, wherein the relationship between axial stress (.sigma.) and axial strain-rate (?a) is determined from a series of relationships based on the equation:
.sigma.= K1 + K2 ln(?a) where K1 and R2 are constants dependent upon the strip material properties, the strip temperature, the strain which the material experiences, and the nature of the axial stress distribution across the strip width.

8. The method of Claim 7,wherein permissible axial stress levels are recalculated during acceleration of the mill to higher rolling speeds, and interstand tension levels are raised to the maximum permissible extent after each recalculation.

9. In a hot strip mill having at least two mill stands where a metal workpiece is compressed and reduced in thickness to form a strip, each mill stand having rolls, the rolls of each mill stand being rotatable at selected speeds by means of a mill control system so that the strip may be placed under tension during its passage between mill stands, a method improving strip flatness during the rolling process, comprising the steps of:
a) selecting a predetermined maximum width reduction (.DELTA. W) which the strip will be permitted to undergo between mill stands;
b) establishing the-maximum per unit width reduction (.DELTA. W/W) acceptable in the strip, wherein W is the strip width upon entering an interstand space;
c) establishing the degree of axial per unit strain (.DELTA. L/L) in the strip associated with said maximum acceptable per unit width reduction in accordance with the relationship .DELTA. L/L = 2 .DELTA. W/W, wherein .DELTA. L equals the elongation of a strip element of length L
while traversing an interstand space;
d) establishing the axial strain-rate (?a) in accordance with the formula:
wherein, t equals the time required for a point on the strip to transverse the inter-stand space;
e) determining the axial stress (.sigma.) needed to produce the established axial strain rate (?a) from an equation of the form:
.sigma. = K1 + K2 ln(?a) wherein K1 and K2 are constants dependent upon the strip material properties, the strip temperature, the strain which the material experiences, and the nature of the tension distribution to which the strip is subjected; and, f) regulating the speed of the rollers in adjacent mill stands to apply axial stress to the strip so that the calculated axial stress is approached or attained.

10. The method of Claim 9 wherein permissible axial stress levels are recalculated during acceleration of the mill to higher rolling speeds, and interstand tension levels are raised to the maximum permissible extent after each recalculation.

11. The method of Claim 9, wherein the method is applied only to the latter mill stands of a multiple mill stand finishing train.
12. In a hot strip mill having at least two mill stands where a steel workpiece is compressed and reduced in thickness to form a strip, each mill stand having rolls, the rolls of each mill stand being rotatable at selected speeds by means of a mill control system so that the strip may be placed under tension during its passage between mill stands, a method for improving strip flatness during the rolling process, comprising the steps of:
a) selecting a predetermined maximum width reduction (.DELTA. W) which the strip will be permitted to undergo between the latter mill stands of a multiple mill stand finishing train;
b) establishing the maximum per unit width reduction (.DELTA. W/W) acceptable in the strip, wherein W is the strip width upon entering an interstand space;
c) establishing the degree of axial per unit strain (.DELTA. L/L) in the strip associated with said maximum acceptable per unit width reduction in accordance with a value of Claim 12 cont'd....
Poisson's Ratio of approximately 1/2 whereby .DELTA. L/L - 2 .DELTA. W/W, wherein .DELTA.L equals the elongation of a strip element of length L while traversing an interstand space;
d) establishing the axial strain-rate (?a) in accordance with the formula;

wherein, t equals the time required for a point on the strip to transverse the interstand space;
e) determining the axial stress (.sigma.) needed to produce the established axial strain rate (?a) from an equation of the form:

.sigma. = K1 + K2 ln(?a) where K1 and K2 are constants dependent upon strip material properties, the strip temperature, the strain which the material experiences, and the nature of the tension distribution to which the strip is subjected;
f) calculating the interstand tension value corresponding to said axial stress;
g) applying the calculated interstand tension value to interstand tension regulation means;

Claim 12 continued ...
h) recalculating permissable interstand tension levels during acceleration of the mill to higher rolling speeds and raising interstand tension levels to the maximum permissible extent after each recalculation.