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.. SK-198 FLAME STRAIGHTENING AND ITS EFFECT ON BASE METAL PROPERTIES .- This document has been approved for public release and sale; its distribution is unlimited. .), SHIP STRUCTURE COMMITTEE AUGUST 1969 ‘.. . ... -

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Page 1: Flame straightening

..

SK-198

FLAME STRAIGHTENING AND ITS EFFECTON BASE METAL PROPERTIES

.-

This document has been approved

for public release and sale; its

distribution is unlimited.

.),

SHIP STRUCTURE COMMITTEE

AUGUST 1969

‘.. .

... -

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.

SHIP STRUCTURE COMMITTEE

MEMBER AGENCIES:

UNITED STATES COAST GUARDNAVAL SHIP SYSTEMS COMMAND

MILITARY SEA TRANSPORTATION SERVICE

MARITIME ADMINISTRATION

AMERICAN BUREAU OF sHIPPING

ADDRESS CORRESPONDENCE TO:

SECRETARY

SHIP STRUCTURE COMMITTEEU.S. COAST OUARD HEADQUARTERS

WASHINGTON, D.C. 20591

.

August 1969

Dear Sir:

Fairing and straightening of ships’ hull platesdistorted by welding during fabrication or by damage duringoperations has been a problem for many years. Flame straight-ening methods found acceptable for mild steels were consider-ed excessively detrimental to material properties of thehigh-strength steels in common use today. Project SR-185,“Straightening Distorted Weldments,” was undertaken to de-termine the extent of deterioration of flame straightenedplates and to develop alternative methods of distortion re-moval. The first portion of the project involved a literaturesurvey. The accompanying report, “Flame Straightening andIts Effect on Base Metal Properties,” by H. E. Pattee, 1?.M.Evans, and R. E. Monroe contains the information from thatreview.

This report has been distributed to individualsand groups associated with or interested in the work of theShip Structure Committee. Comments concerning this reportare solicited.

$incerelv,

&Rear Admiral, U. S. Coast GuardChairman, Ship Structure Committee

-,,-

(

..— .—-

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SSC-198

Summary Report

on

Project SR-185

“Straightening Distorted Weldments”

to the

Ship Structure Committee

FLAME STRAIGHTENING AND ITSEFFECT ON BASE METAL PROPERTIES

by

H. E. Pattee, R. M. Evans, and R. E. Monroe

Battelle Memorial Institute

Columbus, Ohio

under

Department of the NavyNaval Ship Engineering Center

Contract NOO024-68-C-5324

This document has been appoved fop public release and sale;its distribution is unZ-imited.

U. S. Coast Guard HeadquartersWashington, D. C.

August 1969

Page 4: Flame straightening

ABSTRACT

The suitability of flame-straightening methods now used onconventional ship steels for the higher strength ship steels isquestionable. This report discusses some of the potential problemareas that need evaluation to examine this subject. Based on a sur-vey of pertinent literature it is shown that only limited dataapplicable to this subject are available. The data analysis coveredthe nature of distortion, flame straightening techniques, and theeffects of both single and combined thermal cycles and plastic straincycles on material properties. An experimental program is presentedthat is designed to generate background data on conventional steelsand several higher strength steels directly pertinent to flamestraightening. These data will subsequently be evaluated to ascer-tain suitability of the flame-straightening procedure for variousship steels.

ii

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Page

Introduction . . . . . . . . . .

Nature of Distortion . . . . . .

Flame-Straightening Techniques .

Possible Material Degradation asof Flame-Straightening . . . . .

Discussion . . . . . . . . . . .

References . . . . . . . . . . .

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SHIP STRUCTURE COMMITTEE

The SHIP STRUCTURE COMMITTEE is constituted to prosecute a research pro-gram to improve the hull structures of ships by an extension of knowledge pertain-ing to design, materials and methods of fabrication.

RADM C. P. Murphy, USCG - ChairmanChief, Office of Merchant Marine Safety

U. S. Coast Guard Headquarters

Captain W. R. Riblett, USN Mr. E. S. DillonHead, Ship Engineering Division Chief, Division of Ship DesignNaval Ship Engineering Center Office of Ship Construction

Maritime Administration

Captain T. J. Banvard, USN Mr. D. B. Bannerrnan,Jr.Maintenance and Repair Officer Vice President - TechnicalMilitary Sea Transportation Service American Bureau of Shipping

SHIP STRUCTURE SUBCOMMITTEE

The SHIP STRUCTURE SUBCOMMITTEE acts for the Ship Structure Committeeon technical matters by providing technical coordination for the determinationof aoals and ob.iectivesof the program, and by evaluating and interpreting the.results in terms of ship structural design,

NAVAL SHIP ENGINEERING CENTER

Mr. J. J. Nachtsheim - ChairmanMr. J. B. O’Brien - Contract AdministratorMr. G. Sorkin - MemberMr. H. S. Sayre - AlternateMr. I.Fioriti - Alternate

MARITIME ADMINISTRATION

Mr. F. Dashnaw - MemberMr. A. Maillar - MemberMr. R. Falls - AlternateMr. W. G. Frederick - Alternate

AMERICAN BUREAU OF SHIPPING

Mr. G. F. Casey - MemberMr. F. J. Crum - Member

OFFICE OF NAVAL RESEARCHMr. J. M. Crowley - MemberDr. W. G. Rauch - Alternate

MILITARY SEA TRANSPORTATION SERVICE

construction and operation.

U. S. COAST GUARD

CDR C. R. Thompson, USCG - MemberCDR J. L. Howard, USCG - MemberLCDR L. C. Melberg, USCG - AlternateLCDR R. L. Brown, USCG - Alternate

NAVAL SHIP RESEARCH & DEVELOPMENT CENTER

Mr. A. B. Stavovy - Alternate

NATIONAL ACADEMY OF SCIENCES

Mr. A. R. Lytle, LiaisonMr. R. W. Rumke, LiaisonMr. M. L. Sellers. Liaison

AMERICAN IRON AND STEEL INSTITUTEMr. J. R. LeCron, Liaison

BRITISH NAVY STAFFMr. H. E. Hogben, LiaisonCDR D. Faulkner, RCNC, Liaison

WELDING RESEARCH COUNCIL

Mr. R. R. Askren - Member Mr. K. H. Koopman, LiaisonLt.J.G. T. E. Koster, USN - Member Mr. C. Larson, Liaison

iv

Page 7: Flame straightening

introduction

Distortion is a perennial problem in the shipbuilding industry,and much effort has been expended to minimize the distortion that occurs asthe result of the fabrication procedures. While distortion can be producedby many of the assembly procedures used in ship fabrication, its princtpalcause today is welding. Welding is used extensively In modern shipbuildingyards, since it offers many advantages over other assembly methods. However,

as with any complex structure, problems are encountered when ship hullsand structural sections are fabricated by welding. While distortion canbe minimtzed and/or controlled by proper design of the welcbnent and carefulselectton of the weldtng process and welding variables, some inevitablyoccurs. When the amount of distortion exceeds acceptance limits, it must beremoved.

There are three approaches to resolving the problem of weld distor-tion.

(1) bevelopmenc of welding processes and fabrication procedures thatminimize distortion

(.2) Establishment of rational standards for acceptable limits ofdisto~tiori

(3) Development of proper techniques for removing distortion thathas already occurred.

A proper combination of these approaches will be most effective in controllingweld distortion in actual ship fabrication.

The first approach to reduction and control of weld distortion is tominimize distortion. It is much better to build a ship without distortion thanto reduce distortion later. First of all, if we developed a welding processwhich reduced shrinkage and distortion for individual welds, distortion occur-ring during fabrication of a complex welded structure would also be reduced.Presently, however, there is no process which completely eliminates distortion.Accepting this fact, we can turn to the many factors within the welding proce-dure which contribute to the distortion of a large, complex structure such asa ship hull. These factors include welding sequence, degree of constraint,welding conditions, joint details , and preheat and interpass temperature. Itis important to determine how these factors contribute to distortion. A largeindustrial group research program is currently in progress to investigatethese factors. Special attention is being given to shipbuilding problems be-cause many of the sponsors of this research are shipbuilding companies.

The second approach to controlling distortion accepts the factthat some amount of distortion inevitably occurs due to welding. Then, animportant technical problem is to establish rational and practical standardsfor acceptable limits of distortion. The standards should be established onthe basis of:

(1) The structural reliability of the ship

(2) The economic value of the ship

(3) Fabrication cost.

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(4)SECTION D-D “

(b)TEMPERATURE CHANGE (cJ.STRESS ~

FIG, l.Schematic Representation of Changes of Temperature and Stressesduring Welding.

The effects of these dimensional changes on a simple butt weld are shown inFigure 2. Examples of distortion due to longitudirial shrinkage are shown inFigure 3. The armunt and type of distortion that occurs in welchnents such asthose encountered in shipbuilding is much more complex than that shown in

ointa. In 1961 Kerr discussed the problem of distortion in~h~;~ifi~$!~~) %rr indicated that a volumetric contraction of about 10‘parcent occurs in the cooling of the weld zone in mild steel. The liqufdw41d metal solidifies at about 2700 F. But it is highly plaatic at this tf=.With decreasing temperature there Is a progreastve increase in sjkrengthcdthe weld metal until the temperature reaches about 1650 F; during this periodthe weld metal contracts and the stress leval increases. Below 1650 F, theweld metal plasticity decreaaea and high stresses are present in the weld=tal and surrounding .matal; these stresses produce distortion in the weldment.

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Such standards must be rational and practical so that any harmful distortioncan be avoided while unharmful distortion is accepted to eliminate unnecessaryrework. In regard to structural reliability, studies are needed to determinethe adeqaacy of present tolerances. It is now possible to determine analyti-cally the acceptable distortion of a member under given service conditions.It is also possible to determine the maximum weld size that will produce ac-ceptable distortion when welds are made with normal procedures. There isconsiderable disagreement among shipbuilders and ship owners regarding theamount of distortion that can lietolerated from an economic viewpoint. Al-though distortion may not affect a ship’s reliability, it may damage the ap-pearance and thus reduce the ship’s worth. A study, in which classificationsocieties, government agencies, and ship owners are questioned, could beused to establish acceptable standards. Finally, extremely close distortiontolerances can result in extremely high fabrication cost. This is a factorthat must be carefully weighed whenever distortion standards are established.

In fabricating ships with high-strength steels, especially heat-treated steels, it is important to minimize postweld straightening. We havediscussed two ways of doing this. Nevertheless, distortion that exceeds theacceptable limits may occur. Distortion also may occur during service, sayby collision. If this happens, methods are needed to remove the distortioneconomically with minimum damage to the structure. Many techniques havebeen used for removing distortion in a ship hull. Most commonly used tech-niques involve flame heating the plate on spots/or along lines, followed bycooling with water. Sometimes plates are beaten with a hammer while theyare heated. However, these techniques are very much an art, Only limitedscientific information, either analytical or experimental, is available onmechanisms of distortion removal or on material degradation due to these

treatments.

This report primarily considers what is known currently about theeffects of flame-straightening treatments on ship steels.

Nature of Distortion

Distortion in weldments is primarily the result of the combinedeffects of (l) locally-applied heat in the weld zone, and (2) restraintprovided by the relatively cold metal on either side of the weld bead-and byother members of the structure. Because a weldment is heated locally by thewelding heat source, the temperature and stress distribution in the weldmentis not uniform and changes as welding progresses (Figure l). During thewelding cycle, complex strains occur in the solidified weld metal and basemetal regions near the weld during the heating and cooling cycles. The strains

produced during heating may be accompanied by plastic upsetting. The stresses

resulting from khese strains combine and react to produce internal forces thatcause bending, buckling, and rotation.

The distortion encountered in welded structures occur as theresult of three fundamental dimensi+al changes during the welding process:

(1) Transverse shrinkage that occurs perpendicular to the weld(2] Longitudinal shrinkage that occurs parallel to the weld

(3) Angular change that consists of rotatin~ around the weld.

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Fig. 2. Effects of Shrinkage,Causing Plates to TakeShape of Dotted Lines.

A typical distribution of

(a)LONGITUDINAL DISTORTIONOFA BUILT-UP BEAM

(b)LONGITUDINAL BENDING DISTORTIONOFASINGLE-VEEBUTT WELD

(c)BUCKLING DISTORTION

Fig. 3. Distortions Induced byLongitudinal Shrinkage.

residual stresses in a butt weld is

shmrn in Figure 4. The stresses of concern are those parallel to the welddirection, designated rx, and those transverse to the weld, designated cr.

Y

The distribution of the r residual stress along a line transverseto the weld (YY) is shwn in FQurex4 (b). Tensile stresses of high magnitude

are produced in the region of the weld; these taper off rapidly and becomecompressive at a distance of several times the width of the weld. The weld

metal and heat-affected zone try to shrink in the direction of the weld, and theadjacent plate material prevents this shrinkage. The distribution Qf ~

residual stress along the length of the weld ~ is shown by Curve 1 in yFigure 4 (c). Tensile stresses of relatively lW magnitude are produced in themiddle of the joint, and compressive stresses are observed at the end of thejofnt.

If the contraction of the joint is restrained by an external constraint,the distribution of cr Is as shown by Curve 2 in Figure 4 (c). Tensile stresses,approximately unlformyalong the weld , are added as the reaction stress. Anexternal constraint, however, has little influence on the distribution d Wxresidual stresses.

Comprehensive reviews on weld distortion nd residual stresseshave been prepared by Sprara en and associates (2-4~ Kihara and wsubuchi,

(7J and Okerbloom. (g) These references rahouldbe(5,6) Wanatale and Satoh,consulted for further information on this subject.

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-5-Y

~UY

x.— ~1111 +04’ —x

‘x

+1

Y(a)BUTTWELD

Y

cOMPRESSION

Y

(b)DISTRIBUTIONOF UXALONGYY

4+-:’-<:URVE2.-f-xv

/’ REACTION.%,

STRESSx— —x

1 1 1

(c)DISTRIBUTIONOF UYALONGXX

Fm.JRE4. TYPICALDISTRIBUTION OF msD2UAL STRESSES IN BUTT wU3

Fig. 4. Typical Distribution of Residual Stresses in Butt Weld

The methods used to correct unacceptable distortion are becomingIncreasingly a matter of concern to those who design and construct shtps,because of the type of base metals being used. The high-strength, low-alloysteels are attracti~e from the standpoint of weight , strength, and cost; howeverthey are far more senditive to the affects of the st~alghtening parameters thanthe previously used structural steels. The removal or correction of distortionis usually accomplished by (1) flame straightening, or by (2) heating thedistorted area and straightening by mechanical means. While such methods have

been used successfully for many years without concern, there is co<sid~rable

question today in regard to the effect of the straightening parameters onthe mechanical and metallurgical properties Of high-strength base metals.The same concern is present with respect to aluminum which is being usedincreasingly for the fabrication of ship superstructures. The expressedconcern has much basis in fact, particularly since there is little controlof the straightening parameters. For the most part, straightening proceduresare an art rather than a science.

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Fhme4traightening Techniques

A brief review of the literature 3s included in this report to(1) provide background information on flame straightening procedures, (2)define problem areas that arise because of these operations, and (3) enumeratethe variables that can influence base metal properties+ The distortion in

small parts can sometimes be corrected by placing the parts in a press andapplying pressurk; heat may or may not be required. Large structural sections

such as those encountered in ships must be straightened in place. Flame

straightening ts a general term that is applied to most of these straighteningoperations, even though more than a flame may be involved. In some cases,

an oxyacetylene torch is used to heat the distorted area until it reaches thedesired temperature. Then heating ceases and this area %s cooled to producea controlled amount of shrinkage. While convection cooling is often used,the rate of coollng can be increased by spraying the heated area with water.Depending on the amount of distortion as well as the size and location of thedistorted area, this procedure may have to be repeated several times to completelystraighten the area. In other cases, the distorted area Is heated with anoxyacetylene torch; then; auxiliary equipment is used to remave distortion bypressing, hammering, forging, etc. In addition to their use in the shtpbutldlngindustry, these procedures are used widely in other industries for straightening

purposes; they are also used in bending structural members to obtain a desired

amount of curvature.

~01t(9-13)Numerous applications of flame straightening have been reported by

In 1955 the basic principles of flame straightening as applied tosimpie steel beams were discussed with particular emphasi on the effect of

?9-10) ln subsequentvarious heating patterns on the correction of distortion.articles, the details of flame str t b ening the structural members of a largefire-damaged hangar were reviewed. ?~~-~2) Work of this nature is very stifiar

to that encountered in ship fabrication, since it was necessary to straightenload-bearing members in place An article on the fundamentals of flame straight-

ening was published in 1965.(f3) A temperature not exceeding 1200 F was recom-mended for straightening; higher temperatures can produce buckling and materialproperty changes. Data were also presented on the amount of plastic flow thatoccurs when a conventional structural steel (A36) is heated to typical flamestraightening temperatures.

Flame straightening applications in ~ shipbuilding industry havebeen discussed in detail by Bernard and Schulze.f t) Following a reviewof the fundamentals of this process and a discussion of the equipment usedfor straightening, several examples of ship structures that were flamestraightened were discussed. Data are presented on the amount of distortionpresant In welded hull and deck sections before and after straightening(Figure 5). The differences In the heating patterns used to flame straightenthin (less than 0.400-inch-thick) and thick plate are reviewed; intermptedpatterns appear to be most effective. While there is considerable informationon the methods to apply restraint to heated sectfons, few data are providedon the straightening parameters , although the speed at which the torch is movedfor heating is usually given. The heating or straightening t~mperature isspecified as that whtch produces a “red glw” in the p~ate, il somewhatsimilar article on the use f flame straightening in the sheet metal industrywas written by Pfeiffer.(15~ !l%isarticle contains considerable informationon the special heating techniques and methads of applying pressure that,arerequired to straighten thin sheet metal sections. Some of this informationniay be of use in ship fabrication where relatively thin plate is used.

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a. Straightening of a Hull Section

b. Straightening of a Deck Section

UL.--_JlU4 ~

Fig. 5. Flame Straightening of Distortion in Ship Fabrication(14)

Notes: (1) All dimensions are in fi-llftietars(1 mm= 0.040 inch)

(2) Amount of distortion is indicated before and after ( )straightening

(3) Flae heating path wfth 5-burner torches is hsdicat~d

by series of closely spaced lines.

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Flame straightening procedures have also been reviewed in the Sovietliterature by T.salman in 1959; this article is mastly concerned with thecorrection of distortion in welde structural members such as box beams,I-beams, and other assemblies.(16 ? Heating patterns and their effect inproducing a controlled amount of reverse distortion in selected areas aredtscussed. The flame straightening temperatures ranged from 500 to 800 C(932 to 1472 F); the actual temperature to which the part was heated wasdetermined mainly on the basis of plate thickness. Temperatures on the orderof 800 C are too high for use in straightening the quenched and tempered steelssince this is well int the austenit~zing range for such base metals. Guzevich(17)and Olsara,et al., (18~ have dtscussed the effect of cold straightening procedureson the properties of low-carbon steel. Such straightening methods had littleeffect on the tensfle properties of the steel; ductility and impact fltrengthwere decreased sllghtly.

Additional information on flame straightening techniques can befound in the Steel Ship ~onstructicm Hanbook, prepared by the Society of Na

Architects of Japan, (Jy) and in an article by Stitt on distortion control.T$h)

Limited research has been undertaken to study the effects of flamestralghtentng on the properties of base metals.

&,j’’:~;i::;:%E:sstudtes on the principles of flame straightening.Investigation, mild steel bars (1/4-inch-thick by 2-inches wide by 20-incheslong) were bent and straightened; the temperature of the bar stock did notexceed 1300 F during the straightening operatfon. There waa lfttle significantdifference in the mechanical properties of these specimens insofar as theirtensile strength, impact strength, or hardness was concerned. Further studiesof flame straightening as applied so the cambering of steel beams were neportedby Crooker and Harrison in 1965.(2 ~ The authors concluded that flamecambering reduced the bending strength of the beams because of unfavorablerps+dual stresses, unfavorable cold work effects, and lateral distortion.The 10SS in strength could be decreased somewhat by the type of heating patternused during cambering. These conclusions causedprompted some discussion of the original article.t~~7id:;:Q;:r&’ and

discussion centered around the method of testing the cambered beams and thedefinition of failure. For structural purposes, flame cambering had littleeffect on the design allowable.

Analytical studies of flare straightening phenomena have also beenconducted by (1) Wanatab $ ~nd Satoh (2Z~2g)reduction of distortion by spotheating, (2) Masubuchi ( 5 and Kihara - ana~~~f~~f residual stressproduced by spot heating, and (3) Maeda and yada * - shrtnkage distortionproduced by single-and multtple-spo~ heating. titertal degradation, per se,was not considered in these investigations.

Heating patterns for flame straightening have been discussed inmany of the articles reviewed in this section. The patterns used in the ship-building industry are usually variations of the spot or linear heating techniquesshown in Figure 6. In spot heating a number of discrete spots (about 3/4 tol-1/2-inches in diameter) are heated one after another and then cooled; thespots are arranged according to the shape of the area being straightened.Straightening can also be accomplished by heating and coolfng along severallines; linear heating can be done from either side of the panel being straightened.Heat can be applied h straight or curved lines; continuous or interrupted

heating can be used. In a variation of Mn+ar heating (Figure 6c), heating andcooling is done along the back side of a stiffened panel. The relative meritsof various heating patterns are subject to debate; each shipyard has preferred

heating patterns.

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a. Spot Heating b. Line HeatingPanel Panel

c. Line HeatingBack of Welds

Fig. 6. Heating Patterns for Flame Straightening

In summary, numerous studies have been conducted on the use of flamestraightening techniques to correct or reduce distortion in welded structures;on occasion, the ssme procedures have been used to produce a controlled 8mountof distortion in a structural member (a curved beam, for example) to meetdesign criteria. The practical nature of this process is emphasized by thelarge number of “how to” articles on flame straightening as opposed to the

few theoretical articles on this subject. Even fewer studies have been concernedwith the posstble degradation of material properties as the result Of flamestraightening.

Possible Material Degradation as the Resultof Flame Straightening

An analysis of flame-straightentig procedures indicates that thefollowing parameters are most likely to affect the metallurgical and mechani-cal properties of the base metals used in ship fabrication:

(1) Maximum straightening temperature(2) Temperature gradient in the base metal(3) Heating cycle-time at maximum temperature and cooling rate(4) Amount and rate of mechanical straining(5] Number of cycles of heating and straining.

In addition to t.he~rpossible effects on the transformation characteristics andmicrostructure of the base metals, these parameters can act to decrease thetensile and impact strength of the base metals as well as influencing theductile-to-brittle transition temperature. Microcracking can occur as the

result of the fkme-str~fghtening process and the fatigue life of the base

metal can be shortened. The flame-straightening parameters can act singlyar in com~inati~ with one another to influence the base metal properties.

* Fatigue ltfe, as affected by flame straightening, is not to be studiedduring the current program.

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extensive research on the properties of steels as affected bytemperature and strain has been conducted, and there is a vast background aftechnical literature on these and related subjects. Much of this research ha~been directed toward determining the behavior of specfftc steels under real or

simulated service conditions. Other pertinent studies have been concerned withthe metallurgical and physical properties of weldments made with such steels.Some of these studies have been conducted as part of an overall program todetermine the weldabillty of a specffic steel; others have been prompted bydifficulties in obtaining the requtred joint properties in servtce. For themost part this research has little direct association with the problem at hand;however, some of the information relating material propert~es to thermal andstraining cycles may be applicable to the flame-straightening process and itseffect on base metal properties.

This is a limited state-of-the art review of the pertinent litera-ture published during the past 10 to 15 years. It has sometimes been necessaryto be selective in citing articles to illustrate a particular point In thediscussion, because of the large amount of available information.

Effect of Thermal Cycles During Flame Straightening

It is difficult to pinpoint the temperature ttsedfor flame straighten-ing steel structures, because it is frequently specified as the temperature atwhich the steel has a “dull red” glow. This is an indefinite temperature whendetermination depends on the operator’s abflity to discern perceptible changesin color as well as the effect of the surrounding environment. Based on theliterature, it is assumed that most flame-straightening operations are conductedat temperatures in the range of I1OO-12OO F; excursions 100-300 F wide on eitherstaleof this temperature range are qutte likely to occur. The cooling rateafter flame straightening Ls also an indefinite parameter. In some cases thehea~ed area is allowed to cool at a rate determined by the radiation character-L$tlcs of the base metal, by convection due to air currents, and by the transferof heat into cooler areas of plate or structure. In other cases the heated areais cooled with a water spray or an air blast to produce a h~gh rate of coaling.

The low-alloy steels with yield strengths ranging from about45,000 to 75,000 psi are used in the as-rolled or normalized condition;

many of the steels used in shtp fabrication are included in thts category.These steels can be heated to conventional flame-straightening temperatures

(*11OO-12OO F) without significantly affecting their mechanical properties.At higher straightening temperatures a few microcracks may be observed inthe heated area, and some incipient meltfng may occur. Changes in the micro-structure of the base metal can occur due to the effect of the cooling rateon the transformation characteristics of these steels. In 1961, Canonico,et al., reported on research to investigate the effects of a celerated cool-ing on the properties of steels used in”pressure vessels. (297 ABS-B andABS-C steel plates were water-quenched from a temperature of 1650 F, andthe properties of these specimens were determined and compared to the proper-ties obtained with normalized steel plates. Spray-quenching increased thestrength and notch ductility of both steels. TO determine the effect ofthermal straightening on the notch toughness of these steels, articlesconcerned with the notch toughness at various areas 5.nthe weld zone should

be consulted. Areaa in or just beyond the heat-affected zone of mild steelweldments experience temperatures of the magnitude used in lame straighten- ~31)

e those conducted by Ni pes,7

(3°?Masubuchi, et al,ing. Among such ‘tud1e~3~f and Stout ad Doty.(33 ForexaPle, durfng anGrossman and McGregor,

Page 17: Flame straightening

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investigatiim on welding l/2-inch-thick mild steel (0.19C-O.43Mn-O.019Si-0.025P-O.022S). Kihara, et al., observed an increase in the Charpy V-notch15 ft-lb transition areas in areas just beyond the heat-affected zone;these areas of the steel plate experienced temperatures of 750-930 F.Nippes and Savage studied the variation in notch toughness in specimens thatwere heated and cooled to duplicate several of the heat-af ~~$ed st~cturesin a l/2-inch-thick butt weld in an aluminum-killed steel.f Low impactproperties were noted in specimens that represe~ted a region well beyound theheat-affected zone. It, during flame straightening, heat is applied directlyto a welded joint, the metallurgical reactions are more complex; however, theeffects of the flame-straightening procedure on the mechanical propertiesof the welded joint should be insignificant also as long as the straighteningtemperature is not excessive. The joint ductility would prabably increaseslightly, sfnce the joint would be stress relieved.

Such is not the case with the high-strength, low-alloy steels thathave yield strengths in the order of 100,000 psi. These steels are furnishedin the quenched-and-tempered condition , and the temperatures and cooling ratesinvolved in flame stra~ghtening can have a serious effect on the microstructureand mechanical properties of unwelded and welded plate. These steels acquiretheir properties by water-quenching from a temperature of about 1600-1750 Fand tempertng at 1050-1275 F.* Depending on the composttton of the steel andthe heat treatment, the microstructure consists of (1) ferrite plus tempered

batnite or martensite, or (2) tempered bainite and martensite. The compo-

sition and mechanical properties of representative high-strength, low-alloysteels are shown in Tables 1 and 2; most of hese alloys have been used or are

~36~ The transformation characteris-candidates for use in ship construction.tics of two of these alloys (Grades B and F in Table 1) are shown in Figurs 7;these curves illustrate the variation in transformation behavior that must beconsidered in flame straightening a particular high-strength steel. In Figure

7a a considerable period of time elapses before this steel starts to transformh the pearlite transformation range of about 1300-1100 l?. This lapse Of

time insures that transformation to these undeshable high-temperature trans-formation products will not occur unless the cooling rate is very S1OW.Because of Its lower alloy content, the period of time that elapses beforetransformation starts Ln the Grade B steel (Figure 7b) is much shorter than

that of the Grade F steel. In the Grade F steel , a moderately long per%odof time elapses before transformation starts in the ferrite and upper bainitetemperature range of about 1100-950 F. AS a result, relatively thick plates(up to at least 2 tnches thick) can be quenched wfth little or no transforma-tion in this temperature range. This period of time is shorter for the Grade Bsteel, and the thickness of plates that can be quenched to produce the desiredlow-temperature bainitic or martensitic microstructure is l-1/4 inches orless. The transformation products (soft ferrite, upper batnite, and high-carbon martensite) that are produced in this temperature range have a degradingeffect on the notch toughness behavior of the steel even when tempered. Thecurves indfcate that transformation to low-temperature bainitic structuresoccurs in a relatively short time for both steels, and that transformationto martenslte occurs at a relatively high temperature.

~cThe temperature from which the steel is quenched and the tempering tempera-

ture depend on the composition of the steel and the-required strength level.

Page 18: Flame straightening

-12-

Tim,:, sccon~z

a, Grade F (Table 1) b Grade B (Table 1)

Fig. 7. Isothermal Transformation Diagrams for Two High-Strength, Low-Alloy Steels

Problems caused by the effects of temperature alone on base metalproperties can be encountered when the htgh-strength, low-alloy steels areflame straightened.* The extent and severfty of these problems can be anti-cipated by the care that must be exercised in welding these materials, particu-larly wfth respect to-the permissible heat input durtng weldlng. Extensiveresearch on the weldabllity of the quenched-and-tempered low-alloy steels andon related subject areas has been conducted by Government and industry, andcomprehensive procedures for weldtng such steels have been established. Afew of the many articles on this subject are included in the reference list.(37-48) In general, the weldabflity of the quenched-and-tempered low-alloysteels is excellent when the followlng welding processes are used: shieldedmetal-arc s gas-shielded metal-arc, and submerged arc. The weld-cooling ratesfor these processes are so rapid that the mechanical properties of the heat-affected zone of the steels approach those of the base metals in the quenchedcondition. Reheat treatment is not required. Welds made with high-heatinput processes, such as electroslag welding, must be heat treated afterwelding. Aside from the need to design the joint properly and use properlyconditioned low-hydrogen electrodes (assuming that welding is being doneby the shielded metal-arc process), the most important considerations inwelding the high-strength, low-alloy steels Is to select the proper preheattemperature and limit the heat input during welding to recommended levels.Suggested preheat temperatures for several of the steels listed in Table 1are shown in Table 3; maximum heat inputs for Grades B and F steels areshawn in Tables 4 and 5. The maximum heat inputs have been selected to maintainadequate notch-toughness in the heat-affected zone; the strength properties

of the heat-affected zone are not as sensittve to heat Input as the notch-toughness, so higher heat tnputs could be used if notch toughness were not

* These problems are accentuated when the combined effects of temperatureand strain on base metal properties are encountered. This subject isd~scussed in the next sect$on of this report.

Page 19: Flame straightening

Table 1. Chemical Composition of Several heat-Treated Steels.

.

Tablo ~. -Chemical campasitien ~fsovoral ho~t-trcatod stools—.

b[nc

0.20m ax

0.17

0.20nlax

017——0,18Inax

0.18

x0.21

0,12-0.21

0.1o-0.20

0.13-0.20

0.12-0.20

0.1o-020

o.M-0.21

pm 51. —

0.04 ‘ 0.05

Cu I Ni I Cr I Mo ddd.d~,Type

No. 1

No. 2

—.

HY-86

k517Grade A

A517GladeUM517Gradt C

X517Grade II

A517G~ade E

A’517(WwIe F

A517Grade G

Si

Range

rypiCd

Range

ryfdcal

o.70-1.35

1.25—.1.50m ax

1.35

0.1o-0.40

0.28

Oi~

0.70-1.60

1.10-1.56

O.<.;

o.40-0.70

Oi6g

Oi61J

o.15-0.543

0.35

030-0.60

0.40-—o.15-0.3.5

023

0.40-080

0.20-0.35

0.15-0,30

0.20-0.35

0.20-0.35

o,iii-0.35

0.56-0.90

Presentin smali quantitiesmax

0.01

0.04m ax

0.01——0.0251

max

0.015

max

0.02

9.05m ax

0.02——0.025~

max

0.016

0.04-——.........-——

o.20-0.60

0.45

018-0.28

0.15-0.25

0.20-0.30

0.15-0.25

004&-

~ 4&-

040-0.60

0.25——o.20-0.40

0.30

0.15 0.12

,.....

...

.,.—-

. . .

. . .

,..—.0.03max

0.005.-

...

0.03-0.08

...

b

1

0.03-0.08

...

. . .——.

. . .

.,,

. . .-——

. . .

. . .-———-0.025max

oam&

:,0&\-

o.o15-0.035

0.0015-0.005

yKJ:3-

0.0626mm

-——-. . .. . .

. . .

. . .

. . . -—0.02qax

0.665---

...

0.01-’0.63

...

:%

;0:;

,..

...

Range

rypical

0.25max

0.05

,..

...

...

o..w-0.40

;CKJ

00h&-

,..

2&

2.f17

.,.

‘...

...

...

...

Oi7&

.,.

I.60-1.80

1.fi8.—00boo-

0.40-0.65

.,.

o.3c5-1.20

1.40-2.00

0.40-0.66

o.bo-0,90

0.036

0.035

0.035

0.035

0.035

0 035

0.036

II.040

0.040

0.040

0046

0.040

0.040

0.040

1 For firebox quality DhosDhorua Ia 0035 rnax and fmlfur 0.640 max.2 Thephosphorus and su~fw together nhoutd not exceed 0045.~ L4ar be subntltutcd for part or all titanium conLent on a one-to on-basis.

Page 20: Flame straightening

Table 2. Properti~s cf Lnnuitudinal Tensile and Charpy V-!lotchImpact in Heat-Treated St

rablo~. .+ropcfiios dkngitudinal tonsilo and Charpy V-notch impact inh~at-troatid ~teels

(aeeT:%%14)

No.1

NO. 2

HY-80

A517GRADE F

A517GKALIE B

Yield Pointor Strength

(R###Thickness range

(in.) x lo~

To l%, inci, 60Over 1% to 2,incl. 56

Less than ~

1

60-100

% to2, irrcl, 80-96Over 2 80-95

% to 2%, incl. 100Over 2% to 4,incl. 90Over 4 to 6, incL no

TensileStrength(R#X#

x 10$

80-10076-95

1$)

115-135106-E35Mr&13ri

115-136116-135

MinimumElongation

in 2 in.percent(rein)

23123 t

19

2020

18s1716

Rcducticmin Arm, ~.

(rein)

5565

ml5045

40m

Energy AbooV-notch irnpac:t

Longitudinal

::8.;::;

60r@-120°F(Vi inch and oGO@120°F

L30@-120° F

20@-50°F~30@-O°F

L5@AwF

[ For firebox quality elongation in 2 inches is 24~0,I Elongation (or plates uncier ~ inch is 15%.1 Reductiorr in area 40~0 (rein) for p!atea to ~,inch, incl,~ To 2% Inch incI.

Page 21: Flame straightening

-15-

of.primary importance. In shielded metal-arc welding, the stringer-beadtechnique should be used wtthout appreciable transverse oscillation tominimize the heat input; deposition techniques that prolong heating shouldbe avoided. Welded joints made with high-strength, low-alloy steels usuallydo not require stress relieving unless dimensional stability must be maintainedor stress corroston may be involved. Notch-toughness tests have shown thattoughness in the weld metal and heat-affected zone may be impaired by postweldheat treatment in the 110-1200 J?temperature range, especially if the steelis cooled slowly as in the case of stress relteving. Intergranular cracking

in the grain-coarsened regfon in the heat-affected zone may occur also.

What, then, are the effects of temperature on the properties ofhigh-strength, low-alloy steels when they are flame straightened? If anunwelckd plate section is flame straightened at temperatures below 1100-1200 F,

it is not expected that the base metal properties will be seriously affected,although there probably will be some loss in ductility and notch toughness;this is quite similar to a retempering operation. The degradation of basemetal properties becomes more serious when the distorted plate section containsa welded joint. If the temperature in the joint area reaches 950-1200 Fduring the straightening operatton, the notch-toughness properties of theweld metal and heat-affected zone are adversely affected if the plate iscooled slowly. Doty noted a considerable increase in the Charpy V-notchtransiti n temperature when ‘T-I’ welded joints were stress relteved at1200 F.(29) These effects should be less pronounced if the plate isquenched with a water spray after straightening. Also, as mentioned above,intergranular cracking In the heat-affected zone has been observed whenwelded high-strength, steel jotnts were heated to these temperatures. Such

cracking occurs by stress rupture in the early stages of the stress-relieftreatment before the hi h restdual tensile stress from weldtng has beensignificantly reduced.(gg-50)

The consequences are far more serious if efther a welded or unweldedplate sectton is heated above the lower critical temperature of the base metalduring the flame-straightening operation. For example, Burbank flame-heatedunwelded sections of ‘HTS’ steel plate, 3/8 inch thick, to temperaturesbetween 975 and 1490 and water-quenched them.(51) These specimens showed adecrease in Charpy V-notch Impact strength when they were tested homediatelyafter straightening; a further decrease was noted in specimens that weretested 6 months later. A similar behavtor was observed when 5/8-inch-thickplate was heated and quenched. Guided bend tests conducted wfth these materialswere generally unsatisfactory. Burbank noted an improvement in base metalproperties when the plate was held at a temperature of 1100 F for one-halfhour after straightening, followed by slow cooling to 500 F and air coolingto room temperature. Further evidence of the problems that can be encountereddurfng flame straightening Is contained in a case history cited by Doty(@l

a comprehensive article on the welding of quenched-and-tempered steeLs.A penstock fabricator found cracks and water leaks when large Y-branch pipeswere pressure tested. The cracks were located in a transition section of ‘T-1’steel that was hot-formed to produce a flare fitting. Before hot-forming,the transition section was heated to about 2200 F. After forming, thefitting was cooled. Then, ft was reheated with gas burners, water-quenched,and retempered. Examination showed that the reheat-treated region containedmaterial that had been heated to a temperature as high as 2200 F for about10 minutes before cooling; durtng tempering, some areas of the transitionsectton had been heated to 1250 F while others had been heated only to 1050 F,The recommended temperature ranges for austenitizing and tempering ‘T-1’steel are 1650-1750 F and 1100-1275 F, respectively. Because of this irregularheat treatment, the material in the locally reheat-treated region had an

Page 22: Flame straightening

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undesirable microstructure and failed by stress mpture during a subsequentfurnace stress-relieving Operation.

It is not likely that flame straightening will be conducted attemperatures above 2000 F; however, the temperature in a localized area of aplate being straightened may exceed the lower critical temperature of thesteel and even approach or exceed the upper crftical temperature. In eithercase, the mill heat treatment is upset. In the case of ‘T-1’ steel, if completeor partial austenitiZation occurs, some undesired transformation may occur inthe 1300-1100 F temperature upon slow cooling. Further transformation mayoccur in the ferrite and upper bainite temperature region (1100-950 l?)toproduce an undesirable microstructure consisting of soft ferrite, upperbanite with retained austenite, htgh-carbon martensite, or high-carbon

“U;inite. This microstructure is very undesirable from the notch-toughnessstandpoint. If the plate section being flame straightened contains a weldedjoint, the situation is even more complex and serious because notch tough-ness in the heat-affected zone is highly dependent on its microstructure.

Thus, flame straightening of high-strength, low-alloy steel struc-tures must be approached with caution and a thorough knowledge of the metal-lurgical consequences that can occur because of improper straighteningprocedures.

Effects of Thermal Cycles and Plastic Strain During

Flame Straightening

Thus far, only the effects of temperature on base metal propertiesduring flame straightening have been considered. However, strain is alwayspresent during these operations, since the structure is plastically deformedthrough thermal or mechanical processes to achieve the required degree ofstraightness.

It has been recognized that plastic straining at room temperaturereduces the available plastic-deformation capacity by an amount at leastequal to the prestraining. Often, however, much less ductility is retainedthan would be estimated from the prestraiming. An important factor whichcauses the drastic reduction of ductility is aging, a condition to whichplastically strained metal is quite prone. Another important factor is thechange of shape of the discontinult~es during prestraining; when defects arepresent in the material before straining, prestraining will modify the shapeof these defects. Straining of a flawed material in uniaxial tension bluntsthe flaw aridin many circumstances has a beneficial effect. But detrimentaleffects result when prestraining sharpens the defect root. This may occurwhen prestraining is obtained by transverse straining in tension and finaltesting is undertaken with longitudinal tension. Severest damage resultswhen prestraining in compression in the same direction precedes final tensiletesttng.

Many research programs have been conducted to study the effects of

plastic strain and thermal cycles, which occur during welding and otheroperations, on material properties. However, only limited study has beenmade specifically on material degradation due to distortion-straighteningtreatments. Thermal and plast$c changes that take place during the straighten-ing treatments are different from those that take place during other treatments.

Therefore, the nature and extent of material degradation caused by straighten-ing treatments may be radically different from that caused by other treatments.

Page 23: Flame straightening

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Table 3. --Comparison Chart of Suggested Preheat Temperatures when Arc WeldingSeveral Different Steels

..—Table -% -Compnriwn churt of suggested ~rchcat tempcm!urc. when arc welding

severnl diRercnt steels

FlawI’hickn&ss

(in,)

‘rOjf,incl.

% to !%. ]nd.

fito%,lncl.

H to 1. incl.

110lM.incl.1H to 1%, incl.lH to 2, incl.Over 2

Minimum Preheat or Intcr!x$ss TMtDCIatUrC fur IVclding [ndimled Gmk u? Ww’i\Vith Low-I1ydru@rl Elect rud+ F

—... — __——— . . . . ..— - .— —.-— .-——

NO. 1 No. 2 H }“-SJJ I Gradel’ Gr.dr B———— ————..-——.—. .———. -—--..———. . -————— ----

——.

7.575

123125200200200200

——

I A preheat km Peraturc abuve the mini mu nl may be required for hkhh - restrained welds- IWOweld! ‘W-

should bc done when ambient ccmpcraturc is fmlow O“F. If temperature of steel is below -50”F. prehe? tin Kto 50”F or to indicated preheat tcm Dcrature-whfchever is higher—should bc pctfurmcd, The lnw-h~drn~~nelectrodes must be thoroughly dried.

Table 4. --Maximum Welding Heat Input in Joules/inch for Butt Joints in Grade F Steel

T~ble ~, -Maximum welding heat input in Joules/inch for butt i.aints in Grade F s?ecl

Preheat and I Plate Thickness (in.)

27 ,OCKl 3G,000 70,000 121,000 any any any any

2% 21.000 29,000 W ,000 9!).000 173,000 an Y any any

300 17,000 24,003 47.000 ,32,000 126,000 175,00093.000 127,000 I 16fio0

any

400 13,000 19,000 40,000 G5,000 any

Joules /inch of weld =Amperes x volts x GO

.%&d in inches Der MkIUte

h’OTE:Heat-input fimits for temwxaturts and thicknesses included; but not shown. in this table mw’ beobtained by frttcrpolatmn.25~0 higher heat inputs are alIowable for fillet we!d% such as T-hints.

Table 5. --Maximum Welding Heat Input in Joules/inch for Butt Joints in Grade B Steel

Tablw 5.*’! -Maximum welding heat input in Joule!/inch for bun ioi~t$ in Grade B steel

Prebmt and I Plate Thickt~ess (in.)

17,.500 23,700 35,000 47,400 M,mo 8s ,6001% 15,300

any an}-20, gl)o 30,700 41 ,?00 57,400 77,400 ljo.000 any

200 14,000 19,200 2s ,000;;%$ ~ ;;;%

6!),91xJ l;g,j~ 134.000-300 11,500 15,800 ~J ,~oo400 9.000

.545,ml) ]~o .0001~,300 , 18,500 41,900 63:600 9-I.000,, 1 1 1 , I

Joules /inch of weld = ‘m?e~cs x ‘“’t’ x 60Sueed m mc!m net mmute—.

AYOXE: Heat-input limits for tcmpmatures and thicknesses inclurlcd. but not Ybown, in this table may beobtained by interpol:,.lim.25% higher h~~i input, are ~llnwmblcfor Iillct w-ekb, such as T-joints.

Page 24: Flame straightening

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T.husthere is a need for the proposed study, which is direcced specificallytoward the effects of straightening treatments. Nevertheless, some of theinformation concerning material degradations which occur in other treatmentsshould be useful in the proposed study.

A recenc book, preparedly Hall, Kihara, Soete, and Wells, providesa good background on the effects of plastic strain and ternerature on the

tproperties of steels, especially ordinary carbon steels. (4 ) Work with thehigh-qtrength, low-alloy steels is more limited.

Tensile Straining at Room Temperature. Effects of straining bytension at room temperature on material properties have been studied byseveral investigators including Mylonas. (53,54) Mylonas prepared flatspecimens of low-carbon steel, 10 inches wide, containing machined notches ontheir sides. The notched specimens had been subjected to various amounts ofprestrain at room temperature, and final tensile tests at low temperatures(between-12 and -3 F). The plates that were prestrained Ln tension trans–versely to the direction of testing failed at average stresses below virginyield, the lowest value being 70 percent of virgin yield. In contrast, allthe plates that were prestrained longitudinally failed generally at or abovethe virgin yield, but below the ratsed yield point.

These tests illustrate the important role of the direction ofprestraining and confirm generally that prestra%ning that increases the

shallowness of defects increases the embrittlement, while prestrainingthat provokes blunting of the defects leads to a lesser degree of embrittlo-ment.

Compressive-Straining at Room Temperature. The effect of pre-by compression at room temperature also was investigated by

‘traini~~53,55) Notched specimens were subjected to various amounts ofMylonasprestrain in compression. After prestraining, which was done at roomtmnperature, the specimens were kept at -25 1?up to the time of testing,in order to minimize aging effects. Tensile tests were made at temperaturesin the range of about –12 to O l?. All fractures had a brittle appearance.Test results were interpreted as a function of the maximum applied stressin percentage of virgin yield. Many of the specimens broke before fullyielding occurred. One specimen failed at an average stress of 12 percentof virgin yield , and cracking was observed at average stresses as low as9 “percent of virgin yield.

Satoh and Mylonas also conducted studies to determine the effectof surface finish on the ~ompressive prestraining needed to exhaust the tensileductility of the steel. (5 ) Bars of ABS-C steel with as-rolled and machinedsurfaces were prestrained by bending; the effects of.surface finish and amountof prestrain were determined by a reversed bend test prepared by Ludley andDrunker. Bars with machined surfaces had a slightly higher exhaustionlimit than those with as-rolled surfaces; the difference is somewhat more

pronounced for bars tested at -16 F than for those tested at room temperature.

In more recent work, Mylonas, Kobayashi, and Armenakas have beenconcerned with the effect of strong constraint on the duct~lity of prestrained

——

Page 25: Flame straightening

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ABS-B and E-steel bars.(58)

The des<red amount of constraint was obtainedby machining a deep circumferential groove in prestrained and aged (330 Ffor 2 hours) cylindrical bar specimens. The specimens were tested in tension

at -16 F and room temperature. The experimental results indicated a severereduction irIductil:ty for bars that were notched; the embrittling prestraindecreased from about 0.75 for smooth bars (APS-B steel) to 0.05 for notchedbars. In 1968, Kabayashi and Mylonas discussed the effect of small dfs–continuities (represented by small holes drilled in the bar stock before (59)prestraining by compression) on khe prestrain required to produce brittleness.The existence of these cliscontinuities reduced the amount of compressive pre-

strain causing brittleness to (1) one–third or one-fourth the amount neededin soltd bars of E-steel, and (2) two-thirds to one-fourth the amount neededin solid bars of ~S-B steel.

The data on high-strength, low-alloy steels are more limitedthan those available for low- and medium-strength steels. In evaluating

the reversed bend test, Ludley and Drucker included data on ‘T-1” steel. (57)

Also, Doty studied the effect of compressive prestraint (obtained by coldreducti n of plate stock] on the ductility-transition temperature of ‘T-1’steel. ~tg) Prestrainiing produced an increase of about 33 F in thetransition temperature; this temperature was increased by 63 F when the pre-straimed specimen was aged at 550 F for one hour. Stress relieving the

specimens after prestraining produced a slight decrease in the transitiontemperature. Iri1967, Armenakas and Mylonas discussed the effect of com-

pressive prestraining (produced by bending bar stock to obtain the desiredamount of prestraining) on the ductility properties of 18 percent nickelmaraging steel and two titanium alloys, Ti-6Al-4V and Ti-13V-llCr-3Al. (60)The ductilityof the maraging steel dropped sharply at a prestrain of 0.50;the ductility of the titanium alloys decreased more gradually with increasingprestraim.

Tensile Prestraining at High Temperature. Various investigators

‘2) reported tests whereincluding Terazawa, et al.(bl) and Soete, et al.(bprestraintng was accomplished by tension at high temperatures and finalfracture testing was done at room or low temperature.

Figure 8 shows results obtained by Terazawa, et al. on killedsteel 1 inch thick. Cylindrical specimens were prestrained by tension atdifferent temperatures up to 1110 F (600 C). Strains up to 70 percent wereapplied to the specimens. The final tests were performed at room tempera-ture 1 or 2 days after prestratning. The test results, presented inFigure 8, indicate that for a flawless material tested at room temperature,the total ductility is independent Of the amount of prestraining at roomtemperature and equal to the ultimate strain obtained in a single tensiontest. However, when prestraining is done at higher temperature there is asubstantial loss of ductility. For the steel involved here, 390 1? (200 C)and 930 1? (500 C) appeared to be the most damaging temperatures. The lossof ductility at the higher temperatures appears important for prestrainingof 10 percent or”more. It is important to observe that the fracture stresswas practically independent of the amount of prestraining and the temperature

of prestraining.

.—

Page 26: Flame straightening

-20-

120

~ 80

:==

a.E~ 40E

“20 -..

0. 100 200 300 403 500 600

Prestrainirq temperature [“C) Prestroining temperature (“C)

Fig. 9. Compressive Prestrain Resultfor Cylindrical Specimens(61 f

Compressive Restraining at High Temperature. The tests byMylonas, previously mentioned, illustrated the danger of prestrainingnotched specimens at room temperature. It is likely that if this prestrain-ing is done at some critical temperature even more catastrophic results maybe expected. Studies were made of the effects of temperature and plasticstraining by compression on unnotched specimens by several investigators.

For example,63)

Korber~ et al. conducted fracture tests at roomtaperature of cylindrical specimens that had been prestrained by compressionat different temperatures. The specimens were made from a Basic Bessemersteel, an open-hearth steel, and a cast steel. Undamaged (unrestrained)specimens contracted about 70 percent in laminated steel and about 60 per-cent in cast steel, while prestrained specimens contracted less than 5percent. The most dangerous temperaturewas around 48o l?.

Terazawa, et al., conducted similar tests with a mild steel.(61)

The specimens were prestrained at temperatures of 100, 300, 400, 500, and600; ~he amount oi prestraining ranged from 0.3 toof this study are summarized in Figure 9. Seriouswhen the steel was prestrained about 70 percent atand 500 C.

75 percent. The resultsembrittlement occurredtemperatures between 200

Plastic Strainin~ by Bending. Tests made by Korber, et al. haveshown that for each temperature of prestraining there appears to be a

critical strain above which steels behave brittlely in a subsequent tensiletest. This critical strain has been called the exhaustion limit by Mylonas.This exhaustion limit depends on both the temperature at which the prestratn-ing has been done and the temperature of the final tensile tests.

Page 27: Flame straightening

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lzoo~ -“”1 I I I I 1200r I I I I I I I i i

‘ 200ml!ImzJ–jLtr--iI

-.-.-=-bars bent at 75” F i%%% I Wflz

&5 0.20 0.25 0,30 0.35 0.40 0.45 0.50 0.55 0.60Compressive prestroin

Fig. 10. Reversed-Bend Tests of Unaged Fig. 11.

Bars cf E Steel Prestrainedat Various Temperatures (64)

The reversed-bend test prepared by Ludley and

Compressive pfestrain

Reversed-Bend Tests of UnagedBars of E Steel Prestrainedat Various Temperatures (64)

Drucker to simulateplastic straining by compression ~as-alread~ been mentioned. In this pro-cedure, a bar specimen is prestrained by bending to produce the desiredamount of com ressive prestrain on the intrados (the concave section of the

?curved bar).( 7, Then, reversed bending IS done in a tensile machine toproduce tension on the intrados. In 1962, Rockey, Ludley, and Mylonasdetermined the effect of various amounts of compressive prestrain on theductility of the following steels: E-steel, A7, AI!S-C,T-1, and HY-80. 64)The results for tests conducted with E-steel are shown in Figures 10andll.Also shown in these figures are the transition ranges of aged and unagedbars of E-steel.

The fracture toughness and fracture-toughness transition tempera-ture of two mild steels was also determined with another bending test by Dvorak.

(65)

In this test, machined bars were prestrained in compression by four-point load-ing. Three-point loading was used to conduct the reverse-bend tests.

Impact Tests on Plastically Strained Material. Many programshave been conducted to study the effect of plastic straining at differenttemperatures on the impact value of embrittled steel. The results aregenerally interpreted as a function of the increase in the conventionaltransition temperature. For example, Terazawa, et al., conducted Charpyimpact tests of carbon steel that had been prestrained to v r“ous levels

‘i6%ransition(up to 70 percent) at different temperatures (up to 1100 F).temperatures increased considerably when the steel was subjected to plasticstraining of about 35 percent at a temperature between 400 and 550 l?.

Specimens Prepared from Weldments. As descrfbed in a shipstruccure committee report prepared by Masubuchi, et al.(67), many in-vestigators have stud%ed notch toughness at various locations of-a weldedjoint. In most cases, Charpy impact specimens were used; however, otherspecimens, including notched-bar tensile or bending specimens, also havebeen used. F+WrF :2 ~hw~ distributions of the Charpy V-notch 15 ft-lbtransition temperatures in l/2-inch-thick carbon-steel welds made byshielded metal-arc and submerged processes. (60) Transition temperatureswere high in areas 0.4 to 0.6 inch from the weld center, somewhat outsidethe heat-affected zone. The maximum temperature of the embrittled zoneattained during welding was 750 to 930 F.

Page 28: Flame straightening

-22-

i30se-Metal Composition-—

c Mn Si P

= =3 0=6 0025

,Test I

s0,022

I [ i I 1

1 2 3 4

Distance from Center of Weld ,inchesWddingConditiom

WeldingCurrent, Welding Speed,Test Weld ing M8thod Shape of Groove amperes in. /rein——

1 Shielded metal -arc 60°V, O.35” deep 160 ,9.0(a)2 Submerged -arc 60”V, O.16” deep 600 11.53 Submerged -arc 60”V, O.12” deep 500 34.0

(a) For each pass.

Fig. 12. Distribution of Charpy V-Notch 15-FT-LB Transition Temperaturein Groove Welds in +-inch-thick Mild-Steel Plates Made withShielded Metal-Arc and Submerged-Arc Processes (6s)

The above tnvestigatton and many other investigations have shownthat notch toughness is the lowest in areas well outside the zone usuallyconsidered the heat-affected zone. However, this embrittled zone does not

appear to be important in the brittle fracture of welded structures. Btittle

fractures that occurred in ships and other structures frequently initiated

from the heat-affected zone and weld defects. However, no brittle fracturehas been reported that initiated from the embrittled zone near the weld.Nor do brittle fractures propagate through the embrittled zone.

Tests on Specimens Subjected to Simulated Thermal Cycles. Many

investigators, including Nippes and Savage(30*35 ,69,70) conducted tests on

specimens subjected to simulated thermal cycles. Most of the tests conducted

so far have investigated properties of the heat-affected zone of the weld.

A- .—

Page 29: Flame straightening

-23-

1600

1400

~ 1200a“3G

: 1000

e

800

600

400

4,,----- ----

Mz

1 Ii-----------*----I ! I

+ r----------—-—----ABCED

I I 393 379 329’~\321

I I VPN hardness values

I 5 10 5U 100

Time ,seconds

Results Obtained with Synthetic Thermal -Cycle Specimens

EnergyThermal Input,

Cycle j/in.

A 47,000B 47,000c 47,000D 47,000E 75,600

WeldCooling Rate

Initial Plate Peak Temp. Hardness, at 900 F,Temp, F F VPN F/see——

72 2400 393 12.8200 2400 379 8.7300 2400 336 6.3500 24OO 321 2.572 24oO 329 4.5

)0

Charpy V-NomhTrmrsirion Temp. F—.

FractureiO F[-Lb Appearance——

-138 +5-100 +25

-47 +68

+26 +152-16 +71

Fig. 13. Weld Thermal Cycles Indicated on Continuous-Cooling TransformationDiagram of Quenched and Tempered High-Strength Steel (69)

The synthetic-specimen technique has been quite useful for studying the notchtoughness of the heat-affected zone in high-strength steels which undergocomplex transformation during welding.

The effect of the cooling rate on microstructure and notch toughnesscan be investigated systematically with the combined use of the synthetic-specimeu technique and the continuous-cooling transformatiorr (CCT) diagram.Figure13 shows the CCT-diagram of a quenched-and-tempered steel (1OO,OOO psi

Page 30: Flame straightening

yield strength). Also shown here are weld thermal cycles as follows:

(1) Thermal cycles, A, B, C, and D, which represent cooling

curves for ~kie heat-affected zone structures wfth a 2400 Fpeak temperature in.1/2-inch-thick butt welds (heat input:47,000 joules/inch) with various preheating temperaturesup to 500 F

(2) Thermal cycle E , which represents a cooling curve of theheat-affected zone in a weld made with a 75,000 joules/inchheat input.

The notch toughness of synthettc spechnens that underwent thermalcycles A through E is shown in the note of Figure 13. Notch toughness decreasedmarkedly when the cooling rate was reduced by either increasing Intttal platetemperature or increasing energy input. The investigators explained that thepoor behavior of the slowly cooled heat-affected zone was due to the fact thatlow-carbon martensite, which has excellent notch toughness, was graduallyreplaced by a mixture af.ferrtte and high-carbon martenstte or banite. Itmust be mentioned, however, that the effects of welding thermal cycles on’notch toughness of the heat-affected zone depend greatly upon the compositionand microstructure of the material. In the case of hardenable steels contain-ing moderate amounts of carbon , rapid coolfng rates generally cause formationof brfttle martensite. Si ilar studies with D6ac steel were also conductedby Nippes and Emmerich.~70 Y

Dfe.cussfon

A review of the literature was conducted to determine the effectsof flame straightening on the properties af the base metals being straightened.Flame straightening procedures are used extensively in the shipbuilding industryto remove or correct distastion caused by welding and other assembly methods.The technfquea of flame straightening are well-established and there is considerableinformation available on heating equfpment, heating patterns, etc. However,there is a lack of substantiated data that directly relate the physical andmechanical properties of the base metals to the flame straightening parameters.With the increasing use of high-strength, low-alloy steels in shtp fabrication,there iq a need for tiuchinformation, because the properties of these materialsare quite susceptible to degradation by unwise handling.

The parameters that are most likely to affect base metal propertiesduring straightening are temperature, strafn, and various combinations oftemperature and strain. The results of the literature search are discussedbriefly on the bash of these parameters.

(1) Temperature. The temperature to which steel plate isheated for straightening can have a significant bearingon the properties of the base metal. The medium-and high-strength, low-alloy steels are much more sensitive to theeffects of temperature than the low-strength steels.SO long as prolonged heating of the low-strength steelsdoes not occur in a temperature range where they are

Page 31: Flame straightening

-25-

(2)

susceptible ta brittleness, it is not expected thatflame straightening will affect their temperaturesmarkedly. Such is not the case with the higher-alloyedquenched and tempered steels. If straightening Isconducted at temperatures in excess of the lowercrttical temperature, these steels will partially trans-form and undesirable mfcrostructures can form as the steelis coaled; heating to these temperatures will also alterthe mill heat treatment of these steels. Prolonged heatingat lower temperatures can also promote the formationof brittle microstructure.

The Eit.erature contains numerous references to theeffect of temperature on base metal properties.Isothermal transfornmtion diagrams are mostlyused in determining the effects of reheating steels forstraightening. Other pertinent data can be obtainedfrom weldability studies, studies of the heat-affectedzone in welds, etc.

Strain (and Temperature). Extensive studies have beenconducted to determine the effects of strain at varioustemperatures Tn the brittle fracture characteristics ofmany of the low- and medium-strength steels used in ship-building; comparable data on high-strength steels are notso readily available because fewer studies with thesemater~als have been undertaken. However, the strains(extending up to about 75 percent) investigated dur<ngthese programs are generally much higher than thoseto be encountered in the conventional stratght.eningofplate that has been distorted by welding. Thus, thisinformation is of limited value in the current program.The available data indtcate that low strains (less than5 percent) have little effect on the base metal properties.

The current research program will provide some data on materialproperty degradation as the result of flame straightening and mechanicalstraightening at elevated temperatures. The straightening of steel plates,pre-bent to produce small strains , will be conducted at temperatures near1200 ~for the most part; a few straightening experiments will be conductedat temperatures above and below this commonly accepted flame-straighteningtemperature. Steels with yield strength levels of from 50,000 to 100,000psi are included in this work. These data should be supplemented at aEuture date with additional information on the behavior of these and othersteels used in shipbuilding over a more complete range of temperatures.rhe experimental program plan for the present research is shown in Table 6.?late specimens subjected to the various treatments will be evaluated byTarious mechanical property and metallurgical tests. The primary evaluation~ethod will be ‘basedon full section drop-weight tear tests.

Page 32: Flame straightening

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ghtening Studies (Unwelded and Welded Test Specimens)Table 6. Schedule for Stra

Mechanical ThermalPlate Amount of Straightening Straightening

Code Type of Thickness, Distortion, Temperature, Temperature, Number ofNumber Steel inch imch F 1? Test Plates

A517Ditto

!1II11

11

11

II

A517DTttc)

IfIt11

A517Ditto

111111

A537Ditto

!11!

11

A441Ditto

11111!

ABS-13Ditto

11

11

t!

1/2Ditto

11

II

!1

11

1!

It

3/8Ditto

1111II

3/4Ditto

!1!111

1/2Ditto

!1!1t!

1/2Ditto11

ItIt

1/2Ditto

It

II11

None7/16Ditto

!1

9/64Ditto7/16Ditto

22111121

12345678

910111212a

1314151616a

1718192020a

2122232424a

252627

28

28a

13001000RT1300RT

1300-14001100-1200

None1/2Ditto

!1

1200RT

1300-14001100-120011

None3/8Ditto

11II

22111

1200RT

1300-14001100-1200

None7/16Ditto

1!

1200RT

1300-14001100-120011

22111

7/16Ditto

11It

1200RT

1300-14001100-1200

None7/16Ditto

11Ii

1200RT

1300-14001100-1200

.—..—

Page 33: Flame straightening

-27-

REHIERENCES

(1) Kerr, D.M., “welding Distortion in Shipbuilding”, Weldingin Shipbuilding a Symposium, Institute of Welding, London,

England, October 30 to November 3, 1961.

(2) Spraragen, W. and Claussen, G.E., “ShrinkageDistortion in

Welding, A Xeview of the Literature to January 1, 1937”,Welding Journal, 16 (7), Research Supplement, 21-s to 40-s—(1937).

(3) Spraragen, W. and COIVi, M.A.,ItShrinkage~~stOrt~On in ‘eldinglr$

Welding Journal, 23 (11), Research Supplement, 545-s to 559-s—(1944).

(4) spraragen, W. and Ettinger, W.G., “Shrinkage Distortion inWelding”, Welding Journal, 29 (6 and 7), Research Supplement,29-s to 294-s, 323-s tO 335% (1950).

(5) Kihara, H. and Masubuchi, K., Distortions and Residual Stresses Due to Weld-=, Sampo Publishing Company, Tokyo, Japan, 1955.

(6) Kihara, H., Wanatabej M. Masubuchi, K., and Satoh, K., Research onWelding Stress and Distortion,. The Society of Naval Architects Of

Japan, Tokyo, Tapan, 1959.

(7) Wanatabe, M. and Satoh, K., WeldinR Mechanics and Its Applications,Asakura Publishing Company, Tokyo, Japan, 1965.

(8) Okerbloom, N. O., The Calculation of Deformations of Welded MetalStructures, Her Majesty’s Stationary Office, London, England, 1958.

(9) HoIt, J., “Flame-Straightening: A Friend in Need, Part 1“, Welding Rngineer,40 (10), 44-46 (1955).—

(10) HoIt, .J., “Flame-Straightening: A Friend in Need, Part 111’,Welding Engineer,40 (12), 30-31 (1955).—

(l-l)Anonymous, “Flame Buckled this Steel ...and Flame Straightened It, Part I“,Welding Engineer, ~ (2), 40-43 (1959).

(12) Anonymous, “Oxyacetylene Torches Straighten Fire-Warped Steel, Part 11,”Welding Engineer, 44 (3), 31-34 (1959).

(13) Ho~t, R. E., “Flame Straightening Basics”, Welding Engineer, 50 (9), 49-52—(1965).

(14) Bernard, P., and Schulze, K., “Flame Straightening in Shipbuilding”,Mittelunge der BEFA (Beratungsstelle f<r Autogen Technik), 17 (11),2-6 (1966) (German).

(15) Pfeiffer, R., “The Flame Straightening of Sheet and Sheet Metal Structures”,Mitteilungen der BEI?A,14 (9), 1-7 (1963) (German).—

Page 34: Flame straightening

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(16) Tsalman, L. B., “Straightening Welded Structures by Heating wtth an OxyacetyleneFlame”, Welding Production? ~ (3), 29-31 (1959) (Russian).

(17) Guzevich, Yu. D., “Cold Straightening Beams DLstorted by Welding”, AutomaticWelding, ~ (7), 19-22 (1958) (Russian).

(18) Okara, V.G., 13arsht,V.D., Shatailo, D.V., Rozenman, Ya. Sh., and Tsalmzn,

L.B., “The Effect of Cold Straightening on the Mechanical Properties afWelded Joints”, Automatic Welding, 18 (7), 32-35 (1965) (Russian).—

(19) Steel Ship Construction Handbook, Nippon Kogyo Kuzai Renmei, Tokyo (1960).

(20) Stitt, J*R., “Distortion Control During Welding of Large Structures”, Paper

presented at the Society of Automotive Engineers and American Society ofMechanical Engineers, Alr Transport and Space Meeting, New York, New York,April 27, 1964, Paper 844 B.

(21) Harrison, H.L., “straightening Structural Members in Place”, Welding Journal,31 (5), Research Supplement, 257-S to 260-s (1952).—

(22) Crooker, T.W., and Harrison, H. L., “The Effects of Flame Cambering on theBending Strength of I-Beams”, Welding Journal, 44 (12], Research Supplement,

545-S to 548-s (1965).—

(23) Higgins, T.R., Kaopman, K.H., and Grover, L., “Discussion on the Effects of

Flame Cambering on the Bending Strength of I-Beams”, Welding Journal, .45 (6)Research Supplement, 284-s to 288-S (1966].

(24) Watanabe, M., and sa~~~, K., “On the Correction of Distortion in WaldedThin Plate Structures”, Journal of Japan Welding Society, ~ , 194-202(1951).

(25) Masubuchi, K., “calculation and Measurement of Residual Stresses Due to

Spot Heating”, Document No. X-259-60, International Institute of Welding,COmmiSSiOU X (1960).

(26) Kihara, H., Nisida, M., and l?ujita,Y., “On the Residual Stresses Dueto SpaE Heating”, Document No. x-267-61, International Institute ofWelding, Commission X (1961).

(27) Maeda, T., and yada, T., “Fundamental Nature of Shrinkage DistortionDue to Spot Heating on a Rectangular Plate”, Document NO x-327-63, In&sr-national Institute of Welding, Commission X (1963).

(28) Maeda, T., and Yada, T., “Investigation of Shrinkage Due to MultipleSpot Heating”, Document No. X-268-61, International Institute of welding,Commission X (1961).

(2?) Canonico, D.A., Kottcamp, E.H., and Stout, R.D., “Accelerated Cooling ofCarbon Steels for Pressure Vessels”, Welding Journal, 40 (9) ResearchSupplement, 400-s to 404-s (1961).

(30) Nippes, E. l?., “The Weld Heat-Affected Zone”, Welding Journal, ~ (1),

Research Supplement, 1-S to 18-S (1959).

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(33)

(34)

(35)

(36)

(37)

(38)

(39)

(40)

(41)

(42)

(43)

(44)

(45)

-29-

Masubuchi, K., Kusada, T., and Tamura, H. “Effect of Welding on theNatch Sensitivity of Ship Steels”, Jnl. Japan Welding Society, 21 (1)—2-.9 (1957).

Grossman, N. , and McGregor, C.W., “The Brittle Transition Temperature ofVarious Low-Carbon Steels Welded by the Same Method”, Welding Journal,27 (5), Research Supplement, 267-S to 271-S (1948).—

Stout, R.D., and Doty, W.D., ‘TJeldabilityof Steel”, Welding ResearchCouncil, American Welding Society (1953).

Kihara, H., Masubuchi, K., and Tsmura, H., ‘kffect of Welding on theNotch Sensitivity of Steel--Especially on the Embrittled Zone Due towelding”, Brittle Fracture in Mild Steel and Their Welded JoLnts, TheWelding Research Committee of the Society of Naval Architects of Japan,144-152 (1953).

Nippes, E.F., and Savage, W. F., “Tests of Specimens Simulating WeldHeat-Affected Zone, “welding Journal, 28 (12), Research Supplement, 599-Sto 616-s (1949).

Welding Handbook, SectIon 4, American Welding Society, New York, N.Y.Fifth Edition, (1966).

Zick, L.P., ‘~esign of Welded Pressure Vessels Using Quenched and TemperedSteels”, Welding Journalj 34 (9), Research Supplement, 442-s to 448-S—(1955).

Dawson, T.J., “Quenched and Tempered Steels in Ship Structure”,Welding Journal, 40 (4), Research Supplement, 175-S to 181-S (1961).—

Doty, W.D., and Grotke, G.E., “Some Observation on the Weldability Of

Quenched and Tempered High-Yield-Strength Alloy Steels”, ConferenceProceedings, U.S. Navy Bureau of Ships~ Washington, D.C., 34-67,March 21 and 22, 1960.

Aroold, P.C., “Problems Associated with the Welding of ‘T-1’ Material”,

Welding Journal, 36 (8), Research Supplement, 373-S to 381-S (1957).—

Rathbone, A.M., Connor, L.P., and Gross, J.H., ‘Weldability Of a HighToughness Alloy Plate Steel with a Minimum Yield Strength of 140 Ksi”,welding Journal, 43 (12), Research Supplement, 551-s to 563-s (1964).—

Lewis, W.J., Faulkner, G.E., Martin, D.C., and Rieppel, P.J., “SubmergedArc Welding HY-80 Steel”, Welding Journal, ~ (6) Research Supplement,266-s to 278-s (1960).

Sibley, C.R., %eldfng of HY-80 Steel with the Gas-Shielded Metal Arcprocess”, Welding Journal, 42, (5), Research Supplement, 219-S to 232-S(1963).

Doty, W.D., “Welding of Quenched and Tempered Steels”, Welding Journal,44 (7), Research Slipplement, 289-s to 309-S (1965).—

Notvest, K., “Effect of Thermal Cycles in Welding I)6AcSteel”, WeldingJournal. 45 (4). Research Supplement. 173-S to 177-S (1966).

Page 36: Flame straightening

(46)

(47)

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(49]

(50)

(51)

(52)

(53)

(54)

(55)

(56)

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(58)

(59)

(60)

(61)

-30-

Mishler, H.W., Monroe, R.E., and Rieppel, P.Steels for Aircraft and Missile Application,Defense Metals Information Center, Columbus,

J ‘Welding of High-Strength““&IC Report NO. 118,Ohio (1959).

Uchida, J. M., ‘Welding Evaluation of New High Strength Quench and TemperSteels”, Welding Journal, 45 (l), Research Supplement, 31-S to 40-s (1966).—

k,per, C, R.,and Stout, R.D., ‘tieldabilityand Notch Toughness of HeatTreated Carban Steel”, Welding Journal , ~ (9), Research Supplement,385-s to 392-s (1968).

Doty, W.D., “Properties and Characteristics af a Quenched and TemperedSteel for Pressure Vessels”, Welding Journal,> (9), Research Supplement,425-s tO 441-S (1955).

Robinson, v.S., I?ense,A.W., and Stout, R.D., “The Creep-Rupture Propertiesof Pressure Vessel Steels”, Welding Journal, 43 (12), Research Supplement.531-S tO 540-S (1964),

Burbank, B. B., “Straightening Distorted Weldments”,

July 8, 1968.

Hall, W. J., Kihara, H., Soete, W., and Wells, A.A.,Welded Plate, Prentice-Hall, Inc., Englewood Cliffs,

Report No. SR-185,

Brittle Fracture ofN.J. (1967).

Mylonas, C., “Exhaustion of Ductility and Brittle Fracture of E-SteelCaused by Prestrain and Aging”, Ship St~cture Committee Report No. 162(July, 1964} ●

Mylonas, C., Drucker, D.C., and Isberg, L., “Brittle Fracture InitiationTests”, Welding Journal, ~ (l), Research Supplement, 9-S to 17-S (1957).

Mylonas, C., “Prestrain, Size, and Residual Stresses in Static Brittle-

Fracture Initiation”, Welding Journal, 38 (10), Research Supplement,414-s to 424-s (1959).

Satoh, K., and Mylonas, C., “Reversed-Bend Tests of ABS-C Steel with

AS-Rolled and Machined Surfaces”, Ship Structure Committee Report No,SSC-166 (April, 1965).

Ludley, J.H., and Drucker, D.C. , “A Reversed-Bend Test to Study Ductile

to Brittle Transition”, Welding Journal, 39 (12), Research Supplement,

543-s to 546-S (1960).—

Mylonas, C., Kobayashi, S., Armenakas, A., “Exhaustion of Ductility under

Notch Constraint Following Uniform Prestraining”, Ship Structure CommitteeReport No. SSC-173 (August, 1966).

Kobayashi, S., and Mylonas, C., “Exhaustion of Ductility in Compressed

Bars with Holes”, Ship Structure Committee Report No. SSC-184 (June, 1968).

Armenakas, A.E., and Mylonas, C., “Reduction of Ductility by Prestraining

of Maraging Steel and Two Titanium Alloys”, Welding Journal, ~ (12),

Research Supplement, 570-s to 576-S (1967).

Terazawa, K., Otani, N., Yoshida, T., and Terai, K., ‘~ffect of High

Temperature Prestraintng on Retained Ducttlity of Steel,” InternationalInstitute of Welding Document, No. IX-285-61 (1961).

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(69.)

(70)

Soete, W., et al. Eurathm-Contract No. 042/61/9RDB, II-2-4.

Korber, F., ELchinger, A., and Mailer, H., “Behavior of Prestrained Metalsduring Tensile Loading”, Mitteilungen K. Wilhelm Institut Eisenforschung,26, 71 (1943).

Rockey, K. C.,:Ludley, J.H., and Mylonas, C., “Exhaustion of ExtensionalDuctility Determined by Reversed Bending of 5 Steels”, Proceedings ofthe ASTM, 62, 1120 (1962).

Dvorak, J., “The Precompression Bending Test”, Welding Jaurnal, 45 (5)Research Supplement, 235-240-s (1966).

Terazawa, K., Otani, N., Vos!nida, T., and Terai, K., “Effects of HighTemperature on the Notch Toughness of Steel,” International Instituteof Welding,Document NO.IX-286-61 (1961).

Masubuchi, K., Monroe, R.E,, and Martin, D.C., “Interpretative Repurton Weld-Metal Toughness”, Ship Structure Committee Report No. SSC-169

(Ju~Y, 1965) AIso, Welding Research Council Bulletin No. 111 (January,1966).

Kihara, H., Masubuchi,K., and Tamura, H., “Effects of Welding on theNotch Sensitivity of Steel - Especially on the Embrittled Zone Dueto Welding”, Brittle Fracture in Mild Steel and Their Welded Joints,The Welding Research Committee of the Society of Naval Architects of Japan,144-152 (1953).

Nlppes, E.F., Savage, W. l?.,and Alllo, R.J., “Studies of the WeldHeat-Affected Zone of T.-1Steel”, Welding Journal, ~ (12), ResearchSupplement, 531-S to 540-S (1957).

Nippes, E. F., and Emmerich, E.W., “Heat Affected Zone Study of an EutectoidUltra-High Strength Steel’i,Welding Jouraal, 42 (12), Research Supplement,547-S tO 556-s (1963).

Page 38: Flame straightening

UnclassifiedSecutity Classification

DOCUMENT CONTROL DATA - R&D(Security claauiiication ottltle, body ofab. tract andindexing mnotation must be entered when the overall reporti. classified)

!. ORIGINATING ACTIVITY (COr=r~le @hOr~2a. Uk5PORT SECURITY CLASSIFICATION

Battelle Memorial InstituteUnclassified

Columbus, Ohio2b GROUP

3. REPORT TITLE

I Flame Straightening and Its Effect on Base Metal PropertiesI

4. DESCRIPTIVE NOTES (Type of raportandincfusive dales)

Summary Report5. AUTHOR(S) (La~tn~e, f~f~:nHm*, jm~tiaf~

I Pattee, H. E. Evans, R. M. Monroe, R. E.IJ

6. REPORT DATE 7FI. TOTAL NO. OF PAGES 7b. NO. OF REFS

August 1969 31 70ga. CONTRACT OR GRANT NO. 9a, oRIGINATOR’S REPORT NUMBER(S)

IOCC24-68-C-5324b. PROJECT NO.

y.~85c, gb, OTHER REPORT NO(S) (Any otharnumbers ti=tm=ybe#ssi@*d

Ma Import)

d,SSC-198

10.AvAILABILITY/LIMITATION NOTICES

I Distribution of this document is unlimited. I

1. SUPPLEMENTARY NOTES

.—

12. SPONSORING MILITARY ACTIVITY

Department of the Navy

None Naval Ship Engineering CenterWashington, D. C. 20360

13 ABSTRACT

The suitability of flame-straightening methods now used onconventional ship steels for the higher strength ship steels is questionable.This report discusses some of the potential problem areas that need evalua-tion to examine this subject. Based on a survey of pertinent literature itis shown that only limited data applicable to this subject are available.The data analysis covered the nature of distortion, flame-straighteningtechniques, and the effects of both single and combined thermal cycles andplastic strain cycles on material properties. An experimentalprogram ispresented that is designed to generate background data on conventionalsteels and several higher strength steels directly pertinent to flamestraightening. These data will subsequently be evaluated to ascertainsuitability of the flame-straightening procedure for various ship steels.

!

DD 1W%1473a

Unclassified.%curitytiassification

Page 39: Flame straightening

Uncla<slflwl. .

SecurityClassificationI 4.

KEY WORDS

INSTRUCTIONS

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Page 40: Flame straightening

SHIP RESEARCH COMMITTEEMaritime-Transportation Research Board

Division of EngineeringNational Academy of Sciences-National Research Council

This p~oject has been conducted uncle?the guidanc~ of Adviso~yGPoup III, Ship Reseamh Committee. The Committw has cognizance of Ship

Stmetu-re Committee p~ojects in matwials, design and fahication as z=e-‘Latingto impoved ship stmctwes, This responsibility entails recom-

mending resea~eh objeetivas, p?eparing project p?ospeetuses, evaluating

ppoposalz, providing liaison and technical guidance, revieuing p~ojeetrepo~ts, and stimulating p~oduetive awnuez of ~eseareh.

MR. M. L. SELLERS, ChaimnanNaval ArchitectNewport News Shipbuilding

and Dry Dock Company

DR. H. N. ABRAMSON (1,11)Director, Dept. of Mechanical SciencesSouthwest Research Institute

MR. W. H. BUCKLEY (1,11)Chief, Structural Criteria and LoadsBell Aerosystems Company

DR. D. P. CLAUSING (III)Senior Scientist, Edgar C. Bain

Laboratory for Fundamental ResearchU. S. Steel Corporation

MR. D. P. COURTSAL (11,111)Assistant Chief EngineerDravo Corporation

MR. A. E. COX (1,11)General Program ManagerNewport News Shipbuilding

and Dry Dock Company

MR. F. V. DALY (III)Manager of Facilities and Process

EngineeringNewport News Shipbuilding

and Dry Dock Company

MR. J. F. DALZELL (1), CoordinatorSenior Research ScientistHydronautics, Incorporated

C.DRD. FAULKh!ER, RCNC (1,11)Staff Constructor OfficerBritish Navy Staff

(I) =Advisoq L%OUP I,(II) = Advisory (%ozIP II,

PP.OF.J. E. GOLDBERG(1,11)School of Civil EngineeringPurdue University

MR. J. E. HERZ (1,11)Chief Structural Design EngineerSun Shipbuilding and Dry Dock Company

MR. G. E. KAMPSC}IAEFER, JR. (III)Manager, Application EngineeringARMCO Steel Corporation

PROF. R. R. NOTON (11,111)Department of Aeronuatics

and AstronauticsStanford Llniversity

MR. W. W. OFFNER (III)Consulting Engineer

DR. S. T. ROLFE (III), CoordinatorDivision Chief, Applied Research CenterU. S. Steel Corporation

PROF. J. WEERTMAN (11,111)Walter P. Murphy Professor

of Materials ScienceNorthwestern University

CDR R. M. WHITE, USCG (1,11)Chief, Applied Engineering SectionU. S. Coast Guard Academy

PROF. R. A. YAGLE (II), CoordinatorDepartment of Naval Architecture

and Marine EngineeringUniversity of Michigan

MR. R. W. RUMKE, Exeeutioe SecwtarsShip Research Committee

Ship Strain Meawremwt & AnalysisShip Structural DasignMei5aZh?gical Studies(111) =Adviso~ GPOu~ 111,

Page 41: Flame straightening

SHIP STRUCTURE COMMITTEE PUBLICATIONS

I

)

I.

SSC-186,

SSC-187,

“SSC-188,

SSC-189,

SSC-190,

SSC-191,

SSC-192,

SSC-193,

SSC-194,

SSC-195,

SSC-196,

SSC-197,

These doewwnts are distributed byVu. 221s1. These documents hav~

the Clearinghouse, spr~ngf~ald,been announced in the TeehnieaZ

Abstract Bulletin (TAB) of the Defense Doeum&tation Center (DDC),Cmeron Station, Alexandria, Vu. 22314, unde~ the indicated ADnumbems.

Effect of Ship Stiffness upon the Structu~aZ,Responze of a CargoShip to an Impukive Load. by Manley St. Denis and Samuel N.Fersht. September 1968. AD 675639.

IBiennial Repo~tiof Ship Structure committee. : September 1968.AD 675022.

Effect of Repeated Loads on the Lou Tmperatz&e F?aetwe Behavio~of flotehedand Welded Plates by W. !-l.Munse, ?. P. Cannon andJ. F. Kiefner. October 1968. AD 676722.

The Video Tape Reco&ng of Ultrasonic Test Information by RobertA. Youshaw, Charles H. Dyer and Edward L. Criscuolo. October1968. AD 677894.

Bending Moment Distribution in a Marinw Ca~go Ship Model inRegula~ and Ir?egulaY Wave~ of Extreme Steepne~s by Naresh M.Maniar and Edward Numata. November 1968. AD 689187.

Plastic Flotiin the Local on Notches and C~acks in Fe-3Si SteelUnder Conditions Approaching Plane Strain by G. T. Hahn and A. R.Rosenfield. November 1968. AD 680123.

Notch Brittleness afte~ F~actu~e by C. Mylona4 and S. Kobayashi.January 1969. AD 681051.

Development of Mathematical Models for Deserikkg Skip Stmetu~aZRe~ponze in Waves by Paul Kaplin. January 196g. AD 682591.

Feasibility Study ofMode2 Tez+ on Ship Hu_/?Z~irder by HerbertBecker. May 1969. AD 687220.

Recommended Emergency Welding Procedure for T@npora~ Repair6 ofShip SteeZs by A. L. Lowenberg and P. D. Matsoh. May 1969.AQ 688119.

I

Analysis and Interpretation of FuZZ-ScaZe Data on M&?slripBendingSt~esses of Dry Ca~go Ships by Dan Hoffman and Edward V. Lewis.June 1969.

1An Investigation of the Utility of Compute~ Si ‘uZationto PredictShip structural Response in Waves by p. Kaplin T. p. Sarqentand A. I. Raff. June 1969

_.—- —.—-— .. ..... ..-.——.___ - -. _ ___ ._ __L