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    Materials Science and Engineering A 397 (2005) 376384

    Microstructure and mechanical properties of friction stir welded SAF2507 super duplex stainless steel

    Y.S. Sato a,, T.W. Nelson b, C.J. Sterling b, R.J. Steel c, C.-O. Pettersson d

    a Department of Materials Processing, Graduate School of Engineering, Tohoku University, 6-6-02 Aramaki-aza-Aoba,

    Sendai 980-8579, Japanb Mechanical Engineering Department, Brigham Young University, 435 CTB, Provo, UT 84602, USA

    c MegaStir Technologies, 275 West 2230 North, Provo, UT 84604, USAd Sankvik Materials Technology, Sandviken S-811 81, Sweden

    Received 18 January 2005; received in revised form 18 February 2005; accepted 25 February 2005

    Abstract

    Themicrostructure and mechanical propertiesof friction stir(FS) welded SAF2507 superduplexstainless steel wereexamined.High-quality,

    full-penetration welds were successfully produced in the super duplex stainless steel by friction stir welding (FSW) using polycrystalline

    cubic boron nitride (PCBN) tool. The base material had a microstructure consisting of the ferrite matrix with austenite islands, but FSW

    refined grains of the ferrite and austenite phases in the stir zone through dynamic recrystallisation. Ferrite content was held between 50 and

    60% throughout the weld. The smaller grain sizes of the ferrite and austenite phases caused increase in hardness and strength within the stir

    zone. Welded transverse tensile specimen failed near the border between the stir zone and TMAZ at the retreating side as the weld had roughly

    the same strengths as the base material.

    2005 Elsevier B.V. All rights reserved.

    Keywords: Duplex stainless steel; Friction stir welding; Mechanical properties; Microstructure

    1. Introduction

    Duplex stainless steels have a mixed microstructure con-

    sisting of ferrite (bcc) and austenite (fcc) phases[1,2].When

    duplex stainless steels have the optimum phase balance,

    which is usually approximately equal proportions of ferrite

    and austenite phases, they exhibit higher resistance to stress

    corrosion cracking and higher strength than austenitic stain-

    less steels[1].Taking advantages of these positive factors,

    duplex stainless steels are widely used in the oil and gas,

    petrochemical, pulp and paper, and pollution control indus-

    tries[1].

    It is well known that the duplex stainless steels exhibit

    good weldability[1], but the melting and solidification as-

    sociated with fusion welding processes destroy the favorable

    duplex microstructure of these stainless steels. Microstruc-

    Corresponding author. Tel.: +81 22 795 7353; fax: +81 22 795 7352.

    E-mail address:[email protected] (Y.S. Sato).

    ture of the wrought duplex stainless steels has a pronounced

    orientation of austenite islands in the ferrite matrix, paral-

    lel and transverse to the rolling direction, but fusion welding

    produces a microstructure consisting of coarse ferrite grains,

    and both intergranular and intragranular austenite phases in

    the weld metal and heat affected zone (HAZ)[15].In gen-

    eral, the volume fraction of ferrite is much higher than that of

    austenite in the weld metal and HAZ. These changes in mi-

    crostructure cause the loss of low-temperature notch tough-

    ness and corrosion resistance in the weld[1,2]. To alleviate

    these problems,careful control of theweld metal composition

    and temperature are often required during welding.

    Friction stir welding (FSW) is a solid-state joining process

    developed and patented by The Welding Institute (TWI) in

    UK in 1991[6]. Since inception, FSW had been restricted to

    the lower melting temperature materials, such as aluminum

    (Al) and magnesium (Mg) alloys[716]. However, over the

    past 5 years, much progress has been made in FSW of high

    temperature materials by numerous investigators [1725].

    0921-5093/$ see front matter 2005 Elsevier B.V. All rights reserved.

    doi:10.1016/j.msea.2005.02.054

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    Y.S. Sato et al. / Materials Science and Engineering A 397 (2005) 376384 377

    These studies have reported that FSW achieves similar grain

    refinement in the stir zone of the steels as those observed in

    aluminum. Additionally, FSW does not accompany melting

    and solidification, alleviating the formation of porosity and

    adverse phase transformations during the welding process.

    This situation suggests that the favorable duplex microstruc-

    ture of the duplex stainless steel should be maintained, butthere have been few papers dealing with FSW of duplex stain-

    less steel.

    The present study used SAF 2507 super duplex stainless

    steel as the base material. This particular super duplex stain-

    less steel exhibits significantly higher corrosion resistance

    than early grades of duplex stainless steels[1]. The nominal

    chemical composition of the alloy used in this investigation

    is Fe25Cr7Ni3.5Mo0.25NWCu (wt.%). The present

    study applied FSW using polycrystalline cubic boron nitride

    (PCBN) tool to SAF 2507 super duplex stainless steel. The

    postweld microstructure and mechanical properties of the FS

    weld were examined.

    2. Experimental procedures

    Thebasematerialused in thepresent study is a commercial

    SAF 2507 (UNS 2750) super duplex stainless steel, 4 mm

    in thickness. Test plates were prepared with dimensions of

    300 mm in length and 100 mm in width. Light sanding of

    the top surface and joint butt surface to remove oxide and

    contaminants prior to welding was performed using 80 grit

    emery cloth. Before FSW, each coupon was degreased with

    a methanol solvent.

    FSW tool used in this study had a shoulder diameter of25 mm with the pin being 3.8 mm in length. The shoulder and

    pin section of the tool were manufactured from solid PCBN.

    A locking collar was used to hold the PCBN and transfer

    torque from a tungsten carbide shank as shown inFig. 1.

    FS welds were completedon a vertical milling machine fit-

    ted with servomotors and control system. Since the machine

    and tool were exposed to high temperatures during FSW, a

    liquid cooled tool holder equipped with telemetry system to

    broadcast tool temperature was used for the weld trails. An

    argon atmosphere was introduced through a gas cup around

    the tool at a flow rate of 2.8 105 mm3/s (1 m3/h) to avoid

    the surface oxidation. A 3.5 tilt was applied to the tool dur-

    ing FSW. The welding direction (WD) was identical to the

    rolling direction (RD) of the plate. The welding parameters

    were: rotational speed of 450 rpm and weld travel speed of

    1 mm/s.

    Microstructure in the weld was examined by opti-

    cal microscopy (OM) and orientation imaging microscopy

    (OIMTM)[26,27]. Sample for OM examination were elec-

    trolytically etched in a 10 wt.% oxalic acid solution at 30 V

    for 20 s. Details of the microstructure were examined by

    OIM. Cross section for OIM was cut perpendicular to the

    welding direction and then electrolytically polished in 20 ml

    HClO4+ 180 ml C2H5OH solution at 223K (50C). Crys-

    Fig. 1. PCBN friction stir welding tool assembly.

    tallographic data were obtained from several regions, which

    are illustrated as solid squares inFig. 2. The notation CEN

    means the weld centre, which was defined as the centre of re-

    gion swept by the shoulder. The notations ASn and RSn

    indicate that the location of analysis isn mm away from the

    weld centre at the advancing and retreating sides, respec-

    tively. These notations are used throughout the present paper.

    Crystallographic data collection by OIM was performed in a

    PHILIPS XL30-SFEG scanning electron microscope (SEM),

    operating at 30 kV under step size of 0.6m. Each observa-

    tion area was 150m 150m. Crystallographic data were

    expressed by phase map with grain boundaries and {1 1 1}pole figure. In the phase map, austenite and ferrite phases

    were colored with gray and white, respectively, and the thick

    and thin black lines show grain boundaries with misorienta-

    tion exceeding 15 and misorientation between 3 and 15,

    respectively. Coordinate axes of{1 1 1}pole figures are WD(or RD for the base material), transverse direction (TD) and

    normal direction (ND) of the plate, as shown inFig. 2.

    Vickers hardness test was conducted on the cross section

    perpendicular to the welding direction, using a Vickers in-

    denter with a 9.8 N load for 10 s, to examine the distribution

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    Fig. 2. Schematic illustration of locations analyzed by OIM on cross section perpendicular to the welding direction.

    of hardness originating with the duplex microstructure con-

    sisting of ferrite and austenite. Transverse tensile specimens

    were removed perpendicular to the welding direction and

    prepared in accordance with ASTM E8. Tensile tests werecarried out at room temperature on a 445 kN MTS tensile

    testing machine at a crosshead speed of 0.05 mm/s. A 51 mm

    extensometer was used to determine the 0.2% offset yield

    strength.

    3. Results and discussion

    3.1. Microstructure distribution of the weld

    Low-magnification overview of friction stir welded SAF

    2507 duplex stainless steel is presented inFig. 3.In the cross

    section, the left- and right-hand sides of the weld center are

    consistent with retreating and advancing sides of the rotating

    Fig. 3. Cross section perpendicular to the welding direction of friction stir welded super duplex stainless steel 2507. An arrow shows the fracture location for

    the transverse tensile test.

    Fig. 4. Optical micrograph and phase map obtained by OIM of the base material.

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    tool, respectively[2833]. The stir zone is seen around the

    weld center. Theborder between the stir zone and the thermo-

    mechanically affected zone (TMAZ) is very distinct on the

    advancing side, while it is more diffuse on the retreating side.

    It is apparent that the weld interior exhibits a high degree of

    continuity and no defects.

    An optical micrograph and a phase map of the as-receivedbase material are shown in Fig. 4.The base material has a

    typical microstructure of wrought duplex stainless steels con-

    sisting of ferrite matrix with austenite islands. OIM analysis

    revealed that the austenite islands contained a higher number

    of grain boundaries (mostly twin type boundaries) than the

    ferrite. OIM analysis also revealed that the ferrite content was

    about 51%. Averagegrain sizes of austenite andferrite phases

    in the base material were about 4.3 and 5.1 m, respectively.

    Optical microstructures of regions A, B, C and D

    shown inFig. 3are indicated inFig. 5. Region B lies on the

    weld centre, and region D is located on the border of the stir

    zone and TMAZ. Regions A and C are located around 2 mm

    away from the weld centre at the retreating and advancing

    sides, respectively. Region B has the microstructure consist-

    ingof ferrite matrixwith themore elongatedaustenite islands.

    Austenite islands of region B look finer than those of the base

    material. Region A has the similar microstructure to region

    B, while region C seems to contain finer austenite islandsthan region B. Distribution of the austenite islands is finest in

    the stir zone at the advancing side, as shown in micrograph

    of region D. In this region, D, the austenite in the stir zone

    exhibits an average grain size of 2.2m lying immediately

    adjacent to elongated austenite islands in the TMAZ.

    Phase maps of regions RS4.5, CEN and AS4.5 in the weld

    areshown in Fig.6. All regions consist of a ferrite matrix with

    the austenite islands similar to that of the base material. Dis-

    tribution of the austenite islands in regions RS4.5 and CEN

    is similar to that in the base material, but the austenite islands

    contain more grain boundaries than the base material. Region

    Fig. 5. Optical microstructures of regions A, B, C and D shown inFig. 2.

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    Fig. 6. Phase maps of regions RS4.5, CEN and AS4.5 in the weld.

    AS4.5 has more finely distributed austenite islands than thebase material, and theaustenite islands of this region lie along

    the border of the stir zone/TMAZ. Again, the average grain

    size of the austenite phase was finest in this region, averaging

    2.2m. In all regions, the grain size of the austenite phase

    was smaller than that of the ferrite phase.

    Phase map of region AS5.5, located just outside the stir

    zone, is shown in Fig. 7. This has the roughly same mor-

    phology of austenite islands as the base material. However,

    the ferrite matrix in this region contains a relatively higher

    density of sub-boundaries than that in the base material. Av-

    Fig. 7. Phase map of region AS5.5 in the weld.

    erage grain size of theaustenite phase in this region was about4.0m, which is the roughly same as that of the base mate-

    rial, while average grain size of the ferrite phase was about

    4.0m, smaller than that of the base material.

    Grain size profiles of the austenite and ferrite phases are

    indicated inFig. 8. The austenite phase exhibits a smaller

    grain size than the ferrite phase throughout the weld. In the

    stir zone, grain sizes of austenite and ferrite phases decrease

    from theretreating side towardsthe advancingside.The finest

    austenite and ferrite grains are observed in the stir zone near

    the TMAZ. Ferrite content profile across the stir zone in the

    weld is shown in Fig. 9. Ferrite content varies between 50 and

    60% across the weld and TMAZs, which is slightly higherthan that of the base material. The higher ferrite content in

    the stir zone is attributed to the exposure to high tempera-

    tures during FSW and the fact ferrite is more stable than the

    austenite at the higher temperatures in the duplex stainless

    steel[1].

    {1 1 1}pole figures of the ferrite and austenite phases inseveral regions in the weld are presented inFig. 10. The base

    Fig. 8. Grain size profiles of the austenite and ferrite phases in the weld.

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    Fig. 9. Profile of ferrite content in the weld.

    material has the weak{1 1 0}1 1 2 orientation in the austen-ite phase and the relatively strong {0 0 1}1 1 0orientation

    in the ferrite phase, where{h k l} is the crystallographic planeperpendicular to the ND and u v w is the crystallographic

    direction parallel to RD. Regions RS4.5, CEN and AS4.5

    have different texture components, both in the austenite and

    ferrite phases, from those observed in base material. These

    changes in texture are indicative of the intense deformation

    of material during FSW[29,30,32].In region AS5.5, on the

    other hand, the texture component in the austenite phase is

    roughly the same as that of the base material, while the fer-

    rite phase exhibits a different texture component unlike that

    of the base material.

    3.2. Microstructural evolution during FSW

    During FSW, the duplex stainless steel is heated up to

    high temperatures created by frictional heating arising from

    rotation of the welding tool. It is well known that the mi-

    crostructure of duplex stainless steel changes to the fully

    ferritic structure when the steel is exposed to temperatures

    higher than about 1573 K (1300 C) [1]. Numerical calcu-

    lation using the present chemical composition and the ther-

    mochemical database [34] estimated that formation of the

    fully ferritic microstructure required temperature exceedingabout 1600 K (1327 C) in the present steel. The formation of

    the fully ferritic microstructure is followed by nucleation of

    austenite phase at grain boundaries of the ferrite grains dur-

    ing the weld cooling cycle. Therefore, the stir zone should

    have the coarse ferrite matrix with intergranular austenite

    phases, if it is heated up to temperatures higher than 1600K

    (1327 C) during FSW. In the present study, however, several

    microstructural analyses show that all regions in the weld

    have the microstructures consisting of the ferrite matrix with

    austenite islands, although the distribution and morphology

    of the austenite islands areinhomogeneous in the weld. These

    results indicate that the maximum temperature during FSW

    did not exceed 1600 K (1327 C).During FSW, the material in the stir zone simultaneously

    experiences large shear stresses along the pin tool surface, as

    well as exposure to high temperatures [29,30,32]. A previ-

    ous study[33]investigating material flow of FSW using an

    in situ marker technique illustrated that material located at

    the advancing side of the stir zone is displaced around the

    entire circumference of the pin tool, ending up at roughly

    the same location it began, displaced only slightly forward

    of its original position. As a result, this report suggests that

    material in the stir zone at the advancing side receives the

    most severe deformation, which would tend to break up the

    austenite islands producing a smaller grain size. This corre-sponds well with the microstructures reported herein, in that

    the finest austenite grains are observed along the advancing

    side of the stir zone.

    Fig. 10. {1 1 1}pole figures of the austenite and ferrite phases in the base material (BM), regions RS4.5, CEN, AS4.5 and AS5.5 in the weld.

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    Thegrainsizeprofile(Fig. 8) showedthat theaustenite and

    ferrite grains in the stir zone were smaller than those in the

    base material. Additionally, the phase maps (Fig. 6)showed

    that both the austenite and ferrite phases in the stir zone did

    not exhibit a heavily deformed microstructure, e.g. many low

    angle grain boundaries. Both the grain size profile and phase

    maps suggest that dynamic recrystallisation occurred bothin the austenite and ferrite phases during FSW. It is gener-

    ally known that dynamic recrystallisation easily occurs in the

    austenitic stainless steels, while ferritic steels hardly experi-

    ence dynamic recrystallisation because the ferrite phase has

    a high stacking fault energy[35].

    In the case of the duplex stainless steels, however, de-

    formation is localized in the ferrite matrix at high temper-

    atures, because the ferrite phase is relatively weaker than

    the austenite phase[36,37]. Consequently, the recrystallised

    grains are often formed in ferrite phase more easily than

    in austenite phase[3639]. Some research[36,37]suggests

    that the recrystallised grains in the ferrite phase are formed

    by continuous dynamic recrystallisation, which is charac-terized by strain-induced progressive rotation of subgrains

    with little boundary migration. In the present study, the du-

    plex stainless steel experienced plastic deformation by the

    rotating tool at relatively high temperatures during FSW. As

    such, it is likely that the ferrite matrix in the stir zone under-

    goes continuous dynamic recrystallisation through the same

    scenario.

    On the other hand, the morphology of austenite islands

    in the stir zone was much different from that of the base

    material, as shown in Figs. 5 and 6. This suggests that the

    austenite islands also experienced intense plastic strain dur-

    ing FSW, leading to dynamic recrystallisation in the austenitephase.

    After dynamic recrystallisation, the recrystallised grains

    grow during the on-cooling thermal cycle [40,41].As men-

    tioned above, since the ferrite phase is more likely to undergo

    dynamic recrystallisation than the austenite phase, as a result

    of the high temperature deformation of FSW, it is likely that

    the recrystallised ferrite grains would grow early than those

    of the austenite phase. This is likely the reason why the ferrite

    phase exhibits a larger grain size than the austenite phase in

    the stir zone.

    Region AS5.5, located just outside the stir zone, had the

    similar morphology of austenite islands to the as-received

    base material. Grain size and texture of the austenite phase

    in region AS5.5 were roughly the same as those in the base

    material, but the ferrite phase had the different texture com-

    ponents than that of the base material. This result suggests

    that only the ferrite matrix underwent deformation and re-

    crystallisation during FSW because the ferrite phase has a

    lower flow stress at elevated temperature than the austen-

    ite phase in the duplex stainless steel, as mentioned above.

    It is generally known in Al alloys that dislocations intro-

    duced into the TMAZ rearranged or migrate at tempera-

    ture producing a recovered microstructure [4245]. How-

    ever, the ferrite phase in region AS5.5 did not exhibit a de-

    Fig. 11. Hardness profile across the stir zone in the weld.

    formed microstructure. This result suggests that the ferrite

    phase in this region may undergo sufficient plastic strains

    to induce continuous dynamic recrystallisation as a resultof the significant localisation of deformation in the ferrite

    phase.

    3.3. Mechanical properties and effect of microstructure

    on mechanical properties

    A typical transverse hardness profile of a FSW in 2507

    super duplex stainless steel is indicated inFig. 11.Given the

    fact that the ferrite content in the stir zone is roughly uniform

    (Fig. 9), the increase of hardness in the stir zone suggests that

    the hardness profile is related to the grain sizes of ferrite and

    austenite phases in the weld (Fig. 8).Transverse tensile properties of the weld are shown in

    Fig. 12(a). The as-FSW 2507 super duplex exhibits roughly

    the same 0.2% offset yield and ultimate tensile strengths as

    the base material, with the exception of the elongation. To-

    tal elongation to failure based on the standard 51 mm gauge

    length was roughly 50% of the base material. However, given

    the amount of reduction in area as observed in Fig. 12(b),

    the actual percentage of ductility of the FSW specimens is

    likely much higher than reported. All tensile failures oc-

    curred roughly 7 mm from the weld centre at the retreat-

    ing side, i.e. near the border of the stir zone and TMAZ,

    as shown inFig. 12(b). This is consistent with the data pre-

    sented inFig. 11,where the failures tend to move toward the

    TMAZ as a result of the higher hardness, which is propor-

    tional to strength in the metallic materials[9,46],of the stir

    zone.

    It should be pointed out that the tensile specimens used in

    this study did not have uniform thickness (seeFig. 3)across

    the weld. Typically, the thinnest section of a FSW is located

    at the centerline of the weld, as a result of the tilt angle used

    during welding. This is a reason why the transverse tensile

    samples consistently fractured near the border of the stir zone

    and TMAZ, rather than in the base material, which exhibited

    the lowest hardness.

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    Fig. 12. (a) Transverse tensile properties of the weld and (b) cross section of the fractured tensile sample.

    4. Conclusions

    The present study examined the microstructure and me-

    chanical properties of FSW in SAF 2507 super duplex stain-

    less steel. FSW using PCBN tool produced high-quality

    welds in the super duplex stainless steel. FSW significantly

    refined the ferrite and austenite phases through dynamic re-

    crystallisation. The smaller ferrite and austenite grains cre-

    ated increased hardness and strength in the stir zone. As a

    result, weld transverse tensile failures consistently occurred

    near theborder of thestir zone andTMAZ, exhibiting roughly

    the same yield and ultimate tensile strengths as the base ma-

    terial.

    Acknowledgements

    The authors are grateful to Mr. J.W. Pew and Mr. J.N.

    Ostler for technical assistance and acknowledge Prof. K.Ishida and Dr. I. Ohnuma for the thermochemical calcula-

    tion. They also wish to thank Prof. H. Kokawa, Dr. S.H.C.

    Park and Dr. J.-Q. Su for their helpful discussion.

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