9
18 th Plansee Seminar HM 7/1 Precipitation of M 7 C 3 Carbides During Sintering of TiCN-WC-Ni-Co-Cr Alloys Used in Hot Rolling Applications I. Iparraguirre*, N. Rodriguez*, F. Ibarreta**, R. Martinez**, J.M. Sanchez* * CEIT and TECNUN, Paseo Manuel de Lardizábal 15, 20018, San Sebastián, Gipuzkoa, Basque Country, Spain. ** FMD CARBIDE S.A.L., Zorrozaurre 35, 48014, Bilbao, Spain. Abstract The densification of TiCN-WC-Cr-Ni cermets has been analysed by means of dilatometry and calorimetry. Shrinkage phenomena, both in solid and liquid phase, are enhanced by the Cr additions. Carbothermal reduction of oxides is observed to occur at much lower temperatures for high Cr contents. The dissolution of the different additives used in the powder mixtures and the rim formation also depend on the amount of Cr added. Thus, TiC and WC dissolution occurs at lower temperatures as the Cr content increases. In all cases the rim formation requires the presence of a liquid phase. Keywords WC Introduction Recently, the interest in Ti(C,N) based cermets is increasing due to the dramatic rise of tungsten prices [1]. These alloys are candidates for substitution of cemented carbides in a variety of tribological applications due to their excellent combination of high hot hardness, fracture strength, oxidation resistance and thermal conductivity [2-6]. Among these cermets, those with higher metallic contents (> 25 vol.%) are the less studied. These compositions are less dense than steel and, for this reason, are typically used for the fabrication of components working under high inertial loads (i.e. roller guides in hot rolling mills). Apart from Ferro-TiC ® type materials [7,8], TiMoCN-Ni and TiWCN-Ni cermets are typical examples of these alloys [6,9-12], which are obtained by liquid phase sintering of a variety of powder mixtures. In some cases, the carbonitride powders are homogeneous solid solutions within the Ti-Mo-C- N and Ti-W-C-N systems but, in general, consist of different mixtures of binary carbides, nitrides and carbonitrides [3,6,9]. The microstructures of these materials are quite complex including several variants of the “so-called” core-rim structures. This term applies to the ceramic phase, in which grains have a core (α’ phase) whose composition is very different from the surrounding shell (α’’ phase). The last works published on TiWCN-Ni alloys are focused on the behaviour of ultrafine Ti(C,N) powders [10-13],

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  • 18th

    Plansee Seminar HM 7/1

    Precipitation of M7C3 Carbides During Sintering of TiCN-WC-Ni-Co-Cr

    Alloys Used in Hot Rolling Applications

    I. Iparraguirre*, N. Rodriguez*, F. Ibarreta**, R. Martinez**,

    J.M. Sanchez*

    * CEIT and TECNUN, Paseo Manuel de Lardizbal 15, 20018, San Sebastin, Gipuzkoa, Basque

    Country, Spain.

    ** FMD CARBIDE S.A.L., Zorrozaurre 35, 48014, Bilbao, Spain.

    Abstract

    The densification of TiCN-WC-Cr-Ni cermets has been analysed by means of dilatometry and

    calorimetry. Shrinkage phenomena, both in solid and liquid phase, are enhanced by the Cr additions.

    Carbothermal reduction of oxides is observed to occur at much lower temperatures for high Cr contents.

    The dissolution of the different additives used in the powder mixtures and the rim formation also depend

    on the amount of Cr added. Thus, TiC and WC dissolution occurs at lower temperatures as the Cr

    content increases. In all cases the rim formation requires the presence of a liquid phase.

    Keywords

    WC

    Introduction

    Recently, the interest in Ti(C,N) based cermets is increasing due to the dramatic rise of tungsten prices

    [1]. These alloys are candidates for substitution of cemented carbides in a variety of tribological

    applications due to their excellent combination of high hot hardness, fracture strength, oxidation

    resistance and thermal conductivity [2-6]. Among these cermets, those with higher metallic contents (>

    25 vol.%) are the less studied. These compositions are less dense than steel and, for this reason, are

    typically used for the fabrication of components working under high inertial loads (i.e. roller guides in hot

    rolling mills). Apart from Ferro-TiC type materials [7,8], TiMoCN-Ni and TiWCN-Ni cermets are typical

    examples of these alloys [6,9-12], which are obtained by liquid phase sintering of a variety of powder

    mixtures. In some cases, the carbonitride powders are homogeneous solid solutions within the Ti-Mo-C-

    N and Ti-W-C-N systems but, in general, consist of different mixtures of binary carbides, nitrides and

    carbonitrides [3,6,9]. The microstructures of these materials are quite complex including several variants

    of the so-called core-rim structures. This term applies to the ceramic phase, in which grains have a

    core ( phase) whose composition is very different from the surrounding shell ( phase). The last works

    published on TiWCN-Ni alloys are focused on the behaviour of ultrafine Ti(C,N) powders [10-13],

  • 18th

    Plansee Seminar HM 7/2

    particularly, on the dissolution kinetics of WC additions and their effect on the composition of inner and

    outer rims. Apart from the properties described above, corrosion resistance is also critical for certain

    applications, especially when refrigerating fluids are used [14,15]. In such cases, a higher amount of

    chromium is added to the composition of the powder mixtures. The present work is aimed at analysing

    the effect of these Cr additions on the shrinkage, the liquid formation and the microstructural evolution of

    TiWCN-Ni cermets during sintering, since, so far, no reliable data have been published on this matter.

    Experimental

    The compositions of the powder mixtures, given in Table 1, were designed to have a constant Ni content

    (35 wt.%). Cr and W were added as Cr3C2 and WC carbides respectively. Nitrogen was introduced in the

    mixtures as Ti(C0.7N0.3) carbonitride powder and the C/N ratios were selected to be between 3.3 and

    3.8 to ensure a good sintering behaviour. This was adjusted by using TiC powder additions.

    Table 1: Composition of powder mixtures

    Elem.

    Ref.

    C1 C2 C3 C4 C5

    Cr3C

    2 0,0 2,2 4,6 9,0 17,3

    Ni 35,5 35,5 35,4 35,0 35,3

    WC 12,1 12,1 12,1 11,9 10,8

    Ti(C0,7

    N0,3

    ) 38,4 36,5 37,2 37,2 31,7

    TiC 14,0 13,8 10,7 6,9 5,0

    Mixing/milling was carried out in planetary equipment for 7 hours in hexane with 3.5 wt% addition of

    paraffin as organic binder. Afterwards, the powders were dried for 1 h. at atmospheric pressure in a

    thermostatic bath (90+/-2C).Green compacts were obtained by double action pressing at 160 MPa.

    Presintering was carried out in pure hydrogen using a tubular metallic furnace made from an AISI 314

    stainless steel (containing 25.0 wt % Cr) on alumina coated graphite trays. Two presintering

    temperatures where used for fine tuning of the C content: 450C and 650C. A constant heating rate of

    5C/min and a dwelling time of 35 min was used in all cases. The sinterability and mass losses of the

    different powder mixtures was analysed by combining dilatometry (Netszch TA) and thermogravimetry

    /calorimetry tests (TGA/DSC Setaram Setsys Evolution 16/18). These experiments were carried out on 5

    mm high and 5 mm in diameter cylinders using a heating rate of 10C/min up to 1450C (10-1 mbar).

    The onset of DSC and shrinkage rate peaks was determined by using the SETSOFT software [16].

    Sintering was carried out in a conventional graphite furnace with a heating ramp of 10C/min up to

    1300C. The vacuum level used during this step was 10-4 mbar [17]. Above this temperature, the

    pressure was increased up to 100 mbar by including argon in the furnace chamber and maintained

    during the sintering plateau for 1 h. Three sintering temperatures were investigated: 1100C, 1300C and

    1425C in order to analyse the dissolution process of each additive used in the mixtures. The C and N

    contents were measured by means of non dispersive infrared spectrometry and thermal conductivity

    methods respectively. Oxygen was measured by following DIN ISO 4491, placing the sample in a

    graphite crucible and heating in argon up to 1900C. The amount of oxygen is determined by measuring

  • 18th

    Plansee Seminar HM 7/3

    the CO content with an appropriate sensor. Standard ISO 3369 was used for density measurements

    using ethylic alcohol instead of distilled water. The accuracy of this method is about 0.5%. The sintered

    specimens were ground and polished down to 1 m diamond paste for microstructural analysis, which

    was carried out by optical and scanning electron microscopy (FEG-SEM) and energy dispersive X-ray

    spectroscopy (EDS). Phase identification was carried out by X-Ray diffraction (XRD) (with Ni-filtered

    CuK radiation).

    Results and Discussion

    The samples sintered at 1450C-1 h are fully dense. Differences in the absolute values are due to their

    different composition (theoretical values range from 6.6 g/cm3 for composition C1 to 6.9 g/cm3 for

    composition C5) (Fig. 1).

    (a) (b)

    Figure 1: ensification vs. sintering temperatures of samples presintered at (a) 450C and (b) 650C.

    The compositions with chromium contents ranging from 0 wt.% to 4 wt.% exhibit a similar behaviour with

    very limited densification after 1 hour at 1300C and strong shrinkage at 1425C. The materials with

    higher Cr content show much higher densities at 1300C reaching almost full density in the case of

    composition C5 (15 wt.%Cr). The densification of materials presintered at 450C (i.e. with higher C

    activity) is slightly improved at temperatures of 1300C and below. However, this effect is lost when the

    Cr content or the sintering temperature increase.

    Dilatometric experiments confirm that shrinkage in TiCN-WC-Ni-Cr alloys starts at temperatures 20C to

    50C lower as the C activity increases (i.e. for samples presintered at lower temperatures). In addition,

    shrinkage rate peaks are wider for materials presinter at lower temperature (Fig. 2).

    3.5

    4

    4.5

    5

    5.5

    6

    6.5

    7

    1150 1200 1250 1300 1350 1400 1450

    Ge

    om

    . D

    en

    s.

    (g/c

    m3

    )

    Temperature (C)

    C1

    C2

    C3

    C4

    C5

    450C

    3.5

    4

    4.5

    5

    5.5

    6

    6.5

    7

    1150 1200 1250 1300 1350 1400 1450

    Ge

    om

    . D

    en

    s.

    (g/c

    m3

    )

    Temperature (C)

    C1

    C2

    C3

    C4

    C5

    650C

  • 18th

    Plansee Seminar HM 7/4

    (a) (b)

    Figure 2: Dilatometric graphs of samples presintered at (a) 450C and (b) 650C.

    Melting temperatures obtained by DSC are clearly correlated with shrinkage events (Table. 2).

    Table 2: Temperatures corresponding to the melting phenomena found in DSC experiments

    2nd melting event 1st melting event

    Onset Point Peak Onset Point Peak

    Pre 450 Pre 650 Pre 450 Pre 650 Pre 450 Pre 650 Pre 450 Pre 650

    C1 1352 1360 1377 1383

    C2 1336 1346 1366 1371

    C3 1321 1334 1351 1362

    C4 1285 1307 1314 1334 1230 1245 1244 1254

    C5

    1235 1236 1264 1265

    Compostion C1 to C3 (0 wt.% to 4 wt.% Cr) exhibit only one endothermic peak, which moves to lower

    temperatures as the Cr and/or C activities increase. Compositions C4 presents two melting events: one

    following the trend explained above and another one at lower temperature. As said before, in general,

    the eutectic temperatures are reduced as the C activity increases, except for composition C5 which

    shows no significant change.

    Data published for the Ti-W-C-Ni system [18] are consistent with the second melting event in Table 2.

    However the 1st peak has not been described before. A similar behaviour is described for the W-C-Co-Cr

    system [19], in which Cr additions also depress the melting point of these alloys. However, the best

    correspondance is found with the eutectic described in the 15 wt.% isopleth section of the Cr-Ni-Cr

    system which occurs at 1249C. These results suggest that the high solubility of WC and Cr3C2 additions

    in the Ni phase are the key for explaining first melting phenomena in these alloys.

    A summary of XRD analyses of materials sintered at different temperatures is included in Fig. 3.

    -5000

    -4000

    -3000

    -2000

    -1000

    0

    1100 1200 1300 1400

    d(D

    L/L

    0)d

    t (x

    10

    -3)

    Temperature (C)

    C1C2C3C4C5

    450C

    -5000

    -4000

    -3000

    -2000

    -1000

    0

    1100 1200 1300 1400

    d(D

    L/L

    0)d

    t (x

    10

    -3)

    Temperature (C)

    C1C2C3C4C5

    650C

  • 18th

    Plansee Seminar HM 7/5

    Figure 3: Phases detected by XRD in samples of compositions C1, C3 and C5 sintered at different temperatures.

    TiC additions are fully dissolved in the three compositions at 1300C but not at 1150C, whereas WC

    and Cr3C2 are already dissolved at 1150C. M7C3 carbides are detected by XRD only in composition C5

    with (with 17.3 wt.% Cr3C2 additions).

    SEM images confirm that M7C3 carbides are also present in composition C4 (9.0 wt.% Cr3C2), although

    its precipitation is incipient yet (Fig. 4). Therefore, its volume fraction is below the resolution limit of XRD

    analyses.

    (a) (b)

    Figure 4: FEG-SEM images of samples presintered at 450C and sintered at 1425C-1 h (a) Alloy C4 and (b) Alloy C5. Blue

    arrows point to M7C3 crystals in each case

    Mass losses during sintering increase with the Cr content of the alloys and are higher for materials with

    higher C content (Fig. 5). This result indicates that both Cr and C play a significant role on the reduction

    of powder oxides.

  • 18th

    Plansee Seminar HM 7/6

    Figure 5: Mass change (%) after sintering for two different presintering conditions: 450C and 650C.

    These results are interesting if compared with mass loss rates (Fig. 6).

    (a) (b)

    Figure 6: Mass loss rates of samples presintered at (a) 450C and (b) 650C. (Calculated from TGA data)

    These data show that mass losses stabilises at lower temperatures as the Cr content increases,

    confirming that carbothermal reduction of oxides is strongly enhanced by increasing Cr3C2 additions.

    This is clearly observed by measuring C losses as a function of the Cr content of the alloys (Fig. 7a). Up

    to 4wt.%Cr, C losses clearly increase with the Cr content of the alloys. For higher Cr contents losses

    tend to stabilise. Analysing oxygen contents, it is clear that deoxydation is more effective under high

    carbon activities. This can be adjusted with high precision by controlling the presintering temperature

    (Fig. 7b).

    -1.3

    -1.2

    -1.1

    -1

    -0.9

    -0.8

    0 5 10 15 20

    Ma

    ss

    va

    ria

    tio

    n

    ( %

    )

    Cr content (wt %)

    Pre 450C

    Pre 650C

    -0.005

    -0.004

    -0.003

    -0.002

    -0.001

    0.000

    600 800 1000 1200 1400

    d (

    m/m

    0)/

    dT

    Temperature (C)

    C1

    C2

    C3

    C4

    C5

    -0.005

    -0.004

    -0.003

    -0.002

    -0.001

    0.000

    600 800 1000 1200 1400

    d (

    m/m

    0)/

    dT

    Temperature (C)

    C1

    C2

    C3

    C4

    C5

  • 18th

    Plansee Seminar HM 7/7

    (a) (b)

    Figure 7: C and O losses after sintering for different presintering conditions

    (a) (b) (c)

    Figure 8: FEG-SEM images of samples of composition C4 presintered at 650C and sintered at: (a) 1150C-1h, (b) 1300C-1h

    and (c) 1425C-1h. Blue arrows point to M7C3 carbides.

    (a) (b) (c)

    Figure 9: FEG-SEM images of samples of composition C5 presintered at 650C and sintered at: (a) 1150C-1h, (b) 1300C-1h

    and (c) 1425C-1h. Blue arrows point to M7C3 carbides.

    SEM images (Figs. 8 and 9) show that dissolution reprecipitation phenomena are quite complex. At

    1150C, significant differences are found between compositions C4 and C5. Densification is clearly

    enhanced by Cr additions, although at this low temperature dissolution of WC and Cr3C2 particles is not

    completed (Figs. 8a and 9a). It has to be remembered that these rests are not detected by XRD (Fig. 3).

    At 1300C, high densification is found in both specimens. Cr rich M7C3 carbides are already detected in

    composition C5 but not in C4 (compare Fig.8b and 9b). Another difference between these two alloys is

    that in C4 grain growth has been less active with a large fraction of W rich nanometric grains (in light

    10

    12

    14

    16

    18

    0 5 10 15

    -C

    /C (%

    )

    Cr content (wt. %)

    Pre 650

    Pre 450

    60

    70

    80

    90

    0 5 10 15

    -O

    /O (%

    )

    Cr content (wt. %)

    Pre 650C

    Pre 450C

  • 18th

    Plansee Seminar HM 7/8

    contrast in Fig. 8b) already undissolved. In C5 these phases have dissappeared and ceramic grains are

    coarser. On the other hand, at 1300C, incipient rim formation is observed in some carbonitride grains in

    sample C4, but not in C5. Therefore, it seems that Ti-W-Cr-C rim formation and M7C3 precipitation are

    interacting with each other. This is clearly observed by comparing the microstructures obtained at

    1425C-1 h. In alloy C4, many carbonitride grains have an inner rim surrounded by the M7C3 phase,

    whereas in alloy C5, such configuration is rarely found.

    Conclusion

    Melting in TiCN-W-Ni-Cr alloys occurs at lower temperatures as the Cr content increases. Melting

    temperatures are compatible with those found in (Ti,W)C-Ni and Cr-C-Ni systems. In these cermets,

    shrinkage always precedes melting. In some cases, densification occurs mainly by solid state sintering,

    whereas in others a combination of solid state sintering and liquid phase sintering is observed. The

    dissolution of these carbides increases the C activity in the binder phase promoting the reduction of Ni

    oxides. Carbothermal reduction of oxides leads to higher mass losses and gas emission stop at lower

    temperatures as the Cr content increases

    M7C3 precipitation in TiCN-W-Ni-Cr alloys is detected at and above 8wt.% Cr contents. This

    phenomenon is activated by the presence of a liquid phase suggesting that is a dissolution

    reprecipitation process. Therefore, there is a complex interaction with the rim formation in these alloys

    that needs to be analysed in deeper detail.

    Acknowledgements

    The Gobierno Vasco via GAITEK programme is gratefully acknowledged for the finantial support of this

    work.

    References

    1. Critical raw materials for the EU, Raw Material Supply Group, European Commission, Entreprise

    and Industry, July (2010).

    2. Rudy E. US Patent 3,971,656; (1976).

    3. Doi H. In: Almond E A, Brookes C A, Warren R, editors. Proc of Int Conference of Science of Hard

    Materials. Inst Phys Conf Ser No 75, Bristol and Boston: Adam Hilger Ltd; 1986, 489-523.

    4. Suzuki H, Matsubara H. J Japan Soc Powder Powder Metall (1983); 30:257.

    5. Pastor H. Mater Sci Eng A105/106, (1988); 401-9.

    6. Exner H E. In: Viswanadham RK, Rowcliffe DJ, Gurland J, editors. Proc of the Int Conf on the Science

    of Hard Materials, New York and London: Plenum Press; (1983), 233-62.

    7. Das K, Bandyopadhyay TK, Das S, J. Mater. Sci., 37, (2002), 388192.

    8. Degnan CC, Shipway PH, Wear, 252, (2002), 83241.

    9. Ettmayer P, Kolaska H, K. Dreyer, pmi vol. 23, no.4, (1991), 224-30.

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    Plansee Seminar HM 7/9

    10. Jung J, Kang S, Acta Mat., 52, (2004), 1379-86.

    11. Ahn SY, Kang S, J. Am. Ceram. Soc., 83, 6, (2000),1489-94.

    12. Park S, Kang S, Scripta Mat., 52, (2005), 129-33.

    13. Demoly A, Lengauer W, Veitsch C, Rabitsch K, Int. J. Refract. Met. and Hard Mat., 29 (2011) 716

    723

    14. Oakes JJ, Met. Powd. Rep.,42(7-8), 492-499, (1987)

    15. Wan W, Xiong J, Yang M, Guo Z, Dong G, Yi C, Int. J. Refract. Met. and Hard Mat., 31, 179186,

    (2012)

    16. SETARAM Instrumentation. Setsys evolution 16/18. SETSOFT user manual, 39 (2002)

    17. I. Iparraguirre, M. Aristizabal, N. Rodriguez, F. Ibarreta, R. Martinez and J.M. Sanchez, Proc. of

    Euro PM2011, Vol.1 PM Tool Materials, Session 17: 160, Barcelona (2011)

    18. Chen L, Lengauer W, Ettmayer P, Dreyer K, Daub HW, Kassel D, Int. J. Refract. Met. and Hard

    Mat., 18, 307-22, (2000)

    19. Frisk K. 17th Plansee Seminar, Int. Conf. on High Performance P/M materials; Proc. Vol. 2, HM 1: 1-

    10. (2009)