KnE Engineering | XIX International scientific-technical conference “The Ural school-seminar of metal scientists-young researchers” | pages: 121–127

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1. Introduction

An increase in working pressure as a result of using high-strength steels is one of the most promising ways of increasing the economic efficiency of main gas pipelines located in complex climatic conditions. The obvious advantage of using high-strength pipes is a reduction in metal content (pipe wall thickness). The breakthrough in improvement of structural strength of low-alloy pipe steels occurred in the middle of the 1970s in view of the development and introduction into industrial production of thermomechanical controlled processing (TMCP) combining controlled rolling and subsequent controlled cooling [1–3].

Research in recent years has shown that a feature of bainitic steels of strength classes X70 and X80 is the critical role of formation within a fracture (during tensile, impact bending, static crack resistance tests) of secondary cracks, i.e., separations, propagating perpendicular to the main crack plane. It is important to note that separations are observed in contemporary large diameter pipes with ductile crack propagation [4,5]. On the example of contemporary pipe steels with low contamination by inclusions and quite uniform microstructure, it has been demonstrated that cleavages are caused by features of microstructure formed during sheet treatment [4,5], which determines their strict orientation along the rolling direction (RD). In [6], reasons for forming cleavages in high-strength pipe steels with a bainitic structure, low content of carbon and harmful impurities are also connected with preferred crystallographic texture. In the destruction of pipe steel sheets, an important role is played not by the integral texture but by a single weak component (001)[110], as shown in [7–10]. Crack development depends on the presence of extended regions with consistent orientation over a distance exceeding the critical crack size.

In the present work, we investigate the formation of structural and textural states (bainite, ferrite) in sheets of low-carbon, low-alloy pipe steel obtained by TMCP depending on isothermal hot rolling temperatures.

2. Research Methods

We investigate sheet samples (depth 27 mm) of 06Г2MБ low-carbon, low-alloy pipe steel, containing 0.06 wt % C, 1.7 wt % Mn, 0.05 wt % Nb, and 0.05 wt % Mo, (The remainder is Fe and unavoidable impurities). The isothermal hot rolling temperatures (T iHR ) of steel sheets made up 840 C (State I) and 760 C (State II).

Calculations of phase thermodynamic equilibria were carried out using ThermoCalc software. The calculated steel A c3 was equal to 830 C.

The TMCP steel sheets were cut along the RD for mechanical testing. Tests have demonstrated a marked difference between modes I and II (Table 1).

Table 1

Mechanical properties of the samples of low-carbon low-alloy steels.


State T iHR , [ C] Yield strength, [MPa] Tensile strength, [MPa] δ 5 , [%] KCV -60 , [J/cm 2 ] KCV -40 , [J/cm 2 ] Tendency to cleavage
I 840 550-560 610-630 23.5 380–400 350–380 not observed
II 760 530-550 590-610 24.5 360–380 300–340 observed

Metallographic sections are prepared from the steel samples in plane defined by the direction of rolling in TMCP and the normal to the rolling plane. The sample structure is investigated electron microscopically by means of a ZEISS CrossBeam AURIGA scanning microscope (with an accelerating voltage of 20 kV). To determine the orientation of individual grains and analyze the local texture, we use an EBSD HKL Inca attachment with an Oxford Instruments analytical system. The scanning increment is 0.1 μm. The error in determining the lattice orientation is no more than ± 1 ( ± 0.6 on average). Small angle boundaries between the local volumes are plotted on orientation charts when the disorientations are 2–7 and 8–15 ; the boundary thickness in the graphics is 1 and 2 pixel. Large-angle boundaries between the local volumes are plotted on orientation charts when the disorientation exceeds 15 ; the boundary thickness in the graphics is 3 pixels. The texture is investigated by plotting orientation distribution functions (ODF). Analysis of the special boundaries between individual grains involves plotting such boundaries on orientation charts, in the light of the standard Brandon criterion ± ΔΘ in the software. For each boundary, ΔΘ = 15 /Σn) 1/2 , where Σn is the number of coinciding points when three dimensional crystal lattices are superimposed.

In orientation analysis, the laboratory system adopted is the coordinate system whose axes are, respectively, parallel to the direction of hot rolling (DR) in TMCP (X ||DR), to the normal (ND) to the rolling plane (Y||ND), and to the perpendicular direction (PD) that runs along the roller axis (Z||PD). Accordingly, these three directions form a right triad of vectors.

3. Results and Discussion

In the samples I with bainite structure after TMCP (Fig. 1, a), we observe extended regions that run in the direction of rolling (thickness 5–35 μm). These regions correspond to austenite grains deformed by controlled rolling. They have taken on bainite structure as a result of γ α transition. Presumably, the dimensions of the regions corresponding to the initial austenite grains are retained on account of the formation of disperse carbides at the boundaries in hot deformation [1]. In the samples II after TMCP (Fig. 1, b), we observe extended regions with practically parallel boundaries that run in the direction of rolling (thickness 5–25 μm). Elongated ferrite phase grains (thickness to 5 μm) were observed in the samples II after TMCP along the boundaries of the initial deformed γ-grains (Fig. 2, b). This ferrite can be identified as high temperature α-phase existed in steel by isothermal hot rolling. Some α-grains were fragmented. They had time recrystallization.

fig-1.jpg
Figure 1
The microstructure of the steel in the TMCP states in the form of orientation maps (EBSD) – band contrast and intercrystalline boundaries: a, c, e – I-840 state; b, d, f – II-760 state; c, d – distribution of intercrystalline boundaries; e, f – distribution of CSL boundaries.
fig-2.jpg
Figure 2
The microstructure of the steel in the TMCP states (image in backscattered electrons): a – I-840; b – II-760.

All large-angle boundaries are concentrated with disorientations of 49–60 (Fig. 1, c, d). In the spectra of special boundaries observed in all structures, boundaries of the coincidence site lattices (CSL): Σ3, Σ11, Σ17b, Σ25b, Σ33c, and Σ41c are the most strongly expressed (Fig. 1, e, f). This spectrum is the result of shear phase transformation, in accordance with orientation relations intermediate between the Kurdjumov–Sachs and Nishiyama–Wasserman types, as shown in [11]. Such spectra of special boundaries are also seen in the martensite of low-carbon pipe steel [12,13].

EBSD data show that the texture of all the samples consists mainly of the same scattered components: very strong (001)[110] orientations, two { 112 } 110 orientations, and two { 110 }< 223 > (Fig. 3). In the samples II the (001)[110] orientation and the { 112 }< 110 > orientations expressed more strongly (Fig. 3, c, е). The main orientations correspond to relatively uniform regions consisting of crystallites separated by small-angle boundaries.

The applied orientational EBSD technique allowed to define the structurally ferrite in the samples II and analyze the texture. All indicated orientations of the ferrite formed at hot rolling, namely: { 001 }< 110 > , { 11k }< 110 > , are stable deformation orientations of the BCC lattice [14]. It should be noted that, taking into account the crystal-geometric characteristics of structurally ferrite (orientation, shape and size of grains), it can be considered as a kind of "macro defect". Propagation of longitudinal cracks will be predetermined in the crystallographic planes { 001 } of elongated ferrite grains [7,10].

Obviously, the elongated ferritic grains formed during isothermal hot rolling at temperatures below A c3 . It is also obvious that they are the cause of reduction in mechanical properties.

fig-3.jpg
Figure 3
The texture of the steel in the TMCP I-840 (a, b) and II-760 states (c, d) as ODF sections: a, c, e – sections φ 2 = 0 ∘ ; b, d, f – sections φ 2 = 45 ∘ ; e, f – schematic orientations from the direction perpendicular to the RD-ND plane.

4. Summary

The formation of cleavages the destruction of low-carbon low-alloy steel pipe with a bainitic structure obtained controlled thermo-mechanical treatment, due to the presence in the material of the crystallographic texture components (001)[110] and { 11k }< 110 > . The elongated ferritic grains the region with uniform orientation of the (001) < 110 > and { 11k }< 110 > formed during isothermal hot rolling by TMCP at temperatures below A c3 .

Acknowledgements

The work was carried out using the laboratory equipment "Structural methods of analysis and properties of materials and nanomaterials" of the Center of Ural Federal University. The work has been carried with the support of the Russian Science Foundation, grant No. 19-79-20006. Authors are grateful for the assistance the program of support for leading universities in Russian Federation for improvement of their competitiveness №211 of the Government №02.A03.21.0006. The authors thank MMK company for support and assistance in organizing the study.

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