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Materials Technology
Advanced Performance Materials
Volume 38, 2023 - Issue 1
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Research Article

Microstructure evolution and creep-rupture behaviour of a low-cost Fe-Ni-based superalloy

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Article: 2270865 | Received 05 Oct 2023, Accepted 10 Oct 2023, Published online: 23 Oct 2023

Figures & data

Figure 1. Schematic diagram of heat treatment.

Figure 1. Schematic diagram of heat treatment.

Table 1. The chemical composition of the fe-ni-based superalloy (wt.%).

Figure 2. SEM images showing the morphology of (a) carbides and (b) γ′ precipitates in the matrix.

Figure 2. SEM images showing the morphology of (a) carbides and (b) γ′ precipitates in the matrix.

Figure 3. Overall strain-creep (black line) and strain rate-creep time (red line) curves of the fe-ni-based superalloy under the creep conditions of (a) 750°C/130 MPa and (b) 700°C/200 MPa.

Figure 3. Overall strain-creep (black line) and strain rate-creep time (red line) curves of the fe-ni-based superalloy under the creep conditions of (a) 750°C/130 MPa and (b) 700°C/200 MPa.

Figure 4. Morphology of the carbides after creep test under the conditions of (a–c) 750°C/130 MPa and (d-f) 700°C/200 MPa.

Figure 4. Morphology of the carbides after creep test under the conditions of (a–c) 750°C/130 MPa and (d-f) 700°C/200 MPa.

Figure 5. The elemental mapping images of TiC and Cr23C6 carbides in the experimental alloy under the creep condition of 700°C/200 MPa.

Figure 5. The elemental mapping images of TiC and Cr23C6 carbides in the experimental alloy under the creep condition of 700°C/200 MPa.

Figure 6. SEM images showing the morphology of γ′ precipitates under the creep condition of (a) 750°C/130 MPa and (b) 700°C/200 MPa. (c) TEM bright-field image and corresponding (d) EDS elemental analysis results of the experimental alloy under the creep condition of 700°C/200 MPa.

Figure 6. SEM images showing the morphology of γ′ precipitates under the creep condition of (a) 750°C/130 MPa and (b) 700°C/200 MPa. (c) TEM bright-field image and corresponding (d) EDS elemental analysis results of the experimental alloy under the creep condition of 700°C/200 MPa.

Figure 7. SEM and EDS mapping images of PFZs/DCZs in samples after creep at (a, b) 750°C/130 MPa and (c, d) 700°C/200 MPa. (e) elemental mapping of the coarse precipitates in the sample crept at 700°C/200 MPa.

Figure 7. SEM and EDS mapping images of PFZs/DCZs in samples after creep at (a, b) 750°C/130 MPa and (c, d) 700°C/200 MPa. (e) elemental mapping of the coarse precipitates in the sample crept at 700°C/200 MPa.

Figure 8. SEM images showing the fracture morphology of the alloy under the creep conditions of (a, b) 750°C/130 MPa and (c, d) 700°C/200 MPa.

Figure 8. SEM images showing the fracture morphology of the alloy under the creep conditions of (a, b) 750°C/130 MPa and (c, d) 700°C/200 MPa.

Figure 9. EBSD analysis results of the alloy after creep at of 750°C/130 MPa and 700°C/200 MPa. (a, d) inverse pole figure (IPF), (b, e) kernel average misorientation (KAM) figure (red lines: low angle grain boundary (2°–15°); black lines: high angle grain boundary (>15°)), (c, f) coincidence site lattice (CSL) boundary figure, (g) strains calculated by KAM results, (h) the proportion of various coincidence site lattice (CSL) grain boundaries.

Figure 9. EBSD analysis results of the alloy after creep at of 750°C/130 MPa and 700°C/200 MPa. (a, d) inverse pole figure (IPF), (b, e) kernel average misorientation (KAM) figure (red lines: low angle grain boundary (2°–15°); black lines: high angle grain boundary (>15°)), (c, f) coincidence site lattice (CSL) boundary figure, (g) strains calculated by KAM results, (h) the proportion of various coincidence site lattice (CSL) grain boundaries.

Figure 10. TEM bright-field images showing the interaction between dislocations and γ′ particles when crept at (a) 750°C/130 MPa and (b) 700°C/200 MPa.

Figure 10. TEM bright-field images showing the interaction between dislocations and γ′ particles when crept at (a) 750°C/130 MPa and (b) 700°C/200 MPa.

Data availability statement

The raw/processed data required to reproduce these findings cannot be shared at this time as the data also forms part of an ongoing study