4.7 Article

Increasing the creep resistance of Fe-Ni-Al-Cr superalloys via Ti additions by optimizing the B2/L2(1) ratio in composite nano-precipitates

Journal

ACTA MATERIALIA
Volume 157, Issue -, Pages 142-154

Publisher

PERGAMON-ELSEVIER SCIENCE LTD
DOI: 10.1016/j.actamat.2018.07.025

Keywords

Ferritic alloy; Superalloy; High entropy alloy; Precipitate strengthening; Creep; Hardness; L2(1)-B2 phases; Composite (multi-phase) nano-precipitates

Funding

  1. U.S. Department of Energy (DoE), Office of Fossil Energy [DE-FE0005868]
  2. Soft and Hybrid Nanotechnology Experimental (SHyNE) Resource [NSF ECCS-1542205]
  3. MRSEC program at the Materials Research Center [NSF DMR-1121262, NSF DMR-1720139]
  4. International Institute for Nanotechnology (IIN)
  5. Keck Foundation
  6. State of Illinois, through the IIN

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The Fe-10Cr-10Ni-6.5Al-3.4Mo-0.25Zr-0.005B (wt.%) ferritic FBB8 superalloy shows good creep resistance due to the presence of B2-NiAl precipitates, created upon aging. When titanium is added to the alloy, L2(1)-Ni2TiAl sub-precipitates are developed within the B2-NiAl main precipitates. The micro structural evolutions of these B2/L2(1) composite precipitates - radius, number density, volume fraction, edge-edge distance, and B2/L2(1) phase fraction - are studied here for Ti additions spanning up to 4 wt%. As Ti increases from 0 to 3.5 wt%, the alloy strength at ambient temperature rises due to an increase of the L2(1) sub-precipitate volume fraction within the B2 precipitates, which enhances their lattice misfit with the matrix up to similar to 1.26%, and increases coherency strengthening. The alloy strength drops sharply for 4 wt % Ti, consistent with the precipitates losing (i) their composite structure (by becoming a fully L2(1) phase), (ii) their coherency with the matrix (and showing high dislocation density at their interfaces), and (iii) their coarsening resistance (increasing abruptly in size). Creep resistance at 700 degrees C follows a similar trend (raising from 0 to 3.5 wt% Ti and dropping sharply at 4 wt% Ti); this trend is consistent with the lattice misfit between the coherent B2/L2(1) precipitates and the matrix increasing with the L2(1) fraction, thus producing a stronger elastic stress field, which makes the climb bypass of the precipitates by the matrix dislocations more difficult. (C) 2018 Acta Materialia Inc. Published by Elsevier Ltd. All rights reserved.

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