<p>HAYNES<sup>®</sup> 244<sup>®</sup> alloy is a high-strength, low coefficient of thermal expansion (CTE) Ni-based superalloy designed for use up to 760 <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(^{\circ }\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mo>∘</mo> </mmultiscripts> </math></EquationSource> </InlineEquation>C. This alloy offers an improvement in maximum temperature operation and mechanical properties such as tensile strength and creep life over the previous generation of low CTE alloy, HAYNES<sup>®</sup> 242<sup>®</sup>. Uniquely, it is strengthened through a body-centered orthorhombic (BCO) intermetallic phase, <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\gamma ^{\prime \prime \prime }\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>γ</mi> <mrow> <mo>″</mo> <mo>′</mo> </mrow> </msup> </math></EquationSource> </InlineEquation>, a Ni<InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mn>2</mn> <mrow /> </mmultiscripts> </math></EquationSource> </InlineEquation>(Cr,Mo,W) precipitate. The additions of tungsten in the 244 alloy improve the thermal stability of the strengthening domains, compared to the 242 alloy, impeding diffusional effects of dislocation motion at elevated temperatures. To probe the possible deformation mechanisms that occur during high-temperature creep, creep testing in the vicinity of the <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\gamma ^{\prime \prime \prime }\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>γ</mi> <mrow> <mo>″</mo> <mo>′</mo> </mrow> </msup> </math></EquationSource> </InlineEquation> solvus was conducted to understand the interplay of <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\gamma ^{\prime \prime \prime }\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>γ</mi> <mrow> <mo>″</mo> <mo>′</mo> </mrow> </msup> </math></EquationSource> </InlineEquation> phase stability, precipitation of the <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\mu \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>μ</mi> </math></EquationSource> </InlineEquation> phase above 760 <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(^{\circ }\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mo>∘</mo> </mmultiscripts> </math></EquationSource> </InlineEquation>C, and the active creep deformation mechanisms. These mechanisms change from deformation twinning at the lower tested temperatures, to perfect dislocation shearing and noticeable grain boundary dislocation pile-up after the <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\gamma ^{\prime \prime \prime }\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>γ</mi> <mrow> <mo>″</mo> <mo>′</mo> </mrow> </msup> </math></EquationSource> </InlineEquation> has completely dissolved. During the intermediate temperature testing near the solvus, but where the <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\gamma ^{\prime \prime \prime }\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mi>γ</mi> <mrow> <mo>″</mo> <mo>′</mo> </mrow> </msup> </math></EquationSource> </InlineEquation> phase still remains in low volume fractions, a mixed twinning and dislocation shearing mechanism was observed. This manuscript elucidates the implications of mixed character creep deformation during high-temperature testing.</p>

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Dissolution and Creep Deformation Behavior Near the Solvus Temperature of the \(\gamma ^{\prime \prime \prime }\)-Ni\(_2\)(Cr,Mo,W) Phase in HAYNES® 244®

  • Victoria Tucker,
  • Thomas R. Mann,
  • Ian Bowley,
  • Michael S. Titus

摘要

HAYNES® 244® alloy is a high-strength, low coefficient of thermal expansion (CTE) Ni-based superalloy designed for use up to 760 \(^{\circ }\) C. This alloy offers an improvement in maximum temperature operation and mechanical properties such as tensile strength and creep life over the previous generation of low CTE alloy, HAYNES® 242®. Uniquely, it is strengthened through a body-centered orthorhombic (BCO) intermetallic phase, \(\gamma ^{\prime \prime \prime }\) γ , a Ni \(_{2}\) 2 (Cr,Mo,W) precipitate. The additions of tungsten in the 244 alloy improve the thermal stability of the strengthening domains, compared to the 242 alloy, impeding diffusional effects of dislocation motion at elevated temperatures. To probe the possible deformation mechanisms that occur during high-temperature creep, creep testing in the vicinity of the \(\gamma ^{\prime \prime \prime }\) γ solvus was conducted to understand the interplay of \(\gamma ^{\prime \prime \prime }\) γ phase stability, precipitation of the \(\mu \) μ phase above 760 \(^{\circ }\) C, and the active creep deformation mechanisms. These mechanisms change from deformation twinning at the lower tested temperatures, to perfect dislocation shearing and noticeable grain boundary dislocation pile-up after the \(\gamma ^{\prime \prime \prime }\) γ has completely dissolved. During the intermediate temperature testing near the solvus, but where the \(\gamma ^{\prime \prime \prime }\) γ phase still remains in low volume fractions, a mixed twinning and dislocation shearing mechanism was observed. This manuscript elucidates the implications of mixed character creep deformation during high-temperature testing.