<p>This study explores the combined effects of strain-rate and temperature on the compressive behavior and microstructural evolution of Ti–15Mo (wt pct) over a temperature range of <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11661_2025_7860_Article_IEq4.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="28" /> </InlineMediaObject> <EquationSource Format="TEX">\(25\,^{\circ }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>25</mn> <mmultiscripts> <mspace width="0.166667em" /> <mrow /> <mo>∘</mo> </mmultiscripts> </mrow> </math></EquationSource> </InlineEquation>C to <InlineEquation ID="IEq5"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11661_2025_7860_Article_IEq5.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="36" /> </InlineMediaObject> <EquationSource Format="TEX">\(450\,^{\circ }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>450</mn> <mmultiscripts> <mspace width="0.166667em" /> <mrow /> <mo>∘</mo> </mmultiscripts> </mrow> </math></EquationSource> </InlineEquation>C and strain-rates from <InlineEquation ID="IEq6"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11661_2025_7860_Article_IEq6.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="74" /> </InlineMediaObject> <EquationSource Format="TEX">\(1.1 \times 10^{-3}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1.1</mn> <mo>×</mo> <msup> <mn>10</mn> <mrow> <mo>-</mo> <mn>3</mn> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> to <InlineEquation ID="IEq7"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11661_2025_7860_Article_IEq7.gif" Format="GIF" Height="17" Rendition="HTML" Resolution="72" Type="Linedraw" Width="90" /> </InlineMediaObject> <EquationSource Format="TEX">\(3.2\times 10^{3}\,{\hbox {s}}^{-1}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>3.2</mn> <mo>×</mo> <msup> <mn>10</mn> <mn>3</mn> </msup> <mspace width="0.166667em" /> <msup> <mrow> <mtext>s</mtext> </mrow> <mrow> <mo>-</mo> <mn>1</mn> </mrow> </msup> </mrow> </math></EquationSource> </InlineEquation> using a high-temperature Kolsky system. The results show that yield strength (YS) increases with strain-rate but generally decreases with temperature. Work hardening rate (WHR) is higher under quasi-static loading, with dynamic Hall–Petch effect driven by 332 <InlineEquation ID="IEq8"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11661_2025_7860_Article_IEq8.gif" Format="GIF" Height="19" Rendition="HTML" Resolution="72" Type="Linedraw" Width="43" /> </InlineMediaObject> <EquationSource Format="TEX">\(\langle 113 \rangle \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">⟨</mo> <mn>113</mn> <mo stretchy="false">⟩</mo> </mrow> </math></EquationSource> </InlineEquation> twin formation at low temperatures. As temperature rises, dislocation recovery suppresses this effect, leading to a decrease in WHR. At <InlineEquation ID="IEq9"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11661_2025_7860_Article_IEq5.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="36" /> </InlineMediaObject> <EquationSource Format="TEX">\(450\,^{\circ }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>450</mn> <mmultiscripts> <mspace width="0.166667em" /> <mrow /> <mo>∘</mo> </mmultiscripts> </mrow> </math></EquationSource> </InlineEquation>C under quasi-static loading, <InlineEquation ID="IEq10"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11661_2025_7860_Article_IEq10.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="14" /> </InlineMediaObject> <EquationSource Format="TEX">\(\omega \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>ω</mi> </math></EquationSource> </InlineEquation> precipitate strengthening causes an increase in both YS and WHR. These differences are influenced by a shift in the dominant deformation mechanism, which is affected by both temperature and strain-rate. Twinning dominates at high strain-rates across all temperatures, but the amount of twinning decreases with increasing temperature. In contrast, under quasi-static loading, the primary mechanism shifts from twinning to slip as temperature increases. The capacity for energy absorption is greater under high rate loading up to <InlineEquation ID="IEq11"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11661_2025_7860_Article_IEq5.gif" Format="GIF" Height="14" Rendition="HTML" Resolution="72" Type="Linedraw" Width="36" /> </InlineMediaObject> <EquationSource Format="TEX">\(450\,^{\circ }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>450</mn> <mmultiscripts> <mspace width="0.166667em" /> <mrow /> <mo>∘</mo> </mmultiscripts> </mrow> </math></EquationSource> </InlineEquation>C, at which point precipitate strengthening increases WHR under quasi-static loading.</p>

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The Dynamic Compressive Response of the Metastable \(\beta \) TWIP Alloy, Ti–15Mo (Wt Pct), at Elevated Temperatures

  • Emily Pittman,
  • Amy Clarke,
  • Leslie Lamberson

摘要

This study explores the combined effects of strain-rate and temperature on the compressive behavior and microstructural evolution of Ti–15Mo (wt pct) over a temperature range of \(25\,^{\circ }\) 25 C to \(450\,^{\circ }\) 450 C and strain-rates from \(1.1 \times 10^{-3}\) 1.1 × 10 - 3 to \(3.2\times 10^{3}\,{\hbox {s}}^{-1}\) 3.2 × 10 3 s - 1 using a high-temperature Kolsky system. The results show that yield strength (YS) increases with strain-rate but generally decreases with temperature. Work hardening rate (WHR) is higher under quasi-static loading, with dynamic Hall–Petch effect driven by 332 \(\langle 113 \rangle \) 113 twin formation at low temperatures. As temperature rises, dislocation recovery suppresses this effect, leading to a decrease in WHR. At \(450\,^{\circ }\) 450 C under quasi-static loading, \(\omega \) ω precipitate strengthening causes an increase in both YS and WHR. These differences are influenced by a shift in the dominant deformation mechanism, which is affected by both temperature and strain-rate. Twinning dominates at high strain-rates across all temperatures, but the amount of twinning decreases with increasing temperature. In contrast, under quasi-static loading, the primary mechanism shifts from twinning to slip as temperature increases. The capacity for energy absorption is greater under high rate loading up to \(450\,^{\circ }\) 450 C, at which point precipitate strengthening increases WHR under quasi-static loading.