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首页> 外文期刊>Journal of Materials Science >Microstructure and elevated temperature properties of a refractory TaNbHfZrTi alloy
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Microstructure and elevated temperature properties of a refractory TaNbHfZrTi alloy

机译:TaNbHfZrTi难熔合金的显微组织和高温性能

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Compression properties of a refractory multi-component alloy, Ta _(20)Nb _(20)Hf _(20)Zr _(20)Ti _(20), were determined in the temperature range of 296-1473 K and strain rate range of 10 ~(-1)-10 ~(-5) s ~(-1). The properties were correlated with the microstructure developed during compression testing. The alloy was produced by vacuum arc melting, and it was hot isostatically pressed (HIPd) and homogenized at 1473 K for 24 h prior to testing. It had a single-phase body-centered cubic structure with the lattice parameter a = 340.4 pm. The grain size was in the range of 100-200 μm. During compression at a strain rate of ? = 10 ~(-3) s ~(-1), the alloy had the yield strength of 929 MPa at 296 K, 790 MPa at 673 K, 675 MPa at 873 K, 535 MPa at 1073 K, 295 MPa at 1273 K and 92 MPa at 1473 K. Continuous strain hardening and good ductility (ε ≥ 50%) were observed in the temperature range from 296 to 873 K. Deformation at T = 1073 K and ? ≥ 10 ~(-3) s ~(-1) was accompanied by intergranular cracking and cavitation, which was explained by insufficient dislocation and diffusion mobility to accommodate grain boundary sliding activated at this temperature. The intergranular cracking and cavitation disappeared with an increase in the deformation temperature to 1273 and 1473 K or a decrease in the strain rate to ~10 ~(-5) s ~(-1). At these high temperatures and/or low-strain rates the alloy deformed homogeneously and showed steady-state flow at a nearly constant flow stress. Partial dynamic recrystallization, leading to formation of fine equiaxed grains near grain boundaries, was observed in the specimens deformed at 1073 and 1273 K and completed dynamic recrystallization was observed at 1473 K.
机译:在296-1473 K的温度范围和应变率下确定了耐火多组分合金Ta _(20)Nb _(20)Hf _(20)Zr _(20)Ti _(20)的压缩性能范围为10〜(-1)-10〜(-5)s〜(-1)。这些性质与压缩测试过程中形成的微观结构相关。通过真空电弧熔化生产合金,并在测试前对其进行热等静压(HIPd)并在1473 K下均化24 h。它具有单相体心立方结构,其晶格参数a = 340.4 pm。晶粒尺寸在100-200μm的范围内。在压缩过程中,应变率为? = 10〜(-3)s〜(-1),合金在296 K时的屈服强度为929 MPa,在673 K时为790 MPa,在873 K时为675 MPa,在1073 K时为535 MPa,在1273 K时为295 MPa在1473 K时为92 MPa。在296至873 K的温度范围内观察到连续应变硬化和良好的延展性(ε≥50%)。在T = 1073 K和? ≥10〜(-3)s〜(-1)伴随着晶间裂纹和空化现象,这是由于位错和扩散迁移率不足以适应在该温度下激活的晶界滑动所致。随着变形温度升高至1273和1473 K或应变率降低至〜10〜(-5)s〜(-1),晶界裂纹和空化现象消失。在这些高温和/或低应变速率下,合金均匀变形,并在几乎恒定的流动应力下显示出稳态流动。在1073和1273 K下变形的样品中观察到部分动态再结晶,导致在晶界附近形成细等轴晶粒,并在1473 K下观察到完全动态再结晶。

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