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首页> 外文期刊>Kovove materialy >THE SPECTRUM OF RATE CONTROLLING DEFORMATION MECHANISMS OPERATING IN CREEP IN AN Al-8.5Fe-1.3V-1.7Si-l5SiC_p COMPOSITE AT TEMPERATURES RANGING FROM 623 TO 948 K
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THE SPECTRUM OF RATE CONTROLLING DEFORMATION MECHANISMS OPERATING IN CREEP IN AN Al-8.5Fe-1.3V-1.7Si-l5SiC_p COMPOSITE AT TEMPERATURES RANGING FROM 623 TO 948 K

机译:Al-8.5Fe-1.3V-1.7Si-l5SiC_p复合材料在623K至948K温度范围内蠕变时的速率控制形变机理的光谱

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摘要

Creep in an Al-8.5Fe-1.3V-1.7Si alloy reinforced with silicon carbide particulates - an Al-8.5Fe-1.3V-1.7Si-15SiC_p composite - is investigated at temperatures ranging from 623 to 948 K. At temperatures 623, 673 and 723 K the creep is associated with a true threshold stress decreasing with increasing temperature more strongly than the shear modulus of the composite matrix. The true activation energy of creep is close to the activation enthalpy of lattice diffusion in the composite matrix and the true stress exponent of minimum creep strain rate is close to 5. The creep is interpreted in terms of athermal detachment of dislocations from incoherent Al_(12)(Fe,V)_3Si phase particles in the matrix.At temperatures 773, 798 and 823 K the true threshold stress is not observed. The true stress exponent of minimum creep strain rate increases with increasing stress and the true activation energy of creep is higher than the activation enthalpy of lattice diffusion in the matrix. The creep is interpreted in terms of thermally activated detachment of dislocations from the incoherent Al_(12)(Fe,V)_3Si phase particles.At temperatures ranging from 873 to 948 K the true threshold stress reappears. However, its origin is different from that at temperatures 623-723 K. The true activation energy is close to the activation enthalpy of grain boundary diffusion and the true stress exponent of minimum creep strain rate is close to 2.5. The creep at these temperatures is interpreted in terms of superplastic flow.
机译:在623至948 K的温度范围内,研究了用碳化硅颗粒增强的Al-8.5Fe-1.3V-1.7Si合金(Al-8.5Fe-1.3V-1.7Si-15SiC_p复合材料)的蠕变。与复合基质的剪切模量相比,蠕变与真实阈值应力随温度升高而降低的趋势有关,蠕变与673和723 K有关。蠕变的真实活化能接近复合基质中晶格扩散的活化焓,最小蠕变应变速率的真实应力指数接近5。蠕变是根据位错与非相干Al_(12)的热脱离而解释的基体中的(Fe,V)_3Si相粒子。在温度773、798和823 K时未观察到真正的阈值应力。最小蠕变应变率的真实应力指数随应力的增加而增加,蠕变的真实活化能高于基体中晶格扩散的活化焓。蠕变是根据位错从非相干Al_(12)(Fe,V)_3Si相粒子的热活化脱离来解释的。在873至948 K的温度范围内,真正的阈值应力会重新出现。但是,它的起源与温度623-723 K时的起源不同。真正的活化能接近晶界扩散的活化焓,最小蠕变应变率的真正应力指数接近2.5。这些温度下的蠕变用超塑性流动来解释。

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