1979
DOI: 10.1007/bf02697073
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Elevated temperature plastic anisotropy of Ti-6AI-4V plate

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Cited by 6 publications
(3 citation statements)
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“…Similarly, let S x (x x x), S y (x x x), and S z (x x x) denote the flow stresses of a single crystal in the x, y, and z axis, respectively, at a given strain. We can calculate the overall flow stresses S a , a ∈ {x, y, z} of the polycrystal as in (1) and formulate the problem of plastically isotropic design as the minimization of I (S x , S y , S z ). As our approach applies to both elastic and plastic regimes, we avoid introducing duplicate equations by coining the term "property" to refer to either the Young's modulus E a or the flow stress S a and denote it as P a ∈ {E a , S a }.…”
Section: Resultsmentioning
confidence: 99%
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“…Similarly, let S x (x x x), S y (x x x), and S z (x x x) denote the flow stresses of a single crystal in the x, y, and z axis, respectively, at a given strain. We can calculate the overall flow stresses S a , a ∈ {x, y, z} of the polycrystal as in (1) and formulate the problem of plastically isotropic design as the minimization of I (S x , S y , S z ). As our approach applies to both elastic and plastic regimes, we avoid introducing duplicate equations by coining the term "property" to refer to either the Young's modulus E a or the flow stress S a and denote it as P a ∈ {E a , S a }.…”
Section: Resultsmentioning
confidence: 99%
“…Intuitively, it is probable that an ODF with exactly three, equally weighted, non-zero nodes, each one corresponding to the single crystal that maximizes P s along the x, y, or z axis, will give rise to a texture that is isotropic with respect to that property. Formally, we define this ODF as π π π = 1 3 ∑ a∈{x,y,z} e e e j p a , where j p a = argmax j∈[d] θ p a,j . As this ODF is sparse, it is an appropriate baseline for our optimized sparse ODFs and hence more relevant to the analysis in Fig.…”
Section: Additional Objectives and Constraintsmentioning
confidence: 99%
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