2021
DOI: 10.1002/gamm.202100012
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Accessing pore microstructure–property relationships for additively manufactured materials

Abstract: Understanding structure-property (SP) relationships is essential for accelerating materials innovation. Still being in the state of ongoing research and development, this is especially true for additive manufacturing (AM) in which process-induced imperfections like pores and microstructural variations significantly influence the material's properties. That is why, the present work aims at proposing an approach for accessing pore SP relationships for AM materials. For this purpose, crystal plasticity (CP) simul… Show more

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Cited by 11 publications
(4 citation statements)
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“…The descriptorbased nature of the algorithm enables to create large data bases of synthetic 3D microstructure from few observations through interpolation in descriptor space. This exploration of feasible microstructures leads to valuable insight and computationally-obtained process-structure-property linkages like [21] work unit only. TensorFlow [1] is used for just-in-time compilation in order to generate efficient GPU code from a simple Python definition of the descriptors and the loss function.…”
Section: Discussionmentioning
confidence: 99%
“…The descriptorbased nature of the algorithm enables to create large data bases of synthetic 3D microstructure from few observations through interpolation in descriptor space. This exploration of feasible microstructures leads to valuable insight and computationally-obtained process-structure-property linkages like [21] work unit only. TensorFlow [1] is used for just-in-time compilation in order to generate efficient GPU code from a simple Python definition of the descriptors and the loss function.…”
Section: Discussionmentioning
confidence: 99%
“…The relationship between fatigue strength and defect size can be written as normalΔσnormalw=normalΔσw0truea0a+a0$$ \Delta {\sigma}_{\mathrm{w}}=\Delta {\sigma}_{\mathrm{w}0}\sqrt{\frac{a_0}{a+{a}_0}} $$ with normalΔσnormalw$$ \Delta {\sigma}_{\mathrm{w}} $$ as the fatigue limit, normalΔσw0$$ \Delta {\sigma}_{\mathrm{w}0} $$ as the fatigue limit of the material without defects and a=area=π·b·c$$ a=\sqrt{area}=\sqrt{\pi \cdotp b\cdotp c} $$ the square root of the ellipse fitted to the largest projected area of the largest defect with the major half‐axis b$$ b $$ and the second largest half‐axis c$$ c $$ [30,38]. The El‐Haddad constant a0=area0=true1π()falseΔKth,LCFw·Δσw02,$$ {a}_0=\sqrt{are{a}_0}=\frac{1}{\pi }{\left(\frac{\Delta {K}_{\mathrm{th},\mathrm{LC}}}{F_{\mathrm{w}}\cdotp \Delta {\sigma}_{\mathrm{w}0}}\right)}^2, $$ is calculated with the crack propagation threshold normalΔKth,LC$$ \Delta {K}_{\mat...…”
Section: Experimental and Data Analysis Methodsmentioning
confidence: 99%
“…with Δ𝜎 w as the fatigue limit, Δ𝜎 w0 as the fatigue limit of the material without defects and a = √ area = √ 𝜋 ⋅ b ⋅ c the square root of the ellipse fitted to the largest projected area of the largest defect with the major half-axis b and the second largest half-axis c [30,38]. The El-Haddad constant…”
Section: Influence Of Pore Size On Fatigue Strengthmentioning
confidence: 99%
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