2022
DOI: 10.1002/adem.202101513
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A New Approach for Sintering Simulation of Irregularly Shaped Powder Particles—Part I: Model Development and Case Studies

Abstract: Within the FOR3010 Refrabund project, a new type of composite refractory consisting of alumina and refractory metals such as tantalum and niobium is developed. This material is characterized by its ability to conduct electricity, which offers new opportunities for functional parts in high‐temperature environments. To support the development of material properties and production technology, a new simulation approach is needed, which is able to describe irregularly shaped particles of at least two different phas… Show more

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Cited by 5 publications
(15 citation statements)
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References 31 publications
(88 reference statements)
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“…Over the whole time span, the morphological run shows a slightly higher shrinkage than the circular one. This corresponds to the results in Part I, [ 34 ] as tip contacts show slightly higher shrinkage and are more likely to occur with the current contact creation algorithm. The standard deviation is noticeably higher in early stages than in late stages.…”
Section: Resultssupporting
confidence: 85%
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“…Over the whole time span, the morphological run shows a slightly higher shrinkage than the circular one. This corresponds to the results in Part I, [ 34 ] as tip contacts show slightly higher shrinkage and are more likely to occur with the current contact creation algorithm. The standard deviation is noticeably higher in early stages than in late stages.…”
Section: Resultssupporting
confidence: 85%
“…As stated above, this corresponds accordingly to the results of Part I. [ 34 ] Tip contacts show lower neck radii because they act locally as they would be of lower radius. Similar to shrinkage, the standard deviation decreases with time and is higher in the morphological run.…”
Section: Resultssupporting
confidence: 84%
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“…The particle morphology was then statistically evaluated using the following equation describing the radius r in the polar coordinate system φ .rfalse(φfalse)=r0false(1+hnormalpcosfalse(φnnormalpfalse)+ocosfalse(2φfalse)false)with the base radius r0, the height hnormalp of the first‐order peaks as fraction of r0, the number of peaks nnormalp, and the ovality o as a fraction of r0. Details of the used model can be found in the study by Weiner et al [ 20 ] Figure 2b shows the obtained results of least‐square fitting, Equation (), to the extracted data of Figure 2b. As shown, the contour is only roughly reproduced by this equation.…”
Section: Methodsmentioning
confidence: 99%