1997
DOI: 10.1002/aic.690431213
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Modification of Frenkel's model for sintering

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Cited by 238 publications
(271 citation statements)
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“…The results are given in Figure 6, in which we see that all lines overlap. This indicates that the shape evolution of the contact radius y is independent of the flow history, if the round off parameter R n = R × (y n /R) 3 [20] is used. Next, we keep the initial contact radius constant y n = 0.4, and we change the round off parameter R n = [R × (y n /R) 3 , (R/2) × (y n /R) 3 , (R/4) × (y n /R) 3 ].…”
Section: Effect Of the Initial Geometrymentioning
confidence: 99%
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“…The results are given in Figure 6, in which we see that all lines overlap. This indicates that the shape evolution of the contact radius y is independent of the flow history, if the round off parameter R n = R × (y n /R) 3 [20] is used. Next, we keep the initial contact radius constant y n = 0.4, and we change the round off parameter R n = [R × (y n /R) 3 , (R/2) × (y n /R) 3 , (R/4) × (y n /R) 3 ].…”
Section: Effect Of the Initial Geometrymentioning
confidence: 99%
“…From Figure 8, it follows that the curvature κ at point (0, y) increases with respect to the initial geometry until it reaches a maximum value and subsequently decreases. This holds for all different values of the round off parameter R n = [R × (y n /R) 3 , (R/2) × (y n /R) 3 , (R/4) × (y n /R) 3 ]. This behavior is depicted in Figure 9, where the contour line r = g(z) of the two particles is shown at times t = [0, 0.08, 0.2], using R n = R × (y n /R) 3 .…”
Section: Effect Of the Initial Geometrymentioning
confidence: 99%
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