2005
DOI: 10.1590/s1677-55382005000400022
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Urological Oncology

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“…For two adjacent α grains of the same size, we can neglect the grain boundary energy contribution; thus, the driving force of the thin α grain consuming the adjacent α grain along the surface during γ → α transformation is the total energy (the surface energy and elastic strain energy) difference of two adjacent α grains on the surface. For an α grain with a clean surface, the order of the surface energy values with the low Miller index planes is γ {110} < γ {100} < γ {111} . The {111} oriented α grain has no advantage in the surface energy and elastic strain energy.…”
Section: Resultsmentioning
confidence: 99%
“…For two adjacent α grains of the same size, we can neglect the grain boundary energy contribution; thus, the driving force of the thin α grain consuming the adjacent α grain along the surface during γ → α transformation is the total energy (the surface energy and elastic strain energy) difference of two adjacent α grains on the surface. For an α grain with a clean surface, the order of the surface energy values with the low Miller index planes is γ {110} < γ {100} < γ {111} . The {111} oriented α grain has no advantage in the surface energy and elastic strain energy.…”
Section: Resultsmentioning
confidence: 99%