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Atomistic simulations of the face-centered-cubic-to-hexagonal-close . . . The term “high-entropy” denotes the high configurational entropy inside a material system, which can inhibit the formation of intermetallic compounds and stabilize the single solid-solution phase in a simple crystal structure, such as face-centered-cubic (fcc), body-centered-cubic (bcc), and hexagonal-close-packed (hcp) structures [14], [15]
The mechanisms of γ (fcc) → ε (hcp) → α′ (bcc) and direct γ (fcc) → α . . . Here, we reported the strain-dependent direct transformation of γ (fcc) → α′ (bcc) in addition to the γ (fcc) → ε (hcp) → α′ (bcc) sequence in a gradient austenitic 304 stainless steel And we proposed the new mechanisms involved in the two transformation sequences
What is the difference between FCC, BCC, and HCP structures? Atomic arrangement: FCC has atoms at cube corners and face centers, BCC at corners and the center, while HCP is hexagonal-layered Ductility: FCC has the highest ductility, BCC moderate, and HCP lowest
Decoding of crystal synthesis of fcc-hcp reversible transition for . . . Propose a detailed transformation pathway of the fcc and hcp facet pairs for transition metals Identify the facile strategy to achieve flexible switching between different high index facets Demonstrate the novel proton penetration and storage (PPS) mechanism in fcc and hcp lattices
Close Packed Structures: fcc and hcp | Physics in a Nutshell One can easily see that the closest packing of spheres in two dimensions is realised by a hexagonal structure: Each sphere is in contact with six neighboured spheres In three dimensions one can now go ahead and add another equivalent layer
Comparison of SC, BCC, FCC, and HCP Crystal Structures Here are the links for the thorough comparisons of: FCC vs BCC, and FCC vs HCP Here are the crystal geometric ratios for simple cubic, body-centered cubic, face-centered cubic, and hexagonal close-packed