Fig. 10: Cross-section of \(B(\overrightarrow{n})\) in GPa along the (010)β plane using SFTS for the mixed coherency (F33−I = δc − δc = 0, that is, complete coherency loss solely along the [001] direction) case. | npj Computational Materials

Fig. 10: Cross-section of \(B(\overrightarrow{n})\) in GPa along the (010)β plane using SFTS for the mixed coherency (F33−I = δc − δc = 0, that is, complete coherency loss solely along the [001] direction) case.

From: Multiscale modeling of metal-hydride interphases—quantification of decoupled chemo-mechanical energies

Fig. 10: Cross-section of $$B(\overrightarrow{n})$$ B ( n → ) in GPa along the (010)β plane using SFTS for the mixed coherency (F33−I = δc − δc = 0, that is, complete coherency loss solely along the [001] direction) case.

Superimposed in blue dashed lines is the full coherency case (F33−I = δc) presented again for comparison. Black arrows represent the directions that minimize the interfacial coherency strain energy density for the mixed coherency case, \(\overrightarrow{{n}_{0}}\).

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