Slip in MgO and Mg
Based on the principles of the bonding of MgO and Mg and the Peierls-Nabarro stress, explain why slip in MgO is much more difficult than in Mg. For the purpose of this discussion, consider the {0001}<100> slip system in Mg.
As determined in Example 15-6, both the spacing between slip planes and b are 0.280 nm for MgO. For the {0001}<100> slip system in Mg, the interplanar spacing is half of the height of the HCP unit cell or 0.5209 nm/2 = 0.260 nm, and the Burgers vector is the distance between atoms in the close-packed direction or a/2 = 0.32087 nm/2 5 0.160 nm. The Peierls-Nabarro stress is given by Equation 4-2,
τ = c \exp ( – \frac{kd}{ b} )where τ is the shear stress required to move a dislocation, d is the interplanar spacing between slip planes, b is the magnitude of the Burgers vectors, and c and k are material specific constants. Ignoring differences in c and k, we see that the stress required to propagate a dislocation increases as the ratio of d/b decreases. Therefore, we can reasonably expect that MgO with a d/b ratio of 1.0 will require a larger stress to cause dislocations to propagate than Mg (with a d/b ratio of 1.62), thereby making slip more difficult. Additionally, as discussed in Section 4-3, dislocation propagation in ionically bonded materials requires that cations move past other cations and anions move past other anions, creating electronic repulsion that resists dislocation motion.