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Solid Solution Strengthening


The introduction of solute atoms into solid solution in the solvent atom lattice invariably produces an alloy which is stronger than the pure metal. There are two types of solid solutions. If the solute and solvent atoms are roughly similar, the solute atoms will occupy lattice points in the
crystal lattice of the solvent atoms. This is called substitutional solid solution. If the solute atoms are much smaller than the solvent atoms, they occupy interstitial positions in the solvent lattice. If the sizes of the two atoms, as approximately indicated by the lattice parameter, differ by less than 15 per cent, the size factor is favorable for solid-solution formation. When the size factor is greater than 15 per cent, the extent of solid solubility is usually restricted to less than 1 per cent. Metals which do not have a strong chemical affinity for each other tend to form solid solutions, while metals which are far apart on the electromotive series tend to form intermetallic compounds. The relative valence of the solute and solvent is also important. The solubility of a metal with higher valence in a solvent of lower valence is more extensive than for the reverse situation. For complete solid solubility over the entire range of composition the solute and solvent atoms must have the same crystal structure. Some of the following mechanisms will occur on solid solution strengthening.
  • Elastic interaction
  • Modulus interaction
  • Electrical interaction
  • Stacking fault
  • Short range order
  • Long range order

The distribution of solute atoms in a solvent lattice is not usually completely random. There is growing evidence that solute atoms group preferentially at dislocations, stacking faults, low-angle boundaries, and grain boundaries. However, even in a perfect lattice the atoms would not be completely random. For a solid solution of A and B atoms, if B atoms tend to group themselves preferentially around other B atoms, the situation is called clustering. However, if a given B atom is preferentially surrounded by A atoms, the solid solution exhibits short range order. The tendency for clustering or short-range order increases with increasing solute additions. It is likely that solid solution hardening is not simply the result of internal stresses due to the local lattice disturbance from randomly dispersed solute atoms.
A number of types of solute-atom interaction must be considered in explaining solid-solution strengthening. Cottrell locking due to elastic interaction between the solute atoms and the dislocations is certainly an important factor in solid solution strengthening. In view of the valency effects observed in solid solutions, electrical interaction must also be considered. However, estimates show that electrical interaction is only about one third to one seventh as strong as elastic interaction. Thermodynamic reasoning shows that the concentration of solute atoms at a stacking fault will be greater than the average bulk concentration. Thus, there is a "chemical interaction" between these regions and dislocations. In a binary alloy with long-range order each of the constituent atoms occupies special sites in the lattice. In effect, this results in a super lattice with a larger unit cell and a new crystal structure. The interaction of dislocations with long-range order results in a strengthening effect.