Microstructure and Phase Analysis in Mn-Al and Zr-Co Permanent Magnets

In America's search for energy independence, the development of rare-earth free permanent magnets is one hurdle that still stands in the way. Permanent magnet motors provide a higher efficiency than induction motors in applications such as hybrid vehicles and wind turbines. This thesis investigates the ability of two materials, Mn-Al and Zr-Co, to fill this need for a permanent magnet material whose components are readily available within the U.S. and whose supply chain is more stable than that of the rare-earth materials. This thesis focuses on the creation and optimization of these two materials to later be used as the hard phase in nanocomposites with high energy products (greater than 10 MGOe). Mn-Al is capable of forming the pure L1 0 structure at a composition of Mn 54 Al 43 C 3. When Mn is replaced by Fe or Cu using the formula Mn 48 Al 43 C 3 T 6 the anisotropy constant is lowered from 1.3 • 10 7 ergs/cm 3 to 1.0 • 10 7 ergs/cm 3 and 0.8 • 10 7 ergs/cm 3 respectively. Previous studies have reported a loss in magnetization in Mn-Al alloys during mechanical milling. The reason for this loss in magnetization was investigated and found to be due to the formation of the equilibrium β-Mn phase of the composition Mn 3 Al 2 and not due to oxidation or site disorder. It was also shown that fully dense Mn-Al permanent magnets can be created at hot pressing temperatures at or above 700 o C and that the ε-phase to τ-phase transition and consolidation can be combined into a single processing step. The addition of small amounts of Cu to the alloy, 3% atomic, can increase the compaction density allowing high densities to be achieved at lower pressing temperatures. While the structure is still under debate, alloys at the composition Zr 2 Co 11 in the Zr-Co system have been shown to have hard magnetic properties. This thesis shows that multiple structures exist at this Zr 2 Co 11 composition and that altering the cooling rate during solidification of the alloy affects the ratio of the phase composition and therefore affects the magnetic properties. Phase diagrams for the Zr-Co system show that the Zr 2 Co 11 phase is stable to a temperature of 1272 o C, at which point the Zr 6 Co 23 phase is the most favorable. However, this thesis …