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Combustion Driven Compaction of Nanostructured SmCo/Fe Exchange spring magnetic materials can potentially increase the energy-products of permanent magnets.

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Presentation on theme: "Combustion Driven Compaction of Nanostructured SmCo/Fe Exchange spring magnetic materials can potentially increase the energy-products of permanent magnets."— Presentation transcript:

1 Combustion Driven Compaction of Nanostructured SmCo/Fe Exchange spring magnetic materials can potentially increase the energy-products of permanent magnets Powder consolidation has the ability to form composite magnets with arbitrary 3D shapes and sizes, less $ for expensive hard phase, possibility of mechanical fiber reinforcements

2 Approach Obtain high coercivity by ball- milling hard phase Increase magnetization of the ball- milled hard phase by mixing with soft-phase Obtain exchange coupling between the hard and the soft phase by compaction

3 Challenges for compacted nanocomposites Preserve original phases during compaction Achieve strong coupling across interfaces Here compare results for consolidation by three different methods: Hot Isostatic Pressing (HIP), Plasma Pressure Compaction (P 2 C), and Combustion Driven Compaction (CDC)

4 Powder Precursors Sm 2 Co 17 (= Sm(Co 0.67 Fe 0.234 Cu 0.07 Zr 0.024 ) 7.5 )* or SmCo 5 for the hard phase [d ~ 1  m] High crystallinity acicular-Fe nanoparticles for soft phase [length ~ 200 nm, d ~ 20 nm] SmCo and Fe powder precursors were mixed together by gentle milling [*Courtesy of C. Chen, Electron Energy Corporation] [Courtesy of J. Nakano, Toda Corporation]

5 Acicular Fe Nanoparticles TEM of commercial acicular-Fe particles with an average length of 200 nm and average diameter of 20 nm Hydrogen reduction at 400 °C used to remove surface Fe 3 O 4

6 Consolidation Methods Plasma Pressure Compaction (P 2 C) Compaction done at Materials Modification, Inc., 600°C, 45 MPa, 5 min Hot Isostatic Pressing (HIP) Compaction done at Wright- Patterson AFB 550°C, 21.6 MPa, 5 min r

7 Combustion Driven Compaction Compaction done at Utron, Inc. Reach 2 GPa maximum pressure after 500 ms Fast and low temperature compaction 95% of theoretical density

8 Plasma Pressure Compaction (P 2 C): 73 MPa; 5 mins; 600 o C Hot Isostatic Pressing (HIP): 435 kPa; 5 mins; 550 o C Combustion Driven Compaction (CDC): 2 GPa; 500 ms; “room temperature” CDC: Retains H C but here loses M because not aligned Different Compaction Methods

9 X-ray Diffraction and CDC Average Grain size estimates based on Scherrer analysis Powder : 190 nm Pellet : 138 nm No SmCo phase decomposition occurred during CDC (unlike with HIP and P 2 C) Reduced grain-size after compaction 22

10 Different Compaction Methods Plasma Pressure Compaction (P 2 C): 73 MPa; 5 mins; 600 o C Hot Isostatic Pressing (HIP): 435 kPa; 5 mins; 550 o C Combustion Driven Compaction (CDC): 2 GPa; 500 ms; “room temperature” CDC: Retains H C but here loses M because not aligned

11 Pre-Alignment of Powder Powder aligned in pulsed field (3 one second pulses of 10 T) H = 10 T Green-compact formed by Cold Isostatic Pressing (at 35 kpsi)* Further densification using Combustion Driven Compaction (CDC) *Courtesy of S. Sankar, Advanced Materials Corporation

12 CDC and Alignment CDC c-axis Compaction done at Utron, Inc. Studied unaligned, and samples with 2 different alignment directions: c-axis CDC ParallelPerpendicular

13 CDC: via green-compact Compacted parallel to c-axis (BH) max = 1.2 x 10 5 J/m 3 (15.5 MGOe) Compacted perpendicular to c-axis (BH) max = 2.5 x 10 5 J/m 3 (31.3 MGOe) Density ~ 95% in both cases

14 Estimating Alignment Retention Estimate alignment retained during compaction (CDC), using X-ray Pole Figure analysis For a particular Bragg angle, diffraction from corresponding plane is recorded 2 2  Intensity (arb. units) Sm 2 Co 17 X-rays Diffracted beam  

15 Pole Figures For sample compacted in perpendicular orientation (002) sample (110) (002) (110) planes are perpendicular to (002), and are ~randomly oriented In (002) pole figure, I is largest near the edges, suggesting c- axis nearly parallel to the sample surface.

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