Combustion Driven Compaction of Nanostructured SmCo/Fe
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Transcript of Combustion Driven Compaction of Nanostructured SmCo/Fe
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
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
Hard
Soft
Hard/Soft
H
M
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 (P2C), and Combustion Driven Compaction (CDC)
Powder Precursors
• Sm2Co17 (= Sm(Co0.67Fe0.234Cu0.07Zr0.024)7.5)* or SmCo5 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]
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 Fe3O4
Consolidation Methods
Plasma Pressure Compaction (P2C)
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
V
Pressure
Graphite Electrodes also form Mold
Sealed Powderr
Combustion Driven Compaction
Compaction done at Utron, Inc.
Die
Powder
Ram
Gas InletIgnitor
CombustibleGas Mixture
• Reach 2 GPa maximum pressure after 500 ms
• Fast and low temperature compaction
• 95% of theoretical density
• Plasma Pressure Compaction (P2C): 73 MPa; 5 mins; 600oC
• Hot Isostatic Pressing (HIP): 435 kPa; 5 mins; 550oC
• Combustion Driven Compaction (CDC): 2 GPa; 500 ms; “room temperature”
-80
-60
-40
-20
0
20
40
60
80
Magnetization (A-m
2/kg)
-4x106
-3 -2 -1 0 1 2 3 4
Field (A/m)
(SmCo5)0.85 Fe0.15 : PPC
(SmCo5)0.80 Fe0.20 : HIP (SmCo5)0.85 Fe0.15 : CDC
T = 300 K
CDC: Retains HC but here loses M because not aligned
Different Compaction Methods
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 P2C)
• Reduced grain-size after compaction
245403530
Sm2
Co17
Pellet
Powder
(101)
(110)
(111)
(002)
Different Compaction Methods• Plasma Pressure Compaction (P2C): 73 MPa; 5 mins; 600oC
• Hot Isostatic Pressing (HIP): 435 kPa; 5 mins; 550oC
• Combustion Driven Compaction (CDC): 2 GPa; 500 ms; “room temperature”
-80
-60
-40
-20
0
20
40
60
80
Magnetization (A-m
2/kg)
-4x106
-3 -2 -1 0 1 2 3 4
Field (A/m)
(SmCo5)0.85 Fe0.15 : PPC
(SmCo5)0.80 Fe0.20 : HIP (SmCo5)0.85 Fe0.15 : CDC
T = 300 K
CDC: Retains HC but here loses M because not aligned
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
CDC and Alignment
CDC
c-axis
Compaction done at Utron, Inc.
Die
Powder
Ram
Gas InletIgnitor
CombustibleGas Mixture
Studied unaligned, and samples with 2 different alignment directions:
c-axis
CDC
Parallel Perpendicular
CDC: via green-compact
• Compacted parallel to c-axis (BH)max = 1.2 x 105 J/m3 (15.5 MGOe)
• Compacted perpendicular to c-axis (BH)max = 2.5 x 105 J/m3 (31.3 MGOe)
• Density ~ 95% in both cases
80
40
0
-40
-80 Magnetization (A-m
2/kg)
-3.0x106
-2.0 -1.0 0.0 1.0 2.0 3.0
Field (A/m)
T = 300 K
Sm2Co17:Fe (20% at.) compacted perpendicular to c-axis compacted parallel to c-axis
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
Inte
nsit
y (a
rb. u
nits
)
Sm2Co17
X-rays
Diffracted beam
Pole Figures
For sample compacted in perpendicular orientation
(002)sample
(110)
(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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