The critical current density (Jc) of hot isostatic pressed (HIPed) MgB2
wires, measured by d.c. transport and magnetization, is compared with that of
similar wires annealed at ambient pressure. The HIPed wires have a higher Jc
than the annealed wires, especially at high temperatures and magnetic fields,
and higher irreversibility field (Hirr). The HIPed wires are promising for
applications, with Jc>106 A/cm2 at 5 K and zero field and >104 A/cm2 at 1.5 T
and 26.5 K, and Hirr ~ 17 T at 4 K. The improvement is attributed to a high
density of structural defects, which are the likely source of vortex pinning.
These defects, observed by transmission electron microscopy, include small
angle twisting, tilting, and bending boundaries, resulting in the formation of
sub-grains within MgB2 crystallites.Comment: 13 pages,3 figure
We report dc transport and magnetization measurements of J c in MgB 2 wires fabricated by the powder-in-tube method, using commercial MgB 2 powder with 5 %at Mg powder added as an additional source of magnesium, and stainless steel as sheath material. By appropriate heat treatments, we have been able to increase J c by more than one order of magnitude from that of the as-drawn wire. We show that one beneficial effect of the annealing is the elimination of most of the micro-cracks, and we correlate the increase in J c with the disappearance of the weak-link-type behavior.
Abstract. We present the fabrication and test results of Hot-Isostatic-Pressed (HIPed) Powder-in-Tube (PIT) MgB 2 coils. The coils properties were measured by transport and magnetization at different applied fields (H) and temperatures (T ). The engineering critical current (J e ) value is the largest reported in PIT MgB 2 wires or tapes. At 25 K our champion 6-layer coil was able to generate a field of 1 T at selffield (I c > 220 A, J e ∼ 2.8 × 10 4 A/cm 2 ). At 4 K this coil generated 1.6 T under an applied field of 1.25 T (I c ∼ 350 A, J e ∼ 4.5 × 10 4 A/cm 2 ). These magnetic fields are high enough for a superconducting transformer or magnet applications such as MRI. A SiC doped MgB 2 single layer coil shows a promising improvement at high fields and exhibits J c > 10 4 A/cm 2 at 7 T.
We present a detailed analysis of the effect of heat treatments on the microstructure, magnetization, and transport properties of MgB2 wires produced by the powder-in-tube method. We have used commercial MgB2 powder with 5 at. % Mg powder added as an additional source of magnesium and stainless steel as sheath material. We measure the dc transport critical current that can be increased or decreased by more than one order of magnitude as compared with the as-drawn wire, depending on the annealing parameters. We correlate the changes in the critical current with changes in the microstructure, as determined from scanning and transmission electron microscopy analysis. We show through magnetization measurements of short annealed wires that inappropriate annealing conditions result in a deterioration of the connectivity due to the loss of Mg and in inhomogeneous weak-link limited current flow, rendering the critical state model inapplicable. We discuss the optimization of the annealing conditions that strongly improve the connectivity by eliminating most of the microcracks present in the unannealed wires, where excess Mg promotes the recrystallization. The loss of Mg during the heat treatment may be precluded by annealing long wire lengths with a high heating rate.
The microstructures of MgB 2 wires prepared by the powder-in-tube technique and subsequent hot isostatic pressing were investigated using transmission electron microscopy. Large amount of crystalline defects including small angle twisting, tilting, and bending boundaries, in which high densities of dislocations reside, were found forming sub-grains within MgB 2 grains. It is believed that these defects resulted from particle deformation during the hot isostatic pressing process and are effective flux pinning centers that contribute to the high critical current densities of the wires at high temperatures and at high fields.
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