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The resistance of high temperature superconductor (HTS) lap joints under compressive loading is measured and two different HTS tape configurations are tested. The results have shown that joint resistances less than 2 [micro][omega] are possible with only light joint loading configuration.

An electromagnetic bougienage method has used magnetic forces generated between magnetic bullets by a background magnetic field. Analytical methods are developed to obtain the magnetic forces on bougienage bullets and the results have agreed well with the experimental results.

Voltage-current characteristics of semiconductor contact junctions between superconducting wires are examined by means of a voltage-driving method.

Fabrication and testing of a high temperature superconductor (HTS) Levitated Dipole Experiment (LDX) levitation coil is described and discussed.

An overview is presented of research needs involving superconducting magnets for fusion applications.

Tests of NbTi superconducting prototype quadrupole magnets, built for the High Current Transport Experiment (HCX), are described and discussed.

Design of the Muon-to-Electron Conversion Experiment (MECO) solenoids is described and discussed.

Superconducting magnets have been widely used in medical devices for several decades, primarily in thousands of MRI systems worldwide. More recently superconducting magnets have begun to have a small but growing impact on a newer field of medical devices, namely cyclotron accelerators for hadron therapy. This is a form of radiation treatment that uses ionized particle beams (instead of X-rays) to treat a wide variety of cancerous tumors, being particular effective for certain types of pediatric cancer. Although there is growing interest and demand in the medical community for hadron therapy systems, growth in this form of treatment system has been hampered by the very large infrastructure required by conventional accelerator and beam delivery systems, and their concomitant high capital costs. This issue is being addressed by the use of high field superconducting cyclotrons, which offer much more compact accelerators with reduced footprints, along with lower operating costs. In this paper, we describe the background and history of superconducting cyclotrons, and provide a survey of recent developments in this field of application. We also describe the design of a novel, ironless superconducting cyclotron being studied at the Massachusetts Institute of Technology (MIT), Cambridge, MA, USA, and how this technology could be a path towards significantly more widespread deployment of this form of cancer treatment. [ABSTRACT FROM AUTHOR]

Two types of mechanical contact joint termination methods for a 2G YBCO cable have been developed. Each YBCO tape of a cable is connected to a BSCCO tape while the other ends of BSCCO tapes are bundled together and soldered inside a copper tube. Another termination method uses only YBCO tapes. It has been confirmed that both joint termination methods are very useful for 2G HTS cables. Mechanical contact joint resistances between YBCO-BSCCO tapes and YBCO-YBCO tapes have been measured under various contact pressures and contact surface conditions at 77 K. Joint resistance distribution among the tapes in the cable have been also evaluated for both termination methods. These contact joint methods can be used for a demountable joint. Joint resistance is greatly reduced with increasing applied pressure especially for YBCO-YBCO joints. However, in the case of a YBCO-BSCCO joint, the BSCCO tapes may degrade at high pressure. The contact pressure should be optimized to obtain low joint resistance. [ABSTRACT FROM PUBLISHER]

The sensitivity of superconducting magnets to AC losses is well known. If superconducting magnets are this sensitive to AC fields, why not use AC fields for magnet protection, and in particular, for internal energy dump when a quench has been detected? The answer is the large reactive power needed to provide the rate of change of the fields required to quench of a large fraction of the magnet. In this paper we describe a novel approach where quench protection secondary windings external to the magnet are used to minimize the power to initiate the energy dump. The main requirement of these secondary windings is that the mutual inductance between the primary winding and the protection secondary windings has to be small, ideally zero. One means to provide for zero mutual inductance between the protection secondary winding and the primary winding is by designing a protection secondary winding that produces AC fields that everywhere in the volume are normal to the fields produced by the primary winding. Alternatively, appropriate windings can be made so that the coupling in one region is the opposite to that of another region, with zero total mutual inductance. The latter approach results in low voltages at the leads, but could result in high voltages within the coil. We describe several circuit topologies applicable to solenoidal and toroidal windings that satisfy these requirements. Calculations of the heating due to AC fields are presented, including eddy current heating in cable-in-copper-channel conductors. If the quench inducing coil is optimally designed and powered, the hysteresis of the superconductor dominates the heating. Thus, as a portion of the superconducting magnet quenches, the heating power shifts to those zones that are not yet in the current-sharing regime. This approach is an alternative to the use of resistive heating elements, which need to be placed on, or embedded in, the winding pack. [ABSTRACT FROM PUBLISHER]

Electrical edge joint of a stacked high-temperature superconducting (HTS) conductor is explored for electrical joints for a demountable HTS toroidal field coil. Demountable coils would be very useful in small tokamak plasma-facing component-test machines, such as Vulcan. The demountable concept explored in this paper consists of forcing together the edges of stacked HTS conductor embedded in a conductive or a structural material. We carried out a testing program of the edge joint of a stacked YBCO conductor within a copper jacket. The HTS cable has a critical current of 1600 A at 77 K in self-field. The experimental results showed that joint resistance in the edge joint was higher than expected, as was not reproducible. One potential reason for the larger than expected resistance is the damage to the tape edge in preparation of the joint region due to milling/fabrication. Another potential reason was low accuracy in the fabrication of joint surface; the joint surfaces were not parallel to one another. The joint resistance will be reduced by the sophistication of the fabrication process for the joint surface. We also carried out calculations to determine the joint performance of the edge joint in an ideal condition. In the ideal condition, inserting an indium film between joint surfaces or plating copper layer on joint surfaces can prevent joint resistance from increasing due to the misalignment of the contact surfaces and would provide a compliant layer between joints. The joint resistance of the edge joint can become smaller than that of an electrical lap joint when the number of the stacked HTS tape is large. [ABSTRACT FROM PUBLISHER]

Recent International Thermonuclear Experimental Reactor (ITER) Model Coils and tests on Nb3Sn Cable in Conduit Conductors (CICC) showed a significant and unexpected increase in the broadness of the transition to the normal state, resulting in degradation of superconducting properties. To investigate these phenomena, two CICC samples were built with identical 144 strand cables but different conduit materials. One sample had titanium conduit with low coefficient of thermal expansion, the other had stainless steel conduit. The purpose of this experiment was to study changes in strand properties in the cable (critical current, current sharing temperature, n-value), the effects of cycling and high electromagnetic load, and the effect of the conduit on the CICC performance. [ABSTRACT FROM AUTHOR]

The International Thermonuclear Experimental Reactor (ITER) Central Solenoid and Toroidal Field Model Coils (CSMC, TFMC) and the CSMC Insert Coils using Nb33Sn had unexpectedly low current-sharing temperatures and cable "n-values." This paper argues that the anomalous effects can be explained by the high longitudinal strain due to transverse Lorentz loads. Simulated results of earlier experiments with A15 monoliths indicate that the transverse stress "multiplier" is actually a longitudinal strain multiplier due to transverse loading. Irreversible cyclic degradation effects in the cables with the lowest thermal contraction mismatches are explained by showing that a modest precompression is required to prevent tensile cracking of a significant number of individual filaments. Examination of filament breakage due to bending shows the possibility of a well-defined threshold for irreversible damage. [ABSTRACT FROM AUTHOR]

A cryostat housing a pair of previously tested quadrupole magnets has been constructed as a prototype focusing cell for the High Current Experiment (HCX) project. The doublet assembly was constructed with a room temperature beam tube. The magnets were reassembled, electrically connected in series, and tested to the short sample limiting current without further training. The doublet was more sensitive to the current ramping rate as compare with the previous performance. In order to build a compact vacuum jacket for the warm bore structure, a novel radiation insulation made of aluminum coated stainless steel foil was selected. The experiences in assembly of the doublet and fabrication of the cryostat are described. The thermal performances of the cryostat are reported. [ABSTRACT FROM AUTHOR]

Four NbTi superconducting prototype quadrupole magnets have been built for the High Current Transport Experiment (HCX) as part of the multi-beam heavy-ion fusion research activity, led by the Lawrence Berkeley National Laboratory (LBNL). MIT performed quench training and ramp rate tests of the two prototype magnets that were designed and built by the Advanced Magnet Lab, Inc. (AML), based on a novel concept featuring cable-in-groove and multi-layer stacking. Both magnets are splice-free without inter-layer or inter-quadrant joint. Each coil was wound with a continuous NbTi round cable, placed in precise grooves machined in G-11 plates. The two magnets differ in their cable construction and their coil and yoke configuration. Each magnet was tested more than once in liquid helium bath with a room temperature thermal cycle between cold tests. This paper describes the results of the performance tests as well as the instrumentation and the quench protection system. Possible improvements for future coil winding are discussed. [ABSTRACT FROM AUTHOR]

Describes the design, fabrication and test of the react-and-wind Nb[sub 3]Sn Levitated Dipole Experiment floating coil conductor developed in a joint project by Columbia University and the Massachusetts Institute of Technology. Magnetic levitation of a superconducting ring coil; Cable strain; Prevention of degradation of the critical current; Effect of fabrication, winding and operating strains on critical current.

Describes a pulsed magnetic field test facility for testing large scale cable-in-conduit superconductor and joint samples. Pulsed Test Facility (PTF) system; Facility status and schedule.

A small dipole magnet designed for use in high-radiation environments that uses metal-oxide Cable-In-Conduit-Conductor has been constructed and tested for magnetic properties. The conductor consisted of 42 strands of 0.5 mm diameter wires, in a conduit with outer dimension of 10 mm x 10 mm. The magnet carried about 8 kA. This gives an engineering current density of 80A/mm2. The current density in the cable bundle is approximately 1 kA/mm2. [ABSTRACT FROM AUTHOR]

The article presents information on superconductivity. Topics discussed here include, high-temperature superconductivity (HTS), low-temperature superconductors, and magnetic resonance imaging systems. Also discussed are, cuprate superconductors, and deployment of HTS-based conductors and magnet systems.