Products and Capabilities
Wire
Coils
Superconducting FCL Elements
Wire
Definition
Superconductors are well known to carry high current with near zero ohmic loss.
In coil form, such as in an electromagnet, a charged and closed loop can carry
current, and hence magnetic field, for long periods of time (of the order of
months to years depending on the detail design). This makes a superconductor
ideal for high field magnets, and consequently, it is commonly used in MRI and
nuclear magnetic resonance (NMR) systems throughout the world. Hyper Tech is
well equipped to produce two wire formed superconductors: MgB2 and
Nb3Sn.
MgB2 Wire
Nb3Sn Wire
MgB2 Wire
History of MgB2
In January 2001, Japanese University
professor Dr. Akimitsu announced that MgB2 was superconducting up to 39 Kelvin. Since that
discovery, Hyper Tech has been working on making the compound into a high
performing, low cost superconductor wire.
Shortly after its creation, Hyper Tech developed and patented the continuous
tube forming and filling (CTFF) process to make a powder metallurgy based
wire of the MgB2 superconductor. To manufacture a multifilament wire,
numerous monofilaments containing the superconducting powder must be stacked
within a tube and then drawn down to the required wire diameter and length.
Hyper Tech’s patented process involves manufacturing wire starting with a metal
ribbon that is continuously filled and formed into a tube. Traditionally,
manufacturers must fill a tube of fixed length before drawing the wire. This
method results in two problems: 1) the tube filling process results in an
uneven density of material within the tube and 2) larger and larger diameter
tubes are necessary to obtain longer lengths of wire.
In just more than five years, Hyper Tech has consistently manufactured
monofilamentary and multifilamentary wires of up to 4 kilometers in length,
which is necessary to be commercially viable. In order to evaluate the MgB2
wire performance, 740 meters were wound into coils and tested. This enabled
evaluation of superconductivity over the wire length and provided a preview of
potential magnet applications. In November 2005, Hyper Tech fabricated a
solenoid coil producing 2.4 Tesla at 20 Kelvin, 1.8 Tesla at 25 Kelvin, and 0.9
Tesla at 30 Kelvin. This coil met the magnetic field strength requirements to
be viable in many applications, such as MRI systems currently using permanent
magnets (up to 0.35 Tesla).
In August 2006, this milestone was exceeded when a 53-centimeter diameter
test coil, also aimed at the MRI industry, was fabricated using a
react-and-wind process. It too performed at the expected field strength and current.
Why MgB2?
Once the technical hurdles are cleared, the single most important criterion
for the acceptance of MgB2 based magnets in the market place is that
they provide a performance and reliability comparable to or exceeding that of
existing magnets but at a lower life-cycle cost.
When compared with permanent magnets, there are two potential advantages of
MgB2. The first is the possibility of achieving the typical magnetic
field strengths of considerably more than 0.4 Tesla (up to 1.5-2.0 Tesla) with
a lower initial capital equipment cost and lower life-cycle cost. Second,
higher field strengths and larger zones of homogeneous magnetic field can be
achieved with MgB2 superconductor than with permanent magnets.
Compared with low-temperature superconductors, the life-cycle costs of MgB2
coils are lower due to the higher operating temperature and associated
refrigeration cost. In the on-going effort to eliminate liquid cryogen, the
temperature tolerance of MgB2 better suits it for dry operation
using only a cryocooler and conduction cooling.
MgB2 conductors can operate at temperatures of 20 to 30 Kelvin. They
can be supplied in round or rectangular cross sections giving them advantages
in manufacturing and handling as well as a higher coil current density. MgB2
is lighter weight and can be produced at a lower cost than the high temperature
ceramic superconducting tape conductors BSCCO or YBCO-coated when operated in
the 20 Kelvin range. MgB2 wire is versatile in that it can be sized
(amperage and Jc) for the appropriate coil size and performance. MgB2
wire behaves more like a metal superconductor with regard to persistent current
type coils than the superconducting tapes.
Potential applications include MRI systems, superconducting FCLs, transformers, inductors,
reactors, motors, and generators. Of these, the most promising applications are
projected to be MRI systems and superconducting FCLs.
Typical MgB2 Wire Specifications
Hyper Tech can manufacture wires that are 1 to 4 kilometers in length
with 7 and 19 filaments.
| Specification |
Value |
| Diameter | 0.7 mm to 0.9 mm (others available) |
| Number of Filaments | 7 and 19 (higher available experimentally) |
| Condition | Reacted and un-reacted and insulated with S-glass |
| Heat Treatment Temperature/Time | 700 degrees C/20 minutes (Nominal) |
| Jc @ 20 K – 2T | 175,000 A/cm2 (Nominal) |
| Maximum Allowable Axial Strain | 0.35% |
| Continuous Piece Length | 1-4 km |
| Superconductor fraction | 13 – 18% (Under development - increase to 30%) |
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| Multifilament Wire with Solid Cu Core |
Monofilament Wire |
Nb3Sn Wire
Hyper Tech has developed high performance Nb3Sn wire suitable for
applications in high energy physics (e.g., accelerators), research magnets and
commercial applications (e.g., high field MRI systems). The core of this work
is on various types of internal-tin Nb3Sn superconductors.
 |
 |
| Conventional rod-in-tube (RIT) Nb3Sn conductor |
RIT Nb3Sn conductor constructed with splits to lower the effective diameter (deff) of the superconductor |
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| “Tube type” Nb3Sn conductor: sub-elements are fabricated with Nb integral tubes as compared with Nb filaments (rods) in RIT construction |
Low AC-loss Nb3Sn conductor designed for fusion energy applications |
Coils
The development of long length multifilamentary wire production has enabled
Hyper Tech to design and fabricate a series of MgB2 wound solenoid
and racetrack coils. Establishing excellent properties over length in these early
demonstrations has led to producing more realistic coils with MgB2
superconductor wire relevant to specific applications. Long length
characterization in coil form is equally important for the advancement of the
MgB2 superconductor because most commercial applications will
require several
multikilometer lengths of
wire.
Wind-and-react solenoid coils
Hyper Tech has fabricated several solenoid coils wound with long lengths of
Nb/Cu/MonelTM -type multifilament wire employing a wind-and-react
approach. That is, the MgB2 wire is wound onto the finished bobbin
and reacted at 650 to 700 degrees C for 20 minutes and subsequently vacuum
impregnated with epoxy.
Hyper Tech wound one such coil fabricated by the wind-and-react process with
740 meters of 0.83 mm diameter strand totaling 3,463 turns around a 3.8 cm
bore. This coil attained a field of 3.9 T at 4 K, 3.0 T at 15 K, 2.4 T at 20 K,
1.8 T at 25 K, and 0.9 T at 30 K.
 |
| Wind-and-react solenoid coil: 740 meters |
 |
| Ic, Jc and Je as a function of temperature for 740 meter wind-and-react solenoid coil |
React-and-wind solenoid coils
Hyper Tech fabricated a demonstration solenoid coil using a react-and-wind
approach; the bore size in this coil was 53 cm which is relevant to many
applications including specialty MRI systems. The coil generated a field on axial
of 0.12 T at 20 K, which corresponded to predictions based on short sample wire
results.
 |
| React-and-wind solenoid coil: 53 cm bore wound with 820 meters of MgB2 wire |
Wind-and-react racetrack coils
Hyper Tech has fabricated more than 10 single-layer racetrack coils for a
cryogenic rotor in a liquid helium-cooled superconducting generator
demonstration. The racetrack coils were made using the wind-and-react approach.
One coil reached 400 A at 4 K.
 |
| Wind-and-react racetrack "rotor" coil |
Hyper Tech fabricated four complete rotor coil packs for delivery to NASA. Each pack contained 580 meters of MgB2 superconducting wire. The wire was wound in a racetrack form around a copper former and Inconel center core. It was subsequently enclosed within an aluminum housing and potted to fill all voids.
These rotor coil packs are for a liquid hydrogen cooled 2 MW alternating current generator intended for hypersonic aircraft. Four coil packs make up the rotor. The rotational speed of the generator is to be 20,000 rpm.
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| Demonstration rotor coil pack |
A superconducting FCL is a device that uses superconductors to instantly
limit electrical surges before they reach a circuit breaker. Conventional
utility equipment that currently mitigates this problem consists of large
copper coils called line reactors. These are bulky devices that continuously
consume power. Superconductors alone possess the unique physical properties
that allow them to react instantly to current changes. In their superconducting
state, they pass electricity continuously without power losses at normal levels
while limiting current surges. The main advantages of superconducting FCLs are their negligible
influence on an electrical network under normal operating conditions, fast
response to over-current conditions, and response without an external trigger.
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| Schematic of MgB2-based superconducting FCL and superconducting FCL element |
There are several types of superconducting FCLs but they fall into two basic categories:
resistive and inductive. A resistive superconducting FCL operates as described above and is
generally configured as shown in the schematic. They are intended to be passive
and have a recovery time dependent entirely on the selected method of cooling.
If the fault energy is stored inertially in
a heat sink, the recovery time will be long, on the order of minutes, as
determined by the mass of the components. An inductive superconducting FCL is designed to
remain superconducting and stores the fault energy within the coils of the superconductor
while providing the necessary impedance to limit the fault current. The inductive
superconducting FCL is not usually preferred because of its greater size and cost, which are
driven by the large volume of superconductor required.
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