3338 IEEE TRANSACTIONS ON APPLIED SUPERCONDUCTIVITY, VOL. 21, NO. 3, JUNE 2011
Magnesium Diboride Wires With Nonmagnetic
Matrices—AC Loss Measurements and Numerical
Calculations
Lauri Rostila, Eduard Demenˇ cík, Jan
ˇ
Souc, Silvia Brisigotti, Pavol Kovᡠc, Milan Polak, Giovanni Grasso,
Mika Lyly, Antti Stenvall, Andrea Tumino, and L’ubomir Kopera
Abstract—In the superconducting applications, the wires are
exposed to time-varying magnetic field when the current changes.
This generates losses which can be minimized by reducing filament
size, twisting the wire, and increasing the transverse resistivity.
However, the high losses of magnesium diboride wires often arise
from magnetic sheath materials, and therefore, this work presents
new type of wires with nonmagnetic matrix and multi-filamentary
structure. The results of AC loss measurements, in external sinu-
soidal magnetic field, are presented. Two samples were
measured both in two temperature ranges, as two different set-ups
were used, one with fixed LHe bath temperature 4.2 K. Second
one enabled operation temperatures from 23 K up to the critical
temperature of 39 K. Amplitude of magnetic field of the former
set-up was up to 0.8 T and frequency range was from 0.1 to 1.4 Hz.
In the latter one, the maximum amplitude was 28 mT, and the
frequencies were 72 and 144 Hz. The results evidenced that the
superconducting filaments were uncoupled and the measurements
agreed with theoretical models based on this assumption. In
practice, the uncoupling was modeled so that the net current in
each filament was set to zero.
Index Terms—Critical current density, electromagnetic mea-
surements, finite-element methods, multifilamentary supercon-
ductors, numerical simulation.
I. INTRODUCTION
T
HE FAST development of wires has led to their
commercialization. The wires are available in kilometer
lengths and are relatively cheap both due to low material cost
and straightforward manufacturing process, which have made
them attractive for applications. However, especially AC loss
properties need to be improved to make these wires more
suitable for applications where electric current changes rapidly.
Low loss properties are not only needed in power frequency
Manuscript received August 02, 2010; accepted December 05, 2010. Date of
publication January 20, 2011; date of current version May 27, 2011. This work
was supported by NESPA, EU FP6 contract MRTN-CT-2006-035619.
L. Rostila is with Columbus Superconductors S.p.A., 16133 Genova, Italy,
and also with Electromagnetics, Tampere University of Technology, 33101 Tam-
pere, Finland (e-mail: lauri.rostila@iki.fi).
E. Demenˇ cík, J.
ˇ
Souc, and P. Kovaˇ c are with the Institute of Electrical Engi-
neering, Centre of Excellence for New Technologies in Electrical Engineering,
Slovak Academy of Sciences, 84104 Bratislava, Slovakia.
S. Brisigotti, G. Grasso, and A. Tumino are with Columbus Superconductors
S.p.A., 16133 Genova, Italy.
M. Lyly and A. Stenvall are with Electromagnetics, Tampere University of
Technology, 33101 Tampere, Finland.
Color versions of one or more of the figures in this paper are available online
at http://ieeexplore.ieee.org.
Digital Object Identifier 10.1109/TASC.2010.2099197
applications but also in magnets that are charged and discharged
repeatedly. So, on one hand, low loss wires may not only be
supposed for use in state-of-the-art applications, but on the
other hand, they may enable new applications that have not
been considered feasible before.
Typically, high losses are due to ferromagnetic sheath mate-
rials [1], [2] like Monel, Ni, or Fe. Therefore, the first step to
reduce losses is to find a nonmagnetic replacement [3]–[5]. Re-
cently, further steps have been taken with multi-filament con-
ductors, that are twisted to limit the coupling losses [6], [7],
which can be furthermore reduced with appropriate material
choices and wire designs that aim at low transverse resistivity
like in low loss LTS wire development [8]. Currently, measured
AC loss data from wires is very limited. However, mag-
netization losses of a single filament Ti wire were studied by
Safran et al. [9] with the same setup that was used here, as well.
For this work, we manufactured multi-filament wires with Ti
matrix, which in principle, can be produced in kilometer lengths
already. In addition to the low material cost, this type of wire is
cheap, mechanically strong, light, and practically non-magnetic.
The wire’s AC losses were measured with two techniques: cali-
bration free electrical technique in which the sample is conduc-
tion cooled and conventional electrical technique in which the
cooling is based on LHe. For a comparison, the similar mea-
surements were also made for loss optimized cable [6].
The measurements were compared to calculations obtained
with modified Brandt’s method [10], in which -charac-
teristics have been taken into account [11]–[14]. Filaments’ un-
coupling was modeled so that the net current of each filament
was set to zero, in the same way as presented in Ref. [15]. Some
of the calculations were performed with finite element method
(FEM) software using vector potential formulation [16].
II. WIRE DESCRIPTIONS
Both samples were based on titanium which gives them suit-
able magnetic properties for AC use, mechanical flexibility, and
strength. Sample A, made by Columbus Superconductors, was
composed of 19 Ti sheathed single-filament wires, which were
bundled together into a Ti tube (see Fig. 1(a)). After several
standings and heat treatments at 700 , the final form of the
wire was obtained with superconducting cross-sectional area of
0.536 . Later, to stabilize the wire, some of the supercon-
ducting strands can be replaced with copper ones. However, in
this first trial, copper was not included to simplify the manu-
facturing process, but in principle long length production is fea-
sible.
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