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fatigue on critical current and n-value are reported. Fatigue<br />
studies <strong>in</strong>clude stra<strong>in</strong>s up <strong>to</strong> 0.1 %. Scann<strong>in</strong>g electron<br />
micrographs of <strong>the</strong> fatigued conduc<strong>to</strong>rs are used <strong>to</strong> identify<br />
<strong>the</strong> sources of failure <strong>in</strong> conduc<strong>to</strong>rs.<br />
WEA02PO10<br />
Quench Behavior of YBa2Cu3O7 Coated Conduc<strong>to</strong>rs<br />
with an AC Transport Current<br />
J. Schwartz, U. Trociewitz, NHMFL; D. Knonll, D. Nguyen,<br />
P. Sastry, X. Wang, G. Zhang, Center for Advanced Power<br />
Systems, Florida State University; C. Thieme, American<br />
Superconduc<strong>to</strong>r Corp.<br />
Normal zone creation and quench propagation<br />
measurements were performed on YBa2Cu3O7 coated<br />
conduc<strong>to</strong>rs with AC transport current. The m<strong>in</strong>imum<br />
quench energy and <strong>the</strong> quench propagation velocity were<br />
measured as a function of temperature, AC transport<br />
current and frequency. Self-field AC losses of <strong>the</strong> tapes<br />
were also measured at <strong>the</strong> same temperatures and<br />
currents <strong>to</strong> calculate <strong>the</strong> <strong>in</strong>ternal <strong>the</strong>rmal loads. The<br />
samples were conductively cooled <strong>in</strong> vacuum us<strong>in</strong>g a<br />
cryocooler. A resistive heater was used <strong>to</strong> create a local<br />
normal zone whose propagation was followed through<br />
temperature and voltage measurements along <strong>the</strong> sample<br />
length. An analysis of <strong>the</strong> results is presented.<br />
WEA02PO11<br />
Temperature Dependence of Critical Currents and AC<br />
Losses of Bi2Sr2Ca2Cu3Ox and YBa2Cu3Ox Tapes<br />
J. Schwartz, U. Trociewitz, NHMFL; D. Knonll, D. Nguyen,<br />
P. Sastry, X. Wang, G. Zhang, Center for Advanced Power<br />
Systems, Florida State University; C. Thieme, American<br />
Superconduc<strong>to</strong>r Corp.<br />
Critical currents and AC transport losses of YBa2Cu3Ox<br />
and Bi2Sr2Ca2Cu3Ox tapes were measured between 40 K<br />
and 80 K. The AC losses were measured electrically at<br />
power frequency us<strong>in</strong>g <strong>the</strong> lock-<strong>in</strong> method. The samples<br />
were conduction cooled by a cryocooler and a temperature<br />
controller was used <strong>to</strong> ma<strong>in</strong>ta<strong>in</strong> a constant temperature. AC<br />
losses were measured for transport current frequencies<br />
between 50 Hz and 500 Hz. Results of <strong>the</strong> analysis of <strong>the</strong><br />
temperature and frequency dependence of critical current<br />
and AC losses are presented.<br />
WEA02PO12<br />
Optimization and Design of <strong>the</strong> Permanent<br />
Magnet Guideway with <strong>the</strong> High Temperature<br />
Superconduc<strong>to</strong>r<br />
H. Song, J. Zheng, X. Wang, S. Wang, J. Wang, Southwest<br />
Jiao<strong>to</strong>ng University.<br />
To optimize <strong>the</strong> high temperature superconduc<strong>to</strong>r (HTS)<br />
and permanent magnet guideway (PMG) levitation system,<br />
<strong>the</strong> levitation and guidance forces were calculated for<br />
different k<strong>in</strong>ds of <strong>the</strong> PMG. Given a cross section area of<br />
<strong>the</strong> permanent magnet and <strong>the</strong> superconduc<strong>to</strong>r arrays, <strong>the</strong><br />
ratio between <strong>the</strong> thickness and width of <strong>the</strong> PMG has<br />
adverse <strong>in</strong>fluence on levitation and guidance force. It<br />
seems that, <strong>the</strong> more <strong>the</strong> thickness, <strong>the</strong> more <strong>the</strong> levitation<br />
force, <strong>the</strong> less <strong>the</strong> guidance force. Moreover <strong>the</strong> materials<br />
and geometries of <strong>the</strong> PMG were verified, it was found that<br />
<strong>the</strong> iron has great <strong>in</strong>fluence on <strong>the</strong> flux distribution and<br />
even <strong>the</strong> levitation or guidance force. Additionally, <strong>the</strong><br />
cross section of <strong>the</strong> PMG was changed from rectangle <strong>to</strong><br />
trapezium <strong>in</strong> size and its optimum design was present for<br />
<strong>the</strong> given HTS arrays <strong>in</strong> <strong>the</strong> end.<br />
WEA02PO13<br />
Alternat<strong>in</strong>g current characterization of <strong>the</strong> HTS<br />
Bi2223/Ag High Strength Tape under magnetic field<br />
produced by direct current<br />
E. Ruppert Filho, R. Cassiola<strong>to</strong> de Freitas, State University<br />
of Camp<strong>in</strong>as; C. Alber<strong>to</strong> Baldan, C. Yujiro Shigue,<br />
Chemical Eng<strong>in</strong>eer<strong>in</strong>g Faculty of Lorena.<br />
HTS tapes are commercially available for applications <strong>in</strong><br />
power system devices. However <strong>to</strong> do that it is necessary<br />
<strong>to</strong> have <strong>the</strong> superconduc<strong>to</strong>r material characteristic curve<br />
which relates <strong>the</strong> values of <strong>the</strong> critical AC electrical current<br />
circulat<strong>in</strong>g <strong>in</strong> <strong>the</strong> material with <strong>the</strong> magnetic flux density at<br />
<strong>the</strong> material surface at 77K. This paper presents a<br />
methodology <strong>to</strong> construct <strong>the</strong> characteristic curve of <strong>the</strong><br />
HTS Bi2223/Ag High Strength Tape, manufactured by <strong>the</strong><br />
American Superconduc<strong>to</strong>r, under DC magnetic field us<strong>in</strong>g<br />
a short material sample. The DC magnetic field is produced<br />
by an electromechanical device constituted by a magnetic<br />
core with a small air-gap and an <strong>in</strong>sulated copper wire coil<br />
wound on one of its columns carry<strong>in</strong>g DC electrical current.<br />
The material sample is <strong>in</strong>serted <strong>in</strong> <strong>the</strong> air-gap firstly <strong>in</strong><br />
perpendicular position, and after <strong>in</strong> parallel position, related<br />
<strong>to</strong> <strong>the</strong> air-gap magnetic field . Many different curves relat<strong>in</strong>g<br />
rms AC voltage between <strong>the</strong> sample term<strong>in</strong>als with <strong>the</strong> AC<br />
rms current <strong>in</strong> <strong>the</strong> sample are constructed for different<br />
values of <strong>the</strong> magnetic flux density. The critical current<br />
value for each magnetic flux density value is <strong>the</strong> one w<strong>here</strong><br />
<strong>the</strong> voltage on <strong>the</strong> sample reaches a def<strong>in</strong>ed value. Care<br />
must be taken with <strong>the</strong> measurements and position<strong>in</strong>g of<br />
<strong>the</strong> sample <strong>in</strong> <strong>the</strong> test assembly. The methodology, data<br />
test assembly, a lot of results for perpendicular and parallel<br />
position of <strong>the</strong> tape and <strong>the</strong> conclusions are completely<br />
reported <strong>in</strong> <strong>the</strong> paper.<br />
WEA02PO14<br />
Analysis of residual Bi-2212 <strong>in</strong> extracted Bi-2223/Ag<br />
filaments us<strong>in</strong>g X-ray diffraction<br />
O. van der Meer, B. Metz, S. Harkema, B. ten Haken, H.<br />
ten Kate, University of Twente, Low Temperature Division;<br />
V. Vonk, H.Graafsma, ESRF.<br />
Bi-2223/Ag superconduct<strong>in</strong>g tapes are made by a powder<strong>in</strong>-tube<br />
process <strong>in</strong> which <strong>the</strong> Bi-2212 phase is converted<br />
<strong>in</strong><strong>to</strong> <strong>the</strong> desired Bi-2223 phase dur<strong>in</strong>g several heat<br />
treatments. The critical current density Jc of state-of-<strong>the</strong>-art<br />
Bi-2223/Ag tapes <strong>in</strong> self field is about 400 A/mm2, which is<br />
about 15-20% of <strong>the</strong> maximum local values found by<br />
magne<strong>to</strong>-optical imag<strong>in</strong>g. Magnetization experiments<br />
<strong>in</strong>dicate that <strong>the</strong> residual 2212 concentration is closely<br />
correlated <strong>to</strong> <strong>the</strong> Jc of <strong>the</strong> superconduc<strong>to</strong>r. However such<br />
experiments provide no spatial <strong>in</strong><strong>format</strong>ion about <strong>the</strong><br />
location of 2212 still present <strong>in</strong> <strong>the</strong> tape. Quantitative<br />
<strong>in</strong><strong>format</strong>ion on <strong>the</strong> local amount of Bi-2212 and its exact<br />
location is obta<strong>in</strong>ed from X-ray diffraction measurements. A<br />
very small but powerful X-ray beam of 1.5x13 µm2 is used<br />
provided by <strong>the</strong> ESRF. We studied <strong>the</strong> variation <strong>in</strong> residual<br />
Bi-2212 concentrations <strong>in</strong> three different filaments<br />
extracted from one tape and also at different location with<strong>in</strong><br />
<strong>the</strong> s<strong>in</strong>gle filament. Regions of 5-20 µm size with lower and<br />
higher Bi-2212 concentrations are observed. In <strong>the</strong> paper<br />
<strong>the</strong> experimental set-up is presented, characteristic results<br />
are presented and <strong>the</strong> results are <strong>in</strong>terpreted <strong>in</strong> relation <strong>to</strong><br />
<strong>the</strong> transport properties of <strong>the</strong> Bi-2223 filaments.<br />
WEA02PO15<br />
Critical current degradation of Bi-2223 composite<br />
tapes <strong>in</strong>duced by cyclical de<strong>format</strong>ion and fatiguerelated<br />
effects<br />
C.Y. Shigue, U. Oliveira, F. Carvalho-Junior, C. Baldan,<br />
DEMAR/FAENQUIL; E. Ruppert-Filho, State University of<br />
Camp<strong>in</strong>as.<br />
Superconduc<strong>to</strong>rs based on <strong>the</strong> HTS Bi2Sr2Ca2Cu3Ox (Bi-<br />
2223) compound embedded <strong>in</strong> an Ag matrix have been<br />
93 MT-19 2005, Genova