1
Motivation Coupling betw een filam entsaffectsthe tapeperform ance M O im aging isidealforspace-resolved studiesofm ultifilam entary tapes Indication ofcoupling in B i-2223 tapes: Com plete shielding ofasm all applied field -2 -1 0 1 2 0 5 10 ta pe B a = 5 m T B (m T) x (m m) (55 filam ents) Resolving individualfilam ents Optical image Magneto-optical image (remanent state after applied field 105 mT atT =20 K) B i-2223 tape: 55 filam ents , tape w idth = 3.7 m m F lux trappe d in individual filame nts can be s een U ncrossed polarizers B=0 B<0 B>0 Experim ent:flux density profiles Profilesareobtained from M O im agestaken in the rem anentstate after B a =105 m T Tem peratureincrease (i)a decreaseofthe trapped flux (ii) smoothening oftheflux profiles. -0 .5 0.0 0.5 1.0 -1 0 -5 0 5 10 19K 41K 57K 62K 69K 76K 80K 86K 93K 102K 108K Tape x (m m) B (m T) fitting region Coupling betw een filam ents isequivalentto through random superconducting interconnections J c inter J c intra Magneto-optical study of the current distribution in multifilament Bi- 2223 tapes with transport current and in applied magnetic field A.V. Bobyl, D.V. Shantsev, M.E. Gaevski, T.H. Johansen, Y.M. Galperin and M. Baziljevich e-mail: [email protected] University of Oslo, Norway, and Ioffe Institute, Russia homepage: http://www.fys.uio.no/faststoff/ltl/index.htm Full penetration: J = J c Field on thetapesurface (from Biot-Savartlaw , 4 filam ents): B(x) = J c intra F(x-x i ) + J c inter F(x-x 4 ) Fitting experim entwith tw o freeparam eters : J c intra , J c i nter Repeating theexperim ent and fitting for varioustemperaturesgives J c intra (T) , J c inter (T) M odel i= 1,2,3 Results L ow T Above 77 K 0 20 40 60 80 1 00 0 10 20 30 40 50 in ter- filam ent intra-filam e nt J c (kA/m ) T (K ) Fitting -1 .0 -0 .8 -0 .6 -0 .4 -0.2 0.0 0 5 10 15 T = 19 K B (m T) x (m m) 0 2 4 6 8 T = 57 K -0 .2 0.0 0.2 T = 108 K real filam ents “coupling” Experim ent Fits Conclusions Flux distributions on the surface ofa m ulti-filam entary tape w ere m easured by M O im aging.The results w ere analyzed quantitatively on the filam entary scale using a critical-state m odelapproach.W e find that: M O imaging shows directly the existence of super- conducting inter-connectionsbetw een filam ents. W e have extracted the T -dependences of the intra- filam entand inter-filam entcriticalcurrents. The relative strength of inter-filam ent coupling grow s steadily as T is raised from 20 K to T c .A tthe highest T, the inter-filam entcurrentbecom es the dom inant,while at low T the global flux profiles are sim ilar to the predictionsfora m onocore tape. flux creep leads to a noticeable flux redistribution during a 200 m s pulse ofsub-criticalcurrent. We thank NST, D enmark, for the Bi-2223 samples. The finan- cial support from the Norwegian Research Council and NATO is gratefully acknowledged. One of us (YMG) has received support from Centre for Advanced Studies, Norway.

Magneto-optical study of the current distribution in multifilament Bi-2223 tapes

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Magneto-optical study of the current distribution in multifilament Bi-2223 tapes with transport current and in applied magnetic field A.V. Bobyl, D.V. Shantsev, M.E. Gaevski, T.H. Johansen, Y.M. Galperin and M. Baziljevich e-mail: [email protected] - PowerPoint PPT Presentation

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Page 1: Magneto-optical study of the current distribution in multifilament Bi-2223 tapes

Motivation

• Coupling between filaments affects thetape performance

• MO imaging is ideal for space-resolvedstudies of multifilamentary tapes

Indication of coupling in Bi-2223 tapes:

Complete shielding of a small applied field

-2 -1 0 1 20

5

10

tape

Ba = 5 mT

B (

mT

)

x (mm)

(55 filaments)

Resolving individual filaments

Optical image

Magneto-optical image (remanent state after applied field 105 mT at T=20 K)

Bi-2223 tape: 55 filaments , tape width = 3.7 mm

Flux trapped in individual filaments can be seen

Uncrossedpolarizers

B= 0

B< 0

B> 0

Experiment: flux density profiles

Profiles are obtained from MO images taken in theremanent state after Ba=105 mT

Temperature increase (i) a decrease of the trapped flux(ii) smoothening of the flux profiles.

-0.5 0.0 0.5 1.0

-10

-5

0

5

10

19K 41K 57K 62K 69K 76K

80K 86K 93K 102K 108K

Tape

x (mm)

B (

mT

)

fittingregion

Coupling between filaments

is equivalent to

through random superconducting interconnections

Jcinter Jc

intra

Magneto-optical study of the current distribution in multifilament Bi-2223 tapes with transport current and in applied magnetic fieldA.V. Bobyl, D.V. Shantsev, M.E. Gaevski, T.H. Johansen, Y.M. Galperin and M. Baziljevich e-mail: [email protected]

University of Oslo, Norway, and Ioffe Institute, Russia homepage: http://www.fys.uio.no/faststoff/ltl/index.htm

• Full penetration: J = Jc

• Field on the tape surface(from Biot-Savart law, 4 filaments):

B(x) = Jcintra F(x-xi) + Jc

inter F(x-x4)

• Fitting experiment with two free parameters:

Jcintra , Jc

inter

• Repeating the experiment and fitting forvarious temperatures gives

Jcintra(T) , Jc

inter (T)

Model

i=1,2,3

Results

Low T

Above 77 K

0 20 40 60 80 1000

10

20

30

40

50

inter-filament

intra-filament

J c (k

A/m

)

T (K)

Fitting

-1.0 -0.8 -0.6 -0.4 -0.2 0.0

0

5

10

15

T = 19 K

B (

mT

)

x (mm)

0

2

4

6

8

T = 57 K

-0.2

0.0

0.2T = 108 K

real filaments “coupling”

ExperimentFits

Conclusions

Flux distributions on the surface of a multi-filamentarytape were measured by MO imaging. The results wereanalyzed quantitatively on the filamentary scale using acritical-state model approach. We find that:

• MO imaging shows directly the existence of super-conducting inter-connections between filaments.

• We have extracted the T-dependences of the intra-filament and inter-filament critical currents.

• The relative strength of inter-filament coupling growssteadily as T is raised from 20 K to Tc. At the highest T,the inter-filament current becomes the dominant, whileat low T the global flux profiles are similar to thepredictions for a monocore tape.

• flux creep leads to a noticeable flux redistributionduring a 200 ms pulse of sub-critical current.

We thank NST, Denmark, for the Bi-2223 samples. The finan-cial support from the Norwegian Research Council and NATO

is gratefully acknowledged. One of us (YMG) has receivedsupport from Centre for Advanced Studies, Norway.