By Hans Ullmaier
ISBN-10: 3540074244
ISBN-13: 9783540074243
ISBN-10: 3540379630
ISBN-13: 9783540379638
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Extra resources for Irreversible Properties of Type II Superconductors
Example text
G. 20) The macroscopic large ces number force of i n d i v i d u a l and p i n n i n g per u n i t written +K Pv = volume centers. with K p(K) on a flux are a b l e between vorti- of i n t e r a c t i o n s K and K + dK, P v c a n be dK (49 for two force line. 1) is p o s s i b l e is c o m p l e t e l y rigid and cases: (a) If the v o r t e x ning K between If p(K) dK is the n u m b e r forces to p r o d u c e a straightforward only forces of a o and distribution they interaction action o K o is the m a x i m u m exert the c o m b i n e d as $ -K Pv r e p r e s e n t s lattice large the n u m b e r number of statistically of i n t e r a c t i o n s with if there distributed force K will pinbe 55 (b) (o) i ........
C o m p a r e for the (see a l s o C h a p t e r 5). 53 4. Relations between Macroscopic and Local Forces After the discovery of high field hard superconductors in 1961, a rapidly growing number of papers, d e s c r i b i n g measurements of critical current densities Jc in various materials was published. The results clearly d e m o n s t r a t e d the importance of lattice defects conductors. in the current carrying capacity of hard super- A drawback of this early work, the m e t a l l u r g i c a l vaguely known.
5 which depends on the lattice type and the o r i e n t a t i o n of the slip planes of the dislocations with respect to VB. By comparing observed dB/dx values ESSMANN and TRAUBLE Eq. 61) PFD and (1969) were able to show that is indeed fulfilled within the range of low flux den- sities accessible to the d e c o r a t i o n techniques, i,e. the dislo- cations alone account for the observed flux density gradient. They suggested that this is generally true, but their conclusion was questioned by CAMPBELL and EVETTS the following reasons.
Irreversible Properties of Type II Superconductors by Hans Ullmaier
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