Now that YBCO-coated conductors have been commercialized, a number of YBCO coils have been developed. However, their basic performances have not been systematically investigated so far. Here, we demonstrate that of a YBCO double pancake coil. The critical current of an epoxy impregnated YBCO double pancake coil was substantially degraded, i.e. the normal voltage appears above 8 A, only 18 % of that for the dry coil. It was inferred that degradation occurs if the cumulative radial stress developed during cool down exceeds the critical transverse stress for the YBCO-coated conductor (typically 10 MPa). Under these conditions, the conductor was debonded at the interface between the buffer layer and YBCO layers, or fractured in the YBCO layer itself, causing cracks on the YBCO layer, resulting in a significant decline of the critical current. These negative effects are suppressed if the coils are dry wound or impregnated with paraffin, as the bonding strengths between turns are negligible and therefore turns are separated if the cumulative radial stress tends to be tensile. For non-circular coils in which epoxy impregnation is inevitable, degradation due to cumulative tensile transverse stress is still the major problem.

a b s t r a c tCleavage strength for an YBCO-coated conductor at 77 K was investigated with a model experiment. The nominal cleavage strength for an YBCO-coated conductor is extremely low, typically 0.5 MPa. This low nominal cleavage strength is due to stress concentration on a small part of the YBCO-coated conductor in cleavage fracture. Debonding by the cleavage stress occurs at the interface between the buffer layer and the Hastelloy substrate. The nominal cleavage strength for a slit edge of the conductor is 2.5-times lower than that for the original edge of the conductor; cracks and micro-peel existing over the slit edge reduce the cleavage strength for the slit edge. Cleavage stress and peel stress should be avoided in coil winding, as they easily delaminate the YBCO-coated conductor, resulting in substantial degradation of coil performance. These problems are especially important for epoxy impregnated YBCO-coated conductor coils. It appears that effect of cleavage stress and peel stress are mostly negligible for paraffin impregnated YBCO-coated conductor coils or dry wound YBCO-coated conductor coils.

Little is known about the cerebral distribution and clearance of guanidinoacetate (GAA), the accumulation of which induces convulsions. The purpose of the present study was to identify creatine transporter (CRT)‐mediated GAA transport and to clarify its cerebral expression and role in GAA efflux transport at the blood‐cerebrospinal fluid barrier (BCSFB). CRT mediated GAA transport with a Km value of 269 μM/412 μM which was approximately 10‐fold greater than that of CRT for creatine. There was wide and distinct cerebral expression of CRT and localization of CRT on the brush‐border membrane of choroid plexus epithelial cells. The in vivo elimination clearance of GAA from the CSF was 13‐fold greater than that of d‐mannitol reflecting bulk flow of the CSF. This process was partially inhibited by creatine. The characteristics of GAA uptake by isolated choroid plexus and an immortalized rat choroid plexus epithelial cell line (TR‐CSFB cells) used as an in vitro model of BCSFB are partially consistent with those of CRT. These results suggest that CRT plays a role in the cerebral distribution of GAA and GAA uptake by the choroid plexus. However, in the presence of endogenous creatine in the CSF, CRT may make only a limited contribution to the GAA efflux transport at the BCSFB.