By David E. Andrews (auth.), R. W. Fast (eds.)
The 1987 joint Cryogenic Engineering Conference/International Cryogenic fabrics convention used to be held on the Pheasant Run hotel, St. Charles, lliinois from June 14 to 18. Fermi nationwide Accelerator Laboratory, positioned a number of kilometers from Pheasant Run, used to be the host for this convention. there's a good deal of cryogenic study and improvement underway at Fermilab and lots of purposes of cryogenic fabrics and structures are in rou tine, day-by-day use on the Tevatron. The technical application for the joint convention had over three hundred invited and contributed papers from many alternative nations. The CEC board and i've attempted to dramatically shorten the booklet time of this quantity of Advances in Cryogenic Engineering. to be able to support meet the target of the February e-book, I requested the reviewers to accomplish their studies earlier than leaving Pheasant Run, after the convention. i want to thank the entire reviewers for his or her urged and throughtful studies. I a great deal savor the authors following the prescribed structure and responding fast to my requests for revisions.
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Extra info for Advances in Cryogenic Engineering
No. A. , Am. Inst. , New York, (1982), p. 147. 10. O. J. Dragt, Influence of Strongly Curved Large-Bore Superconducting Bending Magnets on the Optics of Storage Rings, Nucl. Instr. and Meth. B 24/25: 877 (1987). 32 TESTING OF A 3 TESLA SUPERCONDUCTING MAGNET FOR THE AMY DETECTOR AT TRISTAN K. Tsuchiya, s. Terada, T. Omori, A. Maki, Y. Doi, T. Haruyama and T. Mito KEK, National Laboratory for High Energy Physics Tsukuba, Ibaraki, Japan K. Asano Hitachi Ltd. Hitachi, Ibaraki, Japan ABSTRACT A 3 tesla superconducting magnet was constructed and installed in an experimental hall at TRISTAN.
The support system must support both the weight of the helium vessel containing the superconducting coil and the axial and radial forces due to the electromagnetic force coming from any non-symmetrical assembly of the solenoid within the iron return yoke. 1 tonnes/mm in the axial and radial directions, respectively. Assuming that the maximum offset of the coil relative to the yoke is 15 mm, the support system was designed to withstand 45 tonnes and 16 tonnes in the axial and the radial directions, respectively.
Z -1000 0 F'ig. 6. 5 Total field, sextupole and octupole components of dipole E 54 versus path length s along reference orbit. 1-'i g 7 Geometry u~ed for computing magnetic field in and transfer map of a 90° bending magnet with mid-plane symmetry. 61 m. needed. 2 T arises at the position indicated in fig. 4 in the end-region of the magnet at an azimuthal angle of 41° measured from the midpoint. 3 K is specified for the conductor. 25 mm . 075 mm thick. A conductor with these specifications has been fabricated by Vacuumschmelze/Hanau.