By Howard T. Coffey (auth.), Peter Kittel (eds.)
The Albuquerque conference middle used to be the venue for the 1993 Cryogenic Engineering convention. The assembly was once held together with the foreign Cryogenic fabrics convention. Walter F. Stewart, of Los Alamos nationwide Laboratory, used to be convention chairman. Albuquerque is close to Los Alamos nationwide Laboratory which has been an important contributor to the cryogenics group because the early days of the long island venture. Albuquerque is usually the house of the Air Force's Phillips Laboratory which has a lead position in constructing cryocoolers. this system consisted of 322 CEC papers, greater than a 30% elevate from CEC-91 and 20% greater than CEC-89. This used to be the most important variety of papers ever submitted to the CEC. of those, 249 papers are released the following, in quantity 39 of Advances in Cryogenic Engineering. once more the amount is released in books. This quantity features a cumulative index for the CEC volumes from 1975-1993 (volumes 21,23,25,27,29,31,33,35,37, and 39 of Advances in Cryogenic Engineering). the 1st 20 volumes are listed in quantity 20. A better half cumulative index for the ICMC volumes (volumes 22 via forty) seems in quantity forty. this can be my first quantity as editor. i wouldn't were in a position to have performed it with no the help of the various reviewers. particularly preferred was once the guide left me through the former editor, Ron Fast.
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Additional info for Advances in Cryogenic Engineering
11 . [(I-i). IminH2p,min - Imax . •. (L) oss ioT-constant -- 4" (8) where i =lrllc and Hp = lcd (1 - i). As expected, the transport loss at large field variation is strongly dependent on both critical current at minimum and maximum oscillating field. This loss calculation will be compared with experimental results in the later section of this paper. (8). The following simple relation3 ,5 is easily obtained. (9) EXPERIMENT The transport loss appears as a dynamic resistance of the superconductor under AC magnetic field.
D. 16 (1982), unpublished. 8 K. Oshima and Y. Kyotani, "High-speed transportation levitated by superconducting magnet" Adv. Cryo. Eng. Y. (1974). , Hestra-Verlag, Darmstadt (1989). A. , "Magnetic suspension and guidance for high speed rockets by superconducting magnets" J. Appl. Phys. 40:2133 (1969). T. M. W. Barbee, "Suspension and guidance of vehicles by superconducting magnets", JAppl. Phys. 40:2161 (1969). T. Danby, "A 300-mph magnetically suspended train", Mech. Eng. 89:30 (1967). T. Danby, " Dynamically stable cryogenic magnetic suspensions for vehicles in very high velocity transport systems", Recent Advances in Engineering Sciences, 5 (A.
IminH2p,min - Imax . •. (L) oss ioT-constant -- 4" (8) where i =lrllc and Hp = lcd (1 - i). As expected, the transport loss at large field variation is strongly dependent on both critical current at minimum and maximum oscillating field. This loss calculation will be compared with experimental results in the later section of this paper. (8). The following simple relation3 ,5 is easily obtained. (9) EXPERIMENT The transport loss appears as a dynamic resistance of the superconductor under AC magnetic field.
Advances in Cryogenic Engineering by Howard T. Coffey (auth.), Peter Kittel (eds.)