By P. Baggett, N. Delagi, R. Leedy, W. Marshall, S. L. Robinson, J. C. Tompkins (auth.), John Nonte (eds.)

The 3rd annual overseas Industrialization Symposium at the SuperCollider, IISSC-held March 13-15, 1991, in Atlanta, Ga.-was a tremendous good fortune. The variety of attendees, exhibitors, and representatives from overseas international locations exceeded the totals of past years. there have been 740 attendees, representing greater than 2 dozen universities and faculties, 32 states, nine nationwide labs, 6 study facilities, a number of executive entities on the neighborhood, country, and federal point, 182 companies & and 14 international locations. greater than a hundred shows, backed through eighty five organisations, extra to the thrill. "Getting all the way down to company" used to be the topic of this year's Symposium. the truth that the Superconducting SuperCollider (SSC) is certainly underway used to be the message introduced by way of the Symposium's keynote speaker, Dr. Roy Schwitters, and accelerated upon through the hole plenary audio system. The venture is relocating from the drawing board to real building, to improvement and procurement of kit, and to answer of the technical matters concerned about advancing the cutting-edge in parts comparable to idea, controls, structures, metallurgy, qc, administration, cryogenics, energy platforms, detectors, interagency cooperation and investment. Plenary audio system incorporated: Paul Gilbert, Chairman of Parsons Brinckerhoff Quade & Douglas, Inc.

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2i~/z. and z. corr:sp~nds to tte 1axial length of the enclosure in which t~e field is contained. The indices i and n are given by i=O,1,2, ... and n=1,3,5, ... which reflects the angular dipole and axial symmetry. , are determined both by the boundary condition on the inner surfa~e of thn: iron enclosure and by the boundary conditions at the cylindrical surface on which the coil pair lies. The B . r). While the normal gradient component of the magnetic potenti~l 's 1continuous, the potential itself is discontinuous across this surface within the coil area and continuous at all other locations.

Figure 1. , B. , can be obtained using (2) and enforcing the continuity of th~1r~al fiefa. , given in (3). The . e. R 1 cIS. R 1 CIS. C n1 + An1.. (6) The coil shape must be specified to evaluate S .. The coil shape used in the present effort approximately represents th~1circular end turns. This shape is shown in Fig. 3 and is made up of five straight sections which together approximate a circular end turn. In this figure, L /2 is the half straight length of the coil and L is the end turn length of the circular end.

1. 2f"n n; dA (A6b) The solution of these equations for a truncated number of harmonics yields the constants in the vector potential expressions given by (Al) and (A2). It is necessary to obtain the vector potential in the innermost region as well as external to the current region. Since all the sources of field are external to the innermost region only a single set of constants, c l ' is required to describe the vector potential. Further, sin~e the set of constants c3 can be related to the set of constants c l by the free space component oInmagnetic field, the components of the magngtic vector potential internal to the current region may be uniquely identified.

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