1988
DOI: 10.1109/20.11567
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Deflection of weakly magnetic materials by superconducting OGMS

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Cited by 15 publications
(5 citation statements)
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“…r 1rsm where 2w is the width and 2h is the height of the thread; x rsm = x m − X rs , and z rsm = z m − Z rs . α 1rsm , α 2rsm , β 1rsm , β 2rsm , r 1rsm , r 2rsm , ρ 1rsm , and ρ 2rsm are defined by figure 4, [17].…”
Section: Magnetic Flux Density Calculationmentioning
confidence: 99%
“…r 1rsm where 2w is the width and 2h is the height of the thread; x rsm = x m − X rs , and z rsm = z m − Z rs . α 1rsm , α 2rsm , β 1rsm , β 2rsm , r 1rsm , r 2rsm , ρ 1rsm , and ρ 2rsm are defined by figure 4, [17].…”
Section: Magnetic Flux Density Calculationmentioning
confidence: 99%
“…The magnetic flux density can be obtained from an analytical twodimensional model where each coil is replaced with two long straight conductors. One conductor with the centre at (x 0i , y 0i ) produces the magnetic flux density B i in the point (x, y) [6]…”
Section: Problem Statementmentioning
confidence: 99%
“…Currently, the University of Twente is constructing a superconducting NbTi-based magnet system that will be installed in the first superconducting MDS demonstrator MDS set-up. The required magnetic field profile is different from other superconducting systems that have been developed for a variety of other separation systems, [3][4][5][6][7], and thus the optimum electromagnet configuration for MDS will also be different. Specifically, the gradient of the magnetic field strength should ideally by onedirectional, since field variations in multiple directions tend to re-mix the feed stream.…”
Section: Introductionmentioning
confidence: 98%