YBa2Cu3Oy HTS, field cooled in 2.3 T, are used in place of permanent magnet
s (PM) as the source of field in magnetic levitation. They produce fields e
qual to their maximum trapped field (B-t,B-max) up to 1.6 T in this work. S
ince commonly used PM produce only similar to0.5 T, replacing them with suc
h HTS trapped field magnets (TFM) significantly increases the magnetic fiel
d and thus the levitation force (F-L) and pressure.
The TFM is opposed by a second HTS which is (1) zero field cooled, (2) cool
ed adjacent to the TFM, or (3) field cooled in 2.3 T. F-L increases by a fa
ctor of 4-10 compared to common levitation systems with PM, up to 393 N (12
5 N/cm(2)). F-L(B-t,B-max) is normalized to a common curve for data sets wi
th different TFM. The stability of the various configurations is determined
by lateral force measurements.