Measurement Techniques for Superconducting Coils

Abstract

This paper describes some of the experimental methods we have used in building high-field superconducting coils. Field-level measurements have been made using Hall probes, magnetoresistance probes, and search coils. Copper magnetoresistance probes are inexpensive, simple, and reproducible enough for routine testing; such probes can be built into a coil. Reproducibility is better than the normal limits of panel meters or X-Y recorders. The search coil and fluxmeter (or ballistic galvanometer) is used as a primary standard for calibrating other probes. Absolute accuracies of about ½% are attainable by calibration against an NMR probe. We have determined field uniformity by direct measurement of the field gradient. A small coil is oscillated ±1 mm at 10 Hz in the magnetic field. The ac voltage from the oscillating coil, which is directly proportional to the field gradient, is amplified and detected with a lock-in amplifier. Numerical integration of the gradients gives high-resolution field plots. This straightforward apparatus can detect a field gradient of 1 G/cm in a 100 kG field. Our coils are constructed in modules, with each module consisting of a pair of disks or pancakes wound from superconducting tape. It is obviously useful to detect which module in the coil is limiting. For this purpose we use a set of shunt resistors across the modules, and record the voltage across the shunts on an oscillograph as the transition from superconducting to normal state occurs. In this way, one can deduce where the normal region originates in the coil, and can tell something about the way in which it propagates.

Progresses and challenges in the development of high-field solenoidal magnets based on RE123 coated conductors

“…Some of the very first superconducting solenoid magnets built in the 1960s were wound either with V 3 Ga tape or Nb 3 Sn tape, whose geometry and architecture are similar to those of modern CCs. Indeed those magnets exhibited a reduced central field, a sizable remnant field after discharge, and large temporal field drift (at constant operating current) [149][150][151]. Since the beginning of the 1970s multifilamentary wires (NbTi and Nb 3 Sn) have become the standard in the industry.…”