Abstract: A device for the safe discharge of a superconducting magnet coil (4) which is located inside a cryostat (2) and superconductively short-circuited by a superconducting switch (7) providing at or in the cryostat (2) a transmitter (10) of electromagnetic energy being located at a temperature level considerably above the cryogenic temperature of the superconducting magnet coil (4), which transmitter can be switched on quickly from outside, and by arranging in the region of the superconducting switch (7) at the cryogenic temperature level of the superconducting magnet coil (4) a receiver (20) for the emitted electromagnetic energy, which transmits the received energy directly or indirectly to a heating device (15) of the superconducting switch (7) or which activates an auxiliary energy source (41) in the region of the superconducting switch (7) , which on its turn effects a heating of the superconducting switch (7), so that it becomes normal-conducting and causes a discharge process of the superconducting magnet c

Abstract: A device for the safe discharge of a superconducting magnet coil (4) which is located inside a cryostat (2) and superconductively short-circuited by a superconducting switch (7) providing at or in the cryostat (2) a transmitter (10) of electromagnetic energy being located at a temperature level considerably above the cryogenic temperature of the superconducting magnet coil (4), which transmitter can be switched on quickly from outside, and by arranging in the region of the superconducting switch (7) at the cryogenic temperature level of the superconducting magnet coil (4) a receiver (20) for the emitted electromagnetic energy, which transmits the received energy directly or indirectly to a heating device (15) of the superconducting switch (7) or which activates an auxiliary energy source (41) in the region of the superconducting switch (7), which on its turn effects a heating of the superconducting switch (7), so that it becomes normal-conducting and causes a discharge process of the superconducting magnet co

Abstract: In order to simplify the process of plotting a pulse sequence controlling the course of an MR experiment, for example an NMR tomographic investigation, by which the excitation of an RF pulse bringing about transverse magnetization, the switching on and off of field gradients acting in different directions, superposed on a constant magnetic field, as well as the acquisition times, it is proposed to generate this pulse sequence by modification of standard pulse sequences and/or by composition from standard pulses. These pulses are offered on a picture screen (22) as simple symbols (42-49), icons, or brief designations for standard pulse sequences (36-41). By clicking-on of the offering fields, for example by means of a mouse (51), these elements can be copied on time axes (58) allocated to them and attached at the suitable release time point onto these axes. The pulse sequence thus determined is stored on-line.