Gradient coil system for nmr machines

Claim 2

Method for the compensation of the magnetic effects of the eddy currents in predetermined zones of an NMR machine provided with a system of gradient coils said to be compensated because said gradient coils are designed to eliminate the magnetic effects of the eddy currents, characterized in that said method comprises a step for the adjusting of the current in these coils so that a magnetic vector potential (A) created by said system of gradient coils or one of the components is reduced to a minimum in said predetermined zones, said components of said magnetic vector potential being geometrical components.

Claim 3

Method according to claim 1 characterized in that the location of the determined zones is chosen so that they are located where there is placed a screen for damping the effects of collapse of a magnetic field (B 0 ) of the NRM machine or a casing of a cryogenic device.

Claim 4

Method according to the claim 1 or the claim 2, characterized in that, for the minimizing, two layers of gradient coils are created in the system.

Claim 5

Method according to the claim 3, characterized in that the layers are made on two gradient mandrels with different radii, respectively called internal and external radii because one of them is inside the other.

Claim 6

Method according to claim 3, characterized in that the two layers are spaced out sufficiently from each another to place, between them, coils for the correction of the main magnetic field of the NMR machine.

Claim 7

Method according to claim 4, wherein gradient coils are made including, on each mandrel, at least two packets of useful conductors each having a given number of conductors, characterized in that a number of useful conductors in a packet of conductors of the external mandrel is intermediate between the numbers of useful conductors of the packets of conductors placed on the internal mandrel.

Claim 8

Method according to claim 4 wherein the conductors of gradient coils of a given type are placed on an interior gradient mandrel, characterized in that these conductors are chosen so that they present conduction sections that are smaller than the conduction sections of the conductors of gradient coils of the same type and are located on an external mandrel.

Claim 9

Method according to claim 3, characterized in that the gradient coils of one and the same type, located on two different layers, are supplied in series.

Claim 10

Method according to claim 4 wherein the system has Z type radiant coils distributed, on each of the internal and external gradient mandrels, in packets of conductors, characterized in that the abscissae measured along the axis Z of the first conductors of the packets of conductors of gradient coils placed on the internal mandrel are respectively smaller and greater than the abscissa of the first conductor of a packet of conductors placed on the external mandrel.

Claim 11

Method according to claim 4 characterized in that coils are made in accordance with the following characteristics: ______________________________________ Z r e n.sub.1 n.sub.2 n.sub.3 d d' d.sub.1 d.sub.2 d.sub.3 ______________________________________ in- 0.386 0.003 2 22 -- 0.0165 -- 0.051 0.248 -- ter- nal ex- 0.481 0.003 -- -- 14 -- 0.036 -- -- 0.177 ter- nal ______________________________________ X or Y r e d d' n.sub.1 n.sub.2 d.sub.1 d.sub.2 D ______________________________________ in- 0.391 0.003 0.016 -- 22 -- 0.0439 0.7479 0.499 ter- nal ex- 0.486 0.003 -- 0.0345 -- 10 0.000 0.8333 0.639 ter- nal ______________________________________ where: XYZ designates the type of gradient coil concerned, r designates the value in meters of the internal radius of a mandrel, e designates the value in meters of the radially measured thickness of the conductors used to form the coils, n 1 represents the number of conductors in the respective packets, d and d' indicate the value in meters of the widths measured longitudinally, d 1 are the abscissae in meters of the packets of conductors.