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DRAFT<br />

Table 2.4.21 summarizes the results of such a harmonic analysis for a separation distance between<br />

the quadrupole and hexapole magnet of d = 250 mm, corresponding to the layout. It can be concluded,<br />

that the magnets are independent. Nevertheless a n = 4 and 8 harmonics are observed,<br />

which are forbidden for the 'stand alone' hexapole and quadrupole magnet due to symmetry reasons.<br />

Appearance of these harmonics is a direct result of mutual influence of the magnets on a magnetic<br />

field distribution. Reducing this separation distance even further will amplify the effect. Figure<br />

2.4.68 summarizes the results of the simulations; it has been concluded that the separation distance<br />

should not become less than d = 250 mm, in order to keep the coupling small.<br />

Harmonic amplitudes, 10 -4 rel. units<br />

8<br />

6<br />

4<br />

2<br />

0<br />

-2<br />

-4<br />

-6<br />

8-pole (n=4), dB/dr = 5 T/m<br />

8-pole (n=4), dB/dr = 10 T/m<br />

16-pole (n=4), dB/dr = 5 T/m<br />

16-pole (n=8), dB/dr = 10 T/m<br />

-8<br />

0,15 0,20 0,25 0,30 0,35 0,40 0,45 0,50<br />

X Axis Title<br />

Figure 2.4.68: Strength of the “forbidden harmonics” depending on the separation distance between a<br />

<strong>Super</strong>-FRS quadrupole and hexapole magnet.<br />

2.4.2.5.1 Multiplet assembling<br />

For the manufacturing and assembly of the multiplets the following has to be considered:<br />

• filling factor: 98%. The laminations should be stamped/cut in a way, which allows compensating<br />

this effect by rotating the laminations. Otherwise it might be necessary to add<br />

thin metal sheets in the back leg region for getting the requested packing across the magnet.<br />

• the possibility to construct removable end blocks must be considered.<br />

• the sag of the yoke should be limited by 0.2 mm.<br />

• thickness variation of the block over the cross section must be less than 0.3 mm<br />

• stainless steel structure: all structural elements (endplate, brackets, structural plates) need<br />

tol be made from SS316LN or SS316L.<br />

The centre of field is defined by the position of the yoke laminations. Locating the magnet, and thus<br />

the position of the dipole field, is initially reached by precise mechanical references given on the<br />

63

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