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DRAFT<br />

The water-cooled radiator consists of a 8 mm thick copper plate with grooves comprising three<br />

Ø6mm stainless steel pipes with a Ø4mm inner hole. The pipes are independently connected to the<br />

water supply.<br />

The segment of the current coil consists of 24 turns of radiation-resistant wire with an average<br />

length of l ≈ 2.12 m. The length of one segment wire is L ≈ 51 m. In total, one magnet needs 306 m<br />

of the copper wire.<br />

The radiation-resistant wire has a rectangular cross-section of 14mm×14mm. It consists of the<br />

central copper bus with the cross-section S=1.09 cm 2 , the magnesium oxide layer 1 mm thick and<br />

copper envelope 0.5mm thick.<br />

2.4.2.3.2 <strong>Super</strong>ferric hexapole magnets<br />

We decided to use standalone hexapole magnets in the <strong>Super</strong>-FRS for two reasons:<br />

• the hexapole components which are required for 2 nd -order image aberration correction<br />

have a rather high field,<br />

• the ion-optical coupling coefficients guide the positioning of correction elements.<br />

Most of the required hexapole magnets will be technically realized as superferric magnets and they<br />

will be installed in a common cryostat together with the quadrupole magnets. Figure 2.4.58 shows<br />

the cross section of the magnet and Figure 2.4.59 shows the 3D model. Its pole tip radius is 235 mm<br />

and the yoke diameter is 800 mm. The coil has a cross section of (20 x 20) mm 2 and a maximum<br />

current density of 132 A/mm 2 is required. The calculated field quality in the aperture is found to be<br />

less than ±1⋅10 -4 , see Figure 2.4.60, which is much better than required.<br />

Figure 2.4.58: Cross section of the superferric hexapole magnet (1/6 part).<br />

55

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