Magnets for RHIC Page: 3 of 6
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000 - -
0 0 I.TR w'
b ---"- 8 --- -
- OSI- - CR
06 003 0201BC2 C
OJ0 pINNER INSERTION
Figure 3. Magnet Layout in the Intersection
Table 1. Characteristics of the Arc and
Intersection Region Dipoles and
Quadrupoles for RHIC (100 GeV/amu
Coil ID Length
130 1.34-2.21 57.4 T/m
80 1.03-1.74 67.4 T/m
Table 2. RHIC Magnet Inventory
Standard Aperture Magnets
Sextupoles @ Q9
Large Aperture Magnets
Skew quadrupoles @ Q2 or Q
A cross section of the current dipole coil de-
sign is shown in Fig. 4. It has a single layer
BORE TUBE \
R=36.45 mm-j 50.01
Figure 4. RHIC Dipole Coil Cross Section.
superconducting coil designed to provide the
required 3.45 T bending field for 100 GeV/amu ions
with a generous margin of safety. The
superconductor used is the same as that used for
the outer coil of the Superconducting Super
Collider (SSC) magnet. Figure 5 shows a cross sec-
Skew quadrupoles 24
Although there are less dipoles than there
are quadrupole and corrector magnets, the arc
dipoles nevertheless remain the dominant cost item
in the machine. For this reason, the R&D effort
has focussed on this device. Various models have
been built, including four in industry,
culminating in a half-length model with prototype
cross section that was built and tested in the past
Nb Ti COMPOSITE WIRE:
DIAMETER 0.6408 RE
-5 m DIAMETER EACH;
b) FIBERGLAES -EPOXY;
KEYSTONE ANGLE -L.*
Figure 5. Cross Section of RHIC Superconductor
- 36 -
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H., Willen E. Magnets for RHIC, report, May 1, 1986; United States. (digital.library.unt.edu/ark:/67531/metadc870325/m1/3/: accessed December 18, 2018), University of North Texas Libraries, Digital Library, digital.library.unt.edu; crediting UNT Libraries Government Documents Department.