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The iron structure of the Belle detector serves as the return path of
magnetic flux and an absorber material for
KLM [4,6]. It also provides the overall support for
all of the detector components. It consists of a fixed barrel part
and movable end-cap parts, both on the base stand. The barrel part,
shown in
Fig.
, consists of eight KLM blocks and 200-mm thick
flux-return plates surrounding the outermost layers of of the KLM
blocks. Neighboring KLM blocks are joined using fitting blocks. Each
end-cap part can be retracted for an access to the inner detectors.
The weight of the iron yoke is 608 and 524 (= 262
2) tons for
the barrel yoke and end-cap yokes, respectively.
Table:
Main parameters of the solenoid coil.
| Items |
Parameters |
| Cryostat |
|
| Radius: outer/inner |
2.00 m/1.70 m |
| Central field |
1.5 T |
| Total weight |
23 |
| Effective cold mass |
6 |
| Length |
4.41 m |
| Coil |
|
| Effective radius |
1.8 m |
| Length |
3.92 m |
| Conductor dimensions |
3 33 mm |
| Superconductor |
NbTi/Cu |
| Stabilizer |
99.99 % aluminum |
| Nominal current |
4400 A |
| Inductance |
3.6 H |
| Stored energy |
35 MJ |
| Typical charging time |
0.5 h |
| Liquid helium cryogenics |
Forced flow two-phase |
| Cool down time |
6 days |
| Quench recovery time |
1 day |
Figure:
An outlook of the solenoid and the cross sectional view of
the coil.
|
Figure:
Barrel part of the iron yoke.
|
Next: Magnetic Field Mapping of
Up: Detector Solenoid and Iron
Previous: Solenoid Magnet
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Samo Stanic
2001-06-02