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Abstracts Brochure - CERN

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MOPCH189<br />

MOPCH190<br />

MOPCH191<br />

26-Jun-06 16:00 - 18:00 MOPCH — Poster Session<br />

Calculating the Muon Cooling within a MICE Liquid Absorber<br />

The key elements of the Muon Ionization<br />

M.A. Green (LBNL) S.Q. Yang (OXFORDphysics)<br />

Cooling Experiment (MICE) cooling channel<br />

are the absorbers that are a part of the MICE<br />

absorber focus coil modules (AFC modules). The boundaries of room temperature solid absorbers are well defined.<br />

The density of most solid absorber materials is also well understood. The properties of solid absorber are most<br />

certainly understood to 0.3 percent. The MICE liquid absorbers are different in that their dimensions are a function<br />

of the absorber temperature and the fluid pressure within the absorber. The second element in the liquid absorber is<br />

the variability of the liquid density with temperature and pressure. While one can determine the absorber boundary<br />

within 0.3 percent, the determination of the liquid density within 0.3 percent is more difficult (particularly with liquid<br />

helium in the absorber). This report presents a method of calculating absorber boundary and the cooling performance<br />

of the MICE absorbers as a function of fluid temperature and pressure.<br />

Cryomodule Development for Superconducting RF Test Facility (STF) at KEK<br />

K. Tsuchiya, H. Hisamatsu, M. Masuzawa, H. Matsumoto, S.<br />

Noguchi, N. Ohuchi, T. Okamura, K. Saito, A. Terashima (KEK)<br />

104<br />

Current status of the cryomodule development<br />

for superconducting RF test facility,<br />

STF, at KEK is presented. The objective of<br />

the STF construction is to have an experience<br />

of 5-m long cryomodule fabrications and to learn an operational method of superconducting RF cavities. The STF<br />

consists of two 5-m long cryomodules, each housing four 9-cell cavities (one for 35 MV/m and the other for 45 MV/<br />

m). In addition to the cavity type, each cavity has variations in its appendices. Thus, two cryomodules must have<br />

different structures for the cavity support and for the port of the RF input coupler. This paper describes the details<br />

of the cryomodule design, the development of the bimetallic joint for connecting the titanium helium vessel to the<br />

stainless steel cooling pipe, and the studies of the magnetic shielding for high quality cavities.<br />

Copper Heat Exchanger for the External Auxiliary Bus-bars Routing Line in the LHC Insertion<br />

Regions<br />

The corrector magnets and the main<br />

C. Garion, A. Poncet (<strong>CERN</strong>) M. Sitko, B. Skoczen (CUT)<br />

quadrupoles of the LHC dispersion suppressors<br />

are powered by a special superconducting<br />

line (called auxiliary bus-bars line N), external to the cold mass and housed in a 50 mm diameter stainless<br />

steel tube fixed to the cold mass. As the line is periodically connected to the cold mass, the same gaseous and liquid<br />

helium is used for cooling the magnets and the line. The final sub-cooling process (from 4.5 K down to 1.9 K) consists<br />

of the phase transformation from liquid to superfluid helium. It is slightly delayed with respect to the magnets. To<br />

accelerate the process, a special heat exchanger has been designed. Located in the middle of the dispersion suppressor<br />

portion of the line it consists in creating a local sink of heat extraction, providing two additional lambda fronts that<br />

propagate in opposite directions towards the line extremities. Both the numerical model and the sub-cooling analysis<br />

are presented in the paper for different configurations of the line. Design, manufacturing and integration aspects of<br />

the heat exchanger are described. Finally, the results of the qualification tests and the expected performance of the<br />

line are given.

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