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Abstracts Brochure - CERN

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TUPLS012<br />

TUPLS013<br />

TUPLS014<br />

27-Jun-06 16:00 - 18:00 TUPLS — Poster Session<br />

and good electrical behaviour. Beam impedance and magnetic field measurements for the selected stripes are also<br />

presented.<br />

Dynamic Stresses in the LHC TCDS Diluter from 7 TeV Beam Loading<br />

B. Goddard, A. Presland, W.J.M. Weterings (<strong>CERN</strong>) L. Massidda<br />

(New Affiliation Request Pending)<br />

222<br />

In the event of an unsynchronised beam<br />

abort, the MSD extraction septum of the LHC<br />

beam dumping system is protected from<br />

damage by the TCDS diluter. The simulta-<br />

neous constraints of obtaining sufficient beam dilution while ensuring the survival of the TCDS make the design<br />

difficult, with high thermally induced dynamic stresses occurring in the material needed to attenuate the particle<br />

showers induced by the primary beam impact. In this paper, full 3D simulations are described where the worstcase<br />

beam loading has been used to generate the local temperature rise and to follow the resulting time evolution<br />

of the mechanical stresses. The results and the accompanying design changes for the TCDS, to provide an adequate<br />

performance margin, are detailed.<br />

Protection of the LHC against Unsynchronised Beam Aborts<br />

B. Goddard, R.W. Assmann, E. Carlier, J.A. Uythoven, J. Wenninger,<br />

W.J.M. Weterings (<strong>CERN</strong>)<br />

An unsynchronised beam abort in the LHC<br />

could cause major damage to other downstream<br />

accelerator components, in particular<br />

the extraction septum magnets, the experi-<br />

mental low-beta triplet magnet apertures and the tertiary collimators. Although the LHC beam dumping system<br />

includes design features to minimise their frequency, such unsynchronised aborts can arise from several sources and<br />

cannot be excluded. A system of protection devices comprising fixed and moveable passive diluters and collimators<br />

will be built to safely protect the downstream LHC aperture from the mis-directed bunches in case of such a failure.<br />

The sources of unsynchronised abort events are described, together with the requirements and design of the protection<br />

devices and their expected performance. The accompanying operational requirements and envisaged solutions<br />

are discussed, in particular the problem of ensuring the local orbit at the protection devices.<br />

Optics Flexibility and Dispersion Matching at Injection into the LHC<br />

A. Koschik, H. Burkhardt, B. Goddard, V. Kain, V. Mertens, T.<br />

Risselada (<strong>CERN</strong>)<br />

The LHC requires very precise matching of<br />

transfer line and LHC optics to minimise<br />

emittance blow-up and tail repopulation at<br />

injection. The recent addition of a compre-<br />

hensive transfer line collimation system to improve the protection against beam loss has created additional matching<br />

constraints and removed a significant part of the flexibility contained in the initial optics design of the transfer lines.<br />

Optical errors, different injection configurations and possible future optics changes require, however, to preserve<br />

a certain tuning range. Here we present methods of tuning optics parameters at the injection point by using orbit<br />

correctors in the main ring, with the emphasis on dispersion matching. The benefit of alternative measures to enhance<br />

the flexibility, such as the use of more separately powered quadrupoles both in the transfer lines and in the LHC, is<br />

also evaluated.

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