Test Results of the Third LHC Main Quadrupole Magnet Prototype at CEA/Saclay

The construction of the third second-generation main quadrupole magnet prototype for LHC has been completed at CEA/Saclay in November 2000. The magnet was tested at 1.9 K. Similarly to the two first ones, this prototype has exceeded the operating current in one training step and exhibited excellent training memory after a thermal cycle. This paper describes the quench performance and quench start localization determined by means of voltage-taps and a quench antenna system developed in collaboration with KEK. As this magnet was equipped with capacitive gauges, the stresses during cool-down and powering have been recorded and are in agreement with FE computations. The newly designed quench heaters have improved efficiency and reproducibility compared to those of the first generation. Magnetic measurements have been performed at various stages. The cold measurements show minor differences with those at room temperature and are similar to those of the two first magnets of this design. These results prove that the magnets are mechanically stable and confirm the design retained for the series production of the 400 LHC main quadrupoles

The New Superfluid Helium Cryostats for the Short Straight Sections of the CERN Large Hadron Collider (LHC)

The lattice of the CERN Large Hadron Collider (LHC) contains 364 Short Straight Section (SSS) units, one in every 53 m long half-cell. An SSS consists of three major assemblies: the standard cryostat section, the cryogenic service module, and the jumper connection. The standard cryostat section of an SSS contains the twin aperture high-gradient superconducting quadrupole and two pairs of superconducting corrector magnets, operating in pressurized helium II at 1.9 K. Components for isolating cryostat insulation vacuum, and the cryogenic supply lines, have to be foreseen. Special emphasis is given to the design changes of the SSS following adoption of an external cryogenic supply line (QRL). A jumper connection connects the SSS to the QRL, linking all the cryogenic tubes necessary for the local full-cell cooling loop [at every second SSS]. The jumper is connected to one end of the standard cryostat section via the cryogenic service module, which also houses beam diagnostics, current feedthroughs, and instrumentation capillaries. The conceptual design fulfilling the tight requirements of magnet alignment precision and cryogenic performance are described. Construction details, aimed at minimizing costs of series manufacturing and assembly, while ensuring the high quality of this complex accelerator component, are given

A Modular Design for the 56 Variants of the Short Straight Section in the Arcs of the Large Hadron Collider (LHC)

The 360 Short Straight Sections (SSS) necessary for the eight arcs of the LHC machine have to fulfil different requirements. Their main function is to house the lattice two-in-one superconducting quadrupole and various correction magnets, all operating at 1.9 K in a superfluid helium bath. The magnetic and powering schemes of the arcs and the fact that the two proton beams alternate between the inner and outer magnet channels impose 24 different combinations of magnet assemblies, all housed in an identical helium enclosure. The cryogenic architecture of the LHC machine is based on cryogenic loops spanning over one half-cell (53 m) for the 4.6-20 K circuit, over a full cell (107 m) for the 1.9 K circuits, up to the full arc (about 2.3 km) for the shield cooling line. This cryogenic layout, when superimposed to the magnetic scheme, further complicated by the cryostat insulation vacuum sectorisation every 2 cells, creates additional assembly variants, up to a total number of 56. The required flexibility in the manufacture and assembly, as well as economic considerations, have led to a modular design for the different SSS components and sub-assemblies. This modularity allows to "specialise" the SSS at the latest possible assembly step of the "just in time" production line. This paper presents the conceptual design considerations to achieve this modularity, the SSS design retained for the series manufacture, and the assembly procedures recently validated on a prototype program at CERN

Modeling of Electromagnetic NDE of Civil Structures

The inspection of civil structures, such as bridge decks, roadways and masonry is becoming an increasingly important area for the application of NDE methodologies. A variety of methods have been used for detecting flaws, cracks and voids as well as locating structural features such as reinforcing bars and tensioning cables. The large size of civil structures necessitates the use of an NDE technique that is capable of rapid inspection of large areas with good penetration. A candidate approach for such inspection is the microwave NDT method. Microwave energy penetrates dielectric materials such as those encountered in civil structures and consequently inspection can be accomplished using noncontact devices mounted on a fast scanning mechanism. The paper presents a numerical model for simulating electromagnetic scattering from two and three dimensional objects embedded in large structures. Such models are useful in the design and development of systems required for microwave imaging of civil structures.</p

DESIGN OF THE LEP MAIN RING WIGGLERS

Il est prévu d'installer huit aimants ondulateurs à trois pôles dans l'anneau principal du LEP au CERN pour avoir des moyens de diminuer le temps d'amortissement à l'injection et pour contrôler l'émittance horizontale du faisceau. La possibilité d'obtenir des faisceaux polarisés est conservée par le choix d'un champ dans les entrefers des extrémités de seulement 40 % de celui de l'entrefer central. L'intégrale de champ égale à zéro est obtenue par l'adaptation des longueurs des pôles. Nous décrivons la conception de l'aimant, ses exigences à l'excitation et ses performances prévues par des calculs magnétiques à trois dimensions.It is proposed to install eight three-pole wiggler magnets in the LEP main ring at CERN, in order to provide a means both for decreasing the damping time at injection and for controlling the horizontal beam emittance. The possibility of having polarized beams at LEP is retained by the choice of a field in the end gaps which is only 40 % of that in the central gap, the pole lengths being chosen to keep the field integral zero. The paper describes the design of the magnet, its excitation requirements and its performance as predicted by three-dimensional magnetic field computations

Design of the LEP main ring wigglers

It is proposed to install eight three-pole wiggler magnets in the LEP main ring at CERN, in order to provide a means both for decreasing the damping time at injection and for controlling the horizontal beam emittance. The possibility of having polarized beams at LEP is retained by the choice of a field in the end gaps which is only 40 % of that in the central gap, the pole lengths being chosen to keep the field integral zero. The paper describes the design of the magnet, its excitation requirements and its performance as predicted by three-dimensional magnetic field computations