Q4 MAGNETS FOR HL-LHC J.M. Rifflet, M. Segreti, E. Todesco WP3 - Q4 magnets for HL-LHC 5th Joint HiLumi LHC-LARP Annual meeting 2015 10 30 Research supported.

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Q4 MAGNETS FOR HL-LHC J.M. Rifflet, M. Segreti, E. Todesco WP3 - Q4 magnets for HL-LHC 5th Joint HiLumi LHC-LARP Annual meeting Research supported by EU FP7 HiLumi LHC - Grant Agreement This work is continued under the collaboration agreement CERN / CEA KE2275/TE

Q4 MAGNETS FOR HL-LHC | P 2 Previous magnetic design using MQ cable Aperture = 90 mm Integrated gradient = 440 T Magnetic length = 3.83 m Nominal gradient = 115 T/m Loadline margin = 20 % Temperature = 1.9 K Nominal current = A Stored energy = 0.73 MJ Differential inductance = 2 × 2.9 mH Parameters 1 layer 3 conductor blocks (octant) 14 turns ( ) 5th Joint HiLumi LHC-LARP Annual meeting

Q4 MAGNETS FOR HL-LHC | P 3 Field quality and unbalanced regime 5th Joint HiLumi LHC-LARP Annual meeting CurrentGradientNormal relative multipoles (× ) in the left aperture (A)(T/m)b1b3b4B5b6b7b10b14b CurrentGradientNormal relative multipoles (× ) in the right aperture (A)(T/m)b1b3B4B5b6b7b10b14b % CurrentGradientNormal relative multipoles (× ) in the left aperture (A)(T/m)b1b3b4b5b6b7b10b14b CurrentGradientNormal relative multipoles (× ) in the right aperture (A)(T/m)b1b3b4b5b6b7b10b14b CurrentGradientNormal relative multipoles (× ) in the left aperture (A)(T/m)b1b3b4b5b6b7b10b14b CurrentGradientNormal relative multipoles (× ) in the right aperture (A)(T/m)b1b3b4b5b6b7b10b14b % unbalanced Nominal current 50 % unbalanced

Q4 MAGNETS FOR HL-LHC | P 4 Field quality 5th Joint HiLumi LHC-LARP Annual meeting % All below one unit

Q4 MAGNETS FOR HL-LHC | P 5 Random geometric field errors 5th Joint HiLumi LHC-LARP Annual meeting % dalphabeta [µm][1/µm][-] Average

Q4 MAGNETS FOR HL-LHC | P 6 5th Joint HiLumi LHC-LARP Annual meeting Simulation : -Collaring (key) -Insulation creep (30 %) -Cooling -Energisation at 110 % of I nom  Magnetic forces are computed at each coil node Mechanical study Mechanical model CAST3M Elastic-plastic

Q4 MAGNETS FOR HL-LHC | P 7 5th Joint HiLumi LHC-LARP Annual meeting min = 10 MPa Azimuthal stress distribution in coil at each main step A self-standing collar solution as mechanical structure is validated Mechanical study

Q4 MAGNETS FOR HL-LHC | P 8 Previous coil ends using MQ cable One of the challenges was the specific cable output B max = 6.1 T (6.0 T in the 2D magnetic design i.e. in the magnet straight part) 5th Joint HiLumi LHC-LARP Annual meeting

Q4 MAGNETS FOR HL-LHC | P 9 Previous coil ends using MQ cable 5th Joint HiLumi LHC-LARP Annual meeting

Q4 MAGNETS FOR HL-LHC | P 10 Protection Specifications Max hot spot temp = 250 K Max voltage to ground = 500 V Voltage detection = 0.1 V Time detection = 10 ms Dump resistor = 32 mΩ QH time of activation = 40 ms ConfigurationsMax temperature (K)Max voltage to ground (V) No Dump No QH QH13968 Dump Dump + QH th Joint HiLumi LHC-LARP Annual meeting

Q4 MAGNETS FOR HL-LHC | P 11 CAD 3D models of all components, tooling and accessories for coil fabrication were ready (end-spacers, copper wedges, beam, mandrel, curing mould…) Curing mould Beam Winding mandrel 5th Joint HiLumi LHC-LARP Annual meeting

Q4 MAGNETS FOR HL-LHC | P 12 CAD 3D model of the single aperture short-model was ready up to the collared coils The internal connection between coils was defined The geometry of the yoke outer diameter is still to be defined with CERN (to take into account the correctors integration in the cold mass) 5th Joint HiLumi LHC-LARP Annual meeting

Q4 MAGNETS FOR HL-LHC | P 13 Winding trial The Cern routine allowed to obtain rapidly the CAD of end-spacers from ROXIE output files A first set of plastic end-spacers was 3D printed at the design office A second set was printed at Cern with Bluestone composite material which can survive the curing temperature The tooling and accessories for the winding trial were fabricated at CEA The tooling and accessories for the winding & curing trial was ready 5th Joint HiLumi LHC-LARP Annual meeting

Q4 MAGNETS FOR HL-LHC | P 14 Winding trial A winding trial performed during the first half of January 2015 validated the geometry of the end-spacers 40 m of insulated cable were received from Cern. This length was sufficient to make two 700-mm long mockups 2 nd winding trial + curing trial was ready to be performed. But STOPPED! 5th Joint HiLumi LHC-LARP Annual meeting

Q4 MAGNETS FOR HL-LHC | P 15 Why it is necessary to change the magnetic design (E. Todesco) 5th Joint HiLumi LHC-LARP Annual meeting New elements Spring 2015: cost and schedule review Large cost of 18 kA power converters – 4.5 MCHF (0.5 MCHF each, compared to  1 MCHF for building the magnet) Spring 2015: beam dynamics simulations a “light” magnet with 3 mH inductance, even with a top class power converter gives for Q4 a tuneshift contribution equivalent to the contribution of the whole triplet Additional elements 18 kA poses problems for test station Ancillary equipment to bring 16 kA to the tunnel are also a overhead This gave reasons to propose a change of design First discussion between CERN and CEA-Saclay in July 2015 New baseline in August, proposal validated in September with the use of 2 layers of MQM cable for the magnetic design

Q4 MAGNETS FOR HL-LHC | P 16 5th Joint HiLumi LHC-LARP Annual meeting Updated magnetic design using 2 layers of MQM cable Since August Aperture = 90 mm (unchanged) Integrated gradient = 440 T Magnetic length = 3.67 m Nominal gradient = 120 T/m Loadline margin = 20 % Temperature = 1.9 K Nominal current = 4590 A Stored energy = 0.81 MJ Differential inductance = 2 × 37.5 mH

Q4 MAGNETS FOR HL-LHC | P 17 Updated coil ends using 2 layers of MQM cable 5th Joint HiLumi LHC-LARP Annual meeting For now, optimization of the return end is quasi finished. Lead end optimization to be done.

Q4 MAGNETS FOR HL-LHC | P 18 Cold test of the single aperture short model The baseline is that the test of the single aperture short model will be done at CEA-Saclay. The solution considered is to use the 8 m vertical cryostat. Cost and labor assessment is in progress Cern will provide the magnetic measurements system 5th Joint HiLumi LHC-LARP Annual meeting

Q4 MAGNETS FOR HL-LHC | P 19 Quaco : New H2020 project (Pre-Commercial Procurement) 5th Joint HiLumi LHC-LARP Annual meeting Proposal submitted to EC in April 2015 for funding R&D for HiLumi Co-funding (70%) of design, engineering and fabrication of 2 Q4 quadrupole by 2 European firm Total contract value: 6.6 M€; max EU contribution: 4.6 M€ Grant agreement signature : November, 23 rd 2015 Start : January 2016 (to be confirmed). 42 months Partners : CERN, CEA, CIEMAT, NBCJ. Leader = CERN (launch tenders on behalf of all partners 3 phases Design (2-4 months); at least 3 contractors Prototype development (10 months) Pilot fabrication (max 22 months); 2 “first of a kind” by 2 contractors

Q4 MAGNETS FOR HL-LHC | P 20 Previous Q4 production for HL-LHC (January 2015) 5th Joint HiLumi LHC-LARP Annual meeting KE2275/TE CEA/CERN collaboration agreement

Q4 MAGNETS FOR HL-LHC | P 21 Actual Q4 production for HL-LHC (new design + QuaCo) With the new magnetic design using MQM cable, the fabrication and test of the short model single aperture is reported to end of 2017/ early th Joint HiLumi LHC-LARP Annual meeting

Q4 MAGNETS FOR HL-LHC | P 22 Conclusion 5th Joint HiLumi LHC-LARP Annual meeting The design of Q4 with MQ (Outer Dipole) cable was nearly finished in June 2015 Low inductance  difficulties of magnet powering  change of cable  use of MQM cable The new design is in progress. It is estimated that about 1 additional year is necessary to finish and test the short model. A new funding approach is used for prototyping phase: PCP 2 “first of a kind” pilots will be built within the QUACO PCP framework. This will prepare for the small series production we seek to hire a short term contract engineer for this project if you know somebody interested, do not hesitate to put us in contact

Q4 MAGNETS FOR HL-LHC Thanks for your attention