1 / 33

Hadron Collider Breakout Session Summary

Hadron Collider Breakout Session Summary. D. Schulte, L. Bottura , B. Goddard, M. Jimenez. Programme. Pleas for Help and a Promise …. Conclusion. Please help by signing up for the email lists FCC-hh- design@cern.ch FCC-hh- beamdynamics@cern.ch FCC-hh- injectors@cern.ch

mahala
Download Presentation

Hadron Collider Breakout Session Summary

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Hadron Collider Breakout Session Summary D. Schulte, L. Bottura, B. Goddard, M. Jimenez

  2. Programme

  3. Pleas for Help and a Promise …

  4. Conclusion • Please help by • signing up for the email lists • FCC-hh-design@cern.ch • FCC-hh-beamdynamics@cern.ch • FCC-hh-injectors@cern.ch • FCC-hh-technologies@cern.ch • FCC-hh-magnets@cern.ch • reviewing and improving our parameters • helping to prepare choices for the baseline design • preparing the future collaboration Will have video meetings Will provide a list of critical issues Actual work needed already now

  5. Some Volunteers …

  6. F. Petrov

  7. A. Seryi

  8. S. Chattopadhyay, Cocroft

  9. Some Things to Address …

  10. M. Jimenez • Technology Challenges and Breakthroughs • Have a list with technical challenges that need to be addressed • And breakthroughs that are required (will push technology in general) • Very good place to find your favorite subject for the collaboration

  11. M. Schaumann • First Look at the Ion performance • Ion luminosity seems good using LHC injector chain • Main luminosity limitations are from the injector chain • Ions place a significant constraint on interaction region design

  12. Magnets …

  13. Breakout-magnets: summary L. Bottura Thoughts on a Friday night Valentine’s day, 2014

  14. Superconductors • Material research: the FCC superconductors are not looking like anything we know from the past, nor HL-LHC. The present potential for improvement is in the range of 20 %... 50%, not enough • 5 years target: work on carrier density, pinning, grains to improve performance in present high-field materials • 10 years target: consider other materials (Fe-based, MgB2, round REBCO) • Very large scale material requirements for LTS (10x ITER Nb3Sn production) and HTS (much above anything done so far) • Actions proposed: • Launch a focussed 16 T Nb3Sn conductor program (factor 2 Jc at 18 T) • Pursue work on HTS materials to make them suitable for accelerator magnets • Consider other issues (protection, filaments/field quality, homogeneity and yield for low cost) • The LTHFSM Workshop could be an incubation center for material R&D • Open questions: • Are exotic materials (Fe-based SC) a realistic candidate for R&D ?

  15. Magnet technology • HL-LHC and companion HFM programs are exploring the 11...13 T operating field range, with ultimate field levels that are relevant to FCC (Fresca2), much experience can be drawn from these programs • Is there a “barrier” at 15 T, or is this only perceived as such ? • In the 16…20 T field range it is not clear what is the best geometry (block, cos-theta, CCT), examine them all • The present design margin, in the range of interest, is very large (20 %) – how to decrease it ? • Training, we cannot afford so many (> 10) quenches • Magnet protection is an issue both for LTS (energy density vs. JE) and HTS (propagation speed and detection)

  16. Matters of optima • Tunnel length, operating field and temperature, SC material selection, are parameters affecting greatly the location of the optimum (minimum cost, maximum performance) • Other constraints (e.g existing infrastructure), and benefits (e.g. the value of R&D at the field frontier) must be considered

  17. My Comments on Magnets • Very interesting for a non-expert • Much to be learned, thanks for the insight • Very active field • Quite some interaction with other experts required for optimisation • Should not forget the insertion magnets • Goal for b*=0.1m (Rogelio Tomas) • Challenges magnets • But helps for overall design • Faster ramp of LHC magnets (O(3minutes)) appears possible • But some studies to be performed • Many issues of LHC re-use as injectors • Need to evaluate aperture needs for injector in 100km ring • Added some slides in the reserve on the different individual talks

  18. In practice • Define a direction for relevant R&D, set challenging (but realistic) targets, describe impact of this technology on other fields, and describe a development plan into a roadmap document to be contributed by the collaborators and edited within the scope of the FCC study • This roadmap document will become a reference for future accelerator magnets R&D proposals (e.g. US-DOE, Horizon 2020), and can be used as a basis of collaboration for FCC design and hardware R&D work • Time scale: 3 months (tough !)

  19. Conclusion • First volunteers • Also some private discussions with no presentation • List of critical items to work on is progressing • Technical items shown by Miguel • Promised to produce first draft soon • Very good discussion on magnets • Progress visible • Still new design ideas • Workplan in preparation • Will continue with video meetings Many thanks to the speakers and the chair Mike Syphers for almost keeping the schedule And to all participants

  20. The Summary that I Cannot Show

  21. Some Key Points from the Talks D.S., Brennan Goddard

  22. Magnets David Larbalestier: LTS and HTS Material Issues for 16 and 20 T Applications • Nb3Sn is still plan A • But have HTS cable, still issues to be addressed AmaliaBallarino: Material R&D toward 16-20T horizon • ITER first large-scale user of Nb3Sn(800 A/mm2 at 12 T, 4.2 K): 500t • HL-LHC needs 2500 A/mm2 at 12 T, 4.2 K • FCC with 16 T magnets: 4,500 tons of Nb3Sn and 10,000 tons on NbTi • FCC with 20 T: 1,400 tons HTS, 6,300 tons Nb3Sn, 11,000 tonsNbTi

  23. Magnets Paolo Ferracin: Overview of HiLumi low beta and FRESCA2 magnets • FRESCAII is block magnet to test HTS inserts • Forces and stresses on coil for FRESCA2 comparable to 16-20 T coils MikkoKarpinnen: 11T Experience • Many lessons learned from the 11T work for the HL upgrade Steve Gourlay: SC Magnet Developments Towards 16T Nb3SN Dipoles • A slanted solenoid design looks attractive and should be tested

  24. Magnets Ezio Tedesco: Design Options for the 15-20T Range • We should review the design margin, it cost a lot Peter McIntyre: Low Cost Magnet Design • We should think about the cost not focus only on the field AttilioMilanese: Injector Magnet Considerations • The LHC magnets can be made to ramp up in 3 minutes, with some sissues to be addressed Rogelio Tomas: Insertion Magnet Challenges • Insertion magnets are also important • Should aim for b=0.1m

  25. David Larbalestier: LTS and HTS Material Issues for 16 and 20 T Applications

  26. 16 T for 100 TeV in 100 km AmaliaBallarino Cosine theta type magnet, Nb-Ti and Nb3Sn. Bore  = 40 mm • Material R&D toward 16-20T horizon • ITER will be first large-scale (500t) user of Nb3Sn, with 800 A/mm2 at 12 T, 4.2 K • HL-LHC needs 2500 A/mm2 at 12 T, 4.2 K • Total amount of conductor neededfor 16 T magnets in 100 km collider wouldbeabout 4,500 tons of Nb3Sn and 10,000 tons on NbTi • For 20 T in 80 km tunnel, 1,400 tons HTS, 6,300 tons Nb3Sn, 11,000 tonsNbTi • Productionquantity of HTS is hugebytoday'sstandards - tooearly to evenstartguessingaboutcost 4300 tons Nb3Sn + 10200 tons of Nb-Ti 9 times Nb3Sn for ITER and Nb-Ti for LHC A. Ballarino, CERN

  27. Paolo Ferracin • Overview of HiLumi low beta and FRESCA2 magnets • Low-beta is 7 m long magnet, accelerator quality coils and magnet at 12 T operational field level, Nb3Sn, cos2theta • FRESCA2 is aiming at 15 T dipole field for HTS insert tests, not accelerator quality, block coils • Forces and stresses on coil for FRESCA2 comparable to 16-20 T coils

  28. MikkoKarpinnen • 11T Experience • Many lessons learned from the 11T work for the HL upgrade • Cannot list them here • Useful input for future R&D

  29. Steve Gourlay The Canted Cosine-Theta (CCT) Magnet • SC Magnet Developments Towards 16T Nb3SN Dipoles • Different winding scheme potentially could make magnets cheaper by reducing stress • Paradigm change? • This seems well worth exploring “perfect” current distribution Superconducting Magnet Group - S.Caspi

  30. Design Options for the 15-20T Range • Need to review required margin Ezio Tedesco

  31. Peter McIntyre • Low Cost Magnet Design • Should consider an overall cost optimisation leaving the dipole field as a free parameter • 5 T 10 K dipole is excellent candidate for rapid-cycling injector

  32. Injector Magnet Considerations • Different options of injector magnets investigated • SPS with Nb3Sn magnets takes 5-10 minutes to ramp, require 25 ramps • LHC magnets can likely ramp faster than now with some modifications in the power supplies (2-3 minutes) • Option with normal magnets in the 100km ring need to be reviewed for impedance and required aperture Attilio Milanese

  33. R. Tomas • Insertion Magnet Challenges • The interaction region contains challenging magnets • They can drive the system design • The interaction region impacts the overall design strongly(the beta-function determines the required beam current) • Should aim for beta-function of 0.1m • High field magnet development essential even if cost is high

More Related