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C ryogenics for cold-powering at LHC P7

C ryogenics for cold-powering at LHC P7. U. Wagner CERN. Topics. B oundary conditions Mechanical Lay-out P rocess Retained cooling circuit Influence on the performance of the existing LHC refrigerators Items do be defined, designed, build and installed Open questions.

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C ryogenics for cold-powering at LHC P7

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  1. Cryogenics for cold-powering at LHC P7 U. Wagner CERN

  2. Topics • Boundary conditions • Mechanical • Lay-out • Process • Retained cooling circuit • Influence on the performance of the existing LHC refrigerators • Items do be defined, designed, build and installed • Open questions 1st HiLumi LHC / LARP

  3. Boundary conditions LHC P7 • Replacement of ARC current feed boxes from LHC tunnel to adistant underground cavern. • ~ 30 kA total current; • ~ 500 m “semi horizontal” SC link line. 1st HiLumi LHC / LARP

  4. Locations I: P7 • Cryogenic supply from existing refrigerators at P6 and P8 • Available fluids for cooling defined by existing infrastructure • Separation of fluids! • No mixing of helium from P6 and P8 refrigerator. 1st HiLumi LHC / LARP

  5. Assumptions • The following assumptions were first formulated in 2010. • They are still the baseline today • Link SC is MgB2 • Splice LTS to MgB2 (magnet to link) requires liquid helium bath. • Max MgB2 temperature 20K • Max. helium temperature 17 K • He consumption for current lead cooling: • As published by A. Ballarino in CERN/AT 2007-5 1st HiLumi LHC / LARP

  6. Helium conditions at interface P7 Worst case considered for study 1st HiLumi LHC / LARP

  7. Transfer line option1: “Flexible” Nexans transfer line • Advantage: • Easier to install; • Potentially allows to install whole length “prefabricated” with MgB2 inside. • Potentially allows to avoid splices on MgB2. • This could be a demonstrator for power lines with interest reaching above the CERN project • Disadvantage: • High heat load; assumed 0.3 W/m cold line; 2.5W/m shield line. 1st HiLumi LHC / LARP

  8. Transfer line option2: Custom made rigid transfer line • Advantage: • Low heat load; assumed 0.04 W/m cold line; 1.5W/m shield line. • These values have been demonstrated for the link line installed in P3. • Allows transfer line with thermal shield supply and return lines. • Disadvantage: • Installation in sections; time consuming; integration of MgB2 will potentially need sections -> splices. • As the consumption on the cryogenic system is relevant for existing installations both options are always compared. 1st HiLumi LHC / LARP

  9. Conclusions from 2011 presentation • For P7, low current case • Heat load on transfer lines defines the cooling flow. • Valid for both TL options. • Flow in excess for current lead cooling is heated to ambient. (“wasted”) • Invest design effort to obtain a transfer line with low heat leak. • Complex custom design transfer line • Shield circuit using 60 K, 18 bar gas (as already realised in P3) 1st HiLumi LHC / LARP

  10. Cost of cooling comparison • Two reference cases • Actual cooling with DFB in the tunnel. • Lower limit. • Reference for comparison as this case does not solve our problem. • LTSC link, as already realised in LHC P3 • Upper limit • Valid reference as possible to implement without any further R&D. 1st HiLumi LHC / LARP

  11. Current Base concept (all sites) • The 17 K limit for the MgB2 link allows only the 5 K, 3.5 bar helium from line C as coolant. • The link will be cooled by helium gas created by evaporating the liquid helium in the spice box. • Thermal shield solution not shown. • Either with 20 K, or with 70 K gas. Helium at max. 17 K Helium from line C 1st HiLumi LHC / LARP

  12. Studied cooling options • In total eight different cooling options were studied • The three most relevant are listed below • “Nexans like” line: • Shield cooling with 20 K gas. • Custom line: • Shield cooling with 20 K gas. • Shield cooling70 K gas and cold return line. 1st HiLumi LHC / LARP

  13. Cooling methods sketch Shield cooling with 20 K gas Nexans and Custom Shield cooling with 70 K gas Custom only 1st HiLumi LHC / LARP

  14. Comparison of cooling methods Values without uncertainty / overcapacity margin Requires TL with three cold lines, discarded for MgB2 as only minor advantage. Kept in mind if integration of Nexans line impossible. Reference . 1st HiLumi LHC / LARP

  15. Equipment modifications • Modify DFBM • Include a link from DFBM to DFBA for the 4 x 600 A leads • (either NbTi or MgB2) • Modify DFBA • Including the “Splice box” and the 13 kA leads for power extraction. • Possibly, but not necessarily with a modified jumper from the QRL 1st HiLumi LHC / LARP

  16. Modified tunnel DFB 1st HiLumi LHC / LARP

  17. Additional equipment • Two link cryostats • Transfer line with shield cooling and integrated MgB2 conductor. • Two new cavern DFB’s • (may be in one cryostat but with separation of the hydraulic circuits) • Two warm lines DN80 • From cavern DFB to helium ring line. 1st HiLumi LHC / LARP

  18. Cavern DFB (principle flow scheme) 1st HiLumi LHC / LARP

  19. Uncertainties as of last year • MgB2 performance and detailed requirements. • Progress has been made, we may consider this a minor uncertainty. • Lead performance and detailed requirements. • Can we assume that the lead performs close to what was published for the LHC lead? • Transfer line design (link cryostat) • Uncertainty remains, less for design but for realisation. 1st HiLumi LHC / LARP

  20. Uncertainties and recommendations 2013 • Nexans like transfer line • Desire to preassemble 500 m of “semi rigid” line with MgB2 conductor. • Handling the preassembled length? • Pulling the conductor without breaking it may be a major challenge! • Alternative: produce the line at the supplier with the MgB2 included; i.e. wind the line around the conductor. • This was quoted by Nexans as possible. • A demonstrator would be needed before any decision. • To be considered when in the project stage to include this approach. 1st HiLumi LHC / LARP

  21. Uncertainties and recommendations 2013 • Any other than the integrated 500 m design might require MgB2 to MgB2 splices in helium gas. • At least a demonstrator that this can be feasible should be developed. • Basically:if we can link MgB2 to HTS at 17K one should be able to realise a link at lower temperature. • The total pressure difference for the 20 K gas between supply and return is only about 150 mbar • The pressure loss budget at the moment is: • 50 mbar in the link line, 50 mbar in the DFB heater, 50 mbar in the return line. • The connection between Q6 (DFBM) and the main link line. 1st HiLumi LHC / LARP

  22. Conclusion 2013 • We are certain that we can supply the cooling for the current feed boxes and the corresponding superconducting link. • We do know sufficiently well what and how we will cool. • In short: • We know what we want to do and we know that we can do it. • But we still need to get a clear idea about the details. 1st HiLumi LHC / LARP

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