1 / 19

ILC prototype undulator project

ILC prototype undulator project. James Rochford For the HeLiCal Collaboration. ILC positron source meeting 31 st Jan – 2 rd feb 2007 @IHEP Beijing. HeLiCal Collaboration. CCLRC Technology Rutherford Appleton Laboratory:

macha
Download Presentation

ILC prototype undulator project

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. ILC prototype undulator project James Rochford For the HeLiCal Collaboration ILC positron source meeting 31stJan – 2rd feb 2007 @IHEP Beijing

  2. HeLiCal Collaboration CCLRC Technology Rutherford Appleton Laboratory: D.E. Baynham, T.W. Bradshaw, A.J. Brummitt, F.S. Carr, Y. Ivanyushenkov, A.J. Lintern,J.H. Rochford CCLRC ASTeC Daresbury Laboratory and Cockcroft Institute: A. Birch, J.A. Clarke, O.B. Malyshev, D.J. Scott University of Liverpool and Cockcroft Institute: I.R. Bailey, P. Cooke, J.B. Dainton, L.J. Jenner, L.I. Malysheva University of Durham, CERN and Cockcroft Institute : G.A. Moortgat-Pick DESY: D.P. Barber, P. Schmid

  3. Talk outline • Specification of an undulator for the ILC • 3d modelling of the undulator • Defines period and bore for operating point 80% • Why operate at 80% short sample • Benefits of operating at 90% • Latest test results from experimental prototypes • Summary

  4. Undulator specification • Undulator period: as close as possible to 10 mm • Field on axis: to produce 10 MeV photons (first harmonic) • Field homogeneity: ≤1% • Vacuum bore: to have beam stay clear of 4 mm => about 5 mm for vacuum bore and about 6 mm for magnetic bore • Superconductor (NbTi) working point : about 80% of short sample critical current. • Modular design -module length: 4 m

  5. High mesh density Iron Conductor 3d model of undulator with iron poles Bore Modelling-predictions Conclusion for NbTi a period of 10 mm means very small bore -unpractical! Realistic figures: Beam stay clear – 4 mm Vacuum bore - 5 mm Winding bore - 6 mm Period - 11.5 mm Modelling predicts relationship between the bore and period

  6. Why operate at 80% 1 The RAL design is based on operation the magnet at 80% along the magnet peak field load line This choice is one of the factors which limits the minimum period that can be obtained for a given bore A design based on operation at 90% could allow some reduction in period or an increase in the bore The justification for operation at 80% is now given The gains from operation at 90% are quantified

  7. Why operate at 80% 2 • Factors defining operating point/margin • Variation in operating temperature • Local variations within the magnet • Global due to operation from a refrigerator at higher To or higher pressure • Variation in Jc superconductor • value ? 1-2% mabye as much as 5% • Variation in Cu:Sc • Figure typically quoted (+/-10%)

  8. Why operate at 80% 3 • Magnet quenching • Enthalpy margin • simplest criterion – energy to raise winding from Top to Tc (critical temperature) • Minimum propagating zone (MPZ) – minimum quench energy (MQE) • Defines the size of normal (non-superconducting) zone which can exist without developing into a magnet quench • Characteristic length L~((2k(Tc-To))/(Jc^2xrho))^0.5 • k=thermal conductivity,Tc= critical temp, To= Op temp,Jc= critical current density, rho =resistivity • For the undulator typically – MPZ length ~ 10mm Energy to Quench ~ 50microjoules • Reliable operation is the balance between energy releases in the winding (wire movement-resin cracks) and stability margin • In the undulator the energy releases will probably be small ( stresses are small) – very difficult to estimate energy release spectrum

  9. Why operate at 80% 4 What does the operating point mean in terms of temperature margin? This is calculated for Prototype 4 operating at 80% at 4.2k It equates to a temperature margin of 1.2K i.e it equivalent to operating at 100% at 5.4K

  10. Why operate at 80% 5 Sensitivity analysis Aim here is to quantify effect of parameter variation on temperature margin and enthalpy margin. Note the enthalpy margin is a relative value Operating point 80% to 90% halves the enthalpy dt 1.2k- 0.6K Variation in Cu:SC @80% dT reduced by 0.2K @90% dT reduced by 0.2K Variation in JC in NbTi @80% dT reduced by 0.4K @90% dT reduced by .5K Variation in operating temp @80% dT reduced by 0.3K @90% dT reduced by 0.3K

  11. Benefit operating at 90% 1 Gains Reduction in magnet period estimated for operation at 90% of short sample rather than 80% ~ 0.25mm Increase in bore ~ 0.5mm Only one of these is available Reduction in manufacturing cost is insignificant

  12. Operating point – conclusion • Magnets should operate in a long string without quenching • Mass production in industry – variations in fabrication quality • Need allowances for • variations in operating temperature (pressure) • variations in wire properties Jc(NbTi) and Cu:Sc ratio • for enthalpy margin/stability • All the effects have been quantified in previous slide • If these effects are assumed to be additive – which they can be – An operating point at 90%of short sample wire performance leaves magnet operation vulnerable to very small variations in fabrication and operating parameters. • Whilst the benefits of increasing the operating point to 90% are marginal • So we consider 80% to be the correct design choice for the undulator

  13. Prototypes programme 1 • Experimental programme at RAL: • To verify modelling and prove technology • Series of five prototypes • Last one has just been tested Final 500mm long prototype-

  14. Prototypes programme 1 • Experimental programme at RAL: • To verify modelling and prove technology

  15. Prototypes programme 2 1st results from prototype V Prototype V details Period : 11.5 mm Magnetic bore: 6.35 mm Configuration: Iron poles and yoke Measured field at 200A (RAL PSU): 0.822 T +/- 0.7 %

  16. Prototypes programme 3 • Prototype V: • Did not go straight to full field before quenching • Magnet warmed between 23-25th to ~150K before testing recommenced • Reason for training is not known may be due to impregnation problem • Quench current 316A • Equates to a field of 1.1T in bore

  17. Prototypes programme 4 • Prototype V: • Achieved a higher critical field than that predicted from manufacturer nominal values • The implication is the wire we are using is at pretty good in terms of super conductor content. • If we assume the upper limit then the observed quench current agrees exactly with the calculated value

  18. Prototypes programme 5 Field is measured at 200A

  19. Conclusions • Experimental programme at RAL: • Modelling of a undulator capable of satisfying the ILC requirements has been completed • The chosen the technology is to use NbTi ribbon operating at 80% of short sample • The testing of the series of five prototypes has been completed • Work on the design and manufacture of a full scale 4m prototypeis now the priority and is well underway.

More Related