Compact and Low Consumption Magnet Design The DESY Experience

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Presentation transcript:

Compact and Low Consumption Magnet Design The DESY Experience Bernward Krause Compact and Low Consumption Magnet Design The DESY Experience CERN, 26.11.2014

Outlook DESY and it‘s accelerators FLASH, PETRA III; accelerator XFEL Influences on electro-magnet design „Combined function“ magnets Example of reducing electricity costs Permanent magnet

DESY‘s accelerators PETRA III: no superconducting magnets, in total ~ 750 magnets FLASH: non-superconducting magnets ~ 180 magnets

The European XFEL Accelerator

Information needed for a magnet design Lattice design of the accelerator defines Magnet types and quantity, iron length, magnetic field quality and magnetic strength Vaccum system defines Magnet aperture (quadrupole and multipole magnets), Gap height and gap width (dipole magnet) Utilities like power supply devices, cooling water and pressure, temperature stabilization defines Magnet coil design

Information needed for a magnet design Beam diagnostics could end up in Special magnet design Tunnel layout and installation defines Magnet weight and geometry Survey and alignment Special equipment added to the magnet (fiducial marks) All these mentioned items have an impact on the magnet design and energy consumption!

„Combined function“ magnets @ DESY The accelerator FLASH and XFEL have no combined function magnets Lack of space in PETRA III for an additional steerer magnet leads to a „combined function“ sextupole magnet. Replacement of the sextupole aluminium coils with copper coils gives enough space for adding an additional coil on each pole. PETRA III sextupole magnet

Simulation with program Opera2d Only sextupole coils on Sextupole and correction coils on

„Combined function“ magnet XBV (for XFEL) Dump layout XFEL BV magnets The BV magnets bend the beam into the dump and two strong quadrupoles (Quads) magnify the beam to allow dump window operation at full beam current. The two quadrupoles are operated at their maximum strength. To obtain reasonable matching of optical functions the BV magnets have to have a slight gradient (machine physicist statement).

„Combined function“ magnet XBV (for XFEL)

„Combined function“ magnet XBV Dipole coils on: B=1.478T Dipole and „quadrupole“ coils on: B=1.478T; G=1.61T/m

„Combined function“ magnet XBV only „quadrupole“ coils on G=1.61T/m

Reducing Electricity Cost: XFEL Beam Switch yard and the septum magnet Kicker Septum

XFEL Septum first ideas in 2007 Efremov Institute, Design Study for XFEL

XFEL Septum first ideas in 2007 High current density in septum blade High power consuption Active parts in beam path Efremov Institute, Design Study for XFEL

Better option for Septum: Lambertson DC Septum B-field inside hole ~2.5 Gauss beam deflection horizontally Nominal current 170 A Current density 3.85 A/mm² Power loss 2.7 kW

Lambertson Septum

A Hybrid Quadrupole for the XFEL undulator intersection Requirements Quadrupole: Gradient between 30 to 100 T/m Length <150 mm; bore hole 15 mm Magnetic axis stability < ± 5 µm

Hybrid Quadrupole with External Adjustment rings* α Quadrupole with shunts and adjusting HMM rods. Rectangular bars from SmCo-alloy are used as PM. Shown maximum flux shunting (=0). *E. Bondarchuk et al. „Hybrid Quadrupole With Variable Gradient and Precise Regulation of the Magnetic Center“, IEEE Transactions on Applied Superconductivity, Vol. 16, No.2, June 2006

Hybrid Quadrupole with External Adjustment Ring max g max max max max Scheme for regulation of the quadrupole magnetic center at Gmax.  - shunt displacement direction at y>0, x=0. Functions G() and () Fine regulation of y() is possible only at small  with the gradient remaining practically unchanged.

Hybrid Quadrupole with Radially Displaced Shunts

Hybrid Quadrupole with Radially Displaced Shunts The aim is to vary the gradient in wide ranges and simultanous to regulate the magnetic center. Solution: the shunt must be sectionalized. Fixed part d1 define the required gradient. Movable part d2 shifts the magnetic center. Detachment force of the whole shunt is ~120 kg Disadvantages: Radiation damage of PM material, Complicated moving devices, Radiation damage of these devices (electronics). Sketch of half of the quadrupole magnet: a0 7.5mm, 1-permanent magnets, 2-fixed part of the shunt (d1), 3-displaceable part of the shunt (d2); H=25mm, h=2mm

The magnet built for the undulator intersection Shift, µm Magnetic requirements for the intersection quadrupole magnet: Gradient 100 T/m (at 140 A) Field quality ΔB/B at radius 3 mm better than 10E-03 (bore 16 mm diameter). Magnetic axis stability at 50% of excitation current for a 10% gradient variation should be less than ± 5 µm.

Summary Up to now no combined function magnets at DESY. Hybrid magnets studied at DESY but not yet manufactured. Magnet design is predominately optimized to reduce manufacturing and running costs. The experiments made demands on the beam quality and saving prospects may play an underpart!

Thank you for your attention