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Design of final-focus magnet for FCCee Pavel Vobly BINP CERN January 2017 Design of final-focus magnets for FCC ee A-A B-B •Transverse section A-A Transverse section A-A Transverse section B-B Design of final-focus magnets for FCC ee Iron Stainless vacuum camber Superconducting coil Nitrogen screen superconducting cable has a rectangular shape in size 1.4 * 0.8 mm Design of final-focus magnets for FCC ee Stainless steel Bandage of superconducting coils Design, of final-focus magnets for FCC ee Superconducting coil Nitrogen screen Distribution of force line Distribution of magnetic induction Design of final-focus magnets for FCC ee gr Relative error of 6th harmonics at the radius of 2 cm is 0.0018 Gradient of 7.5 Kgs/cm at a radius 2 cm Design of final-focus magnets for FCC ee Relative error of 6th harmonics in the radius of 1.2 cm is 0.001 Gradient in lens of 10.5 KgG/cm at radius of 1.2 cm Design of final-focus magnets for FCC E-e Nitrogen screen Stainless steel vacuum chamber Distribution of magnetic lines of force Distribution of magnetic induction in iron Design of final-focus magnets for FCC • 2 cm Gradient 20 Kgs/cm at a radius 1.8 cm Relative error of 6th harmonic at a radius 1.8 cm Maximum magnetic field in area of cuperconducting coil is ~60 kGs Current in superconducting wire is 1.4 Ka.